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Unidentified Aerial Phenomena in the UK
Air Defence Region: Volume 2
Information on Associated Natural &
Man-Made Phenomena
SCIENTIFIC & TECHNICAL MEMORANDUM - No. 55/2/00
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
INFORMATION ON ASSOCIATED NATURAL AND MAN-MADE PHENOMENA
VOLUME 2
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM | 55/2/00
[PHOTOGRAPH - blue image of aerial object dated 19 8 '97]
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
PREFACE
1. This is Volume 2 of a three-volume 'Report on Unidentified Aerial Phenomena (UAP) in the UK Air
Defence Region'. A complete index for all three volumes is at Volume 1. Volume 2 contains working
papers, in no particular priority order, resulting from information collected and conclusions drawn from a
wide variety of phenomena which have been applied to the study of UAP. (R)
2. This wide spread of background information is required in order to understand the relationship
between UAP sightings and their probable explanations. While the majority of UAP reports can easily be
explained as aircraft, satellites, clouds etc., it has been necessary to investigate some phenomenal aspects in
much more detail. A significant, but rare phenomenon, for example, pertaining in the study of alleged
UAP effects on humans, potentially causing them to see (and possibly to hear) exceptional events due to UAP
field effects and the reported degradation of vehicle electrics and electronics, is that no actual UAP electro-
magnetic or other field measurements exist. (R)
3. The aim of the attached papers was to act as a reference source during UAP report analysis,
interpretation and identification. In many cases much more information is available on most of these topics.
That which is included is judged to be sufficient for an understanding in the UAP context. (U)
4. The copyright of reference material used is given wherever this is known. (U)
February 2000 Issued by XX DIS3 not
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
CONTENTS
1 UAP Effects on Humans, Electrical/Electronic Equipments and Objects
2 Ball and Bead Lightning
3 Potential Reasons for Higher Densities of UAP Sightings
4 After Images as a Result of Flashes of Light
5 Detection of UAPs by Radar
6 Exotic Technologies
7 Sightline Rates of Flying Objects & Meteorites
8 Rarity of UAP Sound Reports
9 Black and other Aircraft Programmes as UAP Events
10 Ley Lines, 'EARTH LIGHTS' and UK Earth Fault Lines
11 Collected Imagery and Classification of UAP Shapes
12 Earth's Magnetic Field in the UKADR
13 Visual Meteorological and other Natural Phenomena
14 Meteorological Balloons
15 Air Ships and Hot Air Balloons
16 Sunspot, Aurora and Seismic Correlation
17 Visual Observation of Satellites
18 Projected Shapes/Shadows, Fluorescence & Luminescence
19 Charged Dust Aerosols
20 Optical Mirages
21 Ionospheric Plasma
22 Artefacts
23 Linked Vortex Rings
24 Sprites, Elves and Blue Jets
25 Overview of Magnetic Field Effects on Humans
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 1
UAP EFFECTS ON HUMANS, ELECTRICAL/ELECTRONIC EQUIPMENT AND
OBJECTS
Para. No Page
SENSING THE PRESENCE OF A UAP 1 1-1
Animals 2 1-1
ELECTRO-MAGNETIC FIELD LEVELS 4 1-1
Magnetic Fields (a) 1-1
Electric Fields (b) 1-1
Electromagnetic (EM) Fields (c) 1-2
MAGNETIC FIELD EFFECTS 5 1-2
ANNEXES:
A SOUND
B ODOURS
C TASTE
D EM EFFECTS ON EQUIPMENT & OBJECTS
E DIRECT THERMAL EFFECTS
F NON-IONISING EM EFFECTS ON HUMANS
February 1, 2000 x x x x x x x x x x 5.40
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UAP EFFECTS ON HUMANS, ELECTRICAL/ELECTRONIC EQUIPMENT AND
OBJECTS
SENSING THE PRESENCE OF A UAP
1. The ACCESS Database tables
generated for the UAP study encompass all the
sensing methods and descriptions, of which
humans are capable, except touch. The paper
provides an initial overview. Some of the
topics are considered in further detail in
following working papers. The sensing
methods are:
• Aided or unaided visual sight (including
colours, shapes etc.)
• Sound (Annex A)
• Heat (Annex E)
• Smell (Annex B)
• Feeling (excluding actual touch), for
example sensing air pressure, electrical
fields (static effect on skin/hair, burning
of skin) - Direct Thermal Effects
(Annex D)
• Taste (Annex C)
• Description of the Sighting Location and
Environment
• Non-Ionising Electromagnetic Effects.
(Annex F)
2. Animals Several of the effects are also
found to extend, in various parameters, to other
animals such as farm and domestic animals.
ELECTRO-MAGNETIC FIELD LEVELS
4. On the assumption that some sort of
field emanates from a UAP, though not
necessarily on all occasions, and is apparently
only influential on humans when at close range,
there are three field options, using the most
familiar types of EM considers The following:
(a) Magnetic Fields A magnetic (H) field
can be either natural (e.g. Earth's natural
field), generated, or stored (permanent).
Familiar magnetised materials form permanent
magnetics, while solenoids generate fixed or
varying magnetic fields. In the UAP context
this would either mean the presence of large
(and heavy) field generators on a substantial
and solid 'craft', or a magnetic field being
generated in a UAP comprised of, perhaps, a
plasma which is well-known a magnetic field is
polarised, with lines of force (flux) travelling
towards the opposite polarity either of the
same source or towards the earth's surface. A
magnetic flux can be modulated, although the
rate and shape of the resulting energy time
distribution is affected by the presence of
inductance, capacitance and resistance.
(b) Electric Fields Electric (Electrostatic)
field set up between objects of opposite
electrical potential. Familiar manifestations
of the presence of an E field is hair standing
on end. For an E field to exist a non-
conducting (free space, dielectric/gas) material
must be between the charged entities. In the
UAP context the E field, (for human effect)
would theoretically pass between the UAP
'body' and earth, with the human in between.
The human may be 'earthed' (i.e. standing on
the surface), depending on the scenario.
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(c) Electromagnetic (EM) Fields These are
often described generically as Radio
Frequency (RF) fields as they are widely
used for radio/radar emissions although
the EM spectrum extends over a much
wider range in practice, including IR, UV
and the visible bands. An EM field is
taken to comprise both E and H (Electric
and Magnetic) components, which are
separately detectable and measurable.
Close to their origin (normally known as
the source or transmitter) their relative
amplitudes and phase are usually
complex, but after a short distance the
resultant waveform becomes stable. In
the UAP context the main interest is in
whether a UAP body radiates EM waves,
other than those in the visible part of the
spectrum - which are present anyway, as
the means by which a UAP is most often
seen. The polarisation of an EM field is
defined by the orientation of its E field to
the horizon, but since an EM wavefront
might be rotated, then both elliptical and
circular emissions can occur.
Currently, the field characterisation of a UAP
are unknown but it is a corroborated fact that,
in addition to light (and sometimes heat), some
Sort of field is emanated which has adverse
effects on some people when they are close to
the source. A search was therefore made to
identify possible effects on people exposed to
all three of the main options (a) to (c) above,
both physical and mental. The following
information is included because of its
applicability to the subject, to assist in future
analysis and elimination, and especially
because of the discoveries at Working Paper
No. 25.
Annex D considers EM effects on Equipment
and Objects and Annex F non-ionising effects
on humans.
MAGNETIC FIELD EFFECTS
5. The findings due to purely magnetic
effects are considered to be of prime
importance in the UAP context because of the
response of the human brain and the similarity
to UAP reporting. This has warranted the
separate Working Paper No. 25.
A first general effects summary chart for
electromagnetic (microwave) effects on humans
is at Table F-1.
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ANNEX A
SOUND
1. Sounds which are sometimes reported
accompanying sightings are not unusual in
nature (see para 3, below), and the reasons for
hearing (or not hearing) an airborne object can
be complex. Further, there is wide scope for
mis-reporting of those sounds which are heard.
(Working Paper No. 8 considers this aspect
further.) They range from the violent roar or
even explosion, to the low hum. The more
violent can clearly come from the explosion
which sometimes occurs when a lightning
disappears. However, there are reports that
objects which appear, in general, like small
whistling) or may glow very brightly, can also
cause an explosive (i.e. shock-wave effect) as
they 'leave the ground' or 'take-off' These
events are apparently sometimes accompanied
by the formation of a mist. If the object
changes its temperature or surface pressure,
condensation can occur if the air is moist.
2. If microwave fields are also involved,
the formation of mists may be as the result of
water molecule absorption with the wavelength
forming resonances. (These occur at λ =
0.017m and at four other values when it is an
example where it might be postulated that
several observers were probably exposed to
UAP radiation for longer than normal UAP
sighting periods. This may be other cases
which remain anomalous. It is clear that the
recipients of these effects are in more aware
that they are at right angles to their emission
and transverse direction of the sound and a
wide range of descriptions are therefore used.
3. The most likely reported sounds,
described as 'normal' acoustic, are hums,
humming, buzzing, whistling, beeping or
pulsing, and they are either low or high-
pitched; many may therefore affect areas of
the brain which are in different ways,
depending on the coupling mechanism.
4. Whistling sounds are reported to be
equal or louder than the those of jet aircraft,
even to the point of being heard inside an
aircraft. Changes in pitch have been noted -
not as a familiar Doppler effect, but in cases
suggesting very high nightline (i.e. observer
crossing) rates or abrupt changes of direction.
5. Animals can be 20-30% more
sensitive than humans. Frequent reports
suggest extreme animal reaction to unexplained
sightings. Human audio upper cut-off
frequency is at 20kHz. The cut off, for
example, for cats, is 60kHz and the microwave
density for sound to be induced in cats is about
one quarter of that for humans.
6. It is well established that microwaves
can induce sound, i.e. as well as acoustics.
Experiments show that this is likely to occur at
RFs between 200 and 3000MHz (λ = λ =
0.10m), with power densities of 300m W
cm⁻². Hence PRFs of 50-100Hz can be heard
as humming.
7. An entirely different audio mechanism
can absorb EM energy, which, in turn,
increases temperature, causes expansion and
pressure - which then propagates as vibration
and causes sounds to be heard by the auditory
nerve.
8. Sound effects caused by microwaves
are dependent on head size (and clearly vary
from person to person and antenna type). The
microwave density levels for humans to receive
sound effects is several hundred times the
maximum microwave safety limits. Subjects
receiving these extreme levels often describe
them as producing very highly pitched
whistles.
9. In summary, there are two mechanisms
which can produce sounds which humans have
described when in close proximity to
unexplained phenomena. For weak intensities
and for low frequency those RFs, a modulation
range is the normal human reception
mechanism. Even when no UAP source is
present, if the mechanism of tissue vibration is
caused, then the acute heard is described as
'feeling unwell'. In particular, operating at
450 and 1750MHz, and the new RF for
mobiles in 1760MHz. Of course any pursuit
of this hypothesis must include rigorous
investigation of the positions if it turns out
that UAP radiation is
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ANNEX B
ODOURS
1. Some cases have occurred where
peculiar odours have been reported. These
seem to be produced by microwaves or high
energy electrical fields.
2. These effects are well understood and
can be replicated in the laboratory. Normally
the smell is described as 'sulphurous',
'electrical burning' or ozone-like.
3. During electrical discharges in the
atmosphere many electrical compounds are
formed. Nitric oxide, for example, reacts with
other atmospheric gases to form nitro-benzene,
which smells like bitter almonds.
4. The slow decay of activated nitrogen
can exhibit a white glow and may be the reason
for white trails (or 'tails') sometimes described
by witnesses, whether or not the witness has
smelled the chemical reaction.
5. Reports have been received where a
'strange odour' hangs in the air for some time
after an event.
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ANNEX C
TASTE
1. This effect is usually described as the
taste one can experience when placing a low
voltage (e.g. dry battery) electrode on the
tongue. It is often described as 'metallic' and
'tingling'. The effect is created, for example if
dissimilar metals are placed on the tongue,
creating a battery, with an extremely low (µA)
current flow. However, the presence of 'taste'
in the vicinity of UAPs occurs without touch.
2. The taste is immediate but the decay
much longer. It is reported that this effect can
occur by pulsing and by alternating currents up
to ~1000Hz. The effect is attributed to the
breakdown of the chemicals in saliva. Since
the human body is conductive, it is believed
that bursts of EM energy could cause the
'taste' effect. Estimates are that a current of
>100µA (DC or AC) is required. Less than
1% of a 300+ sample of humans could 'taste'
the presence of microwave energy. This may
well be modified by the presence/absence of
metallic tooth fillings.
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ANNEX D
EFFECTS ON EQUIPMENT AND OBJECTS
1. The reported effects, which seem to be
due to electrical charges, magnetic and
microwave energy are known to have caused:
• Overheating of car batteries.
• Metallic objects rising in temperature.
• Magnetisation, which is sometimes
retained.
MAGNETIC EFFECTS
2. Objects close to reported UAP
sightings have been subject to:
• Permanent magnetism (fences, flag
poles). This seems to imply DC or very
slowly varying magnetic fields.
• Radio interference. Radios can appear to
off-tune (or go off their stations, since,
presumably, they move to a non-
receiving wavelength). This is possibly
due to the magnetisation of the ferrites
used as the antenna cores (i.e. part of the
tuning loop) as in modern
communications/radio receivers.
• Interference with magnetic compasses.
3. In the latter case compass rotation
rates have been noted. The effect (and speed)
can be replicated by exposing the compass to
an appropriate pulsed or varying magnetic
field.
4. France is known to have measured
magnetic field strengths in the vicinity of
sightings as early as the 1970s when an
extensive field measurement system (network of
sensors) was set up for nuclear effects and the
earth's geomagnetic field. Measurements to 1
part in 1000 established the change in field (in
the presence of a UAP) and extraordinarily-
high magnetic fields were sensed. When this
level was translated (i.e. scaled) to a reported
distance of a few hundred metres between
UAPs and radio receivers, from other reports
elsewhere, the magnetic flux was consistent
with the levels needed to cause the radio
receiver effects reported.
5. High frequency magnetic fields,
presumably from nearby UAPs, are reported as
causing battery acid heating (conducting
medium), and other conductors to warm-up,
while non-conductors, e.g. rubbers, plastics
have reportedly remained cold to the touch.
6. French reports suggest that the slowly
varying magnetic fields suspected do not
appear to noticeably cause any body-currents in
humans. The effects of EM fields on humans is
covered at Annex F.
7. A report from Finland in 1977, which
involved 170 troops on the Finnish border
reported all equipment 'jammed' and no
telephones.
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ANNEX E
DIRECT THERMAL EFFECTS
1. Short-range observations, in almost
every reported instance, have been
accompanied by a sensation of heat, ranging
from mild warmth to severe burning. Normally
(but not exclusively) these appear to be line-of-
sight effects.
2. If an object is surrounded by a plasma
(usually described as 'a glow'), it can radiate
broad-band energy well beyond the visible
spectrum. If an object is without plasma (i.e.
seen to have a 'metal' surface), it can radiate
IR radiation from any gases or body heat which
may be present, or energy at UV wavelengths.
3. Reports of 'sunburn', severe sunburn,
and even eye-pain and loss of vision have been
reported. In one event the witness, a
policeman, suffered severe arm-burns through a
long-sleeved uniform. But his body was
otherwise protected by the car door, behind
which he was standing.
4. All indications are that the phenomena
at paragraph 3 above could not be IR or UV
but must have been microwave penetration at
very (ultra) high frequency(s), where even for
humans 'skin effect' (i.e. surface rather than
absorption microwave heating) can occur.
5. In the 1950s several reports were
received (France and South America) of
combined vehicle failure and mild shocks or
'tingling' in proximity to 'hovering' objects.
6. At the time of vehicle failure several
reports (Canada) have resulted in apparent
temporary paralysis of humans until the nearby
object moved away. It is possible that some
muscular control (motor-control) nerves can be
affected by electrical potential. This can be
replicated by medical scientists. One
explanation is that either constant or pulsed
microwave, coupling into the nervous systems,
may cause this affect. Pulsed interference with
the human system is possible because of the
500 milliseconds muscle relaxation delay.
7. At least one fatal incident is reported,
following what was believed to be radiation-
induced from one or more energy levels,
including the possibility of x-rays, or protons.
Effects, ranging from minor skin burns (i.e.
sunburn - like) to the level of blisters have also
been reported (USA).
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ANNEX F
NON-IONISING EM EFFECTS ON HUMANS Para. No
EM FIELD FROM A PLASMA 1
Near Fields 2
UAP Near Fields 3
Variation with RF 7
Athermal Effects 8
Modulations 10
Near Field Coupling 11
Radiation Pattern 12
POTENTIAL NEUROLOGICAL EFFECTS 13
APPLICABILITY TO UAP EVENTS 18
SUMMARY 20
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ANNEX F
NON-IONISING EM EFFECTS ON HUMANS
EM FIELD FROM A PLASMA
1. The EM field from a radiating plasma
is assumed to be present in three forms:
- The Radiation field which diminishes with
range at 1/r
- Induction components which diminish at
1/r²
- A Quasi-Static field which reduces at 1/r³
2. Near Fields The quasi and static-fields
are near field components, only of
significance close to the source (i.e. the
UAP). They are of particular interest in the
study of those UAPs which might be caused
by plasmas or electromagnetic discharges.
Assuming that the dimension D (effective
linear 'aperture') of the plasma is large
compared with the wavelength (λ), then the
near field is taken to extend to a distance
2D²/λ from the source. The Radiation Field
(far-field) is not of interest in this study. In
the normal case of an EM source (for
example, antenna emission) the radiation field
high beyond the near field stabilises with
spatially uniform distributions of the E and
H field components, which are at right angles
to each other and to the direction of
propagation, they are in phase and have a
constant amplitude (for a given direction).
This is sufficient, for example, for radar
calculations. For the near-field there is an
arbitrary phase and amplitude relationship
between the E and H which makes
calculations more complex. To simplify
calculations for the near-field a 'plane-wave
equivalent' value is sometimes used. If the
E field or H fields are known, power density
is evaluated from them using S=EH/Z₀,
where Z₀ is the familiar characteristic wave
impedance of free space 377Ω.
5. It is not clear whether single, multiple
or broad-based radiation frequencies are
emitted from the airborne sources of interest
(UAPs). Unfortunately, the nearest data are
the magnetic field strength measurements
taken, the majority of UAP events only being
present for a few seconds.
6. Standard radiation hazard calculations
assume that at MF/HF the frequencies are
below whole body resonant frequencies and
direct hazard effects can be high. Most of
the work considering health effects from RF
frequencies and direct hazard effects can be
high. The maximum amount the body
absorbs (SAR rate) as between objects of
body-length and the free-space wavelength of
0.4 (for the human object) is significant.
The SAR maximum therefore occurs at
~80MHz (λ = 3.75m), varies with adults and
children and is dependent on whether the
subject is in contact with a conductive ground
or in free space.
7. Variation with RF Below an RF of
~30kHz, thermal and stimulation effects are
negligible in comparison to stimulation
effects and charging of bone and tissue cells.
In the RF range from ~100kHz to 1MHz, the
thermal and stimulation effects are of the
same order (Figure F-1). In the RF range
from ~1MHz the combined experimental
results for RFs up to 100MHz confirm the
power density values which are known not to
affect the human brain. In the above part of
the near-field power density values are not
known. There are, however, some known at
350 and 915MHz; and the new RF for
mobiles in 1760MHz. Of course any pursuit
of this
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from UAPs the following zones on the shaded
diagram are of interest. Lines A and B
(Figure F-1(d) & (e)) are the amplitudes of
biological densities occurring in humans. The
information at Figure F-1 is converted into
incident E and H fields [ILLEGIBLE] with
the shaded diagram are of interest.
8. The source of these values recognises
that the maximum current densities in the
brain of approximately 1mA/m² are in error
by up to an order. Hence, they can only be
treated with caution. In general, the values
are: no biophysical action model and the
recipient to whom it is entrusted in
confidence, to anyone.
9. Athermal Effects Very little agreed
scientific knowledge exists about athermal
effects other than stimulating effects.
Locational absorption of an EM field is
defined by the frequency [ILLEGIBLE]
annex D considers EM effects on Equipment
and Objects and Annex F non-ionising effects
on humans.
10. Modulations No firm conclusions on
humans are also concerned with any
modulation which may be present and this
clearly affects the total time-energy (signal)
received. Note the caution: 'Very few
persons with spatially non-uniform fields of
both salient and transverse directions of
propagation, they are in phase and have a
constant amplitude for sound and a wide
range of descriptions are therefore used.
11. Near-Field Coupling Due to
complicated, near-field structures, with
different phase-difference between the E and
H fields, a consideration of source variation
can lead to complete absorption. Very few
in-version (coupling) have been reported.
Only take place when its orientation
(polarization characteristic) is identical to
the incident wave phase at that point. It is in
that it might be possible for a human to be
close to a UAP radiation, in that within its
near-field while little effect, while a short
distance away the coupling would be such to
cause another human to receive stimulation
resulting in quite different descriptions of
what is being seen. It is suggested that very
low levels of radiation in the near-field (and
possibly below containing relaxation
responses) of a UAP, where it is the nearby
human brain may couple and result in the
near-field. There is also some evidence that
some humans are more susceptible than others
to the fact that often the same person
repeatedly 'observes' UAP events while
others do not.
12. Radiation Pattern Although it may be
assumed the (idealised) shape of the
radiating UAP is spherical and that its
radiation pattern is uniformly omni-directional,
in relation to humans this is not necessarily
the case. Frequent reports suggest that the
(consumed plasmas) take up a variety of shapes
and have 'hot spots' which are visible;
Conventional logic is that the inhomogeneity
and shape variation will lead to a non-uniform
radiation distribution. Hence, there may
well be hot spots of radiation
emanating along some axis - which the close
observer may, or may not, be exposed to.
Further, the objects of interest are often
observed/approached by specific observers in
cars which will provide some screening. On
other occasions the screening is supplied
because some witnesses are in aircraft. There
are cases where people have left their cars and
suffered both immediate and after-effects.
* 'RF Hazards Exposure Limits' European Union
Geneva 1995 Título 3278-E
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POTENTIAL MENTAL EFFECTS ON
HUMANS
13. Neurological rather than biological
effects may be the clue to some human
behaviour after exposure to the near field of
a UAP radiation. Particularly sensitive are
the temporal lobe areas of the brain. Unlike
other parts of the brain, the temporal cortex
is dealing (in the processing between RF
fields and brain activity was confirmed by the
confirmed in the 1980s. In fact for 20 years
or so much of the work has been done on the
one hand to protect humans against RF
hazards and secondly to understand the
viability of microwave weapons. The amount
of scientific papers on human interaction with
RF fields in predigious (over 16,000 research
papers) have been taken using devices which
radiate at most RFs, including ELF (e.g.
50Hz, 50Hz) Much of the work is done on
the broad-band requirements of brain activity
mentioned above and the necessity to
understand hazards from, modules, in one
event from RF broadcast stations etc. In the
UAP context, that maximum absorption (and
logically the source of the brain fields in the
near-field environment) is based upon the
experimental studies of close encounters.
This is of significance in the analysis of
whether a UAP body radiates EM waves, and
the validity of the electromagnetic
measurements taken, the majority of UAP
events only being present for a few seconds.
14. An important flaw is that the reported
effect of (presumed) UAP radiations on
humans is complicated, near-field structures
with important phase-difference between the
E and H fields, a consideration source
variation can lead to complete absorption.
Very few in-version have been reported.
Only take place when its orientation
(polarization characteristic) is identical to
the incident wave phase at that point. It is in
unaware that EM radiation as we currently
understand it.
18. For experimental purposes RF energy
has been launched using resonant dipole
antennas in both E and H orientations! The
amount absorbed was greatest at lower RFs
(longer wavelengths) and at E field
orientations. It is recognised [for the 16,000
research papers] that maximum absorption
and for low frequency brain's response to
close encounters) the UAP Study of Effects)
that maximum absorption (and logically the
source of the brain fields in the near-field
environment) is, whether it be the E, H or
both, is the forward-facing, head absorption
at a more fundamental level. It is of
significance, in the analysis and
interpretation, since such close encounters
(at para. 3 above) in the UAP context, that
maximum absorption (and logically the
source of the plasma) is at or just below the
wavelength, focussing is in the head and it
must be considered that such focusing could
also mean that it may be some focusing
effects or even the occurrence of several
interacting frequencies from a UAP which
cause the reported effects.
F-4
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other than EM radiation as we currently
understand it.
18. For experimental purposes RF energy
has been launched using resonant dipole
antennas in both E and H orientations! The
amount absorbed was greatest at lower RFs
(longer wavelengths) and at E field
orientations. It is recognised [for the 16,000
research papers] that maximum absorption
for the broad-band requirements of the UAP
Study of Effects) that maximum absorption
(and logically the source) in the case of the
forward-facing, head absorption at a more
fundamental level. It is of significance in
the analysis and interpretation, since such
close encounters (at para. 3 above) in the
UAP context, that maximum absorption (and
logically the source of the plasma) is at or
just below the wavelength, focussing is in
the head and it must be considered that such
focusing could also mean that it may be some
focusing effects or even the occurrence of
several interacting frequencies from a UAP
which cause the reported effects.
19. A wealth of other international
experimental measurements (in 16,000
research papers) have been taken using
devices which radiate at most RFs, including
ELF (e.g. 50Hz, 50Hz). Much of the work
is done on the broad-band requirements of
brain activity mentioned above and the
necessity to understand hazards from,
modules, in one event from RF broadcast
stations etc. In the UAP context, that
maximum absorption (and logically the
source of the brain fields in the near-field
environment) is based upon the experimental
studies of close encounters. This is of
significance in the analysis of whether a UAP
body radiates EM waves, and the validity of
the electromagnetic measurements taken, the
majority of UAP events only being present
for a few seconds.
* ² RF Energy, Deposition in a Homogeneous
Model of Man: Near Field Exposure, M.A.
Stuchly et al. IEEE Trans. Biomed. Eng. Dec 1983
SUMMARY
20. Because few persons are exposed to the
postulated UAP radiation, the following
points are pertinent:
- There is no history of after-effects of
UAP exposure reported beyond 'feeling
unwell for a few hours'.
- Unlike other EM radiation sources no
cumulative effects of exposure are
reported or studied.
- It is not certain that the radiation/fields
are conventional and electromagnetic in
nature.
- No other known (even repeated)
exposures to EM radiation (with
conventional modulations) causes the
'close in time' syndrome reported by
many (close encounter) witnesses world-
wide.
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Table F-1 HUMAN EFFECTS THRESHOLD (U)
Microwave Maximum Radio PRF (Hz) Pulse
Threshold Frequency Duration
(mW cm⁻²) (MHz) (µsec)
Heard as: Shockwaves YES * >60,000 - *
Low Pitch YES 12 200-3000 30-100 1-100
High Pitch YES ~2000 Any Any Any
Smell YES * Any [3] Any
Taste[4] YES <13.1 Any <1000 Any
Felt as: Heat[4] YES >8.4 30,000 Any Any
Shock[2] YES * Any Any Any
Burns YES * 30,000 Any Any
Internal Burns YES * <3,000 Any Any
Paralysis YES * <3,000[5] >500 Any
Notes
[1] Reportedly enhanced if >500Hz
[2] Electrical shock
[3] Reportedly enhances smell
[4] >100µ Amp
[5] Added to those microwave heating effects can be the effects of IR
F-6
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Am) {f(MHz)}!"!
Object (UAP)'"! 100{3} 10{30} 1 {300} 0.10{3.000} 0.01 {30,000}
Diameter (m
pe [ee fee [ef | |
ps0 ew fe [wo we fe
Se
@ [Te [ee [we [we [me | vo _|
TABLE F-2: NEAR FIELD DISTANCES|3] (m)
Notes: [I] Assumes that UAP is a radiation plasma or charged mass source with
effective aperture shown. The recorded appearance of plasma balls
exceptionally reaches the largest value shown. However. this should not be
confused with the large triangles. rectangles and other large shapes reported.
These possibly have radiating peaks (c.g. at the "corners" but, as they do not
appear to be (visually) homogencous sccm unlikely to represent a total
radiation aperture
[2] It is not known whether UAPs radiate narrow or wide-band RFs
[3] The standard near-field criteria is used (2D*/2)
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SAR nt/ng/nWiew-2) SAR (ang)
Notes F-I(a) RF 3MHz fs
Figure F-1(b) RF 350MHz Far Field (ImW.cm')
Figure F-1(c) RF 350MHz Near Field for same far field
Figure F-1(d) RF 915MHz Far Field
Figure F-1(¢) RF915MHz Near Field
FIGURE F-1: DISTRIBUTION OF ABSORBED RADIATION
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Frequency
* Notes 1 The longitudinal axis of the man is parallel to the orientation of the field
2 Numerical RMS values apply to the undisturbed field.
c In other parts of the body (e.g. wrists or ankles), depending on the exposure
conditions, current-density values up to tenfold greater are possible
2 For curves A, B and C, see the notes given in Figure F-3
FIGURE F-2: ELECTRIC FIELD-STRENGTHS WHICH INDUCE APPROXIMATELY
THE INDICATED CURRENT DENSITIES IN THE HEAD AND IN THE CARDIAC
REGION OF A MAN
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ab
—— a
10
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is 8
1 ,
ie] [A
4
A
O41
1 10 10% 1 104 108 Hz
Frequency
Key: a}, @ Stimulation of sensory receptors immediately underneath surtace electrodes (Geddes et al., 1969).
b;—bs Ventricular fibrillation thresholds for stimulation times of 1 sec or longer ( by: Imich et al., 1974;
be: Roy et al., 1976; bs: Jacobsen et al., 1974; by: Osypka, 1963; bs: Watson et al., 1973).
D "Envelope® threshold curve for extrasystole elicitation and ventricullar fibrillation; stimulation, 1 sec
of longer (injury threshold),
Cy, Cg Extra-cellular stimulation thresholds of single ceils (c,: Roberts and Smith, 1973; cg: Ranck, 1975).
d Frequency dependence of stimulation thresholds for nerve/muscie systems (modified from
Schaeter, 1940). This curve may be used as a lower "envelope" curve for excitation thresholds for &
single unidirectonal pulses or pulse sequences.
1 Threshold for modulation among different neurons (Chan and Nicholson, 1986).
Ie Modulation of neuronal excitability in rat hippocampal slices (Bawin et al., 1984). *
c "Envelope" threshold value curve for stimulating effects (possibly hazardous).
h,i.j.8 Calculated current densities for the threshold values of electrophosphenes (h: Adnan, 1977)
magnetophosphenes (calculated current densities; i;: Silny, 1981; ip and is: Bernhardt, 1985)
and variations of optically-generated reaction potentials (j: Silny, 1981). B shows the range
over which biological effects are expected and observed.
A Average value of naturally-flowing current density in the tissue; the values of the current
Conanloe dus ts tre ciesbeal SOMET iva bests ov rs Recah ove cone macs Innouret a
macroscopic level. Below this current density, absence of detectable effects is assumed.
1Wikg = The current density range above which additional thermal effects have to be considered.
FIGURE F-3: THRESHOLD VALUES OF ELECTRIC CURRENT DENSITY FOR
DIFFERENT BIOLOGICAL EFFECTS
F-10
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135 ue O.1mAlem?
104 Bs *. ., 102
0.1Alem? res
10-5
10° 10° 10? 108 104 108 108 MHz
Frequency
Key: i Threshold values for magnetophosphenes; the upper curve corresponds to magnetic 4
fields where phosphenes were observed as pattems.
*. | Changes in visually-produced potentials (from Silney, 1981).
0, Experimental values for cardiac stimulations, calculated for humans from experiments
conducted on animals (from Siiney, 1986).
For curves A, B, C and D, see the notes given in Fig. 16.
Notes: 1. The magnetic field is varying sinusoidally.
. Due conductivities and current at a local level, induced body-current densities may
FIGURE F-4: MAGNETIC FLUX DENSITIES WHICH INDUCE APPROXIMATELY THE
INDICATED CURRENT DENSITIES IN THE BRAIN AND THE HEART OF A MAN
F-11
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 2
BALL AND BEAD LIGHTNING
Para. Page
INTRODUCTION 1 2-2
Ball Lightning 2 2-1
Bead Lightning 3 2-2
€ SHAPES, SIZES AND STRUCTURES 7 22
MOTION 10 23
Velocity rT 2-3
SOUNDS 12 2-3
DURATION 13 2-4
RADIATION-HEAT AND LIGHT 14 2-4
Light 15 2-4
Heat 16 2-4
EM Radiation 17 2-4
é ODOURS 19 25: 7
EFFECTS ON HUMANS 20 : 2-5
EFFECTS ON ENVIRONMENT 21 2-5
EFFECTS ON EQUIPMENT 22 2-5
SUPPORTING THEORIES 23 2-6
LABORATORY PRODUCED BALL LIGHTNING 31 2-7
PLASMOID 38 28
February 1, 2000 XXXXXXXXxXxX 5.40
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Para. Page
AURORAL LOOPS 39 2-8
Ball Light Ozone Spheres 39 2-8
Power Intensive Plasma Formations 40 2-8
(PPFs)
BALL LIGHTNING AND AIRCRAFT 41 2-8
PLASMA SHAPE CHANGES AND SIZE 46 2-10
SURVEY OF COLOURS 47 2-10
OPTICAL 'THICKNESS' OF BLACK RADIATORS 48 2-11
THERMO-CHEMICAL REFRIGERATION 49 2-11 &
SUMMARY OF BALL LIGHTNING 50 2-11
CHARACTERISTICS
Near-Terrestrial Events $1 2-11
In-Structure Phenomena $2 2-12
Demise 53 2-12
SUMMARY - RELEVANCE OF BALL & BEAD 54 2-12
LIGHTNING TO UAP REPORTS
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THE CHARACTERISTICS OF BALL AND BEAD LIGHTNING
INTRODUCTION
i A review of the nature of Ball and link. Either lifetime (duration) is explained and
Bead Lightning has been made, because of the stability not, or for example, colour does not
possibility of this being reported: match expected temperatures. For other
theories, for example the vortex explanation,
- Asa visual unexplained UAP sighting - does not explain electrical properties. Apart
since this phenomena can exist up to two from Ball Lightning and Earth Lights, many
* hours after a storm and the luminous such occurrences are known simply as
globe can be retained on the human eye 'atmospheric spherical formations'. While the
(as an after image on the retina) and probability of the occurrence of ball lightning
reported as an object. somewhere on earth has been calculated as
between 10° and 10° per square kilometre per
- As a potential UAP phenomena which minute (equating to about 100 to 1000 balls
can occur in all weather situations - even world-wide per hour); it can only be seen at
in a clear sky. close range and many events must be
unrecorded. Some, of course, are black, others
- The sounds and colours which can be translucent, both have weak thermal radiation.
produced by ball lightning are frequently Reportedly bright spots or 'beams of light' are
similar to those which appear on UK likely to occur when the phenomenon
UAP reports. approaches a conducting object. (Comment:
Lightning, as a topic, has only been seriously often by car owners who report supposed
(scientifically) investigated for the last 200-300 'extra terrestrial' objects with illuminated
years. Reports go back to at least "Globes 'portholes']. The 'beams' often converge
Igneous', (St. Gregory of Tours 6th Century unlike, for example, searchlights and this
* AD), Aristotle 4th Century BC and others in appears to be due to lens effects caused by the
the First Century BC. On occasions the Ball high electric field intensity of the surface, or
variety of lightning is known as a 'solid' or 'shell' of the ball (or other shape seen)
simply 'fireball'. The phenomenon of Ball
Lightning is assessed to involve the disciplines 2. Ball Lightning A study of Ball
of chemistry, meteorology, _ physics, Lightning can be classified under the following
optical and various electrical models and
ee ee pend - Conditions and locations for occurrence.
ly investigated here to a to show
waiduay of damian Cee oa ca ~ Shapes, sizes and structures
identification of many UAP events as ball - Motion (Velocity and Trajectory)
lightning or its similar relation phenomenon wo
"Earth Lights'. Of the numerous explanations
there is generally at least one important aspect - Duration
that is not totally fulfilled and a variety of sd :
theories are put forward to explain the missing ~ Retsin Gitlin
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- Effect on Humans - Enmitted from a 'bend' in conventional
a lightning
- Effect on the Environment
- Effect on Equipment - Drop from clouds (initially)
- Odours On occasions ball lightning has no apparent
- Electrical/Chemical theory ee
Ball Lightning variety =
Sahining decays ina variety of ways- $8 = 4 Bead Lightning Bead lightning (5-
. ; 15%) is much less prevalent than ball lightning
3, Ball Lightning is believed to be formed (85-95%) and is the residue of cloud-to-cloud
from an 'ordinary' flash of lightning - for or cloud to surface lightning strokes where a
hich the flianiliar 'slectsicalistocmes are a row of balls are seen separated by darker
generator. However, it can also occur without regions in a string-like form. Bead lightning is
generally observed at a distance, in contrast to
the presence of a storm or of >
visible/conventional lightning. Apart from ball lightning which is observed nearby. As for
9s 3 ' ' ball lightning, the incidence of the occurrence
these conditions, once present, the 'balls' or n naa
« , of bead lightning is quite low. One survey
beads' can last for a few seconds up to s
: aPieke found only 1600 reports between 1850 and
minutes. Ball lightning can enter rooms PES tie :
, 1978! Bead lightning is also sometimes called
(usually through apertures (e.g. chimneys, - 2 a PHB RR
ind : pearl' lightning. Some 'strings' have been
¥ D 08 aap eae have bye reported as i-sinusoidal in form, while
elongation of the beads (or balls) suggests
space. Instances have been reported where ball sausage or cigar-shapes [often a feature of
lightning has entered aircraft (BOAC 1938 and UAP reports]
TWA 1948 Easter Airlines 1963, USAF KC- precaes
all reports identified as ball lightning occur in occur at low altitude - most probably because
the summer months. 95% are reported in the that is the location of most observers; hence
hours 1300-2359 hours and mostly clustered in this limitation may not be true in practice (see
the period 1600-2000 hours . It has even been para. 22 below). Insufficient evidence exists to
oe 5 ee be certain of all the conditions for ball and bead
reported in the vicinity marshes, volcanoes lightning formation. No single theory appears
ne) a ee to satisfy all the criteria. The ball is sometimes
balls/globes appear in rain, in clear skies, in seen with a halo
still conditions or wind, move against the wind, &
can be vortex associated, in snow, near the 6 Ball lightning is sometimes mistakenly
ground and at altitude. Undoubtedly the largest reported as St. Elmo's fire
occurrence is during storms/cyclonic
conditions. Conditions for ball lightning SHAPES, SIZES AND STRUCTURES
formation appear to be:
: On some occasions bead lightning,
- Charge particle connected often described as a 'string of sausages' (i.e.
: ; elongated beads), converts or "breaks off into
- Frictional action of dust (hence Volcanic a single glowing ball as the pinching effect
links) which separates the components disappears,
- Dependent on the presence of very high leaving a single glowing ball (or balls). Shapes
electrical charges and fields are invariably described as globes. Sometimes
flames seem to be revolving inside the globe
- Possibly dependent on the formation of On rare occasions, two balls have been
natural EM radiation reported linked together (a metre or two apart),
while on others oval, or pear-shaped forms are
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'rod-shaped' systems have been seen, and also - Very rapidly point to point (jumping or
'hollow' spheres. darting)
. . - Attracted to enclosures (e.g. indoors/in
8 Ball dimension reported vary from a
few centimetres to 12-15m in diameter. Some vehicles/aircraft)
examples had ball diameters of 22cm (inside - Rolling (on earth's surface, wet or dry)
eastern Airlines Aircraft, 30cm, 50cm, 60cm, E
8.5m, 12.8m, and a 38cm (rod). A summary of 7 w from Lake
the scientific factors which control plasma - Tuming sharply/abruptly
sizing is at paragraph 30, below. Optical . bol
illusion effects can clearly change the ea ia % En
perception of size. It is important to note that - Spinning or spiralling
an increase of light intensity can be perceived - Floating
as an increase/change in size or shape. The
balls are sometimes hazy in outline and may - Motionless/hovering
not be truly spherical (when not one of the - Divine (thi
pole iving (at high om )
x - Apparently moving at windspeed
9. Within the bounds of the shapes, me s (to a few metres in height)
described above, there appear to be three — ne
structural types: - Darting to a conductor (especially water,
fences etc.)
(a) Balls with a solid appearance with a ome * to an object) or 'pushing' at
dull or reflecting surface, or with a maa ao
solid core in a translucent envelope
(often 30-30cm in diameter). : a a (and floating away from an
, object
(b) A rotating structure.
; - In complex trajectory (20% of reports)
(c) A buming appearance (often <40cm
diameter). - Vortex-associated
Reports suggest that single balls can break up - Float ('squeeze') through a small hole
into smaller ones (or disperse - see para. 12 and then expand to a large ball-shape.
below). 11. Velocity Secondly the ball lightning
often has velocity in one or more of the
* MOTION following categories.
10. The motion attributes reported are, - Often low velocity (including zero)
is reported as moving in one or more of the - Estimated 100-1200ms
following directions or types of movement: Frequently the speed is reported (when near the
ground) as that of a man walking or running.
- Cloud-to-cloud The spiral or rotational form, which is often
- Earth-to-cloud vortex-associated, appears to take the form of a
— hydrodynamic or plasma vortex.
- Ina horizontal path (55% of occasions SOUNDS
and usually of the 'burning'
' eo ype) 12. Many sightings have been made when
~ _ Climbing and bouncing/rebounding the ball makes no sound, while others have:
- Changing course
; - Hissed (hence confusion with St. Elmo's
- Movement opposite to wind direction fire)
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- Exploded (after which they disappear colour change. Some structures seem to favour
either with a pop, a mild bang or a certain colours. The main attributes are
significant explosion)
- Possibly imploded - Rod structures are often purple/violet
. ' s - Solid types (see para. 9) often appear as
Buzzed or "fluttered green/violet
~ Sparked (when colliding with foliage, - Rotating types can have a combination of
objects)
colours
+ Coctied - Buming types are mostly red or
—— sounds occur quite a from red/yellow in appearance
1 OF precipitation - in may be .
no storm present. Termination often occurs pence Meg tS = Gund' @
after a colour change (see para. 15 below). P :
Sometimes a residue is left after an explosion - Hovering or horizontal motion types are
(no further information). often red or red/yellow
DURATION - Predominantly red if "floating" ad
- Blue or blue/white occurs on only 5% of
13, The duration of ball lightening varies reports
from a few seconds to several minutes. - Red or yellow types occur on 60% of
However, most seem to last for up to five reports, imes reported as being in a
seconds, with the longest on record as 15 bluish envelope
minutes.
- Less than 1% change colour
RADIATION - HEAT AND LIGHT =", Ck aed anata tirana ce ties
14, Almost all ball lightning reports are - Can leave behind smoke-colour trial
views is eyierwlipers: 4 oe jenn - Emit, on occasions, bright flashes
the observers recall the added features of sound - Reported blue or white 'hollow'
(paragraph 12, above) and any damage caused, - Leave behind a mist (seen as direct light)
which is dealt with below at paras 20 to 22 or blue or white (in reflected light) in
15. Light Attention is drawn to the re
phenomena visually, and although there are - Smelly types leave behind a brown mist ¥
pick ae sightings fall into the - Colours may be pulsating
16. Heat Reports both of intense heat and
- Blue or blue/green of no apparent heat can be found. The
- Red (or pink/rose-pink) sttributes reported are
- Red changing to white - Apparent colour on the surface and a hot
- Violet changing to white or
- Yellow - "Ball fell into water tank and boiled the
- Yellow changing to white ened
- White to red (0 P nals ae - Absence of heat, despite intense light
occasion for 65 seconds) - ~1% (of those closer than 15m) were
Most sightings fall in the red or red/yellow ee
category. They often disappear noisily after a
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- Temperature emitted burns humans (see - Humans burned on hands, feet and arms
paragraph 20, below). etc (This seems to be
17. EM Radiation An intense E field, set ye "peer a as sometimes
up during st Gickd cal Gl } no heat is repo!
protrusions. This is thought to account for the - Startling and fight (specially with
attraction (often erratic darting movements) of noisy/explosive types of ball-lightning).
globes/balls to sharp edges, pylons, fence etc. Some effects of fright are reported in
The presence of these fields causes sparking, animals. Hairs bristle, dogs/cats cower,
incandescent traces (and radio farm animals stampede in fields
interference/static). The electrical potential is e
quoted as 3-400kVm'. Pyrotechnic Hiamens knocked over.
'streamers', like a fireworks 'burst', Potential electromagnetic mental effects on
accompany the high potentials. EM radiation humans, separate from these other, more
(E plus H fields) are present, but little magnetic tangible physical effects, are considered at
(H_ field) measurement has been made. Working Paper No. | Annex F.
Radiation (measured as RF) in storms can be at
6kHz to 450MHz. When lightning is present EFFECTS ON ENVIRONMENT
@ _the radiation is very wideband 100Hz-
4000MHz, vertically polarised. The power 21 The following effects have been
present is reported to fall off as 1/f*. The logic Teported:
for the radiation is considered at paragraph 23,
below - Holes in the ground (reportedly up to lm
in diameter and over 1m deep)
18 There is no indication of gamma - Furrows in the earth
radiation from either ball or bead lightning.
- Trees uprooted
ODOURS - Granite boulders broken/cracked
19, Odours are frequently present. Most - Water boiled (see 'heat' above (para. 16)
are reported as: and discussion at para. 26 below)
- Electrically-excited —_ atomic/molecular
~ Sharp species, causing single and multiple
- Repugnant atmospheric discharges and micro-
ew lai biloba
- arti
— wee atmospheric dust particles
- Nitric oxide/dioxide : a ce iced ore ee
- Bio-luminescence chemi
- Methane luminescence/due to chemical reactions
- Buming. (not due to thermal sources)
It is known that an increased nitrogen level - Production of visible light at room
persists for long periods after passage of a temperatures (and at other temperatures)
lightning ball. - Atmospheric trails/traces (usually
terminating at the ball, or persisting
Se afterwards). Pyrotechnic in appearance.
20. Serious burns and other effects are MENTS
reported. [It is of particular interest that many SEFECTS ON EQUIP
Of these ave similar to Gees Seppe Sy UAP n Apart from the reported 'static' on
observers}: receiving equipment (see also EM Radiation
(para. 17 above), example effects are
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- Attachment to power lines/electrical - If the body is hot, why does it not rise?
oa (but 10 effect on the system - What constraints could be keeping it at
F level altitude (floating type)
. — of various diameters into - Is the plasma rotating? If so is this the
means of storing it's energy?
~ Stopped (Russian) aircraft engine (1956) - Is the spiral action (seen in vortices) due
- Military fighter destroyed (1948) to the Earth's E and H fields
- Moved ahead of aircraft (Russian 1956) 27. The energy stored (E) must be
. . i proportional to volume, and E must be
— Ole all oe proportional to the cube of the cloud
; dimension. Similarly the light emitted is
The aircraft incidents above were at altitudes proportional to the surface area. Hence, the
from 2500m to 3400m. Some general EM light is proportional to the square of a
effects on equipment (not necessarily ball dimension. Plasma theory shows that a 10cm
lightning) are also discussed at Working Paper diameter ball could glow for 0.01 sec. The
No. | Annex D. maximum energy which, in theory, could be +
stored in a ball appears to be less than could
SUPPORTING THEORIES sustain it. In theory if the ball is lighter or
; heavier than air, then it should, respectively
23. _No single theory seems to support all rise or fall. For equilibrium (hover or "float')
the criteria. The phenomena appears to be the ball density must be 1.29 x 10°gm. cm.".'
sighted only when one or more of the following
are present: 28 To achieve colours, one associates this
- Charged particles or droplets with temperatures:
- High electrical charges in the atmosphere Yellow 2=5800A= 5000°K
(not necessarily caused by lightning) .
- When dust particles are generated (e.g. Rei A 6300A= <onrs.
cong ee Blue A=4700A= —6200°K
- When high concentrations of nitrogen re
saul omnis auetaeel White - 10,000°K to
oes 14000°K
- When marsh gas (methane) is given off oe
- Vortices (incandescent gas vortices). This, of course, does not accord with the
24. Luminosity is. observed' from perception of colours reported when no heat is
: reported. It may be, of course, that, although
droplets of opposite charges. The plasma ;
: i present, no heat was felt/sensed for various
(nsmcld) oy Agha = reasons (e.g. | e, cooling wind, etc.)
luminous material with sizes, structures and sas Za ,
SAG 8 CAE, SHEE. 2 29. The logic is that to glow for longer
25. Bt is Known that bell Ighming ogres on Cie OS Pee 2 oe ae
natural electromagnetic radiation formation. cd cs a
However, it has been impossible to produce in .
PERT , unless the object hes scht 30. The diameter of a spherical ionic
f resi ond. fi eaheapeth 5 plasma is determined by the resonance of the
: parser ya rye' rere — pay ball with the EM oscillations of the external
= Ks equilibrium. wave at which energy absorption is most
efficient. Resonance occurs when (for a
Fg ee sphere), the 2 of the external radiation is 3.65
® : times the sphere diameter. To get typical ball
INIAPAAQQIFIE
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sizes reported, % would have to be 35-100cm. more power applied, the larger the diameter
Hence, the upper limit would be which may be produced Hence, the
3x10*/1=300MHz (whereas 30 and 50MHz are phenomenon might be scaleable
reported from microcharges). It should be
noted that rarely are there any measurements 33 Other characteristics clearly depend on
from real ball lightning; any measurements the materials and size of the electrodes and
quoted are from experiments attempting to their burning temperature when a tremendous
simulate the phenomenon. energy level is applied to a very small surface
area. For aluminium this is of the order
LABORATORY-PRODUCED BALL 4400°F. As might be expected, as the fireballs
LIGHTNING surface they sizzle and hiss, some leave the
surface and produce spiralling smoke trails,
31 Many attempts have been made to leading to the supposition that the fireballs are
produce ball lightning under laboratory spinning (see below). Different electrode types
conditions and it is reported' that (in the USA) produce more or less smoke. Those remaining
it is routinely possible to produce a specific on the water exhibit random motion until they
type of this phenomenon. Golka also claims decay.
that plasmoids can be produced by combustion
* inside a 'microwave oven'. However, it is not 34, Experiments were only made with the
proposed that the ball lightning generated electrodes under water because this method
accounts for all types. In the experiments the enabled measurements to be made before the
fireballs lasted from two to five seconds but fireballs darted off in all directions, making
with only diameters of ~lcm. This has been measurements difficult. Whereas previous
achieved by short-circuiting 60Hz currents as researchers had expected high voltages to be a
low as 1200A across copper and aluminium prime requirement, these experiments were
electrodes under ~2cm of water. Another made at 40-50 volts. Even so, enough energy
researcher (Silberg, unreferenced) describes overall was deposited on occasions to make the
how this phenomenon, produced green fireballs balls leave the surface of the experimental tank
in a submarine engine room, using 260 Volts and leap onto the floor.
and 156,000 Amperes. Ball diameter was 6 to
10cm. For a 10cm diameter ball (volume 35. Aluminium electrodes produce white
515cm*) there are 1.4 X 10 molecules. When fireballs, while iron-to-iron electrodes produce
the medium (used in the switching contacts) is yellow. Either the outer surface or the kernel
nitrogen and an ionisation energy of 15eV per appears to be spinning. As soon as the ball
ion pair for the single ionisation, it can be stops emitting light, it shrinks to sugar-grain
@ calculated that there must be 3.4 X 10* Joules size. If over water these particles sink.
contained in the ball. The ball quickly
disperses unless a source of replenishment 36, It is postulated that if the sphere is
energy is present. spinning a boundary layer phenomena will be
set up, retarding thermal radiation in the same
32. The fireballs produced rise to the way that the filament of an incandescent lamp
surface and remain until exhausted, 1-2KJ of forms sheath layers which keep the filament at
energy having been deposited. The type of a higher temperature
lightning balls produced are reported to be
similar to those observed in aircraft during 37. As a result of these experiments the
flight and, strangely, in submarines during author suggests that, as ball lightning has only
WWII. With higher power the 'ball' can be very rarely been reported inside pressurised
made to travel higher from the surface and aircraft, that the product of the balls was due to
'bounce' and 'dance'. It is postulated that the natural lightning attachment to the aircraft skin
forming a small hole (at 4400°F) with
"a oo consequent formation of a plasma ball on the
'Laboratory-Produced Ball Lightning"
R.K.Golka, Journal of Geophysical Research Vol.
99 No. D5 May 20 1994.
2-7
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U estas [FED
v at
PLASMOID AURORAL LOOPS
38. A plasmoid is postulated as formed by 39. Ball Light Ozone Spheres The
a small solane of plasma (small as compared gravitational yamtsat | ean
., mea ' zs in diameter is it we descend. A
with ~~ ), where d is the diameter of the final 0.5m diameter sphere would experience a force
ball. The energy is formed by RF at 4/3.65d, of 54g. If the sphere was visible ozone, on
and ionisation grows - but eventually becomes sudden expansion when conversion occurs to
stabilised and expands but eventually deviates oxygen (20 litres for a 50cm sphere of ozone),
from resonance and cools and returns to it produces explosive energy. Ozone is the only
d=1/3.65. A weak shock is formed on collapse __ 848 denser than air produced in quantity under
the cep Po : ear aa a ad auiitigaiad discharge. The earth's oka
P oF qa ve i or and ozone spheres are both generally negatively
ere becikahi ca id st be charged. Although blue in colour, if nitrogen is
. P present the explosion colour is yellow
sustained by RF energy at low pressure, and
the concept of a phase-locked loop of EM
radiation at a wavelength stable to the 40. Power Intensive Plasma Formations ¢
circumstances previously has also been (PPFs) In the search for the key characteristics
suggested. It is suggested, in this instance, that of ball (and bead) lightning PPFs, a related
the stable standing wave excites the ambient phenomenon appeared to show some further
gases to glow and that the colour is dependent similarities to UAP reports: of which the most
on the constituents, such as dust etc. in relevant are:
suspension. In some cases it is claimed that
ball lightning has the ability by breca light, - PPF dimensions extend to tens of cm
hence it can be grey or black in appearance. - They can disappear in one point of space
and simultaneously appear in another
Ball Lightning - sometimes has glowing - Sound propagation speeds in PPF are
idee eh much higher than the speed of sound in
Sika gas and may reach 1600 ms".
sphere despite slow - a i temperature inside is
: ' - PPFs can bum metals leaving holes (but
= 1 aliments not affect dielectric material) se
electronic excitation - PPFs do not disturb the gases they pass
through in movement.
It is theorised (Ashby and Whitehead, Large PPFs (e.g. 1m diameter) are known as
Aldermaston 1971), following the collection of METEOXTRONES. Working papers 19, 21
remotely sensed signals during thunderstorms, and 24 describe other types of atmospheric
that because gamma-ray levels soared plasmas
dramatically (X50), on several occasions (for
several seconds) that more complex
explanations than hitherto might be responsible BALL LIGHTNING AND AIRCRAFT
for the plasma production - perhaps involving 41. The reported incidences of ball
(micrometres) However, itis nor clear _'lihting 'ving' ahead or behind aircraft have
Son 4n cue walt a ca brought about some investigations into the
prelims rma : pipe preambles: expected characteristics of ball in the aircraft
one siiple wit s- 8 well Gocmemeated airstream. It seems likely that the incidence of
CCCHTENCES Oy SENKIpSS WHROSSCS. sightings of 'foo fighters' (as they became
known in World War 2) would increase, purely
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AISECRE@: OI Fir
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because of the huge numbers of aircraft flying - Gaidukov [3] reported after modelling the
certainly much more night flying than had been interaction that:
carried out in the short history of manned
flight. - All efforts should be made to avoid
lightning seen ahead (before a ball is
42. — 'It is stated that large radius ball formed)
pay gan Lwrersa roaster bamagd - To avoid the chance of an encounter with
TALMAULING shape : a ball, pilots should 'encircle around a
less constant distance from the aircraft. The AS
raga oes ay ' vertical line passing through the centre of
ball' is able to do so because it is not solid the ligk ,
(otherwise a thrust force of thousands of Kg :
would be needed )! It is postulated that the - Pendulum-like undulations in altitude
layer of air adjacent to the surface of the ball may be seen (by balls ahead), and every
loses its viscous properties. The ball follows effort should be made to place the ball
the aircraft even in manoeuvres. Observations aster, where it will assume a stable
a When it is in the airstream of an aircraft it is once the pilot has ensured that the ball is
postulated that it behaves as a non-deformable ae
solid sphere in the airflow which holds its : 'a
described elsewhere in this Working Paper. (tail chase!) are not unusual
The main reason for interest in close encounters 45. Several comments can be made:
of aircraft with ball lightning is one of flight
safety. It is reported that large balls can be (a) The instances of phenomena of ball
comparable with body diameter of large lightning ahead of, or behind, aircraft
aircraft and can be 'captured' by the exhaust is relatively rare, but the Russian
from engines and 'chase' the aircraft at a research suggests, apart from initial
velocity of 150-200ms' (278-370kts), lightning avoidance, that the aircraft
maintaining an apparent constant range from would be safe with the ball astern.
the tail assembly. :
(b) Reports of balls above aircraft
43. One (TU134) pilot reported that at an 'pushing or forcing' an aircraft to
altitude of 10,000ft and flying at a velocity of descend are of concern, even if the ball
800km hr? (~220ms"), the ball (in this case does not cause physical damage its
* green) "appeared as though tethered behind the presence is clearly menacing to the
aircraft". Another (Russian) crew report, when uninitiated - especially as it occurs
flying at 7500ft altitude were "followed" by a suddenly.
huge ball which was still in 'pursuit' after a (c) A 'collision' from astem is not
fast descent to 4500ft. It refused to leave considered likely.
despite manoeuvre - which was limited for an : es
airliner. (d) A 'collision' head-on is possible and
its imminence might cause violent pilot
44 If the moving object were solid it (control) reaction even though the
would take the force of many Newtons to make contact may not (at the last moment)
it follow an aircraft. Clearly the ball is have actually occurred
sensibly weightless (apart from the mass of the The 'stand off' of the ball lightning from an
gases it contains). It is believed that the aircraft seems to be very much like the
electrical charge of the ball diminishes as situation encountered in several scenarios
ionisation of the air-layer in contact with its where pilots have been scrambled to investigate
surface occurs. The USSR treated the ball 'UFO' sightings. A scenario where this occurs
lightning phenomenon as very important and not only involves the 'stand-off described here
2-9
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but also the 'black' centre described, below, at SURVEY OF COLOURS
para. 48
47. Smirnov' analysed over 4100 ball/bead
PLASMA SHAPE CHANGES AND SIZE reports (indicating that the Former Soviet
Union must have a considerable database on
46 It can be argued that the buoyancy of UAP-type topics). The total power radiated by
the plasma is balanced by charged ion droplet a black body obeys the Stephen-Boltzmann
mass, with the actual shape make-up dependent Law of proportionality to the fourth power of
on the distribution of forces within the ball. temperature and in 4112 samples the
Although some have suggested that the oval temperatures produced the following statistical
shapes occasionally reported are due, not to the colour distribution:
mass of the droplets/particles (which gravity
may pull into a pear shape, individually), but to White 20.4%
the presence of a strong D.C. field, elongating
the ball in the field direction. It is believed that Red/Pink 17.7%
the production of nitric acid (note the section
on nitrous smells) leads to an inflow of air Orange 23.1%
which aids ball stability. The size of the ball : s
seems to be determined at its creation[4] and it Yellow 20.2%
is believed the cycle of change in electric field, '
of ion production, of water demand, and then Green 1.4%
anergy but not ne size. In the Blue/Violet 11.4%
many attempts to develop a theory to explain ; —
ball lightning (and by so doing possibly Mixed Colours 5.3%
understanding the 'earthlights' phenomenon), it en ae ae oa
Se ee Ee Lae atmospheric luminous phenomenon seen as a
ee ae sata dithcak oo cel ball, there is around an 80% likelihood of the
' gee at ths tun cf ee ball (or bead) colour being either white,
recognised theory, though : Red/Pink, Orange or Yellow and around a 20%
century it was recognised that Maxwell's chance of it being one of these four options,
equations could be gmeralised to include rather than green, blue or mixed
magnetic charge and current as the murror-
partners to electric charge and electric current An apparent paradox in the understanding of
Since then 'new physics', has postulated the the intensity (and hence colours) has been that
magnetic photon' as a corollary to the more the calculated radiant power (using colour
widely known convestionsl optical photon temperature to determine intensity) has resulted
Hence, some theories conceming the ball in intensities that seem to be far too large to be
lightning phenomenon have developed using the in agreement with actual observations of heat
'magnetic photon' and 'magnetic charge and light. One of the later theories resolves this
Vortons', in tum, are postulated to occur in by suggesting that the vortons (see para. 46
pairs and create 2 ees re field. above), moving as a gas, exhibit positive
(Comment: This is of particular significance Doppler shifts of the radiant black-body energy
when related bes the discovery that humans to a higher colour temperature (moving towards
exposed to rotating magnetic fields can produce the observer) and to a lower colour temperature
responses strikingly similar to those reported for movement away. Variable cloud shapes
from close encounters with's UAE}. other than balls can occur, it is claimed, if a
ferromagnetic-like interaction of the dipole
forces of the individual vortons occurs
* Smirnov B.M. Sov. Phys. USP 35 650 (1992) and
Phys Rep No. 224 151 (1993)
2-10
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OPTICAL 'THICKNESS' OF BLACK SUMMARY OF BALL LIGHTNING
BODY RADIATORS CHARACTERISTICS
48. A supportable theory suggests that 50. A survey of literature on ball and bead
some balls have a coherent core which is too lightning and its relevance to UAP reports, has
cool to radiate in the optical visible spectrum - shown that:
hence such a volume would appear totally
black. The visible appearance of the - There is a near constant brightness, size
phenomenon depends on optical 'thickness', and shape, which can exist from a few
where: seconds to minutes
- If the body (of gases/particles??) is hot - i aaa have considerable
enough to radiate, then its intensity is
uniform over the surface; independent of - It is possible for an electronically-
the angle the surface makes with the charged body (possibly including ball
sightline of the observer. lightning) to 'attach itself to an aircraft
, : in flight; where, apparently due to a
e : ian ae ee An balance of fields (clectrostatic/magnetic
optical region, it will Saks shai' or EM), it can remain in close proximity
any opti er : radiations aa ae aki (formation abreast or astern)
and hence would be 'seen' as a totally - Ball lightning can enter houses and
NOTE: This later statement would seem to ee
have a significant read-across to frequent
UAP sightings where a black shape (often - Sounds and smells are present on rare
rectangular or triangular) is seen between occasions. These are both often
visible lights at the extremities. Although, described, respectively, as 'electrical'
Black and grey-body radiators are, (e.g. buzzing sounds, or explosions) and
respectively, 'thick' and 'thin' optical sources. smells witnesses associate with electrical
equipment, such as ___ insulators
THERMO-CHEMICAL overheating or rotten eggs.
REFRIGERATION 51. Near Terrestrial Events There is a
. . . tendency for ball lightning not to rise - most
49. Considerable evidence exists to show eae
incid wee ; sightings remain at low level near the earth in a
* a a toe ee ee near horizontal path. This is explained, in
conditions of high humidity are present. theory, in the reasonable expectation that the
paras, Weems ee seabed yr eager a vei 's
— aoe so cn ee re such that the postulated radially-moving
hydrated and this action adds heat to the -""eeative ions form a static charge on nearby
system; keeping the hydration zone (boundary) surfaces which tend to repel the negative body
fai . . . of the ball; keeping it at a distance. This, it is
rly hot. However, if the ions survive long 7 E ithe bales
enough to become hydrated by ~5 water argued, is the most likely reason for 74
lecules it is lated that cooling reportedly try to pass through any aperture (i.¢.
To this thermochemical action is attributed the Window, door, chimney). 'In short, as it moves
characteristics of the reported harml of it creates a field which tends to hold the ball in
occasional human brushing contact with a ball 'Position (e.g. at constant altitude outdoors, or
end the season foe the Choudl faxdistinct across the centre of a room Further, since no
appearance of the edges of the ball. charge builds on the aperture, ee ee ce
proceed - presumably sending a positive charge
somewhere ahead. This may also account for
2-11
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the propensity of balls to 'dart' towards power plasmas of other origins than ball or bead
cables or any object where the radial does not lightning may also decay in the same way.
exceed the local positive value. Hence, in the UAP sighting reports it is almost
impossible to determine the origin of a
ay UrStructure Phenomena The fact that particular UAP because, it is believed, the
P phenomena can reportedly exist in : P rar :
closed inated atracaes that. , behaviour is very similar. Further, if the
to expectations, the existence of the ball is premise that meteors (see Working Papers and
apparently not dependent on an external statistical results at Volume 1) also cause the
Ang : : formation of UAP, then a UAP could be
but must retain it's own electric or magnetic ;
field in order to exist and, once formed, is self- formed during a thunderstorm (as well as from
sustaining until its demise. Within the past year a i
some researchers have suggested that ;
atmospheric plasmas may owe their duration to
a combination of both vertical and horizontal
(ie. orthogonal) magnetic looped fields which SUMMARY - RELEVANCE TO UAP
contain and sustain the phenomena. If this is 54. An examination of a wide range of
the case the process may be applicable to any research into ball and bead lightning has shown
atmospheric plasma - however formed, if the that it is certainly connected with a proportion 2
field are strong enough. It has been proposed of the UAP reports received from within the
[6] that the stability of a volume (ball) of air at UK airspace. Descriptions of these particular
16,000 to 30,000 degrees Kelvin might be forms of lightning correlate in time, colour and
contained within linked magnetic _ lines. motion with qualitative description often given
Discharge arcs (e.g.lightning) advance along by reliable UAP witnesses. Because those
narrow tracks 50-100um in diameter in air. UAP which are formed and then reported as a
These streamers would only occupay a small result of lightning are, of course, transitory in
volume of the ball. It is postulated that some nature and their form is apparently changing as
of these form short circuits, resulting in they head towards demise, it is reasonable that
circulating currents, each loop acting as a coil. the colour descriptions vary, that they exhibit
the physical appearance of the charge- strongly influential electrical field
can be shown by Maxwell's equations that a pyrotechnic displays. All of which are
'magnetic knot' is feasible and this has now unfamiliar to the majority of the population.
conducted energy cannot be stationary and is
postulated to produce a slowly-varying B
magnetic field. The magnetic energy is a REFERENCES:
function of the ball radius, the vacuum
magnetic permeability, the number of magnetic ! "Ball and Bead Lightning" J.D. Barry
lines which are linked and a field normalising Plenum 1980.
function. It is not within the scope of this study 2. "The Nature of Ball Lightning"
to pursue this important phenomenon further, S.Singer Plenum 1971.
other than to emphasise the likely connection es i
between this, the formation of plasmas by 3. Hydrodynamic Model of the
meteors and the effects of varying magnetic Interaction of Ball Lighting with the
fields on humans (Working Paper No 25), in Airstream of an Aircraft in Flight" N.1.
the UAP context. Gaidukov. Technical Physics 38(9)
ane = EE
53. Demise For those balls/beads visible to
humans it is reported that the silent demise is 4. Tumer DJ. "Ball Lightning" Phil
normally a simple fade in brightness and Trans. Royal Society, London 1994.
diameter, while the explosive demise is 5 Fryberger D. "A Model for Ball
sometimes preceded by an increase in Lightning" Ostfold College Norway
brightness and a colour change. Similarly, Report No. 1997:5 Part 1 (1994) Proc.
2-1
UNG h SCIFIEN
5% a i pee pow
ae
, fF i wath itr
a oe ie iP me
Wi GEST iT ial
First International Workshop on
ULAP, Hessdalen
6 "A Model of Ball Lightning as a
Magnetic Knot with Linked Streamers"
A F Ranada, M Soler & J L Trueba
Journal of Geophysical Research, Vol
103 Sep.1998
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 3
POTENTIAL REASONS FOR HIGHER DENSITIES OF UAP SIGHTINGS
Para Page
INTRODUCTION 1 3-1
POPULATION DENSITY 4 3-1
WEATHER/VISIBILITY 5 3-1
TIME OF YEAR 6 3-1
TIME OF DAY 7 3-2
LOCATION 8 3-2
AVAILABILITY AND COMPETENCY OF WITNESSES 9 3-3
HIGH INCIDENCE LOCATIONS 12 3-3
AIR CONTAMINATION 15 3-4
POTENTIAL REASONS FOR HIGHER DENSITIES OF UAP SIGHTINGS
February 1, 2000 X x x x x x x x x x x x 3.40
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POTENTIAL REASONS FOR HIGHER DENSITIES OF UAP SIGHTINGS
INTRODUCTION
1. In the current database analysis it has been important not to misinterpret the reasons for UAP occurrences, by drawing the wrong inferences from a statistical analysis. One of the first analyses to be attempted for the case of UAP sightings across UK aerospace to look for high incidence areas - in the hope (possibly) that this may shed some light on the nature of the phenomena, lead to more focused scientific work and possible more data when sightings occur (e.g. correlation of visual sightings with coincident radar coverage). As the unknown is being investigated, preconceptions are no part of initial assumptions.
2. Taking the extreme case - that UAP are more than natural occurrences - it cannot be assumed that locations where the objects occur will necessarily be of obvious importance to humans. Further, it cannot be ruled out that these appearances may only take place at certain intervals and be entirely unrelated to the relative disposition of the gravitational fields of various bodies in space, or other fields of which we may have scant or even no knowledge at present.
3. On the initial assumption that the phenomena of UAP sighting can occur anywhere, then the presence of larger numbers of sightings in a particular part of UK will be dependent, at first sight, upon:
(a) The population density
(b) The weather/visibility
(c) The time of year
(d) The time of day
(e) Location
(f) Availability and competence of witnesses.
POPULATION DENSITY
4. It would seem logical that if there are a greater number of potential observers, and on the assumption of an equal probability (i.e. equal distribution of UAPs in the UK air space), then higher densities of reports are to be expected in more highly populated areas. However, in areas of greater population there is also a much higher night-time reflecting target and an almost completely different light background level, making conditions for the detection of less bright phenomena much less likely to be seen (as evidenced by astronomical observatories, which have been forced to move away from lit-up areas). The contrary situation is that more sparsely populated areas have fewer potential observers, but little or no interference from ambient surface lighting. It is thus difficult to immediately connect the number of potential observers available in a geographical area against the likelihood of expectation of UAP sightings, since other factors are present. As an initial guide Table 1 shows the population distribution for the UKADR.
WEATHER/VISIBILITY
5. A brief analysis to determine the relative prevalence of sightings in cyclonic and anti-cyclonic conditions has been made. There was no clear evidence of correlation with temperature, dew point, wind, etc. However, the continued prevalence of UAP reports whether Lightning (see Working Paper No 2) was present or not on the same day in the same area was of particular importance in an attempt to discover whether atmospheric conditions are key to the formation of UAP. However, adequately clear visibility for viewing low and
¹ Oceania World Index Johan van der Heijden 1996
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medium altitude UAPs can exist in both weather patterns, although the high pressure clear conditions, rather than the murky conditions in high pressure are likely to provide the best viewing conditions. There is, nevertheless, a possibility that UAP sightings might be connected to weather patterns.
TIME OF YEAR
6. It is instructive to imagine a larger number of reported sightings during dusk and darkness - simply because the greatest number of reports occur when witnesses are seen - and this is rarely the case reported in daylight. Of course, this does not necessarily mean that there are fewer UAPs present during daylight (assuming that their occurrence is indifferent to the presence or absence of light). (Since we do not know what they are we cannot assume any attributes). In addition to weather, it may be that the atmosphere has electromagnetic and ionisation correlates with sightings (see Working Papers No. 1, 2 and 10). It cannot be ruled out that these appearances may be formed particularly if the event is from an unexpected source.
TIME OF DAY
7. Although a time-of-day connection with UAP reports is inevitable because of the relative darkness of day and darkening conditions for 'lights' in the sky, the actual occurrence of the total of these phenomena, within the atmosphere at any given time may not be time-dependent. One must not fall into the trap of assuming that the presence of unexplained objects in the atmosphere (or in near space) is necessarily connected to our world measurements - a cycle of sightings and the rate of occurrence is somehow connected to the routine of life. As this study only involves sightings within the UK's airspace, this investigation will not be in a position to correlate UK sightings with successive sightings (if they were reported or even if they were present) in Europe or other locations, the potential of being important. For example, if there is shown to be a cycle of sightings, we shall have no other option than to measure it in terms of time as we know it. If, for example, this (or one cycle) appears to recur at regular intervals, the problem will then be to fit this time period to a meaningful pattern, perhaps sidereal. It may, of course, be shown not to fit any known pattern (e.g. celestial, seasonal, etc).
LOCATION
8. It is sometimes claimed that UAP sightings are more likely to occur in some locations than others. Apart from the volcanic connection, claimed by some observers (clearly not applicable to UKADGE), it has been noticed that the location is an important database factor in the likelihood of expectation of UAP sightings, since other factors are present. Before useful statistical work can be done on this topic the following must be considered for a rigorous analysis to be made:
(a) The location of a sighting is often given crudely. A 'place name', 'near a place', 'between two places', 'out to sea off xxxx', 'on holiday near xxxx'. The address of the witness can not be the right location of the sighting.
(b) Lat/Long co-ordinates and Grid References are rare (but could be generated approximately from most of the reports).
(c) Port codes might be a good method
(d) Plots (maps) of the following are required in electronic form:
- National Grid/Local Power lines
- How to map sub-station level
- Airfields - Military/Experimental
Establishments
- Air corridors
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- Low Flying Routes for Military
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- National strategic sites
- Power Stations (including nuclear)
- Locations of ancient monuments/
fault lines (to investigate the claim of
heightened probability of UAP
sightings at electromagnetic/gravity-
earth's field changes claimed at these
sites)
AVAILABILITY AND COMPETENCY
OF WITNESSES
9. Clearly only a proportion of UAP phenomena is reported. There is no way of ascertaining what proportion this may be. It can only happen where people are present, therefore there will be large areas of the UK with high UAP activity, but never seen or reported. The phenomena of the lack of radar correlation is considered at Working Paper No. 10 and at Volume 3 for specific in-service systems.
10. The decision to report activity depends on the witness. The more 'responsible' are likely to do so because the UAP sighting is a unique event in most cases: it has caused fright or concern and there is a 'need' to tell someone in authority. Because the sighting is 'airborne' the preferred reporting option is the nearest RAF Station, followed by the coastguard or the police. Timing of reports compared with sighting data, already indicates that some witnesses often wait a day before making a report. [As for all delayed reports there is always the real possibility of forgetting/loss on detail or embellishment!]. Many witnesses delay because of concern about their credibility. A comprehensive report is not usually obtained from the very basic UAP (UFO) reporting form - and the accuracy and detail obtained from a witness depend significantly on the attitude and care taken by the police or other reporting authority. Hence, there is no reliable consistency of reporting - even from the ATC/CAA sources.
11. It is wrong to separate so-called competent/reliable witnesses from others because every scrap of evidence has the potential of being important. For example several single-witness clear sightings can complement a single 'reliable' sighting since these extra sightings:
- Allow multiple angle/aspects to be registered
- Allow object velocities, colours, altitudes and sizes to be calculated independently
- Allow geometry to be used to eliminate heavenly bodies (i.e. planet sightings)
- Allow both silhouette as well as reflected-light viewing
- Allow multi-aspect viewing to ascertain shape, colour and flight profile
- Eliminate the retained after-image sighting of single witnesses - to eliminate overlapping times
- Confirmed UAP geometries and spacings independently
- Eliminate single-human events (e.g. smell, drugs, psychological etc.)
- Usually eliminate the hoax option
- Reinforce credibility of each others reports from a group of independent witnesses
- Allow multiple photography/video to be taken
HIGH INCIDENCE LOCATIONS
12. Within the UKADR it is reported by researchers that the greatest incidence of UAP events are centred on:
- Lothian (Scotland)
- Luce Bay (Scotland)
- South Wales
- Warminster (S. England)
- Pennine Hills
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13. Elsewhere in the world at 20 prime general locations events of UAP occur more frequently. These include France, Belgium and Scandinavia - all of which have airspace adjacent to the UKADR.
14. Hence, reports of UAPs are sometimes received of UAPs entering from, or leaving nearby nations. Only NE Italy and Spain are among the NATO nations reporting the largest numbers of sightings (although these are not recorded in the UK database unless they are officially conveyed through official channels to UK MOD).
AIR CONTAMINATION
15 It is postulated by some plasma and other atmospheric researchers that the presence of certain (from whatever source), such as the introduction of various industrial gases, will affect the density and ability to ionize air molecules in the atmosphere. This is considered further in the relevant Working Papers, principally Number 20. It is noted, in passing, that those nations with higher atmospheric dust-producing conditions (e.g. Volcano and Earthquake Regions), reportedly have a higher incidence of UAP reports. Further, if this theory is true, one might expect to find more incidences of UAP report in close proximity to smoke or gas-producing industries and possibly to various types that are likely to be in higher concentration.
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[World map showing continents and oceans with location markers. Labels visible include: EUROPE, ASIA, AFRICA, ATLANTIC OCEAN, PACIFIC OCEAN, INDIAN OCEAN, BRAZIL, and various UAP incidence location markers across multiple continents.]
FIGURE 1: HIGH INCIDENCE UAP LOCATIONS (J. RANDLES)
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area in population
km² census
1991
Avon Bristol 1,346 920,000
Bedfordshire Bedford 1,235 514,000
Berkshire Reading 749 777,000
Buckinghamshire Aylesbury 1,883 628,000
Cambridgeshire Cambridge 3,409 645,000
Cheshire Chester 2,329 956,000
Cleveland Middlesbrough 583 541,000
Cornwall Truro 3,564 469,000
Cumbria Carlisle 6,809 487,000
Derbyshire Matlock 2,631 915,000
Devon Exeter 6,715 [ILLEGIBLE]
Dorset Dorchester 2,654 645,000
Durham Durham 2,436 593,000
East Sussex Lewes 1,795 691,000
Gloucestershire Chelmsford 3,672 1,445,000
Greater London London 1,579 6,378,000
Greater Manchester Manchester 1,287 2,418,000
Hampshire Winchester 3,777 152,000
Hereford & Worcester Worcester 3,927 668,000
Hertfordshire Hartford 1,634 952,000
Isle of Wight Newport 381 177,000
Kent Maidstone 3,731 [ILLEGIBLE]
Lancashire Preston 3,064 1,365,000
Leicestershire Leicester 2,533 861,000
Lincolnshire Lincoln 5,915 584,000
Merseyside Liverpool [ILLEGIBLE] [ILLEGIBLE]
Northamptonshire Northampton 2,367 573,000
TABLE 1(A): POPULATION DISTRIBUTION UKADR
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Southend on Sea 153,700
Peterborough 148,800
Blackpool 144,500
Colchester 141,100
Brighton 133,600
Blackburn 132,800
Poole 130,900
Newport 129,900
Preston 126,700
Reading 122,600
Torbay (Torquay) 119,500
Saint Albans 122,400
Ipswich 117,100
Oxford 109,000
Exeter 101,800
York 100,600
North Yorkshire Northallerton 8,309 699,000
Nottinghamshire Nottingham 2,164 981,000
Oxfordshire Oxford 2,608 554,000
Shropshire Shrewsbury 3,490 405,000
Somerset Taunton 3,451 459,000
South Yorkshire Barnsley 1,560 1,249,000
Staffordshire Stafford 2,716 1,028,000
Suffolk Ipswich 3,797 630,000
Surrey Kingston 1,679 998,000
Tyne and Wear Newcastle 540 1,087,000
Warwickshire Warwick 1,981 477,000
West Midlands Birmingham 2,992 2,499,000
West Sussex Chichester 1,989 693,000
West Yorkshire Wakefield 2,039 2,013,000
Wiltshire Trowbridge 3,480 555,000
Total England London 130,498 46,168,000
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London 6,803,100
Birmingham 934,900
Glasgow 654,542
Sheffield 500,500
Bradford 449,100
Liverpool 448,300
Manchester 432,600
Edinburgh 421,200
Bristol 369,200
Dudley 300,400
Coventry 292,600
Sunderland 286,800
Sandwell 284,800
Belfast 279,237
Leicester 272,000
Newcastle 261,000
Walsall 255,000
Bolton 253,000
Kingston upon Hull 252,200
Rotherham 247,000
Stoke on Trent 244,800
Wolverhampton 239,800
Plymouth 238,800
Aberdeen 201,099
Southampton 194,400
Swansea 182,100
Northampton 178,200
Saint Helena 175,300
Portsmouth 174,700
Luton 167,300
Dundee 165,548
Bournemouth 154,000
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Cont'd....
[area] [population]
Borders Newtown St Boswells 4,698 103,000
Central Stirling 2,700 268,000
Dumfries and Galloway Dumfries 6,425 147,000
Fife Glenrothes 1,319 338,000
Grampian Aberdeen 8,752 493,000
Highland Inverness 26,137 200,000
Lothian Edinburgh 1,770 724,000
Strathclyde Glasgow 13,773 2,218,000
Tayside Dundee 7,643 385,000
Island Areas - 5,566 71,000
Total Scotland Edinburgh 78,783 4,957,000
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 4
AFTER-IMAGES AS A RESULT OF FLASHES OF LIGHT
Para Page
BACKGROUND 1 4-1
Primary Sensation 3 4-1
Results of Experiments 4 4-1
Flash Duration Dependency 6 4-2
Observer Variability 8 4-2
SUMMARY 9 4-2
RELEVANCE TO UAP SIGHTINGS 10 4-2
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AFTER-IMAGES AS A RESULT OF FLASHES OF LIGHT
BACKGROUND
1. Illusions observed in darkness or low light conditions, after exposure of one or more eyes to a bright light are known as 'positive after-images' and are often similar in colour to the inducing light. Those illusions seen in moderate illumination are called 'negative after images' and are often of the approximation to complementary colours. In practice the actual appearance of after-images is complex and likely to depend on many factors including adaptation from dark to light takes much less time than from light to dark - hence there is an awareness of the appearance of a light in dark conditions much more quickly than the appearance of a shadow in lighter conditions. Excessive eye stimulation, as is well known, produces blindness in the limit.
2. Within the eye the sequence of changes which occur in response after light is absorbed differs between rods and cones: cones suffer further adaptation by the nerve cells of the retina (adaptation of the retina). However, the result is the persistence of the sensation of light after the stimulus has been removed.
3. Primary Sensation Human eye response is a peak at 0.55μm, and a detectability from 10⁻⁶ cd.m⁻² to 5000 cd.m⁻². There is a range of conditions over which the primary sensation produced by a flash of light depends on its luminousness product (i.e. in general, the integration of luminance with respect to time). This is independent of temporal distribution of the flash, and can be demonstrated by regularly repeated flashes as long as 150 years ago and confirmed this century using extremely short (1 sec) durations now possible. The practice holds for flash values down to ~ the total amount of light rather than for longer durations. For longer duration flashes the measurements are less researched. Hence, the integration of flashes is less reliable as a guide at an illumination intensity of 0.5cd.m⁻² at which pulse durations of 27 millisec may have been exceeded (3° fovea fov.). The time duration may be greater than 27 millisec for longer flashes and shorter in period for those which are brighter.
4. Results of Experiments Preliminary experiments [1] to investigate after-image conditions for eye stimuli of different lengths produced the following results:
- Stimuli ~2 sec maximum. The whole course of the (positive or negative) after image, during its first 15 sec, was dependent on total light in the stimulus and not on the light's intensity distribution alone.
- Stimuli 2-5 sec. The result only differed slightly from the 2 sec stimulus length - calculated with some time distribution differences. In particular, there were some differences between positive (dark background) and negative (bright background) after-images.
- In the after-image observation time t=10 to t=30 it is believed that the retinal illumination always decreases monotonically (from white light stimuli), but the after-images produced by other colours may decay at other rates. The actual detection threshold is inversely proportional to flash duration.
5. The human eye can nevertheless distinguish between extremely short spaces between flashes (pulses of light). Experiments have shown that 4 millisec intervals can be distinguished from intervals as little as 0.28 millisec. In the context of UAP observations, pulsed (i.e. modulated) lights should be distinguishable by observers, even from a high modulation (i.e. fast) rate. High modulation rates - and very short duration of individual pulses - should not get mis-reported as steady lights. This is
[1] "Discrimination of After-Images" G.S. Brindley, J. Physiology 147 (1959)
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important, for example, in the context of lights which are 'chopped' by helicopter blades (~50Hz for a main rotor four-bladed Helio).
6. Flash Duration Dependency An important finding of the available data is that the same amount of light (except for the first 15 sec), irrespective of whether it is delivered within 1.68 sec. This is consistent with the hypothesis that the after-image of a brief stimulus from the 15th second until its disappearance at t=100 to 300 seconds later, depends upon photochemical effects. It does not depend upon adaptation or neural mechanisms in the retina or brain (as a result of the activity it is presumed the brain undertakes immediately after an eye stimulus).
7. It is probable, from the evidence available, that after the first 15 seconds, residual effects contribute to the perception of the image seen. Up to five seconds after a stimulus (flash) it is nevertheless believed that neural as well as retinal (there must be no interaction between the dust particles).
- The persistence depends on the chemical consequences in the eye's receptors, not at (5-10 sec only) on the adaptation of the image by the nerve/brain response.
- For very short flashes (e.g. less than 4 millions) high intensities have most effect than lower intensity stimuli when viewed against either bright or dim backgrounds.
- Colours observed following a flash of a particular colour are dependent on the viewing background thereafter.
RELEVANCE TO UAP SIGHTINGS
10. A large number of UAP reports are of very intense lights of diverse colours, many of which are only reported as being of very short duration. Some of these could be the after images of even briefer flashes. Longer duration reports apparently (see para. 6) of up to 15 seconds or more could be attributed to flash stimuli, followed by an after-image. It would appear that sightings are unlikely to be caused by after-images for longer than five minutes. After 10-15 seconds the human observer will be interpreting and adapting what is seen well beyond what is actually registered chemically, due to the flash, within the retina.
11. There is, of course, the possibility of the after-image being 'replicated' by successive intense flashes. However, many flashes are from single (i.e. single) events, e.g. lightning, electrical (i.e. non-continuous) electrical flash-over from (national grid) power lines or overhead train power lines.
12. It seems unlikely that, on the occasion of multiple witnesses of UAPs, that they all receive the same phenomena (after-image); since apart from human observer variability (as mentioned for 8 below), it is unlikely that the plasmas containing these particles comprises two ionic components (one single charged atomic ion and the other positive or negative, multiple charged dust particle). Due to the tendency of the plasma to charge neutrally, a kind of charged cloud forms
[1] Ludlam C "Radar Scattering from Dusty Plasmas" Physica Scripta 45. Univ. Of Tromso, Norway 1991.
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[2] "Further Studies of the Positive Visual
After-Image" C.A. Padgham Op: Acts.
Vol. 4 1959.
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 5
DETECTION OF UAPs BY RADAR
Para Page
DETECTION OF UAPs BY RADAR 1 5-1
Possible Explanations 3 5-1
Current Detection Minima 4 5-2
RADAR REFLECTIONS FROM PLASMA 5 5-2
BALL LIGHTNING AS A RADAR REFLECTOR 10 5-3
Radar Echoing Area 12 5-3
DUSTY PLASMAS AS RADAR REFLECTORS 13 5-3
DETECTION BY UK-BASED RADARS 19 5-4
RADAR SIGHTING REPORTS 21 5-4
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DETECTION OF UAPs BY RADAR
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Conventional theory and radar systems operation suggests that (given a clear radar sightline), the following conditions should occur for radar (UAP) detection to take place:
(a) The target must be radar-reflective. (See Appendix A5)
(b) A minimum detectable signal must return to the radar receiver to satisfy the radar receiver - S/N requirements (i.e. minimum detectable signal).
(c) The signal must be displayed (i.e. in a modern system which uses preset thresholds the display/processing threshold must be adequate for the target being inspected).
For a target track to be formed (a), (b) and (c) must be repeated at the radar's inspection (i.e. update) rate. In modern systems supposed 'spurious' radar responses are likely to be rejected/filtered and unless they fulfill 'plot' requirements, will never be declared from successive plots into 'tracks'. Hence, they will not be seen as targets.
2. There is a significant absence of radar plots/tracks on UAPs. It should be borne in mind that, statistically, it is incontestable that all UAPs in the UKADR are reported by direct (human) sighting(s). In fact, there must be many more UAPs unreported, especially within radar coverage but not within human sightlines (e.g. due to cloud cover, reduction of observers in sparsely populated parts of the UK etc.). Why, therefore, are there not at least even a reasonable proportion of these reported by military or civil radars; either at sea, over land or by aircraft radars?
3. Possible Explanations The number of explanations are possible. The conditions at para 1 above are not being met for one or more reasons:
a. For some reason the radar reflectivities of these unidentified objects are extremely low.
b. Because they do not 'communicate' or appear where aircraft are expected, they are ignored by the operators (or the automatic processing systems) as spurious/short-lived observations.
c. These were are taken to be caused by flocks of birds.
d. When moving fast they exceed the upper Doppler/Velocity capability of the system. This may be, firstly, beyond the Doppler measurement capability of the particular type of
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e. The target cannot be seen because there is no radar sightline (e.g. terrain or low/high altitude). This can only be the case on a limited number of occasions, subject to range.
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g. The object absorbs RF energy at least at the usual wavelengths in use and hence is not detected.
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i. The objects are above the upper radar coverage capability (~100,000ft)
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N_c = 1.24 × 10¹⁸ f_p² (cm⁻³)
f_p is in GHz. For example; a value of ≥1.2 × 10¹¹ cm⁻³ will reflect X(I) Band and all frequencies below. Using these relationships the direct RF to density expression can be derived:
f_p = [N_c.e²/πm]^½ or f_p² = N_c.e²/mπ²
where m = mass 9.11 × 10⁻²⁸g
e = electron charge 4.8 × 10⁻¹⁰
e.s.u. (1.6 × 10⁻¹⁹ amps or
1.6 × 10⁻¹⁹ coulombs)
This can be rearranged such that:
f_p = 8980√N_c/H_s
6. A plasma thickness may vary, hence:
- The location of the critical density 'mirror' is not necessarily at the outer extremity of the plasma.
- Some absorption of the incident energy can occur in the lower density region which the energy encounters before it penetrates to the depth of the critically dense region. This depends on the ambient air pressure.
- Incident radar energy may arrive at the plasma at various angles (θ), hence:
N_c = 1.24 × 10¹⁸(f_p²/cos²θ)
- The refractive index of a plasma is always less than 1, given by:
μ = √(1 - ω_p²/ω²)
where ω is the radian frequency of the EM wave
RADAR REFLECTIONS FROM
PLASMA
5. A plasma is an assembly of small particles of three kinds, +ve, -ve and neutral, moving at random and colliding with each other. In all except very high current discharges there are many more neutral particles than charged particles. Electron oscillates about a mean position with angular frequency ω_p = 2πf_p, where ω_p² = 4πN_e²/m. The oscillations are linear and stationary and do not progress as waves. A plasma will reflect radar energy at all microwave frequencies below the "plasma frequency." A critical-density surface can be formed according to the density relationship:
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and ω_p is the plasma frequency which is related to N_e by:
ω_p = 2πf_p
7. Thus radar energy entering a medium of lower refractive index is similar to that applied (on the same principle) to total internal reflection in optics.
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10. It should also be noted that the greatest visual luminosity occurs when the frequency of the oscillation of ions and electrons is equal to the applied frequency:
4πf²/m_e = 1
BALL LIGHTNING AS A RADAR
REFLECTOR
11. As stated at Working Paper No. 2, ball and bead lightning (which do not always appear as spheres), may have diameters as small as a few cms and as large as 12-15 metres. For the ball lightning sphere of 10cm its gaseous density is known (1.29 × 10³ gm cm⁻³), but its plasma density is not known, unless this can be deduced via its colour/temperature characteristic.
12. Radar Echoing Areas The radar echoing area of ball lightning as a function of physical size. A transition between a strongly reflecting target and an almost completely absorbing target occurs. The possible RCS values for plasma spheres are different from that of metallic spheres (who's RCS is a function of size in relation to the radar wavelength), with the radar echoing area of plasma spheres dependent also on ionisation level. An 'overdense' plasma sphere (or other shape) may be treated as a perfect reflector (retro-reflector for long ranges). This gives, upon interference effects between the backscattered wave and tightly bound surface waves. This gives plasma the properties of a dielectric, even when it is overdense. For example, a collision-less homogeneous plasma sphere with low electron density may have a RCS value of -60dB, peaking between 1 to 3m² as the density increases, but falling to 1m² as the density increases yet further. These values are for D/(E)(L) Band assessments.
DUSTY PLASMAS AS RADAR
REFLECTORS
13 It is argued that 'dust' particles, possibly of ice, form soot(aceous?) plasmas. (These are of the type, see Working Paper No. 13, which are sometimes reported as UAPs). The most recent understanding of dusty plasmas is at Working Paper No 19 "Charged Dust Aerosols". It can be postulated that the plasmas containing these particles comprises two ionic components (one single charged atomic ion and the other positive or negative, multiple charged dust particle). Due to the tendency of the plasma to charge neutrally, a kind of charged cloud forms
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around each charged particle in such a way as to compensate its charge.
14. In a two-component plasma with equal electron and ion temperatures it can be shown that the charge of the dynamic cloud of a single charged ion is composed of 50% accuracy electrons and 50% of repelled ions. The roles of electrons and ions are reversed for the case of a negative ion. Hence, the number of electrons in the surrounding cloud may be small or large, depending on the densities and temperatures of the plasma components. Under these conditions an (EM) wave illuminating the plasma will set in motion the electrons in the cloud and if the scale of the dynamic cloud (Debye length) is much smaller than the wavelength of the illuminating wave, either coherent or collective scattering (from the electron component of the cloud) will occur.
15. It is beyond the scope of this brief paper to pursue the detail of the scattering, other than to note that for radar-wave scattering to be enhanced there must be no interaction between the dust particles.
16. The intensity of the scattering, as a function of the incident radiation λ_o, equals 2πk_s, where k_s is the wave vector number. There are two regimes with little intensity for long wavelengths (2k_sλ²≤1) and a regime at shorter wavelengths (2k_sλ²≥1). The radar scattering is caused by fluctuations of electron density. The scattered power per unit volume of illuminated plasma within a small interval of solid angle, within a frequency interval dω and at wave vector k can be calculated from the Thomson electron cross section.
σ_T = e⁴.97.95×10⁻²⁶m²
where e is the electron radius, E_o is the incident (E field) amplitude and q(Ω) is a polarisation factor defined as:
q(Ω) = |ŝ × (ŝ × E_o/|E_o|)|²
For backscatter q(Ω) equates to 1. The full derivation is at.²¹
17. Anomalous radar scatter has been received at RFs of 50, 274 and 935MHz, using experimental radars. The plasma is not fully ionised.
18. Strong backscatter from this cause occurs principally at high latitudes, in the summer and at considerable altitude (~80km).
DETECTION BY UK-BASED RADARS
19. Backscatter from 'dusty' plasma at an altitude of, say, 50km can theoretically be obtained at a slant range of ~190km from a radar with a maximum elevation angle of ~25°. These radars with a height-finding capability would soon reject the returns because the range/angle/altitude combination would place the target at an unacceptable altitude for manned aircraft. x x x x x x x x x x x x x x x
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20. The detection of phenomena other than mesosphere plasmas is also considered at Volume 2 and is SECRET as it involves the current detection performance of military operational systems.
RADAR SIGHTING REPORTS
21. In an attempt to correlate simultaneous or sequential radar sightings with radar types, only limited UK information is available. In December 1989 5 NATO radars, part of ACCS, were within coverage range of a UAP report. Three radars had detections but two did not. Unfortunately, the radars have since been replaced and records of their parameters,
²¹ Ladlam C "Radar Scattering from Dusty Plasmas" Physica Scripta 45. Univ. of Tromso, Norway 1991.
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in use at the time, are no longer available. In the 1960s, Personal Air Traffic radar had unexplained detections and, over various years, the P-35 Air Interception radar had unexpectedly made UAP detections. In all these cases the effective electrical noise of the radar in question was the cause of the effective radar sightline and in all cases these were subsequently UAP detections. RAF Neatishead, RAF Washington Airfield Approach Radar and the CAA radar at Clee Hill have had in-service UAP radar detections. In all these cases the effective electrical noise of the target must have been enough for the RF in use to produce reflections.
22. Clearly, the ability to respond to radar is variable, and all the radars would not detect all the objects: either at sea, over land or by aircraft radars. A radar which cannot get a return from UAP would nevertheless see all standard aircraft.
23. In the absence of firm radar-to-radar correlation the number of occasions when velocity would be deduced from actual measurements (compared, for example with purely 'eyeball' estimates of equally separated fixes) are few. On only a small percentage of UAP sightings (around 100 to 1000) are there reports from some members of the public are fine. On one radar occasion (visually confirmed from two places), 'out to sea off xxxx', 'on holiday near xxxx' etc are electronically spaced two second fixes. Plots at ranges from 100 to 999Hz in two seconds are possible from our best understanding of the EM environment. Longer modulation (i.e. fast) rates of occurrence are observed in some form. On one source occasion (visually confirmed from at least two places) and in very short durations - and very short duration of individual pulses - should not get mis-reported as steady lights. This is, of course, the possibility that the formation of UAP depends on a plasma.
23. In the absence of firm radio cross-correlation the number of occasions when velocity would be detected from 'dusty' plasma at an altitude of, say, 50km can theoretically be obtained at a slant range of ~190km from a radar with a maximum elevation angle of ~25°. Those radars with a height-finding capability would soon reject the returns because the range/angle/altitude combination would place the target at an unacceptable altitude for manned aircraft. Adequately clear visibility for viewing low and medium altitude UAPs can exist in both weather patterns. At t=10 seconds the after-images are the same.
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/6/99
APPENDIX A5
DETECTABILITY OF PLASMA TARGETS
1. If it is assumed that, in the first instance the target is a spherical plasma body, the following conditions could exist:
- The sphere could be large in dimension compared with the radar wavelength
- The radar echoing area of the simple sphere is a function of its ratio of circumference to the illuminating wavelength [2πa/λ (where a is the sphere radius)]
- For large values of 2πa/λ, the RCS approaches the optical RCS (πa8)
- The sphere, if homogeneous and perfect would be aspect insensitive. (U)
2. In theory it is seen, therefore, that if a UAP was a stable plasma sphere of adequate electron density, a metre in diameter and comprised of entirely reflecting gaseous material, then its maximum radar echoing area for all practical purposes, when illuminated by a EF Band(0.1ns) radar, could be about ~16 square metres. For D/E/(L) Band radars the value computes to ~five square metres. However, there may be several other factors of importance for a plasma UAP which could significantly affect its detectability, and in practice ( as mentioned at page 5-3, paragraph 12), the real values ( L Band) are estimated as falling somewhere between -60dB (0.000001m8) and +8m8. Any surface absorption of the radar signal, which, in theory, should have little effect when the wavelength is large compared to the target dimensions, is not necessarily the case here, as it is by no means certain that the UAP plasma (whether it's outer shell, or surface) can be considered a resonant body. Or, indeed, that it's surface remains a consistent and constant reflector, especially as many UAP reports indicate that the body is constantly changing colour and often varying slightly in shape. The response of the body as a reflector when compared against the characteristics of the radar is clearly a key factor. (R)
3. Target Characteristics Target RCS fluctuation plays a significant role in the detection performance of all radars. In general, radars, (apart from Weapon Control/Tracking Radars, which may dwell for relatively long periods on their chosen target) impact their targets at repeated and sometimes regular intervals the form of dwells or scans, and by illuminating them with bursts of pulses. If a UAP is considered that a plasma UAP has a variable electron density (possibly interspersed with periods of greater plasma stability), then for much of the time the radar reflectivity may vary rapidly, possibly uniquely from pulse-to-pulse (Swerling Case 2), rather than from scan-to-scan (Swerling Case 1). Further, the fluctuations may vary continuously from scan-to-scan (Case 3); or finally, so rapidly as to vary from pulse-to-pulse (case 4). (U)
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object might have. The steady (non-fluctuating case), sometimes called Case 5, is extremely rare in normal radar practice, due to the inherent nature of flying targets.(R)
5. Practical Effects The detection capability of a radar depends on the signal (wanted) to noise (unwanted) ratio. The practical effect of RCS fluctuations, applicable to the UAP scenario, is most simply illustrated by one example. For a typical radar with a requirement of probability of detection (0.95), against a steady target, a signal-to-noise ratio of 4 (+6dB) is required. If the target is fluctuating according to Case 1 above, a ratio of ~48 (16.8dB) would be necessary. In radar range terms this turns out to be a range performance reduction by a factor of 3.24. This effect can be mitigated somewhat by illuminating the target with a larger number of pulses and averaging them out. However, there is a limit to the number of pulses emitted, and which engage on a target from an early-warning-type radar during its typical continuous-scan mode of operation. For targets which exhibit Case 3 and Case 4 fluctuations the situation is even worse - and it is believed that this is the case for UAP plasma - for additional reasons. Firstly, these cases require even more signal than Case 1 to overcome fluctuations from diverse sources but the frequency of reports correlated with other measurable events, such as weather, meteors, etc.
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 6
EXOTIC TECHNOLOGIES
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INTRODUCTION 1 6-1
Exotic Solutions 2 6-1
UAPs AS PROPELLED VEHICLES 4 6-1
ANTI-MATTER (ANTI-PROTON) PROPULSION 8 6-2
Material Storage 9 6-2
NATIONAL CAPABILITY
USA 10 6-2
UK 11 6-2
Former Soviet Union 12 6-2
France & Italy 13 6-2
Rest of The World 14 6-2
ELECTRIC PROPULSION TECHNOLOGIES 15 6-2
Arcjets 16 6-3
Stationary Plasma Thrust (SPT) 17 6-3
Ion Thrusters (ISF) 18 6-3
Field Emission Propulsion (FEP) 19 6-3
PROJECTED ENERGY 23 6-3
TORSION, GRAVITY AND LASER FIELDS 6-4
Torsion Fields: Definition and Properties 24 6-4
Laser Propulsion 27 6-4
MICROWAVE PROPULSION 28 6-4
Summary 31 6-5
OVERALL SUMMARY 32 6-6
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EXOTIC TECHNOLOGIES
INTRODUCTION
1. UAP reports usually describe objects seen at a distance (and these reports can only provide, at best, approximate angular speed and size (and often a very vague diameter). For this reason, the absence of mass or linear velocities the information is almost useless when trying to apply the laws of physics controlling the ability of a 'craft' to land (or hover) and take off again.
The thrust of any object must be slightly less than the body mass on landing and twice its weight for an acceleration on lift-off of 1g. If an object of say 5 or 20 metres diameter were to lift off, some (conventionally understood) effect must be expected on the surface. No such after-effects are reported in the thousands of UAP reports held in MOD.
2. Exotic Solutions Exotic solutions may not be feasible initially, but they often lead to the necessity for some form of force beyond human understanding and contrary to the laws of physics as we understand them. This leads to such ideas as:
- Gravity Cancellation
- Teleportation
- Propulsion without reaction
- Force Fields
3. Intergalactic travel requires ~four million years for a return trip (travelling at just less than the speed of light), or three years, even to a nearby planet at a velocity of 20Km sec⁻¹ - a planet on which we can determine no sign of life in the form which would indicate 'beings' and their technology.
UAPs AS PROPELLED VEHICLES
4. The majority of UAP sightings can be attributed as relatively easily explainable natural or human phenomena - explainable, for
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technology is expanding, principally in the USA. The projected (USAF) priority plan is to produce optionally piloted air-breathing aircraft with a Mach 8-12 capability and transatmospheric vehicles which can operate between the various air-breathing and sub-orbital flight regimes, as well as highly supersonic vehicles at Mach 4 to 6.
7. It is assumed that the fuel options are intrinsic (fuel carried internally), partially extrinsic (some part of the fuel is obtained externally e.g. from the atmosphere) or the propulsion energy is entirely extrinsic (e.g. from some sort of external field). The foregoing examples are understood as representing, respectively, chemical or electric or nuclear (e.g. rocket), air-breathing (e.g. jet engine), or a system which uses a some kind of external field(s), of which the only vehicular example is terrestrial (e.g. levitated train).
9. Material Storage Cooling is among the most serious problems to be solved. Portable storage for containing the 'anti-matter' in the form of rings and ion traps, would be necessary. The particles are typically confined within a plasma volume (e.g. 200cms long) at low pressure, with a vacuum (~10⁻⁷Torr and a magnetic field of 10T). This could all fit into a large truck, including all support equipment for storage times of ~30 to >100 days of storage time. The dimensions given might store ~10¹⁶ antiprotons (~0.8Kg) and is considered to be a factor of 100 down on the limit. According to authoritative sources a few micrograms of antiprotons can be produced annually by a nation with the resources to do so.
NATIONAL CAPABILITY
10. USA In 1987 it was stated that the US could construct an intense source of low-energy anti-protons in three to four years and thereafter deliver (store) 10¹⁰ low energy protons annually. It was hoped that a five to seven year programme might be started (or already had been). This information, which was 1987 closed seminar, was given public-release in 1994. One of the prime applications foreseen is for air-vehicle propulsion. The cost of a R&D programme would be ~$400M, over a 20 year period. In addition to propulsion, non-propulsion applications of anti-matter have been proposed in medical (biomedical imaging), therapy and biomedical detectors.
11. UK That anti-matter is a key topic of interest is confirmed by a series of papers, and, in particular, reports of NATO activities in which UK participate. A recent review paper (P T Greenland, Imperial College London) describes the UK's search for a cause of gravity and the relationship between gravitational mass and inertial mass. Anti-hydrogen has been produced successfully, but the technology to create and control of the anti-hydrogen is not yet achieved to enable instrumentation and measurement to
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be obtained, for example for a comparison with conventional hydrogen. The approach is to trap protons and positrons, separately, anti-protons and positrons both at liquid helium temperatures (than anti-hydrogen is then obtained by the combination). The work so far has used the highest energies achievable by the Low Energy Anti-proton Ring (LEAR). No anti-hydrogen has yet been trapped at low temperature. There are no indications of any current experiments into early developments of future potential applications of anti-matter for propulsion purposes.
12. Former Soviet Union Scientific papers from the USSR reflect an interesting approach to matter storage devices, for example, positron storage rings. These, including the 'IREN' project, are at the design experimental and very early development stages. In particular, important work is proceeding on the use of Gamma-Ray Lasing in the matter and anti-matter research fields.
13. France & Italy French aspirations seem to be significantly aimed at whether some stars (and even some entire galaxies) may exist which are made up of anti-matter. The possibility of this scenario will, in theory, be proved if a anti-matter (single anti-helium) nucleus in cosmic ray flux) are detected in cosmic rays. Results are awaited from a the current Shuttle project. Further research is being funded by NATO and the EU. In 1999, two scientists at the Italian National Nuclear Physics Institute reviewed anti-matter as an area of future research and proposed future experimental projects. They proposed that the possible existence of anti-matter was first postulated in 1928, and that recent eco-atmospheric evidence events were delayed following the Shuttle disaster. As a result four balloon-borne experiments had occurred and the planned space (Italy-Russia) will also examine anti-matter components of cosmic rays. This possible existence of an organized anti-matter, with a symmetric universe and matter and anti-matter separated into galaxies remains a fundamental question.
14. ROW Nations There is no evidence that any ROW nation has scientific or engineering capability leading to real developments in the field of anti-matter.
ELECTRIC PROPULSION TECHNOLOGIES
15. Chemical propulsion requires large propellant mass compared with electrical methods. Once (assuming that) a UAP of undetermined origin could somehow enter and leave earth's atmosphere, (with the capability of some unknown propulsion method) the remaining journey (from wherever it came from and return) could present phenomena which the 'electric' propulsion methods for which the technologies are currently understood provide the propulsion at low thrust levels (mN), as shown at Table 1.
16. Arcjets produce an arc typically in the exhaust nozzle of a chemical thruster. For electric propulsion (EP) although their thrust is higher than other EP methods, there is the mass penalty of the chemical propellant required.
17. Stationary Plasma Thrust (SPT) produces ionised sensors, which draws in from, and from a carbon cathode into the plasma propellant passes through electric and magnetic fields in a discharge chamber.
18. Ion thrusters (IPS) also use ionised sensor propellant.
19. Field Emission Propulsion (FEP) is fifteen times more efficient in its use of specific impulse (Isp) but at low thrust levels.
20. None of the methods at Table 1 were conceived as primary methods of spacecraft propulsion.
21. On board power requirements (for a 1RoN UK IPS design with an Isp of 3466) is ~600W, worst case. The thruster exhaust velocity is ~40 km s⁻¹ for small station keeping. 40Kg of propellant held in a titanium storage tank (mass ~10Kg), would provide a planned life of ten years. Even a small thrust,
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coupled with orbital dynamics could be used to escape from earth orbit.
22. Despite the foregoing possibilities there is no evidence that an extra-terrestrial vehicle (comprising solid matter as we know it and using any of these techniques) has visited earth and left again. Any visitation must be followed by a departure, otherwise artifacts would remain (hence the corresponding reports of 'sonic booms' nearby). Normally, sound is either generated and then emitted by a stationary body due to some internal mechanical or electrical vibrating, oscillating or rotating device (from the selection of its inner materials). The frequency observed will depend on the characteristic of the body. The lack of sound in UAP reports attributed to extra-terrestrial vehicles is likely to be attributable to:
PROJECTED ENERGY
22. Much has been postulated in the scientific press on the possibility of transferring energy to an air vehicle (which would then convert it to thrust), either continuously or in pulses. Technology has reached the stage where it is possible (with proof of principle tests) to transmit RF or laser energy to a moving platform, where it is collected for on-board use. This is dependent on providing and maintaining a suitable tracking system. A Foreign Research Lab Laser system, tested in 1997 allows a small rocket accelerated a parabolic mirror to collect pulsed laser energy from the ground which is concentrated onto inlet air, which in turn becomes a plasma. xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx xxxxxxxxxx
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There are no indications from any UAP event that clustered phenomena can be interpreted include fine details of the design of such a craft other than to list the key features which might have a bearing on the potential UAP
TORSION, GRAVITY AND LASER FIELDS
24. Torsion Fields: Definition and Properties Torsion fields and associated phenomena are governed by the possibility of describing them by use of a scalar and spin. A torsion field is governed by
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Projections and modelling claim a Mach 5 capability, to 100,000ft altitude. The laser provides thermal energy (collected from the beam) and used to produce air-breathing thrust. At altitude, conventional rocket fuels would be used to boost to escape velocity.
MICROWAVE PROPULSION
28. Low frequency microwave beams are not suitable for on-board energy collection. The problems are those of diffraction, and the requirement for large antennas on board the vehicle. Also, the low breakdown threshold of the atmosphere limits the received power density. The selection of high frequencies is limited by the EM atmosphere windows (e.g. 34, 94, 140 or 220GHz). No atmospheric attenuation also increases with increased RFs. It is assessed¹ that a 15m diameter craft could provide a launch station with a 5GHz antenna. With the overall diameter assessed at 10MHz antenna, a larger 350m diameter array would be required to ensure adequate energy (10MW on a one metre diameter receive antenna), to ensure the vehicle at the extremity of the atmosphere because of the extremity of the atmosphere because of the 220GHz atmospheric window). Conceptually, a space-based, (LEO) passive relay station could be used to relay the EM energy from a terrestrial station onto the vehicle in space, where the energy would be converted this time for use as an in-space thruster.
29. It is beyond the scope of this report to include fine details of the design of such a craft other than to list the key features which might have a bearing on the potential UAP connections in answering the enigmatic question - 'Can a craft capable of extra terrestrial travel with the reported characteristics be conceived within the limits of current science?' The key features which follow with UAP-related comments in square brackets
(a) Size The microwave craft proposed reported UAP attributes, and falls within some reported UAP diameters.
(b) Mass A launch mass of 1400Kg is proposed (surface area loading 7.9Kg/m²). This is an aerodynamic (e.g. wing) loading area typical of ultralight aircraft. This leads to the conclusion that a production version by means must be used to lighten the mass even to the point of carrying no propellant and some aerodynamic design can reduce shock wave effects, though not eliminate them.
(c) Materials Thin film materials with adequate tensile and compressive strength would be crucial; something far a figment of the imagination engendered and embellished with the rest of the alleged phenomena. In particular, it is easy to imagine a charged mass to have a done and perhaps it is to attribute volume when it 'takes off' Sound reports, as with other attributes, suffer from not having a first-hand debrief immediately after the event and before reports become forgotten or the information of interest is lost
¹ 'Hyper Energetic Manned Aerospacecarcraft Propelled by Intense Pulsed Microwave Beam': L K Myrabo, SPIE Vol 2557 1995
² 'Propulsion of Small Launch Vehicles using Millimetric Waves': SPIE Vol 2154 1994
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air breathing engine'. The PDE uses microwave-supported detonations to heat the air working fluid and it based on what, in principle, is the air-breathing ramjet. A conventional cyclic engine (i.e. air-breathing and rocket) might be envisaged for a transatmospheric role. Clearly this would only operate in the atmosphere and at velocities of Mach 5-6 are claimed to be possible without an air spike. [Hence, to return to the possible 'UAP' similarities this type of craft could not be extra-terrestrial unless it used another type of propulsion outside the atmosphere]. Another end-atmospheric option is the Magneto-Hydro Dynamic Fanjet (MHDF), where powerful Lorentz forces which are exerted on an external air working fluid. In effect the active microwave-powered plasma antenna normally displaces this passive 'field core' - which is the air channel used for momentum exchange.
UAP events reported are, in fact, not necessarily 'saucer shaped'!
SUMMARY-PROPULSION OPTIONS
31. Propulsion mode is the key factor in considering whether it would:
(a) Be possible to construct a vehicle with reported UAP attributes and potentially (until proved otherwise) with an extra-terrestrial capability, using currently-known 'Earth' technology.
(b) Be possible to conceive such a craft which can move with zero or near-zero sound and change the direction of movement almost instantly.
CONCLUSIONS
32. In attempting to explore the potential technologies which would be essential in order to construct a craft with the exceptional characteristics attributed to UAP it is important to note that:
- No reliable report exists of a landing and take-off of an object known to contain 'beings'
- No reliable reports of occupants can be seen anywhere on earth and not even small artefacts have been left on earth to confirm the existence of a 'spacecraft' in the form of metals or other materials that have apparently ever crashed, despite sighting reports for thousands of years.
- There is no evidence of attempts at communication between the alleged occupants of the 'craft' and humans - or messages/items left behind as a form of language to attract attention. There is no evidence that any nation has a current capability to produce and trap anti-matter for propulsion purposes.
33. Hence, there are no new technologies or methods which could be exploited beyond those already known or being researched. There have been no
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opportunities for accurate size or shape measurements, no examinations of unknown or special materials or of any types of devices which could aid in the determination of what the phenomena comprise or be used in order to replicate the UAP in an air-vehicle as a result of the presence of UAP in the UKADR. In the absence of measurable artifacts, the best estimate of the nature of UAP can only be assessed by a careful analysis of all the available reported characteristics and scientific assessments of data collected from diverse sources but the frequency of reports correlated with other measurable events, such as weather, meteors, etc.
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Thrust Isp Uses
(N) (S)
CSP 1-500 <320 Extensive
ARCJET <1 550 Wide
SPT 0.04-0.20 1600 Limited
IPS 0.002-0.25 3000 Experimental
FEEP <0.001 4000 Future
TABLE 1: ELECTRIC PROPULSION OPTIONS
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 7
SIGHTLINE RATES OF FLYING OBJECTS
&
METEORITES
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INTRODUCTION 1 7-1
SIGHTLINE RATE GEOMETRY 2 7-1
PARAMETERS 5 7-1
INTERPRETATION 6 7-2
EXO-ATMOSPHERIC OBJECTS 9 7-2
Meteorites 9 7-2
Satellites 13 7-3
PLASMAS, CHARGED AEROSOLS AND SPRITES 17 7-3
THE ILLUSION OF OBJECT MOTION 18 7-3
VELOCITY ILLUSION 19 7-4
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SIGHTLINE RATES OF FLYING OBJECTS
INTRODUCTION
1. This brief paper is intended to relate to frequent UAP reports where objects cross through the observer's field of view at what are often, reportedly, extra-ordinarily high velocities. Typical examples are those of satellites and meteorites.
SIGHTLINE RATE GEOMETRY
2. The basic geometry assumption is that, from the initial visual contact, the object continues in a straight line until it goes out of sight due to some local obscuration or reaches the observer's visual horizon. The largest angle through which an object can pass is from horizon to horizon. Usually the angular sector crossed (or at least seen by the observer) is much less. The angle crossed is usually viewed either as azimuth or elevation. On occasions the object is diving and often disappears during the process - and these are usually explainable in horizon-up memories or against debris. The greatest tangential velocity occurs when either the object trajectory is almost overhead or when at a 90° azimuth offset. Velocities always appear to be greater when objects are closer to the observer, even though they are identical to those at greater range which pass through the same enclosed angle but take longer because the distance subtended is greater. The human perception of speed is often distorted by any accompanying sound. Many UAPs are reported as 'silent'. However, it is borne in mind that if any sound is present it can give residual perception of the meteor's energy heard.
3. On the spur of the moment, accounting for surprise and even incredulity, later embellishment, misunderstanding and over or under estimation, it is clear that the velocity and velocity figures given by a UAP witness can be wildly inaccurate. Further, more than one witness at the same event may provide
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The plots are for objects 'flying' at constant altitudes. If an object is either climbing or diving then a different calculation is needed.
INTERPRETATION
6. Figure 2 (for both endo-and-exo-atmospheric targets) enables a target speed to be approximated, based on witness assessments of angle traversed (az or el), range and time of observation:
φ = 2ρ / r t
where φ = Angle traversed (radians) =
Deg/57.29
R = Witness estimate of target range
t = Witness estimate of duration
of sighting
7. The same approximation applies to space-based objects. In this case it is assumed that exo-atmospheric objects can be at any altitude above the earth.
8. It is important to note that the method used is based on the assumption that moving objects travel tangentially through the estimated angle, with respect to the observer's position. Any movement at other angles with respect to the observer would increase the track-length flown and thus, in a given time, increase the object's velocity.
EXO-ATMOSPHERIC OBJECTS
9. Meteorites Diving objects (e.g. often called 'shooting stars') are frequently reported. These are high velocity ionised particles caused by meteor-body friction with air molecules, which then usually travel with a fiery tail/trail, lasting only a few seconds. RF reflection from trails (utilised for scatter HF communications purposes), occurs in the (approximate) 30 to 120MHz range. Meteor-trail duration is measured in hundreds of milliseconds. Two categories describe the rate
at which meteors strike the earth's atmosphere. The periodic group (known as meteor 'showers'), which have a yearly cycle and the sporadic group which are, though more random, occur year-round. In the context of UAP sightings:
- 'Showers' occur for periods from hours to days at a rate of the order 20 to 50 per hour. These are often present, though not always visible, due to the interference of moonlight. The forthcoming occurrence of showers can be predicted, and can be predicted to be known to the (and the meteor stream's orbits) are known - hence the intersection can be calculated. What is not known is the shower density. There is a shower density cycle repeating every 33 years. There is no connection between meteoric activity and sun spots or solar flares.
- 'Sporadics' exhibit a Poisson distribution but with a diurnal variation.
- In addition to the familiar largest fireball-producing meteors there are tiny grains not visible to the human observer. Radio and radar methods allow the latter to be detected. As the meteorite rate may have a bearing on the production and presence of some types of 'UAP' attempts will be made to correlate meteoric density against the trend of UAP reports.
10. This latter condition reflects the fact that at dawn (local time) a meteor that has the longest path in the atmosphere, while at mid-day the meteor will appear to strike the atmosphere at 90°. As the size of meteors varies between smaller than a grain of sand to those that survive and impact the earth's surface (e.g. Tunguska), they vary inversely with probability of arrival. Consequently, large meteorites (which can, on average, strike the earth once in every 250,000 years) make up a significant proportion of all meteoric mass and are not large enough to be seen visually.
* Lowell A C B Meteor Astronomy UP 1954 P248.
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11. Associated with the size is the electron line density (ELD). These are classed as either 'over' or 'under' dense. Under-dense ELD is <2×10⁶ electrons per metre. Over-dense trails are considered to be a tubular plasma cloud (hence the association with other phenomena of interest to this study). The duration of over-dense trails is generally longer than that of under-dense trails. Trails can be manipulated by the effects of both wind-shear and high altitude winds, which distort their tracks. A brief examination of recent UK meteorite velocity measurements shows velocities from about 11km sec⁻¹ (with a maximum of 70km per second maximum, with a mean of around 40km per second). The International Meteor Organisation produce a Meteor Shower Calendar, which is used elsewhere in this report as the basis for some statistical analysis against the UAP report rate. (see Volume 1 Annex F)
12. The probability of observing meteor trails visually is low and apparently not equally distributed over the earth. For correlation purposes it has been found that the best trails occur according to the distribution at Figure 1, and it might be supposed that this density also reflects the most likely locations where higher visual opportunities occur. This changes according to geographical latitude. The meteor scenario, in relation to reported UAP events is an enigma. It does not necessarily note the increased presence of more UAP reports in coincidence with periods of high (or higher) meteoric activity. This does not necessarily mean that observers are only seeing meteors. Further, it does not mean that UAP reports are always caused by meteors. There are bound to be reports generated by a host of other causes. On the other hand it could mean that some UAP are formed by meteors as the residual effect of the meteors enormous energy. These postulations are examined further, statistically, at Volume 1 Annex F, where it is clear that this is the case.
13. Satellites Other frequently reported objects, almost always described as 'steady lights' are probably satellites in low earth orbit (LEO) (see Working Paper No 17). The sightline rate of these is clearly dependent on orbital altitude and speed.
14. Observation curves are at WP No17, and assume an observer is stationary on the earth's surface. Geo-stationary satellites can be ignored, as by definition they have no sightline rate. Low earth orbit satellites have a practical maximum altitude of ~10000Km and orbit at a velocity of ~7Km sec⁻¹. This equates to a sightline rate of about 4° per minute.
15. If an observer spotted a satellite from rise to set (most unlikely) covering a full 180° (45 minutes), or even for 15 minutes, current public knowledge is such that it would be identified as such and not reported as a UAP, or even reported at all.
16. In UK latitudes the satellite orbit would have to be at an inclination >50°. Viewing conditions must also be correct to observe a satellite:
- It is unlikely in daylight.
- Its size must be large (small debris is not detectable)
- The light falling on the satellite, which is then reflected must be adequate. Other data concerning the observation of satellites and hence the probability of being mis-reported as UAPs, is at Working Paper No 17.
PLASMAS, CHARGED AEROSOLS AND SPRITES
17. It is evident that when plasmas, charged aerosols and any high altitude phenomena, which depend on luminosity due to charged particle interaction, are seen to have extremely high These phenomena, often described as 'nocturnal lights' are described at Working Paper Nos 1, 5, 10, 19, 21, and 24. They frequently appear as having significant angular size and, because of their high speeds (some being at altitudes of tens to often kilometres to tens of kilometres), are often
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perceived and reported as flying much lower than they actually are.
THE ILLUSION OF OBJECT MOTION
18. It is important to note that (other types of actual flying objects excepted), with those visual phenomena which are due to certain atmospheric effects, little of substantial physical substance actually moves. It is the light seen by the observer that moves from place to place and it becomes visible in those places because the atmospheric conditions (electrical, particle etc.) allow it to become visible. Hence, the observed variation in colours seen, the duration for which an object is seen, and the time for which a sightline rate is discernible. The visualisation (wavelength) of a UAP, from an electromagnetic charge source, also depends upon air pressure.
VELOCITY ILLUSION
19. The illusion of velocity in receding objects is particularly important in UAP reports, where, as they are often in the dark, leave the observer with no surface references with which to relate speed. This is especially the case when the sky background does not offer a simultaneous view of any aircraft, with which to compare sightline motion. Similarly, in bright sunlight the velocity of a small receding spherical object is particularly difficult to assess. This is dependant on whether the object being viewed is just a spherical (i.e. 'round') light, (which may be bright or dim) or whether it is being viewed as a silhouette. The surface area of a receding sphere is the same as the area of a circle (Πr²) and the enclosed angle resulting (1.subtended) from its diameter, as range increases, will reduce linearly as the ratio of its diameter to range. However, its area appears to the observer to have shrunk according to the square law. The important feature here is that a sphere comprising plasma objects which might not be accelerating away (or even be moving away at linear speed) but is in fact shrinking in size (as its, often brief, lifetime comes to an end as the electrical forces holding it stable collapse), can
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/1/98
[FIGURE: Dome/hemisphere diagram showing meteorite trail distribution with concentric elevation lines at 0°, 25°, 50°, 75°, 105° from horizon to zenith, labeled with 'Zenith' at top, 'Horizon Circle' at bottom right, and angle markers]
FIGURE 1: METEORITE TRAIL DISTRIBUTION (E)
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Velocity
(m/sec)
30000
UAP
Ranges
25000 50(km)
20000
30(km)
15000
20(km)
10000
10(km)
5000
5(km)
0
1 5 10 15 20 25 30
Sight-line Rate (deg/sec)
FIGURE 2 SIGHT-LINE RATES(E)
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 8
RARITY OF UAP SOUND
REPORTS
Para Page
INTRODUCTION 1 8-1
Anomalies 2 8-1
Discussion 3 8-1
Geometry 4 8-1
Future systems 5 8-1
Mis-reported sounds 6 8-1
SUMMARY 7 8-1
February 1, 2000 xxxxxxxxxx S40
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/6/99
RARITY OF UAP SOUND REPORTS
INTRODUCTION
1. An initial overview on UAP sound is at Working Paper No. 1. This paper further sound in the context that there appears to be a correlation between the occasional report of sounds, the frequent lack of sound when high UAP velocities are reported when, usually there are no corresponding reports of 'sonic booms' nearby. Normally, sound is either generated and then emitted by a stationary body (e.g. in building, machine), a continuously vibrating, oscillating or rotating device producing sound due to built or frictional displacement of air. Sound may also be caused by electrical discharge or chemical action.
2. Anomalies When an object is in the air and, however erroneously is considered to be a 'vehicle', a witness normally expects to hear some sort of noise. The faster a UAP is perceived as travelling, then the greater is the expectation of sound. The lack of sound in the vicinity of a travelling object in UKADR is unusual. The basic reasons for the lack of sound in UAP reports attributed to an air-vehicle (and not always nearby) is likely to be due to:
- An over-estimate of the object's actual velocity.
- The presence of some atmospheric conditions (e.g. wind absorbing cloud) that suppressed the sound to an inaudible level.
- The probability that, while reported as being in the atmosphere, the object is in fact in space.
- The object - though travelling sometimes at high speed, has not actually disturbed the atmosphere through which it has clearly seemed to pass.
- The fact that the 'object' may have no mass, or negligible mass. Normally, sound is either generated and then emitted, or generated and then reflected from its ionised gases or an internally-generated colour temperature.
3. Discussion The first effect above is not unexpected as most UAP witnesses are untrained. The second can occur when the sonic shock wave is distorted and the conical pattern of the shock front does not reach the ground. It is also noted that the classic bow and tail shocks may not both be heard as they are at different intensities. Hence, as the public are aware (and may recognise a double shock as a supersonic aircraft), a single shock 'bump' may not be recognised as coming from a genuine aircraft, (the lateral component of a supersonic shock wave causes a variation in intensity. This effect coupled with windspeed means that the source of 'sound heard.')
4. Geometry Unless the observer is along the track of the target, z a few kilometres, the double (or even single) 'boom' may not be heard as some aerodynamic design can reduce shock wave effects, though not eliminate them.
5. Future Systems It is of interest, here in the UAP context, that the first experiments to modify airflow using electromagnetic fields (and plasmas) took place in the 1960s, and is a topic of current interest with its 'read-across' to target signature control (i.e. RCS reduction). It is not clear, at present, how much the reduction of drag will affect the overall audio noise generation and hence the probability of sound heard on the ground is generated by the engine thrust, relatively little being generated by the airframe or sound vehicle body.
6. Mis-reported Sounds Finally, one must consider that sounds may be mis-reported (e.g. mistaken description of the aircraft itself, or a figment of the imagination engendered and embellished with the rest of the alleged phenomena). For example, it is easy to imagine a charged mass to have a drone and perhaps it is to attribute volume when it 'takes off'. Sound reports, as with other attributes, suffer from not having a first-hand debrief immediately after the event and before reports become forgotten or the information of interest is lost
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SUMMARY
7. It seems most likely that the reasons for few
reports of sound (for those sightings in which
nearby aircraft can be eliminated) are that
many objects are beyond the range at which
sound would be heard, are mis-reported in
range, they are satellites, or are 'charged' air
masses of various sorts which emit little or no
sound (e.g. Charged aerosols or plasmas, etc.)
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WORKING PAPER NO.9
'BLACK' AND OTHER AIRCRAFT
AS UAP EVENTS
Para Page
WESTERN PROGRAMMES 1 9-1
SR-71 programme 2 9-1
S.27 X X X X X X X X X 3 9-1
X X X X X X X X X 6 9-1
RUSSIA 7 9-1
UAVs 9 9-2
GLIDERS 10 9-2
PARAWINGS, HANG-GLIDERS & MICROLIGHTS 11 9-2
MIXED AIR ASSETS 12 9-2
HELICOPTERS 13 9-2
AIRCRAFT LOW FLYING ROUTES 14 9-2
VISIBILITY FOR LOW FLYING 15 9-3
AIRCRAFT LOW FLYING AT NIGHT 16 9-3
AIRCRAFT IN FORMATIONS 17 9-3
SPEED WHEN LOW FLYING 18 9-3
USE OF RE-HEAT OR AFTERBURNER 19 9-3
FREE-FALL PARACHUTING 20 9-3
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OBSTRUCTIONS & POWER LINES 21 9-3
PROHIBITED & AVOIDANCE AREAS 22 9-3
SPECIAL NOTE:
This working paper contains NATO RESTRICTED information on the UK low
Flying Zone, for use in UAP report filtering and analysis, which must not be
divulged to the public.
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'BLACK' AND OTHER AIRCRAFT AS UAP EVENTS
WESTERN PROGRAMMES
1. It is acknowledged that some UAP reports can be attributed to covert aircraft
programmes – in which unusual air vehicles may be seen, either at the experimental stage
or in service. UAP reports often describe the shapes that are shown at Figures 1 to 9. It is
noted that certain viewing conditions of these vehicles may be described as 'saucer like' –
hence they are not ignored by observers – as more conventional and familiar aircraft shapes
would be, but are frequently reported as UAPs.
2 SR-71 Programme Figure 1 shows an SR-71. Flights have been conducted since
the 1960s. It is known that this was a US supersonic (M3+) reconnaissance aircraft that
operated over the UK. This aircraft was also known as 'SENIOR CROWN'.
3. X X X X X X X X X X X X X X X X X
X X X X X X X X X X X X X X X X X X X
X X X X X X X X X X X X X X X X X X
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X X X X X X X X X X X X X X X X X X X S.27
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X X X X X X X X X X X
4. Figures 7 and 9 show head-on silhouettes of the F117 and B-2 'stealth' aircraft and of
other aircraft, the body/fuselage shape of which can be reported respectively as 'saucer' or
disc/boomerang shaped' under certain silhouette and lighting conditions. These aircraft types are
unfamiliar as they are rarely spotted in UK airspace.
5. It is important to note that since these aircraft cannot hover then accelerate, they
cannot be the cause of reports where these phenomena occur.
6. X X X X X X X X X X X X X X X X X
X X X X X X X X X X X X X X X X X
X X X X X X X X X X X X X X X X X X X
X X X X X X X X X X X X X X X X X
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X X X X X X X X X X X X X X X X X S.27
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X X X X X X X X X X X X
RUSSIA
7. In 1992 Russia announced a new flying machine, called a thermoplane, constructed
by designers of the Moscow Aviation Institute, according to Moskovskaya Pravda
newspaper. This unusual airship, outwardly resembling a flying saucer, is intended to be
used for ecologically sound highly effective technologies in the field of superblock
construction; control and remote exploration of the environment; and large scale life-
saving operations.
8. According to experts the fuel and economic efficiency of a thermoplane will exceed that
of an aeroplane by five to seven times, two to three 2-3 times for an automobile and can be
compared with a sailing vessel up to a few thousand tonnes displacement. Tests on the
thermoplane are being conducted in Ulyanovsky Aviation Industrial Complex (Volga region).
The diameter is ~40m and depth 16m.
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UAVs
9. There is a significant UAV programme in the USA and Israel and to a lesser extent in
the European NATO Nations. It is possible that experimental versions may be flown
principally over coastal or sparsely inhabited regions of the UKADR in the future. Some of
these may be reported as UAP.
GLIDERS
10. Gliding objects are of particular interest in the UAP context, as they make very little
sound. Further para-wings and hang-gliders also appear to an observer to hover, climb and
descend. On occasions, depending on livery, a glider has briefly reflected light and has been
reported as a UAP, insufficient of the rest of the machine being seen to permit the observer to
recognise the sighting as a glider. Both freeflght and powered gliders fall in this category.
PARA-WINGS, HANG-GLIDERS & MICROLIGHTS
11. There is an increase in the use of sport para-wings and hang-gliders, both unpowered
and powered. The small size (and often similar span to length ratio), make these more
likely to be misreported as a UAP than ignored, as would be the case for a more
conventional aircraft. Different timing windows that can be taken into account for UAP
event analysis. Normally, low flying night flights will show navigation lights.
MIXED AIR ASSETS
12. Except for towing aircraft for gliders, other fixed wing aircraft, especially fast low
jet aircraft are prohibited from glider and hang-glider sites. Hence, within those areas,
a useful filter is that UAP events cannot be
misinterpreted as other military or civil operations. UAP reports from within these areas
are therefore due to either gliders or hang-gliders, or other natural or man-made objects,
which may enter the airspace, (e.g. birds, balloons), or "genuine" UAP events. Note should
be taken of the fact that these sport aircraft, though in use at all times during daylight,
when weather conditions allow are more likely to appear at weekends and holidays.
HELICOPTERS
13. Although helicopters can be seen anywhere and under certain conditions (as a disc
illuminated from above or below) are reported as a disc-type UAP event, this is more likely
to occur within the UK helicopter routes shown in Figures 11 to 14.
AIRCRAFT LOW FLYING ROUTES
14. Although, in principle, the whole of the UKADR is available for low flying (down to
an altitude of 2500), in practice, and excluding the prohibited and restricted areas, such as
danger areas, major conurbations and other specified areas, low flying is limited to the
designated low flying areas. In three designated areas, fly down to 100ft. Although they
are theoretically available for 24hrs per day, low flying is prohibited over land areas
between 2300 and 0700hrs, with few exceptions for non-jet aircraft. This is rare enough to
warrant special permission and then only normally at Fridays. Weekend and Public Holiday
flying is only permitted for small-scale, pre-arranged exercises, and only from 0800-1900,
with the exception of some aircraft used for parachute training. An obvious exception is
that of Search and Rescue operations and helicopter training over sea at weekends and on
Public Holidays. The UK Low Flying System is exclusively for UK aircraft, UK aircraft
based in Germany and NATO aircraft on approved
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flights. Special approval is required for other (non-NATO) nations, who must not fly below
2000ft AGL. Exceptionally UK light fixed wing aircraft may fly down to 50ft.
VISIBILITY FOR LOW FLYING
15. Strict rules apply to visibility for low flying. This is of interest in the UAP context,
as clearly this filters out all manned aircraft if certain conditions exist:
- For low flying aircraft (in excess of 140kts), there must be a forward visibility of at
least 5km and 1500ft horizontal surface or 500ft vertical separation from cloud.
- Light aircraft must have a forward visibility of at least 2km, be clear of cloud and
sight of the surface.
- Helicopters, (flying at 140kts, or less) must either be clear of cloud and in sight of
the surface, or apply the same rules as for low flying aircraft above.
AIRCRAFT LOW FLYING AT NIGHT
16. The UK Night Low Flying System (UKNLFS) is a source of potential UAP erroneous
reports. Restrictions apply as shown at Table 1 with timing that can be taken into account
for UAP event analysis. Normally, low flying night flights will show navigation lights.
AIRCRAFT IN FORMATIONS
17. In the UK Low Flying System a formation is not normally to exceed four aircraft, but
North of 54 degrees North formations of up to 8 aircraft may be flown permitted for various
operational activities.
Special permission is required to exceed these rules and the incidence of larger formations is
very rare.
SPEED WHEN LOW FLYING
18. The maximum speed (all aircraft types) is 520kts.
USE OF RE-HEAT OR AFTERBURNER
19.A characteristic of some UAP reports is that of glowing objects in the sky. Except for
emergencies, it is unlikely that after-burners will be used overland at low altitude at less
than 1000ft for most aircraft. The Jaguar is an exception (500ft)
FREE-FALL PARACHUTING
20.A brief glimpse of a parachute can be sufficiently ambiguous as a UAP sighting.
Manned aircraft are prohibited from the designated parachuting areas. Normally,
parachuting only takes place in daylight.
OBSTRUCTIONS & POWER LINES
21. During analysis it should be noted that while a UAP (e.g. Ball Lightning) may be
observed near to tall structures, aircraft, the crews of which will be aware of these, can be
eliminated, as they will not fly close by. UK tower heights are at 500 and 1500[ILLEGIBLE],
not 1ft. Slow inspection aircraft can be expected in the vicinity of electrical power lines.
PROHIBITED & AVOIDANCE AREAS
22. For the purpose of evaluation of UAP reports it is possible to filter out fixed wing
aircraft (notwithstanding any infringement), where sufficient UAP evidence exists to
determine that its altitude was observed below the avoidance area minimum altitude
(2000ft AGL).
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MONTH START END
JAN 1630 0900
FEB 1730 0700
MAR 1930 0430
APR 2100 0330
MAY 2130 0300
JUN 2100 0300
JUL 1930 0300
AUG 1930 0430
SEP 1830 0430
OCT 1730 0600
NOV 1630 0800
DEC 1600 0800
NOTE: All times Zulu
TABLE 1 LOW FLYING NIGHT-TIME PERIODS
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[PHOTOGRAPH: SR-71 aircraft in flight over mountainous terrain]
FIGURE 1: SR-71 IN FLIGHT (NASA PHOTO)
[REDACTED IMAGE]
S.27
FIGURE 2:
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[TECHNICAL DRAWINGS: ALA-40 thermoplane concept, top and side views]
[PHOTOGRAPH: ALA-40 proof of concept thermoplane under test, large disc-shaped craft on ground]
FIGURE 3: THE ALA-40 PROOF OF CONCEPT THERMOPLANE UNDER TEST AT
ULYANKOVSK IN MID-1992 (P. DUFF)
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[TECHNICAL DIAGRAM: Cross-section and structural diagram of ALA-600 Thermoplane with numbered components]
Structural details of the Thermoplane ALA-600:
1. Front vertical and horizontal stabilizers
2. [ILLEGIBLE]
3. Hot and Cold gas volumes
4. [ILLEGIBLE] balloon spheres
5. [ILLEGIBLE]
6. [ILLEGIBLE]
7. [ILLEGIBLE] Turbojet motors
8. Cargo platform
9. Engines
10. Staff quarters
FIGURE 4: ALA-600 THERMOPLANE (RUSSIA)
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[REDACTED IMAGE]
S.27
FIGURE 5:
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[TECHNICAL DRAWINGS: Lockheed F-22A production configuration, multiple views including side view of two-seat F-22B]
FIGURE 6: PRODUCTION CONFIGURATION OF LOCKHEED F-22A WITH
ADDITIONAL SIDE VIEW (TOP) OF TWO-SEAT F-22B (JANES)
[TECHNICAL DRAWINGS: Lockheed F-117A Stealth Attack Aircraft, multiple views]
FIGURE 7: LOCKHEED F-117A STEALTH ATTACK AIRCRAFT (JANES)
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[TECHNICAL DRAWINGS: Stealthy UCAV concept showing 'roll-over' technique, top view, side view, and cross-section with labels: Two-fin detail, Cross-Section, Low radar penetration offensive slotting]
FIGURE 8: A STEALTHY UCAV CONCENT DEPICTING THE 'ROLL-OVER'
TECHNIQUE FOR REDUCING RADAR CROSS SECTION (TOP RIGHT)
(JANES)
[TECHNICAL DRAWING: B-2 Spirit Stealth Bomber, top-down view with internal structure visible]
FIGURE 9: B-2 'SPIRIT' STEALTH BOMBER (USA)
(JANES)
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[MAP]
THAMES VALLEY
AVOIDANCE AREA
HANG GLIDING SITES
[Map shows grid areas labeled AREA 1A, AREA 1B, AREA 1C and surrounding regions with hang gliding site markers]
[Box, upper right]: THESE CHARTS ARE GRAPHICAL
REPRESENTATIONS ONLY AND ARE
NOT INTENDED AS NAVIGATIONAL
PLANNING AIDS
FIGURE 10
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[MAP]
HELICOPTER ROUTES
MORECAMBE BAY/LIVERPOOL BAY
[Legend box with small text — ILLEGIBLE at this resolution]
LOW LEVEL TRAFFIC INFORMATION SERVICE
IS AVAILABLE FROM NORFOLK 384.6 MHz
[Map labels visible include:]
BARROW
WALNEY ISLAND
FLEETWOOD
BLACKPOOL
LYTHAM
MORECAMBE
LANCASTER
HEYSHAM
HAMILTON NORTH
HAMILTON
BLACKROD
KIRKHAM
FIGURE 11
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[MAP]
HELICOPTER MAIN ROUTES
NORTHERN NORTH SEA
[Map shows latitude lines 55°N through 61°N with helicopter routes radiating from Aberdeen area]
[Locations visible include:]
EDAY
DUNDEE
ABERDEEN
[Various offshore platform/field labels — partially ILLEGIBLE]
LOW LEVEL TRAFFIC INFORMATION SERVICE IS
AVAILABLE FROM ABERDEEN 124.60MHz
[Box, lower right]:
THESE CHARTS ARE GRAPHICAL
REPRESENTATIONS ONLY AND ARE
NOT INTENDED AS NAVIGATIONAL
PLANNING AIDS
FIGURE 12
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[MAP — landscape orientation]
SOUTHERN NORTH SEA HELICOPTER ROUTES
[Map shows helicopter routes across the Southern North Sea with offshore field/platform labels — most labels ILLEGIBLE at this resolution]
FIGURE 13
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[MAP — landscape orientation]
HELICOPTER MAIN ROUTE
BETWEEN HUMBERSIDE AND THE
ROUGH AND WEST SOLE FIELDS
[Map shows helicopter routes with offshore field labels and coastal locations — smaller labels ILLEGIBLE at this resolution]
FIGURE 14
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[MAP]
LOW FLYING AREAS 1A, 1B
and 1C
HANG GLIDING SITES
[Map labels visible include:]
THAMES VALLEY
AREA 1C
[Additional area labels and hang gliding site markers — partially ILLEGIBLE]
[Box, upper right]: THESE CHARTS ARE GRAPHICAL
REPRESENTATIONS ONLY AND ARE
NOT INTENDED AS NAVIGATIONAL
PLANNING AIDS
FIGURE 15
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[MAP]
LOW FLYING AREA 2 and 2P
HANG GLIDING SITES
[Map shows low flying area boundaries with hang gliding site markers — smaller labels ILLEGIBLE at this resolution]
[Box]: THESE CHARTS ARE GRAPHICAL
REPRESENTATIONS ONLY AND ARE
NOT INTENDED AS NAVIGATIONAL
PLANNING AIDS
FIGURE 16
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 10
LEY LINES, EARTHLIGHTS AND UK EARTH FAULT LINES
e Para Page
LEY LINES 1 10-1
Study Objective 7 10-2
ELECTRO, THERMO AND TRIBOLUMINESCENCE 10 10-3
EARTHLIGHTS 13 10-3
Summary 14 10-5
EARTHLIGHT REACTION 15 10-6
HISTORICAL 16 10-6
GEOLOGICAL 17 10-6
January 26, 2000 -i- XKXXXKKMOK S.4.0
aia). va a oP
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> ' ce ent 4
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reference to ancient sites and markers etc.
LEY LINES, EARTHLIGHTS AND UK found on Ordnance Survey Maps
EARTH FAULT LINES
LEY LINES
rE This aspect is briefly investigated
because of the suggestion that the location of
Gk me eee Salt alt ee
linked in some way and even in coinci : Be i aadinal iat fin and alignment
The same "LEY LINES' wes coined in 192% of ancient sites, such as stone circles, the
from the old terminology the 'lay' or 'lie' of results of which have suggested that these
the land. were accurately constructed (and that ancient
¢ civilisations must have had knowledge beyond
2. The suggestion of a UAP connection expectation). In the UK much of this is based
seems to have originated from a French on 'accurate' measurements of standing
investigator who postulated that there was a artefacts (which often turn out to be spaced at
'tendency for UFO sightings to appear in multiples of ~2.72 feet - the so called
straight lines'[1]These were then called 'megalithic yard' - a human pace!)
6. In the research briefly explored the
3. Further investigators ({2] and [3]) alignment of three such sites is statistically
respectively linked archaeological and invalid. Four-point ley lines are also rejected
astronomical interests to the theory. as inadmissible on the grounds of probability.
However, 'ley lines' of many objects spread
(or nearly straight) line which some have
connected with ancient sites. These comprise 7: Rationale The only significance in
hill forts, stone circles, earthworks (e.g. long including LEY LINES in this UAP study was
ae burrows, mounds), stone markers, ancient to note that (should clusters of sightings or
abbeys and churches built on old pagan lines of sightings appear) in the analysis, ley
locations. The postulation is that these are lines may be a factor, since some of the
found to be in alignment or near-alignment. locations which form ley lines involve rocky
There is other evidence that they often occur formations. Hence, there may be a tenuous
over water-bearing underground _ fissures. connection with tribo-or chemi-luminescence,
They are also supposedly associated with where certain archaeological formations are
'magnetic currents (or some type of unknown said to produce visual effects when they
'current' or "force') which allow, for example, fracture. There may also turn out to be some
water to be located by some, while seeming to sort of connection with the carth's
have physical effects on others. On occasions geomagnetic field. The action of rocks
a plan of several ley line groups has fracturing to produce light has been proven in
(reportedly) shown replica astronomical laboratory experiments. | One particular
patterns (e.g. BEAR). Numerous plots of Norweigian location where this has occurred
these 'ley lines' can be made by simple consistently, with similar rock formations to
parts of the UK.
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8. Hessdalen is a small valley in the all the way from 0 to 30,000
middle part of Norway, South East of knvhour. Sometimes the
Trondheim. In that valley strange unknown radar saw something moving
lights first showed up hundreds of times at a low speed, but no lights
between 1981 and 1985. It was given the were seen by eye. Clearly,
name "The Hessdalen Phenomenon"and the something was there, but only
project was linked with the Norwegian the radar could detect it.
Defence Research Establishment.
- Laser
9. In June 1983 "Project Hessdalen" A lemerbem wes disected
started, the main purpose of which was to toward the light and the
collect as much scientific data as possible. tchevicer of te light
During the autumn a research programme was reportedly changed. Out of
established, and the work in the field started mie cocesions the light
21 January 1984 and ended 26 February 1984, er % Sgt mnpe,
m — oy > ents pe state when rete
—— 'aeaieal . was switched off There =
=, Camera with grating could, of course be several
Three pictures showed a interpretations placed on this
continuous spectrum but no phenomena [the most bizarre
spectral-lines were seen. of which is that known as a
"Close Encounter of the Sth
: IR-viewer kind' - see Volume 1 of this
This instrument was used too report]. A more realistic
little to draw any conclusions. explanation may be that the
laser light, being coherent,
Sometimes there were electro- light/energy supplied by the
magnetic _— signals ~—with 'earthlight' to produce a
harmonics of about 80MHz. different colour for the human
observer - which would then
. Seismograph clearly revert to its original
No local _seismographic colour unless some other more £
activity was detected. [This, permanent or ongoing change
of course is contrary to the was taking place anyway -
expectation of the effect being for example a decay in the
initiated by normally energy of the airborne mass
- Geiger-counter
= Magnetograph
The magnetic field did No radioactivity was detected.
sometimes change when the But the source was lkm away
lights showed up. There also when this instrument was
seemed to be a correlation used. Sometimes the lights at
with the magnetic pulsation. Hessdalen lasted for more
than two hours in one place
- Radar before they moved. Literally
The lights could be seen on hundreds of instances have
the radar. The speed varied
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been reported, as to seven
times a week and two to three
times a day.
Despite all the blanks drawn during the
investigation some 20 scientists researched the
phenomenon during 1994 and their reports
were either not available or not available at
the time this MoD study was made.
ELECTRO THERMO AND TRIBO-
LUMINESCENCE FROM ROCK
FORMATIONS/EARTH FAULTS
10. Statistical studies have shown [1] that
geology and UAP events tend to be linked.
Research [2] in 1977 confirmed that (French)
events reported over 25 years correlated with
locations of rock formations and a similar
study in Leicestershire (1972-1977) gave
almost the same statistical results. In 1981 t
he US Bureau of Mines carried out
experiments in which granite core was
crushed under darkened test conditions in
which recordings were made and a line was
established between anomalous aerial lights
and geological sites.
11. Although these luminous effects were
earlier attributed to piezo-electric action
several other scientific explanations have been
proposed, including natural radioactivity,
cosmic rays and light from friction or tribo-
luminescence. The latter would involve
reactive electrons moving between conduction
and valence bands in three-dimensional lattices
and which contain defects. Some connection
with tribo-luminescence is also reported - a
simple example of which would be the
electrical charging of materials by friction -
Tribo-luminescence is the emission of visible
radiation due to frictional forces - in effect
'cold light emission'.
12. Example, fault lines where
'Earthlights' have been seen are shown at
Figure 5. It is clear from other sources [3]
that sightings are often directional rather (as
might be expected) omni-directional, that the
observer must normally be within a few
hundred metres of the phenomena and that the
lights appear within a few hundred metres of
a rock (old) fault-line. Overseas,
particularly in the USA, there is evidence of
increased UAP sightings in areas of tectonic
volatility – for example in the Cascade
Mountain Range in Washington State. The
description of these correlates with light seen
in Leicestershire, first prior to the 1957 UK
earthquake.
EARTHLIGHTS
13. The phenomenon of 'earthlights' is
based on the fact that physical and electronic
forces accumulate in areas of seismic activity,
possibly over weeks or months, and the
resultant stresses in rock formations could
result in rock fractures. At the moment of
fracture (and proved by laboratory
experiments) light is emitted. Electrically
charged particles before bursting, which is
manifested as light when the fracture occurs.
Whereas an earthquake releases energy in a
major form, pre- and post-earthquake stresses
are the likeliest time for earthlights to be
reported. It is claimed that this anomalous
light phenomenon occurs:
(a) Along the earth's faultlines.
(b) At ± 2km from the faultline
(though some references state
and exceptionally 20km from
an epicentre).
(c) At land or sea (underwater
faultlines, for example, Loch
Tay). On some occasions
the lights have sometimes
been described as green and
'globe shape' but have been said
to change to triangles
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(d) When exceptional
meteorological conditions are
present.
(e) When increased man-made
pollution (air particles
capable of holding a charge)
are present.
(f) When there is a gaseous
presence or chemi-luminescent
(i.e. rock to rock friction) also
occurs.
The key characteristic are:
(a) Balls, streaks, sparkles or
phosphorescent arcs, wisps of
formations or 'boomerangs'.
(b) Lights that change shape, fly,
occur near the surface or at
height and are often described
as 'domed', 'domed' or
'surged'.
(c) Mostly reports are likely at
night, even though the
phenomena occur in daylight.
(d) An (apparently) scouted shape
is found.
(e) Sounds are sometimes heard.
(f) An emission of EM waves (or
other unknown energies) in a
variety of forms are present.
(g) Shapes appear and disappear
and normally take the form of:
- Triangles 'with
rounded corners'
- Discoids
- Spheres (Globes,
Boloids and Orbs)
(see also (i) above).
- Tadpoles (square
front with tail).
These can all flash, 'flutter', 'flicker'
or 'fly' in motion. Occasionally they
are described as 'basketball' size, but
diameters of 4 to 100m have been
reported.
(h) More than one light can move
together, leading to the
impression:
- That they are each
certainty of a solid object.
- That they have some sort of
intelligence which regulates
their spacing.
(i) Lights can merge or split,
often giving rise to some
reports, the impression that
they are intelligently controlled (see also
para 15 below).
(j) Between lights in a cluster
there is the appearance of
blackness in outline. Three
lights, for example, give the
appearance of a solid triangle
and this is an effect - the
brain will interpret what it sees
clearly seen as 'blacker' than
the background in absolute
absence of light.
(k) Lights may move towards a
witness when approached.
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(l) Lights seem to be attracted
(frequency of occurrence is
apparently higher) near to:
- Mountain peaks,
quarries, rock ridges,
caves and mines. (20
cases of sightings in
the 1920's era in
Chipping Norton area
of Oxfordshire and in
limestone quarries of
Banbury e.g. 1923).
- Power lines,
transmitter towers.
- Water.
- Areas of mineral
deposits.
(m) In daylight they appear as
'metallic' discs, hazy glows
or haloes or 'cloudy cigar
shapes', but colours have
been reported, mainly an
amber-yellow and white; with
rapid colour changes. When
red is reported the core is
often described as red. A well
reported example appeared on
the Fakenham-Norwich road
in 1908, lasted 20 minutes,
had a red core and was 50-
60ft high.
(n) Low-level seismic activity is
apparently necessary.
(o) The phenomenon appears to
be 'weightless'.
(p) Some can be seen on radar –
others not. (see Working
Paper 5 & Volume 3)
SUMMARY
14. Some comments can be made about
the long list of earthlight attributes
above.
(a) Electroluminescence is understood to
be the release of luminous energy from
rock when electrons move from higher
to lower energy levels due to friction.
(b) Fault lines and 'ley lines' often
coincide, as do the ancient buildings
(stone circles, religious sites (often
Christian churches, built over former
Satanic worship sites, etc.)
EARTHLIGHT REACTION
15. It is noted (at para 8-Hessdalens) that
the earthlights reacted when remotely
irradiated with a laser. (No further
information is available, as the Hessdalen
report is still in the process of being published.
It is of interest, however, that a Ship's Captain
(in the Baltic Sea) claimed (in 1951) that
earthlights were triggered 'on' by his ship's
radar. The lights 'took the form of
phosphorescent arcs which gyrated clockwise
and anti-clockwise.' Working paper 8 & 9
on 'SPRITES' considers this phenomenon
further.
HISTORICAL
16. It is of interest that the phenomena of
earthlights has been observed for, perhaps,
thousands of years. In medieval and Victorian
times these were variously described as
'Spook Lights', 'Luminous Vapours', 'Fairy
Lights' (Ireland), 'Fireball Spirits', 'Kitty
Candlestick', 'Ignus Fatuus', 'Jack-o'-
Lantern', 'Boggarts', 'Dragons', 'Will-o'-the-
Wisp', 'Corpse Candles' and 'Orbs' (Windsor
Castle early 1990s). It remains likely that what
is seen becomes matched to the understanding
of the day. What was once a simple type of
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misunderstood apparition, becomes a space-
craft or similar 20th Century-related
technology entity. They were frequently
connected with swampy or marshy conditions
on the one hand and described as having a
yellow core, violet edges and sometimes red.
More recently some have been attributed as
being methane-based (CH4) with a trigger of
P2 H2 (hydrogen phosphide).
17. As a sample of the pedigree of what is
reported today, much further back (AD 584)
brilliant rays of light which seemed to collide
were reported and (in AD 583) 'rays' or
'domes' were observed in France. On 3
August, AD 989, three brilliant round objects
were seen to join together. A fire breathing
dragon came out of the sea. In Japan a
'spinning ball of fire like a red wheel hovered'
– with many witnesses. While from the terrace
of Windsor Castle on 18 August 1783 four
eminent scientists (including Fellows of the
Royal Society) observed and reported
(Philosophical Trans. Royal Soc 1784) an
object which hovered, moved, changed
luminosity and changed shape, brightened and
finally exploded (This, in fact was probably
ball lightning rather than an earthlight). Other
historical earthlight arenas (which will be
relevant when a database analysis is done for
the present day) are:
- Llwndeb, Barmouth and
Harloch (see Ley Line/Fault
Line map) and Llangolan.
( 40 mile wide strip).
- Haverfornwest, St. Brides
Bay, Milford Haven, 'Stack
Rocks'.
- Colwyn Bay to Shotton
(24km wide extension island).
- Denbigh (e.g. 1979 and
1984).
18. During the Second World War what were
(now understood) clearly earthlights were
reported by Commander-in-Chief Devonport.
In 1915 Naval Intelligence investigated
earthlights in the Isle of German Bight (?)
both in the Warminster and Dartmoor areas
and further displays are recorded in 1981 at
the Standing Stones of Drizzlecombe. Similar
phenomena are reported in the USA. These
are often reported for several days, weeks or
months in a particular area – after which they
are not seen again, perhaps for years.
19. It appears that there may be more than
one type earthlight since medieval minors were
well aware that their interest in the phenomena
was the proximity of earthlights to copper and
iron ore.
GEOLOGICAL
20. As an aid to the statistical analysis of
locations of UAP reports, Figure 8 shows the
geological structure of the UK. This may be
required if it becomes necessary to:
- Isolate what are believed to be
earthlights to specific geographic
and geological locations and types
of rock formation.
- Further correlate (and thus
eliminate those UAPs) with rock
types known to produce earthlights
when under seismic stress, (as it is
suggested that low magnitude
seismic disturbance may be
sufficient to provide the conditions
for light phenomena).
21 Fault Systems. There are several Earth
Fault Systems which cross the United
Kingdom. The location of these is shown for
the whole country (known as the DENT Fault
System) at Figure 9.
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BIBLIOGRAPHY
[1] "Flying Saucers & the Straight Lines
Mystery Criterion" Michal Aires
1958.
[2] Ley Lines in Question" Williamson &
Bellamy ISBN 0437-15205-8.
[3] The View over Atlantis" J. Mitchell
SAGO Press 1969.
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[PHOTOGRAPH: Two orange/reddish lights against dark background]
FIGURE 1: UK EARTHLIGHTS (OR POSSIBLY BALL LIGHTNING)
NOTE: Location Carismas Moor, Skipton, Yorks; police photograph (copyright Sgt. Anthony
Dodd)
[PHOTOGRAPHS: Two images side by side showing amber light against dark background]
FIGURE 2: PROBABLE UK EARTHLIGHT (OR PLASMA/AEROSOL OR CHARGED
PARTICLE VORTICE)
NOTE: location Rossendale, Lancs. (copyright David Milner)
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[PHOTOGRAPH: Red/orange glowing object against black background]
FIGURE 3: TRIBOLUMINESCENCE
NOTE: Laboratory-produce as a result of rock crystal fracture (copyright P. Devereux)
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[PHOTOGRAPH: Three reddish/orange objects of varying sizes against black background]
FIGURE 4: EARTHLIGHTS
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[MAP: Outline map of the United Kingdom with earthlight locations marked as stars]
L. Carloway
Berbecula
Latheronwheel
Garvie Bay
Garroch Bay
Oban area
Llanbedr
Barmouth
St. Brides
Bay area
FIGURE 5: UK EARTHLIGHTS LOCATIONS (P. DEVEREUX)
NOTE: Frequent earthlight reporting areas shown as stars. Larger stars indicate greater
frequency of sightings.
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[DIAGRAM: Cross-section showing fault lines near Warminster]
Warminster
Cley Hill
Warminster Fault
Longbeat Fault
FIGURE 6(a): CLEY HILL FAULT-LINE (NEAR WARMINSTER) (P. DEVEREUX)
[DIAGRAM: Map showing earthlight ball/ball lighting course with dotted track line]
FIGURE 6(b): EARTHLIGHT BALL/BALL LIGHTING COURSE (P. DEVEREUX)
NOTE: 1984 Wrexham to Thackley (near Shipley). Boldines solid, phenomena track dotted.
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[MAP: Coastal map of Barmouth-Harlech area, Wales, with fault lines and earthlight locations marked]
Pontlleurfa
HARLECH
Llanfair
Pensarn
Dolfrey Ardudwy
Llyns Aardudwy
Egrin Chapel
Bondeldu
● Barmouth
BARMOUTH
FIGURE 6(c): FAULTLINE BARMOUTH-HARLECH, WALES
NOTE: Particular earthlight activity 1984-5 and since.
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[MAP: Sketch map of the Pennines region showing earthlight zones]
AREA 6
LEVBURN
AREA 5
CLITHEROE
PENDLE
BLACKBURN
BURNLEY
KEIGHLEY
ILKLEY
SHIPLEY LEEDS
AREA 4
BRADFORD
HALIFAX HUDDERSFIELD
WAKEFIELD
AREA 3
OLDHAM
MANCHESTER
Devil's Chair
Lowden Fell
SHEFFIELD
[ILLEGIBLE]
FIGURE 7: 'PROJECT PENNINE' EARTHLIGHT LOCATIONS
NOTE: A simplified sketch map of the area of the Pennines found by Project Pennine to harbour
zones of repeated earthlight activity.
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[MAP: Geological map of United Kingdom - northern section (Scotland and northern England), colour-coded by rock type]
I S H S E A
FIGURE 8: Geological Structure of UK
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[MAP: Geological map of United Kingdom - southern section (England and Wales), colour-coded by rock type]
ENGLISH CHANNEL
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[MAP: Geological map continuation - additional section, colour-coded by rock type]
[ILLEGIBLE]
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INDEX
[LEGEND: Colour-coded geological map key with rock type descriptions]
[ILLEGIBLE]
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[ILLEGIBLE]
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[ILLEGIBLE]
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[ILLEGIBLE]
[ILLEGIBLE]
[ILLEGIBLE]
[ILLEGIBLE]
[ILLEGIBLE]
[ILLEGIBLE]
[ILLEGIBLE]
[ILLEGIBLE]
Note: the dot only specifies deposits for symbol [ILLEGIBLE]
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[MAP: Tectonic and fault system map of UK and surrounding North Atlantic region]
LAURENTIAN GREENLAND SHIELD
0 KM 1000
MARITIME PROVINCES
[Map labels include: CALEDONIAN ZONE, HATTON BANK, North Atlantic, Fenno-Scandian Province, Midlothian Terrane, GRABEN RIFTS, Wrench Faults, EAST MIDLANDS PLATFORM, FSS, DFZ, CELTIC SEA, WESTERN APPROACHES]
FIGURE 9
KEY
AL- ALSTON BLOCK
AS -ASTRIGG BLOCK
DFZ- DENT FAULT ZONE
DHFZ - DOWSING HEWITT
FAULT ZONE
WNB -WEST
NETHERLANDS BASIN
FRACTURES
ILIGHTS
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WORKING PAPER NO. 11
COLLECTED IMAGERY AND CLASSIFICATION OF UAP SHAPES
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COLLECTED IMAGERY AND CLASSIFICATION OF UAP SHAPES
CONTENTS
1. The material in this section has been collected from a number of sources - news
reports, photography and video records. The sources are not limited to UK reports, as the
intention is to use the material as a reference/correlation catalogue and to hopefully use the
material as a filter to separate the explainable from the inexplicable, if possible. In some cases
– particularly since the advent of personal video cameras – the original material is in colour.
Shape and light colours (colours) are therefore the trigger which identify the end results in
incident reports. Shapes have been generically categorised as follows:
- SPHERES (Includes 'BOLS' and multiple Figures 1 – 7
spherical lights)
- DISCS (Only circular in plan – and thus, on Figures 8 to
frequent occasions from different 28.
aspects, the same event may be
described by other witnesses as
'balls' or spheres)
- CIGAR These have a larger mid-chord than Figure 29
discs and tend towards 'long airship'
shapes, with much less 'sharp' ends
than discs
- STAR/POINT Seen as balls of light, with the star -
effect due to atmospheric optics
- OVAL Described as a variant of 'discs', but -
with a wider mid-chord and without
(the sharpness of 'cigars')
- TRIANGLE/PYRAMID/CONE/ The outline shape is formed, not by a Figures30 to
RECTANGLE/CYLINDER solid object, although not a simple 35
outline – but by three or more coloured
lights at its extremities, forming the
'corners'. A cylinder is often
described which is, in fact, formed by
a row of lights (balls). A vertically
oriented cylinder is sometimes seen –
see Working Papers No 21 and 24
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- RECTANGLE/DIAMOND As for Figures 30 – 35, but where the As for
flying angle changes the lighting to Figures 30-
form diamond/rhomboid patterns 35
- BOOMERANG/ARC Figure 36
As can be seen (Vol. 1 Tables 1 and 2) certain combinations of shapes and lights can be
attributed to definite causes. Shapes and lights are the initial key to filtering the known from
the inexplicable. Little is gained in analysis of purely descriptive unknown shapes and lights
reports unless further information, such as imagery, correlation from multiple witnesses, or
data from which to obtain angles, sizes, sounds, smells, or velocities is available.
For the purposes of the database it was necessary to identify the whole range of shapes
frequently reported. It is of course inevitable that these are due to a whole range of different
underlying phenomena, described in the other working papers in this Volume.
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SPHERES
08:53:07 |
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FIGURE 1: SPHERES
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FIGURE 2: KENT UK, SEPTEMBER 17-20 1993
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11.) AGEQRBTA b= er
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FIGURE 3: MEXICO POLICE PHOTOGRAPH ™ (JULY 1991)
Note [1] Four police officers at range ~5O0 yards. Some lens distortion.
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% wool * Py
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FIGURE 4: LOWESTOFT 1997
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ee
A a e a ied & af T
ee
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|
a deg Ste A oe AP ae earl ea yee rs seg Ei lt er ae ee ere ka oT Sake
Sai teh Shas bee eat We em PSN Le Ma ee Peg peer y ie edie, |i er Eg of
aes Rey tats Wie Reg NE Ey gor ees De oF on Bra Ma Ae ne aD sae Sr Pa
ong eta i. ees + Ce bet Sate het)
Poe eae SEE melhor ae re ad i a i We re ee Pole. Pisa Deas TiS Tag et
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w z wy
i -
ae : —" z
i Poe
FIGURE 6: FRANCE 1974 &
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= - a [ae
FIGURE 7: AIR-TO-AIR UAP
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|= i chtand a4 dans - jy ll
DISCS Ee eal
all le ee a ey
a a ee a a ee ee
FIGURE 8: LAKE CONISTON ENGLAND 1954
FIGURE 9; JAPAN 1958
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* FIGURE 9: AUSTRALIA 1972
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li cepiach
i UK RESTRICTED ; |
oe" he i
'
\
\
baat Nic
FIGURE 10; AUSTRIA 1971
FIGURE 11: OREGON USA 1950
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'ww i W of Lome ee ed ee
-_
cd —
FIGURE 12: 1958 SOUTH ATLANTIC (BRAZILIAN NAVY)
; "
—_?
FIGURE 13: USA 1952
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3 Pe he . os aad ;
| SF 7 2 5
i ™,
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'ts
-
FIGURE 14: ual
'Sala ae ee ater Tiebeag e 8 pet oe
Tyee Mata ess oi igl RaNR oe o ogted aera Oe 5 aa Cate ae
9F-] fiber tei aah as a ic rs ee ad Cee ae
¥ k 4
FIGURE 15:
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€ ahi
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Gee fad light
FIGURE 16: POLICE SKETCH 26 APRIL 1984 UK
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wi YY /
: sd
FIGURE 17: SILVER DISC (20-30 FEET DIAMETER) 1993
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ay UK RESTRICTED ;
INC SSRRED I CI
= ! ges Es
HT econ, | RR ee ill ey eae eee
a He. oa. ae glee NA Sie
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tebe cet. 2S ec 1, as
aoe AADC Eee EUSA EE gl ss
Pecan Teeenpr | SIM p ARR ol oer |
FIGURE 18: PERU
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PIRIAL AAAITE=@ es
a | . 1
a se ele
a UK RESTRICTED |.
FIGURE 19(a): OPEN SKIES - CLOSED MINDS [N. POPE]
' ry
z Py *
. |
» # = '+
: - a @
el
a0 "e
* = _
ba » *
FIGURE 19(b): OPEN SKIES - CLOSED MINDS [N. POPE]
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FIGURE 20: JAPAN (TOKYO) SEPTEMBER 1986"!
Note [1] Sixteen witness event for 25 minutes 180 miles North of Tokyo. Appeared to rotate.
11-19
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| IATIORG Pie | rie
i i UK RESTRICTED rr"
FIGURE 21: ARGENTINA - LAKE BARILOCHE (~1978)
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FIGURE 22: CANADA - VANCOUVER ISLAND 1981
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a a : a ,
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i j , f [a ) a
INF/SEORE a
VWJied beetii bi
ir aes i Ge ee Ne cee ee ea
eae. ae OE a eee
CORES ee a ee ee
ee ae
eer. Se i ee i ea
bac Rete ae Se et a
FIGURE 23: OREGON 1966
Pe SO RU
See cca aioe sae aestuarii ssn as Senor eh
oe AS SOAR Se
URE EGRESS SS pennies neste incerta
(a a eae
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FIGURE 24: MALAYSLA 1966
11-22
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|) | Ukkestriérep =
ie | t.
iv GL EAT,
at I ue? lees fas?
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FIGURE 25: SPANISH AIR FORCE 1976
FIGURE 26: DENMARK 1974
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FIGURE 27: MEXICO (RESPECTIVELY MARCH AND JUNE 1992)
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FIGURE 28: ROCHDALE LANCS., 1975
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'CIGAR' TYPES
FIGURE 29: 'CIGAR' TYPE
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TRIANGLES
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FIGURE 30: TRIANGLES/PYRAMID/CONES
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FIGURE 31: BELGIUM LOCATION EUPEN (2 SECOND AT ZOOM SETTING 100-150MM AT F4) 30-31 MARCH 1979
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FIGURE 32: BELGIUM (AS FIGURE.. ABOVE. BLUE FILTER ENHANCEMENT REVEALED UNDERLYING TRIANGULAR SHAPE (ALL OF WHICH IS VISIBLE ON ORIGINAL)
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FIGURE 33: SOVIET UNION - LOCATION ZAGRESK MARCH 1990 (NOTE UNDERLYING EQUILATERAL TRIANGLE)
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FIGURE 34: VIDEO FRAME - BELGIUM 31 MARCH 1990
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/\
/ \
/ • \
/______\
300 - 800 ft.
FIGURE 35: SHAPE UK, RUSSIA, BELGIUM
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BOOMERANG/ARC
FIGURE 36:
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 12
EARTH'S MAGNETIC FIELD IN THE UKADR
Para Page
INTRODUCTION 1 12-1
FIELD MEASUREMENTS 2 12-1
Field Intensity 3 12-1
Field Angles 4 12-1
Local Variations 6 12-1
UNITED KINGDOM MAGNETIC SURVEY 7 12-1
COMPARISON WITH MEDICAL EXPERIMENTS 8 12-2
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EARTH'S MAGNETIC FIELD IN THE UKADR
INTRODUCTION
1. Earth's magnetic field has been
briefly researched because of:
- The possible connection of
field strength with UAP
events.
- As a comparison with the
magnetic field strengths
used during the magnetic
field experiments reported
at Working Paper No 25.
FIELD MEASUREMENTS
2. Over the period 1987-95 eight
international stations, comprising a Sub-
Auroral Magnetometer Network
(SAMNET) monitored the changes every
five seconds. Earth's internal magnetic
field changes only slowly in direction and
magnitude, but there are also magnetic
effects due to the flow of charged particles
in the upper reaches of the atmosphere (the
ionosphere) and in space. Day plots have
been taken every 1 second, since 1995.
Each station records the magnetic field in
three orthogonal directions. The stations
cover the UK, Sweden, Norway, Finland
and the Faroe Islands.
3. Field Intensity The magnetic field
is calculated (in Nano Teslas) from the
International Geomagnetic Reference Field
(IGRF). The total intensity in the UK is
49,000 to 50,000 nT (1nT = 1ɣ). Changes
in intensity are ~30nT per year. The
horizontal component of the field is about
20,000 nT in Southern UK and 15,000 nT
in Northern UK.
4. Field Angles The field inclination
angle is ~70° with typical changes of one
to two minutes (of angle) per year. For
epoch 1970 the declination angle is
between -6 and -12 degrees, with changes
of ~6 minutes of angle per year.
5. The North magnetic pole is
migrating NW by 9km per year (79.1°N
28.9°E). For the chart shown at Figure, the
1ɣ = 10^-5 Gauss = 10^-9 T = 1nT. The
plotted readings show no sudden or
unexplained variations but rather a steady
decline in magnetic intensity level over the
50 to 60°N lines of latitude straddling most
of the UKADR.
6. Local Variations No information
is available on small variations which may
occur in specific locations. Particularly, no
field peculiarities are present in the main
plots to indicate the possibility of
influencing geographical clustering of UAP
reports.
UNITED KINGDOM MAGNETIC
SURVEY
7. Data gathered nationally by a
network of 51 stations (survey points),
established between 1985 and 1988, allow
local (crustal) magnetic variations to be
monitored. Global models accurately
represent the main part of the geo-
magnetic field, originating in the earth's
core. At the surface there are
perturbations caused by magnetised rocks
and electric currents in the ionosphere and
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atmosphere. While there are errors which
are superimposed on the global model, in
the UAP context it is just possible that the
high density measurements of field
strengths in certain areas may contribute
either singly or in combination with other
factors to produce UAP. The associated
solar phenomena (solar flux and sun-spots)
are considered at Working Paper No 16.
[1] British Geological Survey, Edinburgh
[2] Persinger is Referenced at Working
Paper No 25 which describes the results of
his experiments on the human response to
modulated magnetic fields, which are of
prime importance to the overall findings of
this study.
COMPARISON WITH MEDICAL
EXPERIMENTS
8. A comparison of the national UK
magnetic values at Working Paper No
25 with those used by Persinger and
others, in their medical experiments, has
shown that the key difference between the
experimental field which produces human
responses and descriptions of experiences
surprisingly like those of close encounter
UFO/UAP reports, are those of
modulation. It is noted that the modulated
experimental values used by Persinger,
and which cause the surprising effects on humans, are only about 1/500
of the steady field level experienced daily in
the UK.
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[Map/chart image]
FIGURE 1: INTERNATIONAL GEOMAGNETIC REFERENCE FIELD FOR UKADR
Notes: - Solid lines are total intensity (in Gammas, where 1ɣ = 1nT).
- Dashed lines are secular changes (gammas per year).
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 13
VISUAL METEOROLOGICAL AND OTHER NATURAL ATMOSPHERIC
PHENOMENA
Para Page
LENTICULAR CLOUDS 2 13-1
MAMMA 6 13-1
NOCTILUCENT CLOUDS 7 13-1
MOTHER OF PEARL CLOUDS 8 13-2
DUST DEVILS, TORNADOES & WATER SPOUTS 9 13-2
CONDENSATION AND DISSIPATION TRAILS 10 13-3
GLORY/CORONAS 11 13-3
HALOS & ARCS 12 13-3
SUN DOGS 13 13-4
ST. ELMO'S FIRE 14 13-4
BIRDS 15 13-4
MOTHS 16 13-5
SOLAR RADIATION 17 13-5
SUN PILLARS & LIGHT PILLARS 20 13-5
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VISUAL METEOROLOGICAL AND
OTHER NATURAL ATMOSPHERIC PHENOMENA
1. This paper briefly investigates a
number of additional atmospheric visual
phenomena, mainly meteorological, which
can give rise to UAP reports because they
are unfamiliar to most witnesses:
- Lenticular clouds
- Dust Devils
- Moon and Sun
'Dogs'
- Aurora
- Twisters
- Ice Clouds
- Glory/Corona
- Condensation Trails
and Distrails
- Halos
- Mother of Pearl
Clouds
- Mamma
- Noctilucent clouds
LENTICULAR CLOUDS
2. Examples of lenticular, disc-like
(Lenticularis) clouds are shown at Figures 7
to 9. These are clouds which are oval or
lens-shaped. No further explanation is
required to show that they can easily be
visually mistaken for, or can filter
through into reports of disc-shaped
'UFOs'. Key factors in the filtering process
must be:
- They are usually visible
using reflected light (e.g.
ambient daylight or
moonlight), but on some
occasions they may be seen
in silhouette as disc shapes.
- Lenticular clouds have no
inherent glow (other than
natural external
illumination).
- They will either appear to be
stationary (dependent on
geometry) or move slowly
(at wind rate).
- They will not manoeuvre.
- Conditions to climb are rare
(e.g. through or close to
external agency) conditions
are present.
4. Lenticular clouds often form:
- Over hills
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- At the top of cumulus clouds
to form a 'cap-cloud'
(pileous cloud).
- With a 'metallic grey'
colour.
4. If cumulus cloud below a cap-cloud
evaporates or disperses the lenticular cap
can descend (sink). They can remain poised
or slowly wavering above hills. Lenticular
effects can form with several basic cloud
types, e.g. Altocumulus Lenticularis,
Cumulus Pileus, Stratus-Cumulus
Lenticularis etc.
5. Some photographs ( for example, at
Figure 2) show that lenticularis clouds (or
'wave clouds') can appear as billows (i.e.
ovals/lens-shaped discs with a hole in the
centre) and also with laminated appearance.
Pileous laminations occur when humid
layers are sandwiched between dry air
layers. At Figure 5 little imagination is
required to describe 'a dome on top'.
When the top of a wave-cloud is 'bow-
shaped' and smooth this usually indicates
that the air above is stable and dry. The
size of lenticularis clouds may extend for
kilometres. However, in particular, ice
particles with pyramidal ends are suspected
of producing bright arcs of diffraction at
odd radius halos. It should be noted that
some effects can be related to the
polarisation of observers' sun-glasses!
MAMMA
6. These protuberances occur when
small-scale convection changes cause
portions of cloud to sink in clear air below a
cloud formation. The sinking elements mix
with the clear air and usually evaporate.
However, if they contain rain or snow
crystals, the shapes shown at Figure 6 can
occur. These particularly occur below the
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thick clouds associated with thunderstorms.
Mamma can also occur at the lower ends of
cirrus cloud formations.
NOCTILUCENT CLOUDS
7. Noctilucent clouds have the
appearance of decayed cirrus but are
typically at 80Km altitude in the
mesosphere. They can shine for an hour or
so after sunset but they are not seen if the
sun is above the horizon. If the sun is more
than ~10° below the horizon noctilucent
effects are not seen. Noctilucent
noctilucent clouds appear between May and
August at latitudes 50°-70°N. (This
includes the UKADR.) It is reported
that these may be caused by dust particles
which catch the lower stratosphere during
unique atmospheric dust due to dust produced
in the solar system by collisions among
minor planets. Noctilucent effects can also
be caused by terrestrial-based light sources
shining on the underside of disc-shaped or
laminar clouds. Noctilucent clouds are the
highest clouds in the atmosphere.
MOTHER OF PEARL CLOUDS
8. 'Mother of Pearl' (or nacreous)
clouds (Figure 9) are rare but can be seen
typically at 80Km outside November
and March. They have iridescent bands of
colour. One possible sky is a corona
(limiting the time of occurrence). They
occur only at altitudes of the order 22-
30Km and probably comprise super-cooled
droplets with ice crystals.
DUST DEVILS, TORNADOES &
WATER SPOUTS
9. These occur in unstable layers of
dry air over hot ground. They are visible
because of the dust (which may rotate in
triangular formation). Because no sound
may be heard this increases the likelihood
of an unwary observer, who may only see
the birds for a few seconds as they wheel,
producing a brief visual sensation. A bright
sunlight seagulls have high reflectivity.
The specular reflection from the body reported
by some radar observers can make it a
bird as the bright flash obscures the wings.
Clusters of sightings tend to occur in areas
of 'greatest watchfulness' - for example
near airfields and population centres. The
radar echoing area (i.e. RCS) of birds is
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angle) is said to be 22°. Halos from the sun
can be either above or below the horizon.
Halo activity is persistent and is known to
many of the public, however it results in
some UAP reports. Over a 40 year period
(Netherlands) it was noted that average halo
conditions existed for 227 days of the year,
peaking in 1972, when 300 days were
recorded.
13. On other days conditions existed for
both circular and non-circular events.
Halo Arcs occur in solar elevations and are
caused by pyramidal crystals and occur
when they fall through the air with certain
axes vertically orientated. Halo rings of
unusual radii can be predicted when the
faces are not in random orientation. From
those in random orientation six concentric
odd-radii halos should result at 18.3,
19.9, 22.9, and 23.8 degrees. Each of these
six halo types has been imaged this century,
but most of the 12 (yet undiscovered) forms
are, at most solar elevations, completely
below the horizon and thus only visible
from airborne platforms in cool climates.
The 12 halos divide into 32 individual arcs
in the sky, of which only ten, so far, have
been photographed. Halos still escape a
complete understanding. In particular, ice
particles with pyramidal ends are suspected
of producing bright arcs of diffraction at
odd radius halos. It should be noted that
some effects can be related to the
polarisation of observers' sun-glasses!
Although the photograph at Figure 13 is
artificially produced (a Halo light passing
through a single vertically orientated
hexagonal ice crystal (the periodic spots
shown are the actual projection on a wall),
it is noted that these shapes are markedly
similar to some UAP reports where
'multiple balls' are described.
SUN DOGS
14. A 'sun dog' (parhelion) is a mock
sun, a parhelion (See also para 20 and
Figure 14)
ST. ELMO's FIRE
15. This is commonly mis-identified as
ball (or bead) lightning. It has been reported
for hundreds of years and is a corona
discharge from a 'grounded' point in a
strong electric field, hence, it is usually
observed as a glowing object hovering over
an earthed object before or during a
thunderstorm. It is commonly blue or blue-
white in appearance and about the size of a
large orange. However, much larger
diameters - up to 30cm - have been seen. It
decays (dimly, sometimes slowly and
sometimes quickly), with a lifetime of
(usually) many seconds, which may extend
to minutes. A characteristic distinction
between St. Elmo's Fire and Ball/Bead
lighting is that the latter has motion. The
exception is when St. Elmo's Fire moves
along a conductor.
BIRDS
15. Small flocks of birds (e.g. gulls) can
be reported at night as UAP due to their
reflective under-bellies can be seen in
triangular formation. Because no sound
may be heard this increases the likelihood
of an unwary observer, who may only see
the birds for a few seconds as they wheel,
producing a brief visual sensation. A bright
sunlight seagulls have high reflectivity.
The specular reflection from the body reported
by some radar observers can make it a
bird as the bright flash obscures the wings.
Clusters of sightings tend to occur in areas
of 'greatest watchfulness' - for example
near airfields and population centres. The
radar echoing area (i.e. RCS) of birds is
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briefly considered at Volume 3 as a source
of radar false alarms in the UAP context
Certain areas of the UKADR' (e.g. breeding
areas) are prone to the presence of birds
concentrations, shown at Figures 10 to 13,
and are therefore more likely to be areas
where UAP are mis-reported.
MOTHS
16, Clouds of large moths, usually in
some country areas, can briefly reflect light
and appear as a 'vehicle'. Swarms of
spruce budworm moths are said to be
luminous
SOLAR RADIATION
17. LAZAREV, ? writing in the Journal
of Optical Technology, explains the
'outbreak in Flying Saucers' (in Brazil and
S.Africa) by "atmospheric optical
phenomena which manifest themselves
especially distinctively at twilight, near the
visible horizon of the earth"
18. It is claimed that this is associated with
the increase of optically active air mass,
coincident with sharp reduction of the
brightness of the atmosphere combined with
the enhanced contrast of the phenomenon
against the twilight background. In
particular (in the locations mentioned
above) these formations were observed over
volcanic areas and faded after a time. This
is attributed to Fresnel reflection from
clouds of heated gases (air, CO:, water
vapour, volcanic sulphurous gases, aerosols
etc.). Sometimes these ring-like formations
were observed for several minutes,
19. Lazarev has also reported the entry
of a snowball core (of a minicomet) into the
atmosphere (26 September, 1990) and
possibly again on 20 June, 1992 (at the
PINAL 1)
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MIR orbital complex). The frequency of
occurrence of cores of minicomets into the
earth's atmosphere (observed from space-
station MIR) is assessed at ~20 per minute
SUN PILLARS & LIGHT PILLARS
20. A vertical column of light can
sometimes be seen either below or above
the sun, usually when the sun is at low
elevation angles. Sun pillars are produced
when correctly orientated ice crystals reflect
sunlight or when hexagonal columnar ice
crystals fall through the air with their long
axes orientated horizontally. Example Sun
Pillars and Sun Dogs are shown at Figures
14to 16. Light Pillars are similarly formed
from strong light sources other than the
sun, Itis possible to observe Light Pillars
which do not reach to the ground - another
source of UAP activity with 'searchlights?
beaming downwards
* UK Military Low Flying Handbook
(NATO Restricted) Edition 82 Dec, 1997.
? A I Lazarev, State Optical Institute, All
Russia Scientific Centre, St Petersburgh
1997,
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FIGURE 2: LENTICULAR CLOUD [1]
[1] "Cloud Study". Ludlam and Scorer, Muray 1960
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FIGURE 4: LENTICULAR CLOUD
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RS. Score
FIGURE 6: MAMMA [1]
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FIGURE 7(a): GLORY [1]
FIGURE 7 (b): LIGHT PATH
FIGURE 7(c): TOROID
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FIGURE 9: 'MOTHER OF PEARL'
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FIGURE 14: SUN PILLAR & SUN DOG (R GREENLER)
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00,
WORKING PAPER NO. 14
METEOROLOGICAL BALLOONS
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Radiosonde Launch Sites a AG
Size and Shape 3. ag
Location 4 14d
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METEOROLOGICAL BALLOONS
1. A probable cause of UAP reports which
must be considered is that of radiosondes
and their lifting balloons
2. Radiosonde Launch Sites There are
eight operational upper air stations in the
United Kingdom, just part of a world wide
network of some 900. The stations in the
UK 'release helium- or hydrogen-filled
balloons four times a day at midnight,
midday, six o'clock in the moming and
evening. The transmitter, (the proper name
is a radiosonde), sends back information
about the temperature, pressure and the
water content of the upper atmosphere
Wind speed and direction may also
determine, either by using a NAVAID
system or in some cases, the balloon and
radiosonde are followed by radar. The
distance the balloons travel away from the
launch site is dependent on the wind
strength, but they will quite readily reach a
height of up to 15 miles (about 80,0008)
above the ground before they burst. The
equipment descends on a small parachute.
3. Size and Shape The Meteorological
Office currently useS balloons which are
spherical and 1.5 to 2m in diameter at
launch. The actual radiosonde is
suspended some 30m beneath the balloon
and, for visual purposes, can be ignored
4, Location The location of radiosondes,
con their lifting balloons, is known from
LORAN C: and could be used to eliminate
suspected UAP mis-reporting
'5. The location of the release points in the
United Kingdom are shown at Figure 1
The incidence of mis-reported radiosondes
as "UAPS" is likely to be higher in the
vicinity of these launch sites.
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 15
AIRSHIPS , HOT AIR & TETHERED BALLOONS
Page Para
Object Sizes 151 1
Report Incidence 15-1 2
Meteorological Balloons 15-1 3
Tethered Balloons 15-1 4
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AIRSHIPS AND HOT AIR BALLOONS
1, Object Sizes Airships and hot air balloons
are frequently mis-reported as UAPs, probably
because their appearance in the UKADR is still
relatively rare in some parts of the country, and
the fact that they are at low altitude. However,
ballooning is a growing sport and an increase in
false alarms from this source can be expected
Both UK-produced and imported balloons can
be expected in UK airspace, including balloons
of novel shapes (e.g. cylindrical). The situation
is enhanced by the fact that balloons are often
silent for long periods, and airship engines are
relatively quiet. Table 1 shows a selection of
typical parameters for airships. Balloon
diameters are typically 22m with a height of
26m. The use of gas burners at night is a
particular source of reports of 'glowing
spheres', particularly in Southern England
2. Report Incidence If a number of design
proposals proceed, the incidence of both cargo
and passenger airships can be expected to
increase, however, their appearance will still be
relatively rare to most observers, compared
with other familiar air-objects such as aircraft
and gliders,
3. Meteorological Balloons These are
described at Working Paper No 14
4. Tethered Balloons — While tethered
balloons are less likely to be mis-identified as a
UAP, by stationary observers, an observer in a
moving vehicle may catch a glimpse of a
tethered balloon in the appropriate weather and
1g conditons and submit an event report,
In the UK, tethered balloons of up to 208 in
diameter may fly up to 200% AGL, without
tether streamers (the presence of streamers
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would almost certainly have eliminated many
false reports).
5. It should, however, be noted that the
presence of a tethered balloon may, in fact,
attract an atmospheric UAP which is seeking an
attracting electrical potential, since a charged
mass of air may be attracted to the balloon or it's
tether.
6. Tethered balloons may remain in one position
for up to 10 days
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Length (m) Diameter (m) Height (m)"
Skyship P600 59 16 20
USA 7 35 6.77
USA 39 10 -
USA 2s 8 Z
USA 675 167 202
COLT 34 125 eS
UK 30 n -
GERMANY 68 4 -
TABLE 1 EXAMPLE BALLOON DIMENSIONS
Note [1] Including Gondola
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WORKING PAPER NO. 16
SUNSPOT, AURORA AND SEISMIC CORRELATION
Para Page
SUNSPOT, AURORA AND SEISMIC CORRELATION
Solar Cycle Oa
Auroral Phenomena S164
CORRELATION OF UAP EVENTS WITH SEISMIC ACTIVITY 6 16-2
TECTONIC ELEMENTS OF THE UK 8 16-2
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SUNSPOT, AURORA AND
SEISMIC CORRELATION
i Solar Cycle At the commencement
of the UAP study it was recognised that the
UAP enigma, which has apparently been
present in some form for recorded history,
might be due to a simple natural explanation.
However, itis only in the last 50 years that an
increasingly large number of UAP sightings
have been recorded. While it was recognised
that the phenomenon may eventually be shown
to be due to a combination of natural events,
rather than a single cause, the solar cycle is
cone of the more obvious candidates for
investigation. The frequency of occurrence of
UAP reports against Known earth phenomena,
such as solar activity, has been checked.
However, as this transient solar phenomenon
repeats in an eleven (~11.4) year cycle, long-
'term statistical comparison will not be possible
unless a very large spread of UAP events are
centered into the database and, clearly, it would
not be viable, purely in the interests of Defence
Intelligence, to do 0. Investigations, reported
in Volume 1 of the Study, were necessarily
limited to monthly comparisons taken over a
year. No direct correlation was found for solar
flux or sunspot number. This does not mean
that, in the future, there will not be shown to
bbe some weak correlation, connection or
contribution, when taken together with other
natural effects
2. One of the reasons for considering sunspot
correlation is because the cycle seems to derive
from a more fundamental 23 year magnetic
periodicity on the sun and, it has been suggested,
in some quarters, that UAP and magnetic
activity are connected in some way on the earth
The solar magnetic cycle has a period
approximately twice that of sunspot (flare)
activity. The electromagnetic emissions from
the sun vary in power, penetrating power, degree
of fluctuation and intensity distribution over the
earth. The direct effects of electromagnetic
radiation are confined to the sun-lit hemisphere
of the earth. During each new 11 year eycle the
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polarity of the pattem of magnetic activity
reverses
3. Within the 11/23 year cycle,solar surges
appear (solar flares) which produce complex
magnetic fields. Therefore, even to make
correlations between the frequency of UAP
reports and spurious magnetic activity will
require at least several years of reports in the
UAP database - or ideally, a filter to remove
'identifiable distractors, such as aircraft.
Figures 2 to 4! show portion of the solar
cycles 21-23. Cycle 21 started in June 1976,
Cycle 22 in September 1986 and Cycle 23 (the
current Cycle) in May 1996. It is clear that to
carry out any meaningful statistical analysis a
the dat for a lengthy period of UAP sighting
reports is required, As an initial sample the
daily measurements were obtained for the period
1986-1996 and used for correlation studies
reported at Volume 1
4. Proof of the postulated UAP-solar connection
may be difficult to confirm even if all the statistics
were available because it must be remembered
that UAP statistics will have been significantly
skewed in the more recent decades by the addition
of airships, aircraft, satellites, etc. to. the reasons
for sightings (ie. man-made events)
5 Auroral Phenomena Magnetic and
auroral phenomena (M-Region disturbance) occur
'at 27 day intervals over months or even years
(Figure 1). These recurrent effects are most
prevalent during the last three to four years of the
11 year cycle - unexpectedly when normal sunspot
activity is low. The terrestrial effects are much
less vigorous than the effects caused by flares, but
they can last several days, reaching a peak when
the carth is at its greatest distance above or below
the plane of the sun's equator.
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CORRELATION OF UAP EVENTS WITH
SEISMIC ACTIVITY
6. On the assumption that major luminous events are also connected with seismic activity, it should be possible to correlate this coincidence if enough UAP event evidence is available to compare with seismic records. The rationale for supposing that seismic (structural) strain causes luminescences is described (Working Paper No. 10). If this were a reliable guide then the onset of a key of UAP events could possibly be predicted? There are, however, several problems areas:
- The number of UAP events which are clearly luminous/airlight-related, must first be separated from all other UAP sightings.
- The UK land-mass suffers serious seismic activity only at a low rate but hundreds of low-magnitude events occur which must influence rock-stress conditions from day to day.
- The UK distribution of probable 'earthlights' cannot be expected to be evenly spread because of the variability of the geological structure and sporadic reporting; as many of the rocky areas of the UK are in sparsely populated areas.
7. Persinger[9] has analysed luminosity events across (Six nations) using reports taken over a 100 year period (1820-1920), where it is shown that peak years of peak earthquake activity were also the same years of maximum UFO reporting. While this type of analysis could be made for the period for which the findings hold UAP reports (1987-1997), some of the early reports are limited in number and sparse in detail, and a more realistic exercise is to take a year sample (1987-1997), where the statistical value will be higher. Distinct UAP-Earthquake to Fault-line
links were found with UAP, in a French investigation as long ago as 1960. It has already been established elsewhere in this study that UAP events may be due to many different effects, no possible cause must be ignored.
TECTONIC ELEMENTS OF THE UK
8. As an aid to possible future analysis of UAP events, the UK earth-fault system has been briefly investigated. The most useful reference for this purpose is at [4]. A full database should enable UAP location correlations to be made with this fault map if seismic activity is the cause. It is assumed that if earthquakes are formed at or near fault positions they may travel some distance (e.g. 10km or more) before dissipating. Under some circumstances (e.g. attachment to a charged body such as an aircraft), they may travel much further, depending on air target velocity
9. The total annual release of energy in the world's earthquakes corresponds to up to 10⁴kW and although the largest earthquakes are responsible for most of the seismic release it is estimated that ~20,000 small quakes occur. A moderate earthquake generates ~10⁷ watts per sq km (particularly over large cities) No trigger mechanism has been discovered to predict earthquakes reliably (in which case this might explain the increasing incidence of UAP reports. Many events exhibit the property of 'dilatency' for example (with increase in volume during deformation). This, in turn, causes an increase in fractures and hence a change in resistivity/electrical conductivity, which, in turn, must affect the production of early luminous seismic movement and to be detected by animals in advance of human detection systems/instruments and a precursor to earthquakes).
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10 Commercial data is available (at a small cost) to support further investigations, if required.
11 SIDC Brussels at www.sidc.com/solar J Avental 1988
12 British Geological Survey, Edinburgh
13 Persinger M A
'Geographical Variables and Behaviour' Laurentian University Canada (1983)
14 Underhall J R, et al " The Dent Fault System……" Journal of the Geographical Society, London Vol 145 (1988)
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[FIGURE: Graph showing annual means and moving 11-year and 22-year means of relative sunspot numbers from 1700 to 1960, with three panels: top panel showing annual means (y-axis 0-200), middle panel showing moving 11-year means (y-axis 0-150), bottom panel showing moving 22-year means (y-axis 0-80). X-axis spans years 1700 to 1950.]
FIGURE 1: MEANS OF RELATIVE SUNSPOT NUMBERS, 1700 TO 1960¹
¹ HANDBOOK of Geophysics and Space Environments Air Force Cambridge Research Laboratories.
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[FIGURE: Graph showing solar cycle sunspot numbers for cycles 21-23. Y-axis ranges from 0 to 210, showing sunspot activity over time with a heavy smoothed curve overlaid on the raw data.]
FIGURE 2: SOLAR CYCLE SUNSPOT NUMBERS (CYCLES 21-23)
Note: The heavy curve is a smoothed approximation. In the UAP context finer grain required (Figure 3)
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[FIGURE: Graph showing solar cycle No 21 (1976-1984). Y-axis ranges from 0 to 190, showing monthly sunspot numbers over time with a smoothed curve.]
FIGURE 3: SOLAR CYCLE No 21(1976-1984)
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[FIGURE: Graph showing example detailed solar flux/sunspot numbers for Jan/Feb 1996. Three data series plotted: Solar flux (upper line, scale 0-120), Sunspot number (middle line), and Planetary index (lower line, scale 0-10). X-axis shows dates from approximately day 96100 to 96230.]
FIGURE 4: EXAMPLE DETAILED SOLAR FLUX/SUNSPOT NUMBERS
FOR JAN/FEB 1996 (U)
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WORKING PAPER NO. 17
VISUAL OBSERVATION OF SATELLITES
Para Page
Orbital Period 1 17-1
Inclination 2 17-1
Re-entry 3 17-1
Satellite Brightness 4 17-1
Comparison of Brightness with Stars 5 17-1
Cylindrical and Balloon Satellites 6 17-1
CONDITIONS FOR VIEWING SATELLITES 7 17-1
Earth's Shadow 9 17-2
Repeat Observations 12 17-3
Spells of Visibility 14 17-3
Angles of Elevation 16 17-3
Flash Periods 17 17-3
Sightline Rates 18 17-3
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VISUAL OBSERVATION OF SATELLITES
1. Orbital Period This could be relevant to UAP studies, as an event (i.e. satellite mistaken for a UAP) could be observed once or more on the same pass or on successive passes. The orbital period (i.e. in this UAP context the time of appearance or reappearance) is shown at Figure 1. Thus if the orbit altitude is changed from 200km to 1500km the orbit time changes from 88 to 116 minutes Hence, UAP reports at these approximate times and at these approximate time intervals could be satellite sightings.
2. Inclination This is the angle at which the plane of an orbit cuts the equator. It determines the maximum latitude reached by the satellite and hence its potential usefulness at a set of CHADR.
3. Re-entry The effect of air drag (even with much reduced density) causes LEO satellites (especially to re-enter the atmosphere for observers (often in films or video taken from the same platform. Less well known (to terrestrial observers) is the projection of aircraft shapes on to cloud layers and the consequent moving shadows seen from beneath the clouds. Further, it is possible for rainbow-like arrays to be produced through sunshine via aircraft windows, which can be projected on to clouds some kilometres distant. These can be reported as UAPs with colours.
4. Satellite Brightness Brightness depends on size, shape, surface finish and 'phase angle' relative to the sun. A spherical satellite (e.g. 40m in diameter (Echo 2 balloon)) on a thin disc, at the other extreme, may have all its surface illuminated facing the sun. This occurs if a spherical satellite is in the West. If the sun is in the west when the
5. Comparison of Brightness with Stars It is possible that some UAP reports (from those with knowledge of astronomy) may rate the UAP in terms of the stellar magnitude scale defined by referring to standard stars/planets and even compare a UAP in terms of that (i.e. a familiar star (e.g. a Pole Star). The stellar 'magnitude 1' is the brightest with 'magnitude 6' roughly the faintest. The Pole Star has a magnitude of 2.1, Series 2 is used from UAP reports). Mars and Salvut-type systems have a magnitude of ~1 (i.e. 2.5 times brighter than a star of magnitude 0 such as Vega, itself 2 times brighter than the sun).
6. Cylindrical and Balloon Satellites are visible from the side-on area of the cylinder (i.e. length x diameter) and then taking the curve root to give the apparent brightness. (e.g. A 2 × 16m² cylinder side area) = 4m diaspherical equivalent). Clearly the areas would be less when corners do not give the maximum. Cylinders viewed may fluctuate, if they are tumbling, giving the impression of flashes of light. Balloon satellites are very sensitive to air drag. They may break up in space, producing several reflecting objects.
7. CONDITIONS FOR VIEWING SATELLITES This is a key topic for UAP filtering. A satellite can only be seen:
- If illuminated by the sun
- If the observer is well in shadow
- If the satellite is against a dark background
¹ "Observing Earth Satellites" Desmond King-Hele MacMillan 1983
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8. Certain conditions apply for viewing to occur, and which set the conditions (or eliminate!) the possibility of a satellite being mistaken for a UAP:
- The sun must be at least 10° below the horizon (giving a shadow height of at least 100Km).
- The satellite must be higher than the shadow.
- Faint satellites can only be seen when the shadow height is >100km but less than the satellite's height, (which may be as low as 200km).
9. Earth's Shadow Evening observations of low satellites are only possible after sunset when the sun is between 10° and 18° below the horizon. The sequence is reversed in the morning: the daily shift in the satellite's angular position at zenith of a cross UK plane swings westward. For example, a 500Km altitude satellite reaches a point where the shadow height is less than 500km and the satellite will be visible in the evening for some weeks, but as it swings further west will be invisible because of the glare of the sun (the further west it goes). Next, it will pass over in daylight for many weeks, then into morning twilight and after this potential morning visibility will once again enter eclipse before repeating the cycle.
11. It is observed that (using the 100 and 400 curves at Figure 5) at 50°N at 0 January, the period for satellite viewing is only from 17:12-18:18hrs. By April that has lengthened to about 1 hour and from approximately 20 May to 20 July a satellite could be seen at any time of the night. In June any satellite higher than 300Km is continuously visible (it appears in the context of the UAP window figure, the observation period is greater than 50%). There are all seasons to be cautious when in association with potential UAP windows of observation (the viewing period is significantly more than Figure 5 might suggest (since this is plotted for a satellite overhead). Clearly the satellite might be at some other elevation angle. In the dark eastern sky it is sometimes possible to observe before the end of twilight. For a satellite at 400km altitude at longitudes up to 10° to the right of the observer it is possible to observe up to 40 minutes longer than the figure indicates.
12. Repeat Observations Observation of a satellite on successive evenings is subject to longitude changes at which it crosses the latitude of the observer. A satellite appears to be ~1° (0.984°) further west on successive nights due to the 360 981° rotation in 24 hours because the earth rotates through 360° 27hrs 56 minutes and spends
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the remaining four minutes 'catching up' on the small angle each needed to be in the same direction relative to the same satellite. Clearly the satellite will have a time-shift in arrival at the observer's latitude, by several seconds. The daily shift to the West is shown at Figure 6 for near circular orbits. Hence, from the UAP aspect, the same satellite will be slightly shifted in track and timing and elevation changes as the day shifts toward the West, changing the number of days/nights when the orbit just grazes the visibility window in the North or South.
500Km altitude satellite reaches a point where the shadow height is less than 500km and the satellite will be visible in the evening for some weeks, but as it swings further west it will become invisible because of the glare of the sun (the further west it goes). Next, it will pass over in daylight for many weeks, then into morning twilight and after this potential morning visibility will once again enter eclipse before repeating the cycle.
14. Spells of Visibility Satellites (in circular orbits) pass over a track on a north or southbound track. It is important to note the concept of 'spells of visibility' because these are likely to generate successive spurious UAP reports. It can be shown that evening visibility lasts for e/(e+1) days, where e is the length of one evening's visibility (in days and the value e (the daily westward shift) is given from Figure 6. For example, for a satellite at 400km at zenith (e is ~2 hours per evening/night, the value of e is zero (Figure 6), hence the spell of visibility is reduced to 10/5 minutes, then 2.8 (Figure 6), hence the spell of visibility is reduced to 10⁰·³/3 = 2.8 days (Figure 6). As the satellite altitude increases 1 month. This rule of thumb becomes inaccurate after ~ 1 month - but is of no concern for UAP elimination since the observation height is 500Km. Hence the satellite will be in shadow and visible unless its height exceeds 1000Km.
15. After a spell of visibility a circular orbit satellite becomes visible again (from the same location) after 144/4 (1+e) days or 12(1+e) months. Slightly different rules apply to eccentric orbits.
16. Angle of Elevation This is one parameter which often causes UAP reports. See Figures 8(a) and 8(b) show the angle/range/altitude relationship.
17. Flash Periods It is possible to time the satellites flash period. This feature may appear in UAP reports. Flashers seen with the naked eye from MOLNIYA satellites have been reported at once per minute (from 40,000km range). These flashes tend to come from flat satellite surfaces (cf UAP reports). Many events exhibit the property of VENUS at its brightest.
18. Sightline Rates UAP reports occasionally include times and angles. Some examples are:
(a) Satellite at 200km altitude. The minimum orbital speed is 7900m.s⁻¹ (e.g. SKYLAB altitude 235km)
(b) Satellite at moon distance travels at 975m.s
(c) An equatorial orbit (circular) at 10,200km passes once every eight hours.
(d) A 100-300 nautical mile high orbit passes, typically, once every 90 minutes.
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[FIGURE: Graph showing orbital period of a satellite (y-axis, minutes, ranging approximately 85-130) versus its average height above the Earth (x-axis, km, ranging 0-1800). Numbers on the curve give average speed in km/second. Earth's orbital speed shown as approximately 8.07 km/s.]
Figure 1: Orbital period of a satellite versus its average height above the Earth (U)
[FIGURE: Black and white photograph showing the descent of Skylab 1 over Australia on 11 July 1979, appearing as a bright streak against a dark sky.]
Figure 2: Photograph of the descent of Skylab 1 over Australia on 11 July 1979 (U)
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[FIGURE: Graph showing Spherical Satellite Visual Brightness for given Range and Diameter. X-axis shows Distance from observer (km) ranging from 200 to 2000 (top axis) and 200 to 2000 (bottom axis). Y-axis shows Stellar magnitude. Multiple curves shown; numbers on curves indicate satellite diameter in metres. Note: Changing the diameter by a factor of 10 changes magnitude by 5.]
Figure 3: Spherical Satellite - Visual Brightness for given Range and Diameter (U)
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[FIGURE: Diagram showing Example Satellite Visibility Sectors. Depicts a circular Earth with North Pole at top and South Pole at bottom. Labels indicate: 'Observing area' (top), 'Sky dark, satellite visible' (right), 'Sunlight' (left arrow), 'Satellite orbit' (circle around Earth), 'Sky bright, satellite not visible' (lower left), 'Twilight zone' (lower left area), 'Satellite visible' (lower right), 'Observing area' (bottom). Earth is shown with hatching on the shadow side.]
Figure 4: Example - Satellite Visibility Sectors (U)
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[FIGURE: Graph showing Satellite Viewing Windows for Latitude 50°N for Earth's Shadow Altitudes up to 7000Km. X-axis shows Local mean time (hours) from 17 to 24. Y-axis shows months from Jan 1 to Dec 21. Contour lines show shadow altitudes (1000, 2000, 3000, 4000, 5000, 6000, 7000 km). A shaded region labelled 'Daylight' is shown in the centre. The visible window curves around either side of the daylight region.]
Figure 5: Satellite Viewing Windows (for Latitude 50°N) for Earth's Shadow
Altitudes up to 7000Km (U)
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[FIGURE: Graph showing Daily Shift of Observed Position to the West for given Orbital Period. X-axis shows Orbital Period (minutes). Y-axis shows daily westward shift (degrees). Multiple diagonal lines shown.]
Figure 6: Daily Shift of Observed Position to the West for given Orbital Period (U)
Note: X (Degrees) is Nodal Regression.
[FIGURE: Map showing 90 Minute Orbit Tracks at 65° Inclination over the British Isles and surrounding area. Diagonal parallel track lines cross the map from lower left to upper right, showing successive ground tracks. Latitude lines at approximately 51°, 55°, 60° and longitude lines at approximately 0°, 5°W are visible.]
Figure 7: 90 Minute Orbit Tracks at 65° Inclination (U)
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[FIGURE: Graph showing Satellite Elevation to 800Km Altitude. X-axis shows Ground distance (km) from 0 to 1000. Y-axis shows Height (km) from 0 to 800. Curved contour lines show elevation angles from approximately 0° to 90°, fanning out from the lower left origin.]
Figure 8(a): Satellite Elevation to 800Km Altitude (U)
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[FIGURE: Graph showing Satellite Elevation to 3000Km Altitude. X-axis shows Ground distance (km) from 400 to 3600. Y-axis shows Height (km) from 0 to 4800. Curved contour lines show elevation angles from 0° to 60°, with labels at 10°, 20°, 30°, 40°, 60°, 80°, fanning out from the lower left.]
Figure 8(b): Satellite Elevation to 3000Km Altitude (U)
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DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
- - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
WORKING PAPER NO. 18
PROJECTED SHAPES/SHADOWS, FLUORESCENCE, LUMINESCENCE
& SONOLUMINESCENCE
Para Page
PROJECTED SHAPES AND SHADOWS 1 18-1
FLUORESCENCE AND LUMINESCENCE 3 18-1
ABSORPTION AND SCATTERING 4 18-1
Gas Absorption 6 18-2
Aerosol Fluorescence 7 18-2
Scattering Intensity 8 18-2
Pollution 9 18-2
SONOLUMINESCENCE 10 18-2
January 26, 2000 i xxxxxxxxxx S.40
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PROJECTED SHAPES AND
SHADOWS
1. Frequently UAP reports suggest shadow shapes (i.e. objects apparently seen in silhouette). It is believed that a proportion of these are projected shadows from any object which is opaque, or near opaque at the wavelength of the surrounding light. Thus a shadow with a fairly sharp edge is reported, although much closer examination would show that the shadow is not absolutely sharp.
2. The shadows of aircraft and helicopters are frequently seen on the ground, often in film or video taken from the same platform. Less well known (to terrestrial observers) is the projection of aircraft shapes on to cloud layers and the consequent moving shadows seen from beneath the clouds. Further, it is possible for rainbow-like arrays to be produced through sunshine via aircraft windows, which can be projected on to clouds some kilometres distant. These can be reported as UAPs with colours.
FLUORESCENCE AND
LUMINESCENCE
3. Earthlights are seen in the dark but they are not observed by reflected light. They actually provide the light energy which the eye receives and be classed as 'fluorescent'. Here luminescence is always longer than that of the absorbed light. In the UAP context it seems unlikely that if fluorescence is indeed the mechanism of making an aerosol cloud appear as a visible mass) this could be caused by radiation from the particles by any radar system. The source radiation must be shorter in wavelength than visible light, leading to the postulation that the cause
- Photo-luminescence is that generated by radiant energy
- Bioluminescence is generated by bio-chemical reaction.
- Cathodo-luminescence is generated by electron bombardment.
Luminescence is called fluorescence or phosphorescence, depending on the rate of decay, phosphorescence persists for some time. Fluorescence ceases when electron bombardment stops (i.e. within ~10⁻⁸ sec.). Therefore, to obtain continuous fluorescence, to continuous electron bombardment is needed. (See also para 6 below)
ABSORPTION AND SCATTERING
4. When ambient light impinges on a gas its intensity is affected by the absorption and, as a result its velocity will be less in the medium than in free space. The medium may not reduce the intensity by equal amounts for all wavelengths. No substance is known which absorbs all wavelengths equally, although some can approach this condition over a wide range of wavelengths. Normally one would expect selective absorption to occur.
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appears between what are taken to be highly charged 'balls' seen as sources of coloured or white light, usually at the extremities, forming a triangle, cone or rectangle.
6. Gas Absorption The absorption spectra of gases at ordinary pressures show narrow dark lines, although it is possible to find regions of continuous absorption. After an atom or molecule has taken up energy from light it may collide with another particle and an average increase in the velocity of particles may occur. Each atom energised can only exist for 10⁻⁷ to 10⁻⁸ sec and unless a collision occurs the energy will be re-emitted as a photon. At low pressures the time between collisions is long, hence the gas becomes a source of radiation and there is not true absorption. The re-emitted light often has the same wavelength (resonance radiation). Under some circumstances the re-emitted light may have a longer wavelength than the incident light. This is known as fluorescence. In either resonance or fluorescence some of the light will be removed and dark lines would be seen in an examination of the spectral response.
7. Aerosol Fluorescence If it is postulated that some UAP comprise clouds of aerosol particles, then it is necessary, briefly, to examine fluorescence from solids. According to Stoke's Law the wavelength of the fluorescent light is always longer than that of the absorbed light. In the UAP context it seems unlikely (no the diameter of making an aerosol cloud appear as a visible mass) this could be caused by radiation from the particles by any radar system. The radiation source must be shorter in wavelength than visible light, leading to the postulation that the cause
may be IR or UV bursts from a natural source.
8. Scattering Intensity The scattered intensity is proportional to the incident intensity and to the square of the volume of the scattering particle and on wavelength. Hence, if an aerosol cloud exists (say, at high altitude) and is radiated with a light source, the reflected light seen by an observer will be critically dependent on particle size. Long waves would be expected to be less effectively scattered than short ones because the particles themselves present obstructions to the waves, which are smaller (compared with their wavelength) for long waves than short ones. The intensity viewed is proportional to 1/λ⁴. As red light (λ = 7200) has a wavelength 1.8 times as great as violet light (λ = 4000) the law predicts (1.8)⁴ or ten times greater scattering for the blue. Hence particles much smaller than the wavelength of either colour Hence, if white light is scattered from sufficiently fine particles the scattered light always has a bluish colour. If the size of the particles is larger, then the scattered light becomes whiter.
9. Pollution In passing it is suggested that the reported increase in atmospheric pollution (particularly over large cities) may have a bearing on the charged aerosol phenomena (reported at Working Paper No 19) and thereby the increasing incidence of UAP reports. That there is a clear connection with the particles in suspension of the medium, and volcanic zones is repeated elsewhere in the report.
SONOLUMINESCENCE
10. Sonoluminescence is the production of wide-spectrum light, visible by the human eye, due to the compression of gas
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bubbles by sonic (i.e. sound air pressure)
shock waves. While this can be easily
reproduced under laboratory conditions
under water, and the light emitted extends
from IR to UV, covering the entire human
eye spectrum, it is not clear whether the
conditions could (perhaps exceptionally)
exist in the atmosphere. If this is so, then
sonoluminescence could be a candidate
source for the very short UAP lights (e.g.
<1 second), which are frequently found
when examining the UAP reports.
Although it is some 60 years since the
discovery of the effect little serious work
on understanding and quantifying the
phenomenon has been done - mainly
because of lack of measurement
technology
11. The science behind the
sonoluminescence effect can be
summarized as:
- A very small volume must be
present (appearing, for example, as a gas
bubble (cavity) in water) which must
contain a gas other than pure oxygen or
nitrogen. However, even a 1% impurity is
sufficient to invoke sonoluminescence.
- Successive rarefactions and
compressions must be present for the gas
to pulsate rapidly.
- The radius of the gas bubble will
expand when the pressure goes negative
(e.g. for a bubble in water the radius can
typically change from 4 to 40 microns).
- The sudden collapse (Rayleigh
1917) reaches supersonic velocities (1.4
kilometres per second quoted), stopping
only when the gas in the bubble reaches a
'hard core' minimum radius (when the
molecules can get no closer together)
- Photons of several eV energy
level are emitted, at which time the
temperature is estimated as being in the
tens of thousands of degrees. At this
point the bubble surface is reported to
'bounce', with a surface acceleration which
can attain values causing a non-linear
amplification effect (focussing) of the
energy.
- Several alternative theories are
currently proposed for the micro-detail of
the effect. However it is clear that flash
duration depends upon, among other
factors, the intensity of the emission and
the gas/water mixture. The longest flashes
occur with the brightest emissions. The
effect is also pressure dependent.
- There are close analogies with
cavitation bubbles in sonar.
12. The fact that this effect can be seen by
the unaided eye was perhaps first reported
in the original version of EXODUS
(20:18), where 'and all the people saw the
sounds'. This was removed in later
translations (presumably as being
'impossible'). If the sonoluminescence
effect can be produced, even under
exceptional conditions in the atmosphere, it
may account for some UAP reports.
18-3
FIGURE 1: INTENSITY OF SCATTERING VS WAVELENGTH (RAYLEIGH'S
LAW)
18-4
DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 19
CHARGED DUST AEROSOLS - DUSTY PLASMAS
&
ATMOSPHERIC PLASMAS AS REFLECTORS AND ABSORBERS
Para Page
Introduction 19-1
Streamlined Shaping 4 19-1
UAP Model 6 19-2
Motion 8 19-2
Particle Characteristics 9 19-2
Speed of Cloud 10 19-2
Lights 13 19-3
Colours 14 19-3
Electrical Attraction 15 19-3
Radar Reflections 17 19-4
SUMMARY- Dusty Plasmas 18 19-4
ATMOSPHERIC PLASMAS AS ABSORBERS &
REFLECTORS
Plasma Lifetime 22 19-5
Reflection 23 19-5
Absorption 24 19-5
INTERACTIONS
Plasma Interaction with Objects & Aircraft 26 19-5
January 26, 2000 i xxxxxxxxx S.40CHARGED DUST AEROSOLS - DUSTY
PLASMAS
1 Introduction There are numerous
reports of unidentified flying objects of cigar,
toroidal, spherical and a host of other regular
shapes moving in earth's atmosphere due to
the action of forces of an unknown nature.
Depending on the witness's perception at the
time, the object can have 'navigation lights',
'searchlights', be of various single colours or
even multiple colours. The objects reportedly
can change flight direction suddenly, stop,
accelerate or decelerate. Reports have also
have included 'buzzed by shining glass balls or
cones' or 'like soccer balls made of glass'.
Mukharev (Russia)¹ takes all these factors
into account in his hypothesis that aerosol
aggregation can accumulate electrical charges
due to the action of the same process (charge
mechanisms) as in thunderstorms and there are
several types of 'dusty plasma'. For example,
'Dusty Dense' plasmas and 'Dust in a Plasma'
are different. In the former the particles
remain electromagnetically trapped in the plasma
volume. A strong electric field is needed in
the gas to overcome the ionisation rate and
maintain the structure against electron loss.
An equilibrium is achieved by the balance
between ionisation in the plasma volume and
the charged particles lost at the extremities.
Within the core of the effect the particles take
up an ordered structure (rather like a crystal
lattice). Russia has taken a particular interest
in combustion plasmas since 1994, and the
science of dusty plasmas has recently achieved
several milestones. Several researchers have
used microspheres as the experimental
medium [As area of potential interest: there
is in the possible use of microspheres as chaff
to produce false targets]
2. When dust particles are between separated
charges (e.g. visualise as in a volume between
capacitor plates) the dust will suspend in a
matrix and a balancing of the charges causes
the dust to suspend in flat layers. By using a
laser beam it has been found that the dust can
be moved, or the crystal lattice 'fractured'.
The radiation intensity of a low power laser
(compared to the particles) can be moved, or
the crystal lattice 'fractured'. The radiation
of a low power laser (compared to the particles)
momentum given to them depends on their
size, distribution, surface area and mass. If the
particles are not balanced, the dust will fall
under gravity. Since the particles can be made
to form specified alignments, there are specific
radiation applications eg depending on the
this technology, but the UAP content is
potentially a special case - since clearly if the
charging were to become too large, the aerosol
would vanish. The overall equilibrium of the
charged particles in the medium is thus defined
by external conditions. It is suggested that
Dusty Plasmas may well be closely related to
at least some of the UAP reports, which
frequently display characteristics that observers
of such a cloud, especially one with
bright spots and turn this into a UAP, with
portholes!
19-1
fuselage shaped, (e.g. cigar), flattening sphere
(i.e. disc or flat cigar), or even triangular, with
curved edges. As the EM field within a
planar, then all extremities of the original
aerosol charged body (whatever its original
format) will tend to be 'smoothed'. Eventually
the EM field within the charged envelope will
dampen and dissipate and the more sharpened
contours will no longer arise and so be no longer
recognised as a shape (i.e. as a UAP), or will
vanish completely.
5. If high intensity EM field values occur,
a gas discharge is possible at its maxima, giving
rise to 'bright lights' on the surface of the
UAP (see paragraph 13 below).
6 UAP Model Mukharev, commencing
with a postulated spherical aerosol, considers
the natural equations for the electrical and
magnetic oscillation modes, and derives a
model. It is postulated that the initial
excitation is by streak lightning.
[Comment: Note that this can be present in
either a 'wet' or 'dry' electrical storm
condition]. The model estimates the dielectric
constant of the medium from which the sphere
comprises and Mukharev points out that this is
similar to the dielectric constant of a plasma. It
is determined by the character of the time-
dependence of the field in which the source is
located. The ratio of the internal and external
dielectric constants sets the conditions. This
will depend upon whether the aerosol is one
which damps with time (in which case a
negative dielectric constant is obtained), or one
where the field is sinusoidal. It is thus shown
that the amount of energy of the EM field
within, say, a 1m³ volume of the aerosol cloud
is only ~8 Joules. Therefore, it is claimed that
the field of the UAP could be excited by a
spark discharge.
7 The postulation shows that the
aerosol cloud can remain within boundary
conditions which do not result in immediate
breakdown, but have a finite lifetime. For
the purposes of the model it is shown that
the Lorentz Force (Earth's Magnetic Field)
is negligibly small compared with the
aerodynamic drag force. The outcome is a
postulated UAP which has motion.
8 Motion As the cloud moves in the
atmosphere the aerosol particles located at
its surface are removed by the air stream.
(The energy of the EM fields associated
with these particles being transferred into
EM momentum.) As a consequence of the
momentum conservation law, the EM
momentum arising within the closed system
of the cloud must be compensated by the
mechanical momentum. Hence, a force
arises at the leading edge of the cloud which
causes the cloud to accelerate until the force
becomes equal to aerodynamic drag. After
some time the cloud gradually decelerates
because of the dampening field.
9 Particle Characteristics The
particles may be variable in diameter and the
entire mass of material in the aerosol cloud
can amount to only a fraction of a gram. It
has been suggested that this low mass,
resulting in absence of inertia, may be the
reason for the exceptional 'manoeuvrability'
attributed to UAP and associated also a
tendency towards rapid acceleration.
10 Speed of Cloud It is possible to
relate particle size to the drag-force by using
the Reynolds number for the particles
moving in a laminar stream, at velocity v:
Re = γv₀r/η
/where
19-2
where: γ is the density of the
atmospheric medium, r₀ the particle
radius for 1.5μm. The velocity of
laminar noiseless motion is shown
below.
For this situation Re must be ≤10 (since the radius
of the particles, their velocity for γ = 1.29kg.m⁻³
must be inter-related by the conditions
~1.4 x 10⁻²s⁻¹. Thus the higher the observed
velocity of the UAP the smaller the dimensions of
the particles forming it. Examples are:
Particle Radius 1.5μm 0.05mm
Velocity(metres 280[?] 3
per second)
2340[?]
Notes [1] Up to an altitude of ~3Km
[2] At an altitude of 15Km, where
the density of the atmosphere
has decreased.
11. It is therefore noted that, at 15Km altitude,
the aerosol cloud can move at up to about seven
times the speed of sound. Hence, this correlates
with reports of fast-moving UAPs, much faster than
aircraft. An aqueous aerosol moves at high velocity
and evaporates quickly. Hence, life time can be
short. A long-lived aerosol cloud forming a UAP
can only consist of solid dust particles of very small
size.
12. The energy of the EM field in the
cloud and the aerodynamic (i.e. atmospheric)
drag force are proportional to the cloud
volume. Therefore the velocity and path taken
should not depend on cloud dimensions. For
example, if a charged aerosol cloud has moved
distance L (e.g. 40km) with a velocity v (e.g.
30ms⁻¹) a volume density can be calculated (in
this case 4 x 10⁻²m³).
13 Lights For a high field potential (e.g.
>10⁵V/m) an electrodeless corona discharge
should occur on the surface of discharge zones of
high intensity, resulting in localised discharge
zones of high field intensity. The light intensity
varies throughout the aerosol, localised discharge
zones can occur - due to alternate regions of
maxima and minima. Hence, it is postulated
that 'navigation lights' are observed. In the E₀
mode, for example two 'lights' or a luminous
strip can be formed. If the number of discharge
zones increases, the number of 'lights' will
increase which will be equally distributed
around the cloud as luminous zones or
'portholes'
14 Colours It is suggested that different
colours might be produced by the presence of
particles in the discharge zones.
15 Electrical Attraction If the discharge
connects with some conducting object (Earth's
surface or aircraft), the number of 'lights'
can be see by the unaided eye. It is
postulated that when 'searchlight
beams' are reported from UAPs that most of
the very high concentrated discharge cone
and can cause damage by the high voltage but
very small intensity current. This can lead to
involuntary closure of electronic and electrical
circuits (switches) and have adverse health
effects on humans (see Working Paper No.
26). On the ground the discharge can leave
marks, bend grass etc.
19-317. Radar Reflections No information has
been found on the possible radar reflectivity
from charged dust aerosols, so it is claimed
available on radar scatter from 'Dusty
Plasmas'. There may well be some overlap in
the terminology and applicability. The latter
topic is covered at Working Paper No 5, on
radar reflectivity.
SUMMARY
18. Dusty Plasmas The work reviewed
above shows that it is theoretically possible for a
charged cloud of particles to exhibit
characteristics of visibility and motion similar
to many UAP reports with the particular
implication that atmosphere-borne particles
must be present strengthens the proven
correlation with dust-laden scenarios, e.g. near
volcanoes and earthquakes. For the uninitiated
it would not take too much imagination to
observe such a cloud, especially one with
bright spots and turn this into a UAP, with
portholes.
19. As the formation of clouds (of the charged
aerosol type) would clearly depend on the
presence of atmospheric-carried particles, it
may well be worth making correlation studies of
sightings of UAPs with geographical locations
where dust is produced, e.g. quarries, or where
other pollution particles are emitted (e.g. from
power stations or factories). It may also be useful
to compare the number of sightings in areas -
taken both during and after cessation of work
where dust or other particles are produced. For
example, where factories have closed or applied
dust/smoke control regimes, or where dusty
quarries operated but no longer do so. However, a
considerable amount of effort would be needed
to properly investigate this suggestion. The
critical information is not available on the database
created for this study.
20 The topics of 'dust in plasmas' and 'dusty
plasmas' have become of particular importance
in the last two to three years. These plasmas
can easily be produced under laboratory
conditions, but much more research is required
to understand all the mechanisms involved.
This may well point towards an understanding
of such plasmas in the atmosphere.
ATMOSPHERIC PLASMAS AS
REFLECTORS & ABSORBERS
21 The electromagnetic properties of a plasma
at atmospheric pressure is an inter-disciplinary
topic, combining plasma physics, radio wave
propagation and UAP reports. Plasmas in the
atmosphere can either reflect or absorb
electromagnetic waves, depending on plasma
characteristics. A high reflection co-efficient
requires a grazing angle of incidence. A high
absorption requires a high collision rate, a low
electron density and a plasma transition of about
one wavelength. The power to sustain a
plasma in air is high because of the short
plasma lifetime unless continuously
replenished. The bandwidth, as an absorber,
can extend from Metric to I Band. However,
absorption peaks at VHF/UHF. In an
atmospheric plasma, electrons undergo
numerous collisions with atoms and molecules
in the background gas(es) and the collisions
dominate the electron dynamics (which will
be feeding the plasma to heat and damp the
essential electron motion. The collision rate
is a function of both gas density and where
water vapour has an effect - so that, for
example, 50% relative humidity approximately
doubles the sea-level dry air collision rate.
22 Plasma Lifetime The plasma lifetime
is essentially determined by the plasma
density (altitude). The presence of gases
other than those normally in air can change
the lifetime by a factor of ~10,000 for helium
19-4
23 Reflection If a rapid transition occurs,
from free space to plasma (caused, for
example, by the presence of large
electrical/electromagnetic forces), the plasma
will reflect. If the transition is diffuse, the
plasma will reflect at a grazing angle. If the
plasma transition gradient is too long, then the
plasma patch will transmit (i.e. allow through)
more energy than it reflects.
24 Absorption The absorption bandwidth
depends on the collision rate of each particle
and the plasma gradient. An atmospheric
absorber which is lightweight, has high
attenuation per wavelength and can be
switched on and off. Quite apart from any
UAP-related properties, it is seen that there are
potential military applications in the control of
EM scattering and Low Observables.
25. The power requirements to sustain a
plasma are dependent on the plasma volume,
electron density required, the energy to
generate electron-ion pairs and the lifetime
required, and, of course the altitude (pressure)
and the medium.
INTERACTIONS
26 Plasma Interactions with Objects and
Aircraft The interaction of plasmas alone, or
when surrounding other objects are complex,
since plasmas can act both as reflectors and
reflectors. In addition, for transmitters, it has
been shown in practice that the presence of a
plasma can enhance an antenna mounted
into an antenna mounted on a body, thus
modifying its performance, causing an increase,
for example, in radiated power. The increase in
radiated power is a function of the ratio of
plasma frequency to signal frequency. In the
UAP context it seems likely that the response
of an impinging EM wave-front on reaching a
plasma might be affected. If the radiation
from a plasma is capable of modifying an
antenna on transmit, then presumably it will do
so on receive - hence it seems possible that the
presence of a plasma in proximity to a radio
receiver (especially at VHF/UHF) may modify
the receiver front-end characteristics and even
fine tune - or disrupt normal reception. This
may well be the cause of reports that receivers,
in what could be termed the 'near field' of a
UAP, suffer some function (receive and/or
transmit) until the UAP and receiver are
separated. Usually the UAP moves away or if
the vehicle stops knocking, it is hurriedly
driven off. In the context of radio
transmission, the frequency dependence of this
phenomenon also depends upon the inductive
reactance introduced by the plasma layer
improving the antenna (towards resonance and
reducing the resistive losses), such that the
efficiency is maximised. [Apart from the UAP-
related aspects, a factor of military importance
may be that the antenna can be made smaller.]
27 Interaction with Aircraft Because it is
usually unclear as to what the entity comprises,
coupled with the surprise factor, most
encounters with what are clearly charged
masses have been assumed to have been with
ball lightning (Working Paper No 2). Whether
this is the case - and whether charged aerosols
are a variation of the same physical realisation -
is not currently clear. The laws of motion of a
plasma ball and the effects when in close
proximity to an aircraft in flight are of special
importance here. It is assumed that the drag
on the ball diminishes with time, due to the
leakage, where the air layer is adjacent to the
ball; the ball is treated as a non-deformable,
non-deformable solid sphere, in aerodynamic
terms, in a flow of non-compressible fluid. The
ball is also set in long visual distance (slant
ranges) of ~100km, where, it is calculated,
the diameter can be several hundred
metres. [As an example, an object of 90.5m
diameter at 100km range has the same
angular extent as that of the moon.]
19-5
This force would be several tons! (which is much less
in practice. It seems probable that the air-
stream would lose some of its various physical
properties over the surface of the sphere (i.e.
the presence of the plasma, it is suggested,
would reduce drag). This has been shown to
be the case in experimental observations.
Frequent reports in Russia suggest that
plasmas/charged bodies start to respond to the
presence of an aircraft at a range of about
(0km. N 1. Gaidukov and others have
published papers on this phenomenon
(and indeed the Russian Aviation authorities
now advise them) that if the plasma appears
to 'attract' the aircraft, it is suggested to
climb to make the mass fall astern, where it will
remain until it dissipates in the slipstream. It is
not clear whether these are the same claims as
the four finalists they have received as
'UFO's', and their particular interest in the
phenomenon, and the large number of
published papers.
19-6
DIS SCIENTIFIC & TECHNICAL MEMORANDUM 55/2/00
WORKING PAPER NO. 20
OPTICAL MIRAGES
Para Page
OPTICAL MIRAGES
Optical Conditions 1 20-1
Object Position 2 20-1
UAP CONTEXT 3 20-2
17 February 1999 i xxxxxxxxx S.40OPTICAL MIRAGES
1 Optical Conditions An optical
mirage is a phenomenon associated with
the refraction of light in a cloud-free
atmosphere, resulting in the apparent
displacement of a distant object. The
refraction is caused by abnormal air
densities, which cause the light to travel in
a curvilinear path. Object shapes can be
distorted and scintillation can cause rapid
changes in the observed colour, shape and
position of the object. For a stationary
observer the effect can last several hours; for a
moving observer only seconds or minutes.
Mirages have the following characteristics:-
- Mirage images are seen at
low grazing angles near the
horizontal plane.
- Mirages can only be seen if
there is a long uninterrupted
sightline.
- Mirages are associated with
atmospheric gradients which
give anomalous propagation.
- Focussing and interference of
the wavefronts can give
rapid movement and
enhanced brightening.
- Distortions and colour
changes can be
accompanied by multiple
images.
- Objects on the surface (e.g.
ships) can appear as if they
are elevated.
2 Object Position The amount the
object is apparently (visually) displaced
from its true position (angle) depends on
the variability of the density of the medium
(hence its value of refraction index). The
effect is well understood in physical optics,
and is pressure (P), temperature (T) and
wavelength (λ) dependent. The spatial
variations can be expressed in terms of P, T
and λ and the resulting practical values of
refraction (minutes of arc per km) for the
ratio of temperature to altitude is
significant. In the simplest terms this
means that:
- One degree of arc
represents the largest
angular change between the
true and false (mirage)
position of an object.
- When the image appears
above the true position this
is know as a superior
mirage. When below the
true position, the term used
is an inferior mirage.
- There must be the
coincident conditions of a
temperature inversion and
the presence of light to
illuminate the object at
grazing angle.
- Vertical stretching can lead
an observer to under
estimate the true distance
to the luminous object.
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UAP CONTEXT
3. The key factor in eliminating or
including the mirage phenomena as a
potential UAP event is that of low grazing
angles and long distances, since it is
unlikely (from the type of UAP details
usually received) that the other detailed
meteorological conditions will be known.
In the UKADR the combination of long
path lengths and low grazing angles is
more likely to occur at sea.
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WORKING PAPER NO. 21
IONOSPHERIC PLASMA
Para Page
Formation of Plasma 1 21-1
Extent 3 21-1
Motion 4 21-1
Power 5 21-2
Radar Echoes 6 21-2
17 February 1999 i xxxxxxxxx S.40IONOSPHERIC PLASMA
1 Formation Of Plasma Within the
troposphere operate powerful processes
which orientate the separation of electric
charges; for example, thunder conditions
give rise to huge vertical separation of
charges. Meanwhile it is understood, that
wind is responsible for horizontal charge
distribution. When charges are displaced it
is possible for the creation of image
charges which make the ionosphere
unstable, with the result that a downward
electron stream is ejected from the bottom
of the ionosphere which may produce
'airglow' in a narrow high altitude band.
Because these visible manifestations can be
seen at night, they are often described as
'nocturnal lights'. They appear to have a
close connection with one class of UAP
sighting.
Figure 1¹ Shows the mechanism, which is
explained in the following sequence:
- Due to wind over the
earth's surface and/or a hilly
region a positive charge is
deposited on the hills.
- A negative charge becomes
attracted to the moving air
mass (shown moving to the
right on the figure).
- Corresponding 'mirror'
charge images are formed
with an upward E field (E₀)
above the hills and a
balancing downward field
(E_D) restores equilibrium.
The ionisation due to E₀ causes
instability and an electron
stream from the ionosphere is
downward-accelerated by
the electric field.
- 'Airglows' (UAPs) are
formed when electrons are
stopped in the lower
atmosphere.
- The glows or 'nocturnal
lights' occur in a relatively
thin altitude layer and
visually appear as bright
spots of approximately similar
size moving across the night
sky.
2 The supporting theory is explained
in some detail at¹. It seems likely that the
reports of 'silvery discs' at very high
altitude are not the same phenomenon. Below
ionospheric altitudes researchers agree that
air conductivity cannot prevent the conditions
if the middle atmosphere can become
electrically de-coupled from the
ionosphere. The ground and the
ionosphere can be considered, in effect,
two plates of an enormous capacitor. The
conductivity of the ionosphere is of solar
origin (hence, the investigations elsewhere in
this report on possible solar flux/solar flare
connections with the rate of UAP reports).
3 Extent The size of 'nocturnal
lights', which is believed to be produced by
an electron stream which penetrates to the
lower atmosphere, is considerable, in order
to be seen at long visual distances (slant
ranges) of ~100km, where, it is calculated,
the diameter can be several hundred
metres. [As an example, an object of 90.5m
diameter at 100km range has the same
angular extent as that of the moon.]
¹ BROVETTO P AND MAXIA V 'On the
Instability of the Ionospheric Plasma....'
IL NUOVO CIMENTO July 1995
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4 Motion A high angular velocity is
produced because the phenomenon is light
(i.e. nothing or very little mass actually moves
physically). It is analogous to a
'searchlight spot' moving across a hill,
which very naturally can move rapidly
(the 'beam' causes the UAP report).
5 Power Light emission occurs
when excited molecules or ionised atoms
re-combine (or relax), with a sharp
increase when the electrons are stopped
at the path end, when the electrons are
stopped, in the E₁₀ mode, for example.
At the path end, when the electrons are
stopped, in the E₁₀ mode, for example.
The power of an ionospheric plasma
'beam' is estimated as between 0.3 and
3kW. A long-lived aerosol cloud forming
a UAP would typically be above aircraft
altitude i.e. normally above 15Km (short-
lived ones can occur lower). The power of
reflected light will vary through the
volume (because of the renewal of particles
as the cloud moves). This will give rise to
a reactive force with will maintain its motion.
6 Radar Echoes Radar echoes can be
obtained due to the conductivity of the
ionised air. The light emitting layer, caused
by the electrons, is probably a few tens of
metres in height. In some instances,
this would be well above the maximum
range capability of typical terrestrial search
radars, and beyond the slant range of most
interecept radars. Detection of UAP from
No 5 and at Volume 3.
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FIGURE 1: CONDITIONS FOR IONOSPHERIC PLASMA FORMATION
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WORKING PAPER NO. 22
ARTEFACTS
Para Page
'Angel Hair' 1 22-1
Metallic Artefacts 2 22-1
Summary 3 22-1
17 February 1999 i xxxxxxxxx S.40'ANGEL HAIR'
1 It is believed that this fibrous
material resembling filaments, spider webs
or candy-floss-like streamers is formed by
reciprocal attraction between polarised
dust particles. Sometimes the material is
sticky. It can be carried large distances
before being deposited and has been
likened to long chaff and has even been
named 'spacegraas'. It can leave a smoky
or musty deposit. The thin filaments appear
to be an electrostatic precipitation of
atmospheric dust, which is unstable,
which eventually disintegrates and
vanishes. On at least one occasion a UK
witness has collected what was probably
'angel hair' in a jar, believing it to have
come from a 'UFO' which 'hovered at the
bottom of his garden'. The author of this
report personally observed this material
drifting in a light breeze in Norfolk on a hot
but breezy summer's day in 1997.
METALLIC ARTEFACTS
2 Although no such artefacts have
been found in the UKADR, it is claimed in
Russia and Ukraine that items have been
scientifically analysed. The results are not
known. The Russians, like the USA, have
never produced the artefacts which are
claimed by some media reports to have
been found. This seems to be quite
extraordinary in view of the fact that it
would be reasonable to expect that this
might solve the extra-terrestrial hypothesis
of 'UFO' origins once and for all. The
Brazilian claim of 'extra-pure aluminium'
artefacts was not sustainable after analysis.
have not been shown to be of unknown
elements. It is a fact that some
materials have entered the earth's
atmosphere as a result of meteor activity
and have survived to impact. Analysis
has shown nothing to connect these with
any type of flying vehicle or threat.
MOD does not hold any such material.
SUMMARY
3 No proven tangible artefacts have
been obtained by the public for display, or
shown by governments to exist. The
metallic materials analysed scientifically
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WORKING PAPER NO. 23
LINKED VORTEX RINGS
Para Page
LINKED VORTEX RINGS 1 23-1
Experimental Vortices 2 23-1
Challenger Spacecraft Video Recording 4 23-1
17 February 1999 i xxxxxxxxx S.40LINKED VORTEX RINGS
1 Quite apart from the possibility of
water spouts, dust eddies, whirlwinds and
similar atmospheric vortex phenomena,
which can be reported as UAPs, there is
the possibility of linked vortex rings, such
as those filmed from the US spacecraft
Challenger on its post-launch ascent. It is
suggested that aerial formations of this
type (which can be related to the UK
sightings) may be related to the UK
sightings) may be related to the UK
sightings of the type shown at Working Paper No 11,
Figures 2 to 7.
2 Experimental Vortices Experimental work
has been done¹ on linked vortex rings and
the phenomenon has been modelled. Initially the vortex
rings are formed separately. Under certain
conditions, when collisions occur, linking is
possible of distinctively separate rings.
Some results shown at Figures 1(a) and
(b). The appearance of linked vortices to
an observer clearly depends:
- The viewing aspect
- The relative position of the
viewing light source
3 If the ring assembly is rotating
slowly then the component strands might
be visible. The Challenger example cited
shows the complex component strands
(which, overall, could be described as being
contained in a cylindrical volume) rotating
(rolling) about its radius at an estimated
rate of about 50-60 times a minute.
However, if the structure was not rotating
and viewed, for example, end-on, it would
appear as either a solid ball, reflecting light
according to the scattering of its
component particles or as a dark spherical
silhouette if between the sun (or light
source, such as light cloud background)
and the observer.
4 Challenger Spacecraft Video
Recording The few extant reports on this
topic (which were erroneously connected
with the Challenger incident) only because
the Department had collected open-source
material on this space-launch as a
records check, it is noted that the video
footage taken by the Challenger crew
seems to be very similar indeed to a
number of UAP reports received by the
Department. Some examples are at Figure
2. Unfortunately the imagery taken from
the video does not do justice to the
original, which can clearly be seen 'rolling',
or 'tumbling', as described above.
5 No attempt has been made in this
brief investigation to correlate the 'linked
vortex' postulation with the conditions for
their formation in the atmosphere or of a
possible combination of this effect with an
electrical/charged particle or EM field
effect.
¹ 'Linking of Vortex Rings' Aref and Zawadzki.
Nature Vol 354 Nov 1991.
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[Figure showing 9 illustrations of linked vortex rings in various configurations, arranged in a 3x3 grid]
FIGURE 1(a): LINKED VORTEX RINGS
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[Figure showing 8 illustrations of linked vortex rings in various configurations, arranged in a 4x2 grid, labeled a through d on each side]
FIGURE 1(b): LINKED VORTEX RINGS
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[Black and white photograph showing a luminous curved/loop-shaped object against a dark background]
FIGURE 2: ROTATING/TUMBLING OBJECT (CHALLENGER SPACECRAFT)
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WORKING PAPER NO. 24
'SPRITES', 'ELVES' AND 'BLUE JETS'
(ATMOSPHERIC AND IONOSPHERIC PHENOMENA)
Para Page
INTRODUCTION 1 24-1
SPRITES 2 24-1
Measurements 4 24-1
Effect on RF Propagation 7 24-2
TERRESTRIAL GAMMA FLASHES 8 24-2
BLUE JETS 9 24-2
POSSIBLE UAP LINKS 10 24-2
EXTERNAL ENERGISATION 11 24-2
OBSERVATION OF SPRITES 12 24-3
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SPRITES, ELVES AND BLUE JETS
INTRODUCTION
1. Three types of transient optical luminous vertically-orientated phenomena have been observed at high altitudes above thunderstorms: 'Elves' at roughly 90km, which is an enhanced airglow, 'Sprites', a reddish glow from 50-90km and an upward-moving bluish beam above the anvil cloud tops, known as 'Jets', below 40km. Large area multi-cell thunderstorms lead to the formation of vertically-orientated cylindrical structures of gravity waves closely resembling those observed in optical emissions associated with transient luminous glows. These are believed to occur as a result of transfer of large amounts of charge (from clouds at altitudes of 5-(10km) to the ground. Apart from the visual effects, these charge transfers are known to generate upper ELF Band signals (>300kHz). The Sprite path can also be located at high altitudes between the ionosphere and cloud tops. The luminous emission at low altitude is red. The likely explanation is gas breakdown by the electrical electromagnetic fields of lightning discharges. Some Sprite 'bluish tendrils' were observed to extend down to 20-30km altitude. Horizontal magnetic field variations have also been observed in the frequency range of the earth-ionosphere cavity resonances. These phenomena have been studied recently in the USA, Germany and in the Antarctic.
SPRITES
2. Sprites are the older known phenomenon, first being reported 100 years ago. They last tens of milliseconds and can thus be sensed by the human eye. They are sometimes described as 'fan shaped' or
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'carrot-like' in shape. They can extend laterally for several kilometres. Other observers have reported 'upward forks', due to divergence of the streamers.
3. Electric field discontinuities can occur over stratiform clouds at 10-16km altitude and this is believed to be due to the positive ground-to-cloud discharges. Satellite-based instruments have also detected gamma-ray flashes (see para. 7, below). Current theories suggest that Sprites, Gamma-ray Flashes and Blue Jets are all types of discharge produced by a run-away air breakdown.
4. Measurements A TV slit spectrograph recently recorded 25 events and measured optical wavelengths in a band from 540 to 840μm, including other measures have spanned from 436-850 nanometres. The fleeting columns of luminosity have also been imaged by CCD cameras. Sprites are found to have a bright core less than 2km in horizontal dimension; they followed the associated lightning (below the (cumulonimbus) cloud) within a few milliseconds, and rose to peak intensity at 0 to 3 ms, fading a few tens of milliseconds later. Sprites can easily be observed from aircraft and from the ground, and have been seen from spacecraft.
POSSIBLE UAP LINKS
10. Although the field 'trigger' levels and current flows involved in finally ionising the atmosphere to produce sprites and blue jets in visible form are large (assuming all other field conditions and particle conditions are ready), it is postulated that a situation could exist where the charged atmospheric field types are at the point of transition in which an added potential might cause a trigger to occur. This is a vehicle for being reported because a ship's Master reported a visual UAP event when his radar was first switched on (at sea). It is often reported that, since this occurred on a merchant ship, that the RF was I Band (standard 9375MHz maritime search).
EXTERNAL ENERGISATION
11. The phenomenon is a gas ionisation process for which, when the right threshold conditions exist an additional charge is required to trigger the event. It is believed that, for example, a remote, rather than close-by, lightning charge could find the pre-charged volume and cause the glow to be triggered. A short bibliography is at the end of this paper. Since the initial quantification of the effect is quite recent, the following key attributes are taken from the best available (ie most relevant to this study) published papers. Further work would be needed to confirm the postulation that a radar (or laser in some cases) could cause the ionisation to occur, thus making a pre-charged but hitherto invisible mass become visible to the human eye. Although the possibility might be linked with sprites/blue jets it is recognised that the 'added' energy available from terrestrial (or airborne) sources will be tiny in comparison with the huge energy levels in electrical storms. However, the principle is established that any highly charged gas could finally reach ionisation point by the
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addition of extra energy. Hence, it does not seem unreasonable that if swamp-gases, (if they are a component of earthlights), or even incompletely formed ball-lightning, might react to the addition of external energy. This, it is suggested, might account for the so-named 'close-encounters of the fifth kind', where it is claimed by ufologists that an airborne visual object appears to respond to, or be modified, by probing it with a terrestrial beam of energy. Since the shipping incident described at para. 11 above, was at I Band, the implications are that this is at least possible with I Band military radars (e.g. Air Intercept Radar) if the critical atmospheric conditions exist.
OBSERVATION OF SPRITES
12. It is clear that a visible and measurable phenomenon of red (Sprites), possible with blue offshoots ('tendrils') or blue (Blue Jet) columns exist, and that they can be seen:
- From aircraft, in particular, because they appear where high-flying aircraft are likely to be.
- Above thunderstorms.
- On occasions from ground-level when the cloud-breaks allow a sight-line.
The phenomena appear for a few milliseconds and could be reported as UAPs. Working Paper No. 4 confirms that the human eye will detect and possibly retain an after-image on the retina. Finally, they can be 'triggered' by a radar in the vicinity.
BIBLIOGRAPHY:
[1] Cummer S.A. & Inan U.S. "Measurement of Charge Transfer in Sprite-Producing Lightning..." Geo. Phys. Res. Letters Vol. 24 p 1731-4 15 July 1997.
[2] Nemicoff et al. "Full Wave Calculation of 30 VLF/ LF Wave Fields Radiated from a Lightning Discharge" ISAP 1996 Proc. 1996 Int. Symp. Ant. & Prop.
[3] Milikh et al. "Model of Red Sprite Optical Spectra" Geo Pages Res. Letters Vol. 24 15 Apr. 97.
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WORKING PAPER NO. 25
OVERVIEW OF MAGNETIC FIELD EFFECTS ON HUMANS
Para Page
INTRODUCTION 1 25-1
NEUROLOGICAL RESPONSE TO MAGNETIC FIELDS 4 25-2
Temporal Lobe Activity 5 25-2
Magnetic Flux Levels 10 25-3
KEY FINDINGS 14 25-4
COMPARISON WITH EARTH'S NATURAL MAGNETIC FIELD 19 25-5
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OVERVIEW OF MAGNETIC FIELD
EFFECTS ON HUMANS
INTRODUCTION
1. As a result of research (and ignoring man-made air-objects which are frequently mis-reported as UAP) and other natural though exceptional meteorological phenomena, such as cloud formations, there appears to be four types of electrical charge-related formations that can occur in the atmosphere, covered in the Working Papers Nos. 1,2,10,19 & 21.
- Ball Lightning
- Ionospheric Plasmas
- Earthlights
- Electrically-charged Aerosols
It is known that visible and invisible fields can be sensed when close to a UAP. In the absence of any other postulations it is assumed that the fields are electromagnetic or magnetic (or both) in nature. Further away from the object only the emissions in the visible part of the electromagnetic spectrum are sensed, as is frequently the case by human observers, photographic, film and video camera detectors. The results summarised are those of medical experiments in which the aim was to study the human brain response to external fields, particularly in the area of epilepsy. There is no UAP connection given in the scientific papers. The connection is made here, because of the apparent relevance to this study.
2. The fields investigated for medical purposes in Canada have several common characteristics, and the scenario which, in
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Range Power Power
(m) at at
Observer Source
(m Gauss) (m Gauss)
1 1 1
1 1 25
10 1 100
20 1 400
25 1 625
NEUROLOGICAL RESPONSE TO
MAGNETIC FIELDS
4. On several occasions Persinger, et al [1], carried out measurements on volunteers to assess the (medical/neurological) response to low-frequency magnetic fields, while making concurrent EEG pattern readings on the subjects. In 1990 18 male and 18 female volunteers (University Students) with ages ranging from 18 to 23 years were exposed to 9Hz, 4Hz, and 16Hz fields, plus a sham (control) field. The field strength was varied 0.2mG to 1.0mG (100nT) and pulsed at both polarisations. The fields were generated by solenoids (ref, via a filter circuit, with square waves. The resulting imaging effect was caused by the successive rising and falling edges of the square wave and the components 0.1μf, 5.19mH and 5.2Ω resulted in an impulse, with duration <0.1msec. The experimental decrease returned to zero polarity within 0.1msec, proceeded through a maximum reversed polarity at 0.6msec
and then returned to the zero condition at 1.0msec. Thus, the amplitude of the maximum reversed polarity was 1/6 of the initial rise peak, with a positive and negative mirror at the beginning of each wave. Hence (in the first test case) a 4Hz square wave passed through the circuit, generated 4 initially positive and 4 negative pulses per second. The test chamber was opaque to any other radio interference.
5. Temporal Lobe Activity A significant temporal lobe activity was registered. These areas are the most electrically labile of the human brain. It was demonstrated that people who already possess high levels of activity in this area are likely to experience:
- Mystical or paranormal activities
- Fear
- 'Out of body' activities
- Tingling or vibration.
6. The psychological profile of such people is that they are naturally disposed towards inordinate interests in poetry, mystical or the paranormal, philosophical (religious) and a sense of special purpose, infrequent unusual or unusual events (such as transient social or astronomical events) acquire a special personal meaning. There are strong connections between temporal lobe response activity and epilepsy.
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the only influence present - the magnetic fields.
8. Two further important factors are noted:
- No artefacts were present in the test area to visually suggest themes (for example a space theme is known to evoke 'alien' presence, a reflection artifact is known to evoke reflections on the figure of the person within a room)
- Elaborations and ruminations are known to depend on the personality of the person. People who display frequent temporal lobe signs understand more frequent and intense experiences.
The former was circumvented by placing the subjects in a plain chamber with low intensity red lighting. The second was, to an extent, reduced by taking an adequate population sample.
9. Instrumentation placed on the subject's head measured the temporal lobe bipolar electromyoencephalographic activity. Test results (see para 12-15) with separate experiments with 85 volunteers, described at paper[1], below) are contained in Table 1. There was a general increase in all classes of experience when the fields were at 4Hz and 9Hz, compared with 16Hz (and sham) values. It was noted that people who display more intuition (than sensing), perceiving (than judging) and feeling (than thinking), tend to display enhanced temporal lobe signs. The intensity of the spinning and tingling were less than the other 'symptoms' reported.
10. In 1991 Persinger et al continued their neurological experiment, with human subjects. This time they were exposed to spatially-rotated complex magnetic fields (aimed across the temporal lobes of the brain. It was discovered that the fields markedly increased the interaction with the brain. Exposure resembles Several field frequencies and pulse patterns were used. The results indicate that a person's temporal lobe profile affects the types and intensities of experience reported when exposed for short periods to fields of this type. The full list of 'symptoms' produced is shown at the figures in Table 1. They appear to be amazingly similar to those reported by people who have had close encounters with a UAP. The waves used in the Table are those reported by the 85 male and female volunteers (20 to 37 years).
11. Magnetic Flux Levels The magnetic field strength was 1mG (100nT). A 16Hz pulsed wave generated more experiences of thought intrusion than a 4Hz wave. A 1Hz sine feedback ringing (also at 4Hz) evoked more visual memories and image than the mirror image of the same wave. The effects included vivid visual sensations, memory fragments, a sense of intense meaning, intrusion of ideas or images, mystical experiences and alterations of boundaries defining 'self'.
12. It was deduced that an applied magnetic wave would only be minimally effective (compared with the filtered square wave used) unless the
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current densities are sufficient to produce potentially dangerous disruptions in neuronal assemblies.
13. During the experiments the 1Hz to 1kHz magnetic ambient background level was 0.025mG (2.5nT) and hence was negligible. The rotating magnetic field was either applied in a ringing or in a 'polar burst' of plasmas with the ability to backscatter in the VHF/MF RF Bands. The sprite plasma conducting columns are known to be a few per second rotated once every two seconds. The research showed, once again, that the phenomenological profile of a person within the experimental setting is a function of his (or her) temporal lobe activity, and the demand characteristics of the setting and the magnetic field patterns.
14. The conclusions of the experiments showed that:
- Magnetic fields, rotated bilaterally once every two seconds (over the subject's temporal region) evoked stronger and more frequency experiences than when the field was static.
- Moving yellowish-green and purplish lights were only reported when the field was 'ON'.
- The only 'frequency-specific' effect (within the 4-16Hz range used) was in the enhanced number of thought intrusions when at 16Hz, rather than at 4Hz.
- Smells were reported (when clearly there were none in the test-chamber in reality).
- Normal people, placed in exotic introspective-oriented settings, report experiences that suggest temporal lobe signs and symptoms.
- There is some suggestion that effects might be cumulative.
- The sensitivity of time response as well as what is 'seen or felt' is likely to be conditioned by the subject's personality.
15. In 1996 another experiment was made[3] when another 33 subjects were exposed to four test conditions, a control (sham), left lobes, right lobes, and both left and right together. The field level was 10mG (1 microT) and with 1mG (or 0.1 microT) applied on the other side. Exposure periods lasted 15 minutes (Three segments of five mins on, five mins off). The objective was to increase long term memory effects. The group whose left hemispheres had been exposed exhibited approximately twice the number of accurate ideas relative to other test conditions. The results show that the concept of the 'signature', or the 'information' within a magnetic field may be more important than its intensity.
KEY FINDINGS
16. The key question is what does this all mean in the UAP context? The
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following observations are considered important.
(a) As seen at Table 1 the effects on a human of weak magnetic fields, used for the neurological experiments described, are uncannily similar to those reported by witnesses who have had 'close encounters' with a UAP. The effects experienced depend upon the phenomenological profile of the person.
(b) If a human brain is affected in this particular way it seems that a UAP might be emitting similar levels of magnetic energy since it produces the same effect on an observer.
(c) In the wider context the 'alien', 'time', 'lost', 'spaceship' and other descriptions only ever occur when the observer is very close to the UAP - implying that the human is probably within the UAP near-field. Horizontal magnetic (or electro magnetic) emissions are given off in every direction, but at least some fall within the energy levels given, at the point where they can reach the observer. Clearly, if the observer is some distance away, to achieve an adequate level the source must be greater and attenuated by the time it magnetically couples with the subject.
(d) A magnetic field is not the only emission from a UAP, as visible colour emissions are seen by observers at all distances and, on occasions heat is also reported. A spectrum of emissions is, reportedly, present during the medical experiments carried out.
The magnetic field strengths used on the human volunteers, although low, had a dramatic effect. It seems likely that very much stronger source fields must emanate from UAPs if:
- The memory effects last longer.
- The magnetic energy is, reportedly, sufficient to disrupt electronic and electrical equipment, some metres from the UAP.
17. The magnetic field from a UAP could be directional (even highly so) - hence relative aspect of an observer or equipment nearby, to peaks and nulls of magnetic field, might also determine the local effects. The orientation (left or right temporal lobes) of both of the humans to the received direction might be critical.
18. With reference to Table 1 it should be noted that these responses were obtained in a test chamber with zero visual stimulation. If the subject was confronted with a visual stimulation in the form of a nearby UAP it can easily be appreciated how the 25 responses listed could, however unwillingly, fit into an 'extra-terrestrial' scenario in the mind of the subject. It is clear that the effect could
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be sufficiently vivid as to be so real to the witness(es) concerned to warrant a UAP report to the authorities. In 20 out of 25 instances the reports due to the magnetic fields in the test chamber tally with effects felt and reported during close proximity to a UAP. Close encounters are infrequent; witnesses at greater distances do not report these effects. It seems logical to conclude that they are at a range where the field energy is negligible. If the effect is caused purely by a magnetic field, then it seems possible that the field exists between the UAP and earth, with the flux lines 'leaking' to earth sensibly mostly beneath the object, with some fringing effects.
COMPARISON WITH THE
EARTH'S NATURAL MAGNETIC
FIELD
19. Working Paper No. 12 briefly reports on the natural magnetic field to which every citizen is exposed. It is noted that this amounts (average at mid latitude for the UKADR) to a gamma field value of about 48,850. [Also expressed as 0.485 Gauss or 48,500n Tesla]. Hence, as noted at para 4 above, the bio-magnetic field was only 100nT (i.e. nearly 500 times less than the natural field). The key observation is that although being weak in comparison, unlike the earth's field, the experimental field was pulsed/rotated. It therefore seems possible that fields produced by one or more plasma types listed at paragraph 1 above, and for example, a plasma conceptually produced by a 'noted' energy source may also 'pulse' (though, of course, not necessarily at the same rate observed visually, where witnesses very close to UAP events
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Experience Number Magnetic Field % of Occasions Reported UAP
Experiments Effect Correlates
1 'Felt Dizzy or Odd'[5] 80 *
2 'Felt presence of
someone or
something'[6] 36 *
3 'Felt Tingling
Sensations' 76 *
4 'Saw Vivid Images'[6] 65 -
5 'There were pleasant
vibrations' 67 -
6 'I felt as if I had left
my own body
(detached from)' 46 *
7 'I experienced anger' 20 [7]
8 'I heard a ticking
sound' 50 *
9 'There were odd
smells' 9 *
10 'There were odd
tastes in my mouth' 13 *
11 'I felt as though I was
somewhere else' 69 *
12 'Experienced
childhood thoughts' 42 [7]
13 'Some idea kept
recurring' 77 *
14 'Felt as though
spinning' [6] *
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Experience Number Magnetic Field % of Occasions Reported UAP
Experiments Effect Correlates
16 'Dream-like images' 32 ✓
17 'Lights varied in
intensity' 16 ✓
18 'Experienced fear or
terror' 40 ✓
19 'I felt the experiences
did not come from
my own mind' 20 ✓
20 'I cannot move' [6] ✓
21 'Colours blue-
purple'[2] [6] ✓
22 'Colours yellow-
golden'[3] [6] ✓
23 'red-yellow'[II] [6] ✓
24 'I am moving
forward through a
closed space on all
sides' [6] ✓
25 'Floating' [6] ✓
Notes [1] "I see something mechanical turning round and round"
[2] "I am flying in the sky"
[3] "I see bats and birds flying"
[4] "There is something in here with me"
[5] "Colours are seen in order, first No. 21, then 22, then 23".
[6] No percentages were given in the results published.
[7] The experiences 7, 8, 13 are not observed in any UK UAP reports. It is,
of course, possible that these responses are suppressed by the fact that
(unlike the medical experiments) UAP witnesses are additionally
confronted with the strong visual stimulus of a steady or fluctuating bright
white or coloured object in close proximity.
TABLE 1: CORRELATION OF MAGNETIC EXPERIMENTS AND UAP REPORTS
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[Graph showing signal amplitude vs time in millisecs, with three waveforms labeled a, b, and c. The x-axis shows POINT x (TIME) from 0 to 290, with markers at approximately 40, 80, 120 (marked as 125), 160, 200 (marked as 209), 250, and 290. The y-axis shows AMPLITUDE. Three distinct waveform patterns are visible: waveform 'a' at the top shows irregular oscillations, waveform 'b' in the middle shows smoother wave patterns, and waveform 'c' at the bottom shows burst/pulse patterns.]
FIGURE 1: RINGING & BURST MODE MAGNETIC MODULATIONS
NOTE: HORIZONTAL SCALE IN MILLISECS
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