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A 2010 Defense Intelligence Reference Document, part of the DIA AAWSA (AATIP) series, arguing the technical feasibility of deuterium-fueled thermonuclear pulse propulsion for manned deep-space missions.
Aatip Dird Documents 2018 2019 Dird 11 Dird Advanced Nuclear Propulsion For Manned Deep Space Missions Text
A 2010 Defense Intelligence Reference Document, part of the DIA AAWSA (AATIP) series, arguing the technical feasibility of deuterium-fueled thermonuclear pulse propulsion for manned deep-space missions.
DIA-08-1003-007, dated 11 March 2010 with an information cutoff of 1 December 2009, was prepared under the Defense Intelligence Agency's Advanced Aerospace Weapon System Applications (AAWSA) Program. The author argues that at the present state of science, spacecraft driven by deuterium thermonuclear reactions could reach the outer solar system and eventually the focus of the Einstein gravitational lens at 550 AU. The paper builds on the Orion nuclear-bomb propulsion concept and the 1978 British Interplanetary Society Project Daedalus, replacing a pusher plate with a magnetic mirror that reflects the plasma fireball of a thermonuclear microexplosion. It also discusses GeV proton-beam ignition, magnetic insulation, inductive charging to gigavolt potentials, and conjectured chemical keV superexplosives capable of igniting a deuterium-tritium reaction.
At the present state of science and technology one can build spaceships driven by deuterium thermonuclear reactions, able to reach the outer limits of the solar system.p.7
This concept is generally credited to Stanislaw Ulam, but I know from conversations I had with Heisenberg that a similar idea had been presented to Heisenberg by Wernher von Braun in Berlin in or around 1942p.5
We have little reason to expect that new fundamental laws of physics that could lead to a breakthrough in propulsion still await discovery.p.6
I had a dream last night, about a new form of nuclear weapon, and [I am really scared of it.p.6
The first and most important step toward this goal is to reach the focus of the Einstein gravitational lens at 550 AU (astronomical units).p.7
In the Orion bomb propulsion project, a large number of fission bombs, or fission- triggered fusion bombs, were proposed to lift the spacecraft into space.p.8
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UNCLASSIFIED / (POR OPEtGRH-UGE-OAiee Defense Intelligence Reference Document RS Acquisition Threat eH pe 11 March 2010 ICOD: 1 December 2009 DIA-08 -1003-007 Advanced Nuclear Propulsion for Manned Deep Space Missions UNCLASSIFIED / 2@Re@EEbGEHUGE- Ohi
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UNCLASSIFIED / A=@m Advanced Nuclear Propulsion for Manned Deep Space Missions Prepared by: (b)(3).10 USC 424 erense inte Author: (b)(6) Administrative Note COPYRIGHT WARNING: Further dissemination of the photographs in this publication is not authorized. This product is one in a series of advanced technology reports produced in FY 2009 under the Defense Intelligence Agency, [{(b)(3):10 USC 424 Advanced Aerospace Weapon System Applications (AAWSA) Program. Comments or questions pertaining to this document should be addressed to |(6)(3):10 USC 424° (b)(6) AAWSA Program ; Manager, Defense Intelligence Agency, ATTN: Bldg 6000, Washington, DC 20340-5160. UNCLASSIFIED / /B@RPage 37 · born-digital extraction
UNCLASSIFIED / -42@R-OEEEGR Rie Sein [9] F. Winterberg, "Can a Laser Beam ignite a Hydrogen Bomb?”, United States Atomic Energy Commission, classified January 27, 1970, declassified, July 11, 2007, S-RD-1 (NP — 18252). [10] F. Winterberg, J. Fusion Energy, DOI 10.1007/s10894-008-9143-4. [11] Y.K. Bae, Y.Y Chu, L. Friedman Phys. Rev. 54, R1742 (1995). [12] G.S. Janes, R.H. Levy, H.A. Bethe and B.T. Feld, Phys. Rev. 145, 925 (1966). [13] F. Winterberg, Atomkernenergie, 39, 265 (1981). [14] 0. Buneman, Phys. Rev. 115, 503 (1959). [15] L. Davis, R. List and A. Schliiter Z. Naturforsch. 13a, 916 (1958). [16] F. Winterberg, J. Fusion Energy, DOI 10.1007/s10894-008-9189-3. [17] F. Winterberg, Laser and Particle Beams, 26, 127 (2008). [18] 1.D. Balcomb et al. “Nuclear Pulse Space Propulsion System,” Los Alamos scientific Laboratory, classified November 1970, declassified July 10, 1979, LA - 4541 - MS. [19] S. Fuelling, private communication. [20] R. Kidder in the Proceedings “Physics of High Energy Density”, Academic Press, New York 1971. [21] F. Winterberg, in the same Proceeding p. 398. [22] B. Muller, J. Rafelski, W. Greiner, Phys. Lett. 47B(1), 5(1973). 31 UNCLASSIFIED / / P@"@FFtCGHL-UGE-ON
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UNCLASSIFIED / (POR OPEtGRH-UGE-OAiee Defense Intelligence Reference Document RS Acquisition Threat eH pe 11 March 2010 ICOD: 1 December 2009 DIA-08 -1003-007 Advanced Nuclear Propulsion for Manned Deep Space Missions UNCLASSIFIED / 2@Re@EEbGEHUGE- Ohi
UNCLASSIFIED / A=@m Advanced Nuclear Propulsion for Manned Deep Space Missions Prepared by: (b)(3).10 USC 424 erense inte Author: (b)(6) Administrative Note COPYRIGHT WARNING: Further dissemination of the photographs in this publication is not authorized. This product is one in a series of advanced technology reports produced in FY 2009 under the Defense Intelligence Agency, [{(b)(3):10 USC 424 Advanced Aerospace Weapon System Applications (AAWSA) Program. Comments or questions pertaining to this document should be addressed to |(6)(3):10 USC 424° (b)(6) AAWSA Program ; Manager, Defense Intelligence Agency, ATTN: Bldg 6000, Washington, DC 20340-5160. UNCLASSIFIED / /B@RUNCLASSIFIED / /SQR.A EELS ode SE OP Contents PRG Fg Cie cassis niivcus cas secivaventeascneoneceevasuaviuldasasdvacadacepadeensuucuauautuasraanintys ecavesuuneaas Gielicsecavade v ENEPOGUCTION v4 caccsecscerencoscesccurescocsucdscseonsaesoususcesesseeeses Nievasenivscassphecdeceas dds yevanssesedawesiees 1 Deuterium, Argon Ion Lasers, and KeV Superexplosives ........cs0000 jusuweseangsnanpaaenaene 1 Magnetic Insulation and Inductive Charging.............. scsbabeesbeeeys auvevesuetinemusessasscaveeee 3 Magnetic Insulation Su uWabeuinuseeunuces uiywheananduevenusunauewsaasadaden GeueuweGasawaneneseueesensusouxuauees 3 Inductive Charging....... dictdeneswaweeauncacasins deatyeeed saNenducndesawaukanasnceae duescauseucpeowscuaseceua Deuterium as the Preferred Nuclear Rocket Fuell...sccscssscnsscevecsecnncnncsnscanenececesceceessss 5 Magnetic Entrapment of the Charged Fusion Products and the Stopping of the Proton Beam in Dense Deuterium ....... wiiterwccswazeawaus vaetewseus eedeuatecevetmranens sudeienaeeseeuuus 6 Solution in Between Two Extremes ...ccccssssesssensescsecesnensuencarecauseaenceseaesesnenaeseseesenses LO The Nonfission Ignition of Small Deuterium Nuclear Explosives .......scccccscssseeseenee 13 Delivery of a Gev Proton Beam Onto the Deuterium Fusion Explosive ....csesene. 15 Lifting of Large Payloads Into Earth Orbit ..........cccserecercresesuseverececussvececevereesensereree LO Neutron Entrapment in an Autocatalytic Thermonuclear Detonation Wave —- a Means to Increase the Specific Impulse and to Solve the Large Radiator Problem18 Testing the Deuterium Microdetonation Concept.......ccccscsescceres sia iailueuouvatuinsiuesecaeue 20 CONCIUSIGM si ccasirecuciersaisisdasitaeaccdedweuszaasadesaaneedewsnCadluesoaeatenceovedeusubcaasyvausedsuctvesaaxoeeesk 25 Appendix: Conjectured Metastable Superexplosives Formed Under High Pressure for Thermonuclear Ignition .....ccccssccsenececensnene saadneuseasadadaugaennecucusnenssceatasencucnsnssanceas 26 Bombardment of a Solid Target With an Intense Relativistic Electron or Ion GAIN ike vidas trcwakacoewewdacuccikabaivcacveceavuseueas Stee sanenr SUCCES ET ECAR TERE TT EET T HERE TUTTE SEE REMERON 28 Hypervelocity Impact BORG RS CEREEAEERAAKERER EKA REA SGUGREEREEBER ES RARER ESRARARAEREAEAAERET ERE RE ER RENEE he 28 Bombardment of a Solid Target With Beams or By Hypervelocity Impact, Followed By a Convergent Shock Wave... gcdvecunanavehes Janaaueweacesve svaeduveduieans 28 RGEPETCNCES sii cisntcacscwcuescescis evacnsadcaiaues cas tenewedsudaucdaucwccuduns Wien dawed¥oaddevexdbaunvaawanecaneneios 30 UNCLASSIFIED / /#@R@6636044-065-082—==
UNCLASSIFIED / /®@R=@5526541-065-68i2i—== Figures Figure 1. Ignition With 10’-Ampere GeV Proton Beam..... Seluawaedan Sdicvusuavaubexs ~Ll Figure 2. Pure Deuterium Fusion Explosion Ignited With an Intense Ion Beam .. us 14 Figure 3. Screening of the Spacecraft........0. deateadvascisinesuacens saeaaiedetss sdhuiceinepavateamasce 14 Figure 4. Superconducting “Atomic” Spaceship... ..cscsscsccenecceeereeneeneeueanne ipaueeameanaat 15 Figure 5. Argon Ion Laser [Qmiter......ssccnccccercnseecenaneseucveneneusnansnena scinnnaetnaakevaanewacae sok ¥ Figure 6. Autocatalytic Thermonuclear Detonation = a Soft X-ray wcccserescssseres 18 Figure 7. Ordinary Marx Generator. ......cscceee dials cnaduiudenbadueueeesdacciucuciamcvavwnsaswance 2k Figure &. Super Marx Generator ..ccccccccrencncconenaneusnansnanenenauanenarcnenauas judegianiedaeuaeiasine eo Figure 9. Artist’s Conception of a 1.5--km-Long Super Marx Generator Jcuuuedbewareeas 21 Figure 10. Detail View of a Section of the Super Marx Generator ......:cscscsesesersreres 22 Figure 11. Injection of GeV - 10 MA Proton Be@aim....sescssncncsenenccenanecsnenenanenenecenenanes 22 Figure 12. Showing a Few Elements of the Super Marx Generator .......cscsssesaseneres 22 Figure 13. The Superconducting Toroidal Capacitor and Its Discharge Onto the TAO raise awcnc vawenaawacnatenadtanscswtate wads cisiud cnvesnsasderagsewes puvenvedunnauences wens 24 Figure 14, Explosives .......cccscnecueesesesccecesecescvecerssusevavecsreseseraresscansvercrusesseaparsceseserer 26 Figure 15. With [Increasing Pressure, Electron-Bridges are Formed Between Shelis Inside Shells Melting Into Common Shells ...... cnuaaaanatuaauadnaneenaeee 26 Figure 16. p-d, PreSSure ......ccscscseceseseveseveseveveveresesurerereverarerevercreresnrerssesuseseraravavares 29 Figure 17. Inertial Confinement Fast-Ignition Configuration........cscsce dtuigwen’ siecuve 30 Tables Table 1. The Charged Fusion Products of a Detonation in Deuterium: Their Energy and Velocity ........cccccssssseess Gard uavabieucnuneduue cna cevesneuuassueleesenassuiideveuniewes 5 Table 2. Critical Ignition Currents for Thermonuclear Reactions ekeawasasds dotndes eres 8 UNCLASSIFIED / SPOR OPT ECIAL SSE ene
UNCLASSIFIED / +F@R-95556001018.5-0aLavn Advanced Nuclear Propulsion for Manned Deep Space Missions Preface My interest in space flight datesto when I was about 10 years old and received as a birthday gift a popular book about the feasibility of space flight. From it I learned for the first time about Oberth and Goddard and of the possibility of reaching the Moon with a multistage rocket. This occurred at the same time that Hahn and Strassmann announced the discovery of nuclear fission, with the possibility of an atomic bomb by a fission chain reaction. Having been born in Germany in 1929, I received my Ph.D. in physics under Heisenberg in 1955. Inspired by the 15-megaton hydrogen bomb test conducted by the United States in 1952, I have been deeply interested in the nonfission ignition of thermonuclear reactions by inertial confinement since 1954. At the time all fusion research in the United States was still classified, but I had quite independently discovered the basic principles of inertial confinement, the Guderley convergent shock wave, and the Rayleigh imploding shell solutions. In 1956 I presented my findings at a meeting organized by Von Weizsacker at the Max Planck Institute in Goettingen. The abstracts of this meeting reside today in the University of Stuttgart library. In 1958 I had delivered a paper at the 2nd United Nations Conference on the Peaceful Use of Atomic Energy on Nerva-type nuclear rocket reactors, The paper turned out to be of some importance as I was invited by the U.S. government to come to the United States under “Operation Paperclip.” In San Diego I met Ted Taylor and Freeman Dyson, who were working on the famous “Orion” nuclear bomb propulsion concept. This concept is generally credited to Stanislaw Ulam, but I know from conversations I had with Heisenberg that a similar idea had been presented to Heisenberg by Wernher von Braun in Berlin in or around 1942, Because of my idea to use the Guderley convergent shock wave solution for thermonuclear ignition, Ted Taylor and Freeman Dyson were interested in my joining their group. But because at that time this work was classified and I was not yet a U.S. citizen, this was not possible. In 1967 I saw a new possibility for the nonfission ignition of thermonuclear microexplosions by intense relativistic electron and ion beams, driven by a high-voltage Marx generator. This ignition concept could be used not only to control the release of energy by nuclear fusion, but also to propel a spacecraft, replacing the pusher plate of the Orion concept with a magnetic mirror, reflecting the plasma-fireball of the thermonuclear microexplosion (Reference 1, 2). This idea was adopted by the British Interplanetary Society in its 1978 Project Daedalus starship study, replacing a neutron-rich deuterium-tritium (DT) thermonuclear explosive with a neutron-poor deuterium-helium3 (DHe3) explosive (Reference 3). Unlike the DT reaction, in which 80 percent of the released energy goes into neutrons, most of the energy in the D-He3 reaction goes into alpha particles, which can be deflected by a magnetic mirror. But UNCLASSIFIED / /&@2-05bb6bAiedSE-Obiee
UNCLASSIFIED / / BAR QEELGL Ala GInG Pies because He3 is not abundantly available everywhere, it was proposed to “mine” it from Jupiter’s atmosphere. Studies have been conducted on spacecraft propulsion with the matter- antimatter annihilation reaction, however, it is an enormous technical challenge to produce antimatter in appreciable quantities. The idea of using nano-gram amounts of antimatter for the ignition of fission-fusion microexplosions appears to have credible potential, but even there the production and storage of nano-gram quantities of antimatter pose serious technical problems (Reference 4). We have little reason to expect that new fundamental laws of physics that could lead to a breakthrough in propulsion still await discovery. Very much as America was discovered only once, it is quite possible that all the fundamental laws of physics relevant to propulsion have been discovered, challenging our imagination to find out if they are sufficient to invent propulsion systems that ultimately might bring us to Earthlike planets of nearby solar systems. I conclude this preface with an imaginary talk by Ted Taylor to Freeman Dyson as recorded by the latter’s son, George Dyson, in his book Project Orion -— The True Story of the Atomic Spaceship (Reference 5), followed by a dream of Ted Taylor’s. “Freeman’s hope for the Orion had rested on the fact that there seems to be no law of nature forbidding the construction of fission-free bombs,” and on the belief that “improvements in the design of the nuclear devices (by reducing the fraction of total yield due to fission} might achieve reduction factors of 102 to 10°. This belief in small, fissian-free bombs has largely evaporated.” “One exception is Ted (Taylor). He remains convinced that small, clean bombs could propel Orion - but he still fears more than ever that such devices would be irresistible as weapons, until we outgrow the habit of war. There are lots of different routes to that final result of a very clean bomb.” “Could you make a one-kiloton explosion in which the fission yield was zero, which is bad news on the proliferation front, but could turn Orion into something quite clean?” “Freeman thinks Ted is wrong -— and Ted hopes Freeman its right.” I for my part think Freeman is wrong. Many years later, shortly before his death, Ted Taylor reported: “I had a dream last night, about a new form of nuclear weapon, and [I am really scared of it.” He reported that when he woke up, he wrote down his dream, and it appeared scientifically sound and feasible. What was it? We never will know with certainty, but I have a guess: it is the possibility of chemical superexplosives (explained in the appendix) powerful enough to ignite a thermonuclear bomb. vi UNCLASSIFIED / /@@8.-0:4516146L. 35 5.0 Bl Moms
- UNCLASSIFIED / / FO R-OPEECERE OSE UNTT Introduction As Hermann Oberth proved for chemical rockets in his 1923 book The Rocket into Planetary Space (Reference 6), this paper will try’ to prove for thermonuclear rockets the following: e At the present state of science and technology one can build spaceships driven by deuterium thermonuclear reactions, able to reach the outer limits of the solar system. e Such spaceships permit the manned exploration of the entire solar system and beyond, with the ultimate potential to reach nearby solar systems. e The cost in research and development to build such spaceships will be high but still well within what is economically feasible. e Using the same physical principles as for deuterium fusion rockets will also lead to the realization of clean nuclear energy, justifying the expenditures for these large projects. Deuterium can be used as the rocket fuel of choice in addition to any inert material that is suitable as a propellant. This propellant material is available on most planetary bodies and particularly on the comets of the Oort cloud. The main idea is that by gradual radial expansion from the Sun by building bridges over the Cort clouds, which presumably surround all suns, Earthlike planets in neighboring solar systems can eventually be reached. The first and most important step toward this goal is to reach the focus of the Einstein gravitational lens at 550 AU (astronomical units). At this location, one can use the Sun as the lens of a super telescope, an idea first proposed by Claudio Maccone in 1993. Present knowledge is that there are planets in nearby solar systems that are likely Earthlike planets. It is only with this gigantic telescope that one can determine if life on these planets is possible. But because of the complexity of this task, a manned mission to the Einstein gravitational lens focus is likely to be needed, possible only with advanced nuclear rocket propulsion. Deuterium, Argon Ion Lasers, and KeV Superexplosives The goal is a spacecraft that can be refueled while landing on a planetary body, which can be a planet, an asteroid, or a comet. With heavy water available on many planetary bodies but in particular on comets, this suggests the use of deuterium (D) as the thermonuclear rocket fuel. Ignition of deuterium though, is more difficult than ignition of the deuterium-tritium (DT) reaction or of the deuterium-helium3 (DHe?) reaction. The OT reaction is the easiest to ignite, but 80 percent of the energy goes into neutrons, which cannot be deflected by a magnetic mirror. In the DHe? reaction all the energy goes into charged fusion products, but in a mixture of D with He? there are still some neutron-producing deuterium-deuterium (DD) reactions. More important is the fact that, unlike deuterium, He? is largely unavailable. There is some indication of He on the surface of Moon. In the Daedalus starship study by the British Interplanetary 1 ‘UNCLASSIFIED / APO} OFRGHEUSr-Onr
UNCLASSIFIED / 2Q3.05516044=-06E One Society, it was proposed to “mine” He? from the atmosphere of Jupiter. In either case, the cost to recover appreciable amounts of He? would be very high. For the DD reaction, the situation is quite different because there the instantaneous burn with deuterium of the T- and He?- reaction products of deuterium makes possible a detonation wave in dense deuterium. In this detonation wave, only 38 percent of the energy released goes into neutrons, compared with 80 percent for the DT reaction. Deuterium can be extracted from water with relative ease in three steps: e Water is electrolytically split into hydrogen and oxygen. e The hydrogen gas, composed of Hz and HD, is cooled down until it liquefies, whereby the heavier HD is separated by the force of gravity from the lighter H2. e The newly produced HD is heated and passed through a catalyst, splitting HD into H2 and D2, according to the equation (Reference 7) 2HD —* Hz + Dz. Since the gravitational field on the surface of a comet or small planet, from which the D2 shall be extracted, is small, the apparatus separating the liquid HD from Hz must be set into rapid rotation. The comparatively small amount of energy needed for the separation can ideally be drawn from a ferroelectric capacitor (for example, a barium-titanate capacitor with a dielectric constant ¢ + 5,000), to be charged up to many kilovolts by a small fraction of the electric energy drawn from the deuterium fusion explosions through a magneto hydrodynamic loop (Reference 2). One can also draw this energy from a small on-board nuclear reactor requiring only a small radiator, slowly charging the capacitor. Alternatively, one may store the needed energy in the magnetic field of a superconductor. For the launching of the spacecraft into Earth orbit, a very different scheme is proposed. It requires special materials that are readily available on Earth but not on extraterrestrial bodies serving as landing points to refuel the spacecraft. There the primary resource is water from which deuterium is obtained. In the Orion bomb propulsion project, a large number of fission bombs, or fission- triggered fusion bombs, were proposed to lift the spacecraft into space. Since this would release a large amount of highly radioactive fission products into the atmosphere, it was one of the causes that killed Orion. Even though large payloads can be brought into Earth orbit by chemical rockets, this remains very expensive, and an acceptable less expensive nuclear alternative is highly desirable. There appear to be two possibilities: e A laser driven by a high explosive, powerful enough to ignite a DT microexplosion, which in turn can initiate a thermonuclear detonation in deuterium (Reference 8). e Asecond, more speculative possibility is the conjectured existence of chemical kiloelectronvolt (keV) superexplosives. These are chemical compounds formed under high pressure, resulting in keV bridges between inner electron shells and able to UNCLASSIFIED / AP@?eOPPPCRRE SS OnerT”
UNCLASSIFIED / /POfeOPFIGEAE-UG5-O8lia~ee: release intense bursts of keV X-rays capable of igniting a DT thermonuclear reaction, which in turn could ignite a larger deuterium detonation. To realize the first possibility, one might consider pumping a solid argon rod with a convergent cylindrical shock wave driven by a high explosive (Reference 9). If the argon rod is placed in the center of convergence and reaches a temperature of 90,000 °K, the upper ultraviolet laser level of the argon will be populated. Following this heating, the argon cylinder radially expands and cools, with the upper laser level frozen into the argon. The energy thus stored in the upper laser level can then be removed from the rod by a small Q-switched laser, the resulting powerful laser pulse optically focused onto a thermonuclear target. To realize the second possibility, one would have to subject suitable materials to very high pressure (Reference 10, 11). These energetic states can be reached only if during their compression the materials are not appreciably heated, because such heating would prevent the electrons from forming the bridges between the inner electron shells. Details of the second possibility are provided in the appendix. Magnetic Insulation and Inductive Charging Two concepts are of great importance for the envisioned realization of a deuterium fusion-driven starship: e The concept of magnetic insulation, which permits the attainment of ultrahigh voltages in high vacuum (Reference 1). e The concept of inductive charging, by which a magnetically insulated conductor can be charged up to very high electric potentials (Reference 12). MAGNETIC INSULATION In a greatly simplified way, magnetic insulation can be understood as follows: if the electric field on the surface of a negatively charged conductor reaches a critical field on the order of Ec ~ 10’ V/cm, the conductor becomes the source of electrons emitted by field emission. The critical electric field for the emission of ions from a positively charged conductor is ~ 108 V/cm. Therefore, if in a high-voltage diode the electric field reaches ~ 107 V/cm, breakdown will occur by electric field emission from the cathode to the anode. But if a magnetic field of strength 8 measured in gauss is applied in a direction parallel to the negatively charged surface, and if B > E, where E (like B) is measured in electrostatic cgs units, the field-emitted electrons make a drift motion parallel to the surface of the conductor with the velocity. ft ar (1) To keep va/c < 1 then requires that E < H. Let us assume that H = 2x 10* G, which can be reached with ordinary electromagnets, means that — < 2x10* esu = 6x 10° V/cm. UNCLASSIFIED / /2@R-O551G604iedSE-ORioGee
UNCLASSIFIED / (POR'SPPICTALT USE ONLY For a conductor with a radius of A~10m = 102 cm, an example for a small starship configuration, one can reach a voltage on the order of FA < 6 x 109 volts. INDUCTIVE CHARGING To charge the spacecraft to the required gigavalt potentials, we choose for its architecture a large but hollow cylinder, which at the same time acts as a large magnetic field coil. If thermionic electron emitters are placed inside this coil and the magnetic field of the coil rises in time, Maxwell’s equation Vx ae (1/0) @B/artinduces an azimuthal electric field inside the coil: ; ee E,=-5-8: (2) where B = B- is directed along the z-axis, with r the radial distance from the axis of the coil. In combination with the axial magnetic field, the electrons from the thermionic emitters make a radial inward-directed motion yo =o e-- (3) By Maxwell’s equation div E = Amer, this leads to the buildup of an electron cloud inside the cylinder, resulting in the radial electric field E = 2aner (4) This radial electric field leads to an additional azimuthal drift motion v, =cE, /B. (5) superimposed on the radially directed inward drift motion vr. For the newly formed electron claud to be stable, its maximum electron number density must be below the Brillouin limit: mo < fmax = B2/ 4 mez (6) where mc? = 8.2 x 10°” erg is the electron rest mass energy. For 8 = 2x10*G, one finds that Mmax # 4x 10!5 cm. To reach with a cylindrical electron cloud of radius R a 4 UNCLASSIFIED / #®@2=@2EtGhti=-U6E-e2%
UNCLASSIFIED / /@@-2-0.5546041-055-0iiiniae potential equal to V requires an electron number density 7 = v/ mR’. For V = 10° valts ~% 3x10°esu and R = 107cm, one finds that nm ~ 210° cm, well below Amax. Deuterium as the Preferred Nuclear Rocket Fuel To appreciate the importance of deuterium as the preferred and abundantly available nuclear rocket fuel, one must consider the secondary reactions with D of the He? and T reaction products from D-D fusion. Taking these reactions into account, one obtains from 6 deuterium nuclei an energy of 26.8 megaelectronvalts (MeV) in charged fusion products, made up of He? and H, and an energy of 16.55 MeV in neutrons. This means 62 percent of the energy is released into charged fusion products and 38 percent into neutrons—a substantial improvement over the DT reaction, in which only 20 percent of the energy goes into He‘, Of interest also is the average velocity, averaged over the momentum of the charged fusion products, because it is a measure of the maximum specific impulse, respectively the maximum exhaust velocity: 6 >; ALY, =I v= (7) For the six charged fusion reaction products (given in Table 1), one obtains ys 1.5x 10° cm/s. Table 1. The Charged Fusion Products of a Detonation in Deuterium: Their Energy and Velocity Energy |MeV| Velocity 10° [cm/s] He He He UNCLASSIFIED / /*@f-OFERSGRRE SSP OnNtTr”
UNCLASSIFIED / 482.2. O551G60 04S hae ie Because the 6 charged fusion products are accompanied by 9 electrons, they have to share their kinetic energy with 9 electrons. This reduces the maximum specific impulse by the factor //(6+9)/6 = V2.5 to v = 0.95x10%cm/s. A reduction of the specific impulse does not occur if the electrons have enough time to escape the burning plasma behind the detonation front; that is, in a time shorter than the time for them to be heated by the charged fusion products. The time needed for the electrons to be heated by the charged fusion reaction products can be computed from the range Ao of the charged fusion products and their velocity v in a plasma at the temperature 7. For the He* fusion products, the range is given by apr, 342 ie atkT) ,a@ = 2.5x10*4 [cgs] (8) This time is (9) It then has to be compared with the time the electron can escape the burning plasma behind the detonation front, given by Li e rf, (10) where re is the radius of the burning deuterium cylinder, and ve the electron velocity. One thus has ae vo OAK, Wag T ~y, atkTy? (11) Putting 7 = 1023 cm, T » 108 K with v, ~ 109 cm/s, v~ 10° cm/s, one finds ¢,,./r7~ 2.57,. Therefore, ¢,,.< crequires that ~< 0.4 cm. Fo exe To reach the highest specific impulse possible, one should make the deuterium cylinder as thin as possible. Magnetic Entrapment of the Charged Fusion Products and the Stopping of the Proton Beam in Dense Deuterium If a fission bomb is used to trigger a thermonuclear detonation, so much energy is available that almost any radiation implosion configuration is likely going to work. As an example, one may place a fission bomb and a sphere of solid deuterium in a shell of 6 UNCLASSIFIED / /2@R-@FFTGERESSEONTT
UNCLASSIFIED / /605-@05EEGEHEUSEORtT” gold, in the two foci of an ellipsoidal cavity. The radiation released by the exploding fission bomb, by ablating the gold, launches a convergent shock wave into the liquid deuterium. With the temperature in the shock wave approximately rising as I/r, where ris the distance of the shock wave from the center of the deuterium sphere, the ignition temperature is reached at some distance from the center. But only if this distance is larger than the stopping length of the DD fusion reaction products, typically a few cm, is a radially outward-moving detonation wave ignited. This configuration is essentially the same kind of “hohlraum” (cavity) configuration used in the indirect drive mode of laser fusion for a small DT sphere. A configuration of this kind can still be used to burn deuterium if the DT microexplosion is used to trigger a larger deuterium explosion. For a starship that will depend on deuterium as its only rocket fuel, this possibility is excluded. But another possibility arises if the ignition is done with a 107-ampere gigaelectronvolt (GeV) proton (or deuterium) beam. If focused onto one end of a slender, cylindrical deuterium rod, the beam not only can be made powerful enough to ignite the deuterium, but its strong azimuthal magnetic field entraps the charged DD reaction fusion products within the deuterium cylinder, launching a deuterium detonation wave propagating with supersonic speed down the cylinder (Reference 13). There the fusion gain and yield can in principle be made arbitrarily large, depending only on the length of the deuterium rod. The range of the charged fusion products is determined by their Larmor radius a h ~B (12) where ? my lf2 a a &2MAE) (13) € Z In equation (13), c, e are the velocity of light and the electron charge, M the hydrogen mass, A the atomic weight, and Z the atomic number. EF is the kinetic energy of the fusion products. If the magnetic field is produced by the proton beam current I, one has at the surface of the deuterium cylinder the azimuthal magnetic field B,=0,21/r (14) Combining equation (12) with equation (14) and requiring that ~ <r, one finds that UNCLASSIFIED / SPOR OPPPOCERE OSE CONEY
UNCLASSIFIED / /SQ2.0551G5¢=-USEONEY ewe (15) where Ic = 5a. In Table 2, the values for a and Jc for all the charged fusion products of the DD reaction are compiled. For all of them, the critical current is below Ic = 3.84 x 10° A. Therefore, with the choice J ~ 107 A, all the charged fusion products are entrapped inside the deuterium cylinder. Table 2. Critical Ignition Currents for Thermonuclear Reactions Ln A (A a a aC 2.5x10 1.25x10 For the argon ion laser configuration proposed for the launch into Earth orbit, where a small amount of DT serves as a trigger for the ignition of a larger amount of deuterium, the ignition of a magnetic field supported detonation wave in deuterium is possible there with an auxiliary high-explosive-driven megampere current generator, setting up an axial magnetic field, by an azimuthal current around the rod. The charged fusion products there are spiraling down the rod. The current needed to entrap the charged fusion products are there on the same order of magnitude; that is, ~ 107 A. For the deuterium-tritium thermonuclear reaction, the condition for a propagating burn in a sphere of radius r and density p, heated to a temperature of 10® K, is given by pr = 1 g/cem?. This requires energy of about 1 megajoule (MJ). For the deuterium reaction, this condition is pr => 10 g/cm?, with an ignition temperature about 10 times larger. That a thermonuclear detonation in deuterium is possible at all is due to the secondary combustion of the T and He? DD fusion reaction products (Reference 8). The energy required would be about 10% times larger, or about 104 MJ—for all practical purposes out of reach for nonfission ignition. However, if the ignition and burn are along a deuterium cylinder, where the charged fusion products are entrapped by a magnetic field within the cylinder, the condition pr >10 g/cm? is replaced by pz210 g/cm? (16) where z is the length of the cylinder. UNCLASSIFIED / /2@2-O6556RirHUSE-CHEY
-UNCLASSIFIED/ /®@R-@FF1IGEA-6E-08-¥ If the charged fusion products are entrapped within the deuterium cylinder, and if the condition pz >10g/cm? is satisfied, and finally, if the beam energy is large enough that a length z > (10/p) cm of the cylinder is heated to a temperature of 10° K, a thermonuclear detonation wave can propagate down the cylinder. This then leads to large fusion gains. | The stopping length of single GeV protons in dense deuterium is much too large to fulfill inequality (Reference 16). But this is different for an intense beam of protons, where the stopping length is determined by the electrostatic proton-deuteron two-stream instability (Reference 14). In the presence of a strong azimuthal magnetic field, the beam dissipation is enhanced by the formation of a collisionless shock (Reference 15) with the thickness of the shock by order of magnitude equal to the Larmor radius of the deuterium ions at a temperature of 10° K, which for a magnetic field on the order of 107 G is on the order of 10° cm. For the two-stream instability alone, the stopping length is given by (17) where c is the velocity of light, w; the proton ion plasma frequency, and ¢=n,/n, with nm the deuterium target number density and np = 2x10'*cn3, the proton number density in the beam. For a hundredfold compressed deuterium rod, one has n=5x10%cm'3, with @ =2x10'"s. One finds that ¢=4x10° and 2=1.2«x107 em. This short length, together with the formation of the collisionless magneto-hydrodynamic shock, ensures the dissipation of the beam energy into a small volume at the end of the deuterium rod. For a deuterium number density n=5x10"cm3, one has 9=17g9/cm3, and to have pz >10 g/cm? requires that z2>0.6cm. WithA < z, the condition for the ignition of a thermonuclear detonation wave is satisfied. The ignition energy is given by Ey ~ 3nkTar-z (18) where T # 10° K. For hundredfold compressed deuterium, one has ar* = 10 cm2, where initially it was ar? =10°'cm?. With ar? =107 cm? and z=0.6cm, one finds that E, <10'*erg or < teu 1G]. This energy is provided by the 10’-ampere GeV proton beam lasting 10°’ seconds. The time is short enough to ensure the cold compression of deuterium to high densities. For a 103-fold compression, found feasible in laser fusion experiments, the ignition energy is 10 times less. In hitting the target, a fraction of the proton beam energy is dissipated into X-rays by entering and bombarding the high Z material cone, focusing the proton beam onto the deuterium cylinder. The X-rays released fill the hohlraum surrounding the deuterium 9 UNCLASSIFIED /+2@-@E6Gh- UGE CHE
UNCLASSIFIED / /2@2-95516041-U6>0N2-= cylinder, compressing it to high densities, while the bulk of the proton beam energy heats and ignites the deuterium cylinder at its end, launching in it a detonation wave. If the GeV -107-ampere proton beam passes through background hydrogen plasma with a particle number density n, it induces in the plasma a return current carried by its electrons, where the electrons move in the same direction as the protons. But because the current of the proton beam and the return current of the plasma electrons are in opposite directions, they repel each other. Since the stagnation pressure of the GeV - 10’-ampere proton beam is much larger than that of the electron return current, the return current electrons will be repelled from the proton beam toward the surface of the proton beam. The stagnation pressure of a GeV proton beam is (Mx proton mass) P= pc =nM yc (19) For n, = 2x10'*em3, one obtains p, = 3x10'*dyn/cm?. For the electron return current, one has (m electron mass) p, = hmv {20) With the return current condition n,ev, =n,ev,, where for GeV protons vy, =c, one has v,fe= n/n, (21) Taking the value n, =5x10°cm, valid for uncompressed solid deuterium, one obtains v., 10° cm/s and hence p, = 5x10° dyn/cm. This is negligible against pi, even if ne is 103 times larger, as in highly compressed deuterium. The assumption that the magnetic field of the proton beam is sufficiently strong to entrap the charged fusion products within the deuterium cylinder is therefore well justified. Solution in Between Two Extremes With chemical propulsion, manned space flight to the Moon is barely possible and only with massive multistage rockets. For manned space flight beyond the Moon, nuclear propulsion is indispensible. Nuclear thermal propulsion is really not much better than advanced chemical propulsion. Ion propulsion, using a nuclear reactor to drive an electric generator, has a much higher specific impulse but not enough thrust for short interplanetary transit times needed for manned missions. This leaves propulsion by a chain of fission bombs (or fission-triggered fusion bombs) as the only credible option. There the thrust and specific impulse are comparatively huge, but a comparatively small explosive yield is desirable. Making the yield too small, the bombs become 10 UNCLASSIFIED / /(@®=@EE6G5ir-U6E-ONi ==UNCLASSIFIED /+F@?-@FEtGi- UGC extravagant in the sense that only a small fraction of the fission explosive is consumed. This problem can be overcome through the nonfission ignition of small fusion explosions. A first step in this direction is the nonfission ignition of deuterium-tritium (DT) thermonuclear microexplosions, expected to be realized in the near future. This reaction was chosen for the first proposed thermonuclear microexplosion propulsion concept, with the ignition done by an intense relativistic electron beam (Reference 1, 2). But because in the DT reaction 80 percent of the energy is released into neutrons that cannot be reflected from the spacecraft by a magnetic mirror, it was proposed to surround the microexplosion with a neutron-absorbing hydrogen propellant, increasing the thrust at the expense of the specific impulse. For this reason, in the “Daedalus” interstellar probe study by the British Interplanetary Society (Reference 3), the neutron-less helium3-deuterium (He?-D) reaction was proposed, because for such a mission the specific impulse should be as high as possible. But even in a He?-D plasma, there are a some neutron-producing DD reactions. There is no large source of He? on Earth, though it might exist on the surface of the Moon and in the atmosphere of Jupiter. In the DD reaction, much less energy goes into neutrons, but it is more difficult to ignite. The situation is illustrated in Figure 1. On the upper left side is the experimentally verified ignition of a DT pellet with the X-rays generated in an underground test from a fission bomb (Centurion Halite experiment at the Nevada Test Site). For the ignition of the DT reaction with propagation thermonuclear burn (that is, detonation), one requires a few megajoules, with a density xradius target product, pr = 1g/cm2. On the upper right side is the 15-megaton “Mike” test, where with the Teller-Ulam configuration a large amount of liquid deuterium is ignited with a fission bomb. For the DD reaction propagating thermonuclear burn (that is, detonation), one requires that pr = 10g/cm?. At the bottom is the proposed hypothetical deuterium target, where a detonation wave in a thin cylindrical deuterium rod is ignited by a pulsed 10’-ampere GeV proton beam, utilizing the strong magnetic field of the beam current. Solution in between two extremes £2 10") L210" 4 prez | afem- pr= 10 gem Centurion — Halite (DT Pellets) Mike Test (Teller/Ulam Configuration) FSi J p22 10 g/en* f2INA Hypothetical D-D Ignition with Super Marx Generator Figure 1. Ignition With 107-Ampere GeV Proton Beam (Reference 16) 11 UNCLASSIFIED / AP@ieOFPEGE=U6EOhE
UNCLASSIFIED / (POR OPEL esl ort” To estimate the order of magnitude of what is needed, we consider a spacecraft with a mass of M, =10°ton =10°g, to be accelerated by one g =10*cm/s?, with a thrust T=M,¢g =10? dyn. To establish the magnitude and number of fusion explosions needed to propel the spacecraft to a velocity of v=100 km/s = 10’ cm/s, we use the equation T =c— (22) where we set ¢c =10° cm/s, equal to the expansion velocity of the fusion bomb plasma. We thus have dim 7 _ 10*g/s = 10 kg/s (23) dt o¢ The propulsion power is given by = SF (24) which in our example is P =5~10'’erg/s. With F=4x10' erg equivalent to the explosive energy of one kiloton of TNT, ? is equivalent to about one nuclear kiloton bomb per second. From the rocket equation yv=cln ve (25) where “ois the initial and “1 the final mass, and setting M,. My. am , where AM <<» is the mass of all used up bombs, one has vacen{14 Sit) 5 Att (26) Here vy is the velocity reached by the spacecraft after having used up all the bombs of mass AM. If one bomb explodes per second, its mass according to equation (23) is mo = 10% g. 12 UNCLASSIFIED / #F@fe@FFter-Us-CnePUNCLASSIFIED / -P@?-@5FtGR-U6i-Oiiis Assuming the spacecraft reaches a velocity of »v = 100 km/s =106’ cm/s, the velocity needed for fast interplanetary travel, one has AM =10*g, requiring NV = AM /m, =10" 1- kiloton fusion bombs, releasing the energy £, =5x10'° x104 =5x10" erg. By comparison, the kinetic energy of the spacecraft E, ={1/2)M, v2 = 5x 1022 erg is 10 times less. In reality it is still smaller, because a large fraction of the energy released by the bomb explosions is dissipated into space. One can summarize these estimates by concluding that a very large number of nuclear explosions are needed, which for fission explosions, as well as for deuterium-tritium explosions, would become very expensive. This strongly favors deuterium, which is more difficult to ignite than a mixture of deuterium with tritium but is abundantly available. The following text tries to show how bomb propulsion solely with deuterium might be possible. The Nonfission Ignition of Small Deuterium Nuclear Explosives With no deuterium-tritium (DT) microexplosions yet ignited, the nonfission ignition of pure deuterium (DD) fusion explosions seems to be a tall order. An indirect way to reach this goal is by staging a smaller DT explosion with a larger DD explosion. There the driver energy, but not the driver, may be rather small. A direct way requires a driver with order of magnitude larger energies. The generation of GeV potential wells, made possible with magnetic insulation of conductors levitated in ultrahigh vacuum (in a laboratory on Earth), has the potential to lead to order of magnitude larger driver energies (Reference 1). It is the ultrahigh vacuum of space that enables this to be achieved without levitation. Therefore, the spacecraft, acting as a capacitor, can be charged up to GeV potentials. If the spacecraft is charged to a positive GeV potential, a gigajoule intense relativistic ion beam below the Alfvén current limit can be released from the spacecraft and directed to the deuterium explosive for its ignition. If the current needed for ignition is below the Alfvén limit for ions, the beam is “stiff.” The critical Alfvén current for protons is I, =3.1x10’ By [A], where B=v/e,y =(i- f”) ae with v the proton velocity and c the velocity of light. For GeV protons, 7, is well in excess of the critical current (Reference 15) to entrap the DD fusion reaction products, the condition for detonation (Reference 13). . In a possible bomb configuration shown in Figure 2, the liquid (or solid) D explosive has the shape of a long cylinder, placed inside a cylindrical “hohlraum” h, A GeV proton beam I coming from the left, in entering the hohlraum, dissipates part of its energy into a burst of X-rays compressing and igniting the D bomb-cylinder. With its gigajoule energy lasting less than 10’ seconds, the beam power is greater than 10'* watts, sufficiently large to ignite the D explosive. The main portion of the beam energy is focused by the cone onto the deuterium rod, igniting at its end a detonation wave. 13 UNCLASSIFIED / -P@R-@6EEGHiGE-Odl eoUNCLASSIFIED / #@R-@25652650-062-68-¥4 Figure 2, Pure Deuterium Fusion Explosion Ignited With an Intense Ion Geam., D deuterium rod, h hohlraum, I ion beam, B magnetic field, R miniature target rocket chamber, Ha solid hydrogen, L laser beam to heat hydrogen in miniature rocket chamber. Because the condition for thermonuclear burn and detonation depends only on the critical current (Reference 15) and not on the radius of the deuterium cylinder, one may wish to make the diameter of the deuterium cylinder as small as possible, because as it was shown above, the specific impulse can become largest, with the electrons not taking away kinetic energy from the charged fusion products. Therefore, the yield of the deuterium fusion explosions can be made much smaller, eliminating the need for Orion- type shock absorbers, but the thrust there is also much smaller. For very-deep-space missions, that would not be a disadvantage. A problem in either case is that 38 percent of the energy is released as neutrons. In hitting the spacecraft, they lead to its heating, requiring a presumably large radiator. For a long and thin deuterium rod, this problem can likely be reduced by a boron diaphragm on the deuterium rod, as shown in Figure 3, because boron is a good neutron absorber. It can be enhanced by a hydrogen moderator, because the absorption cross section for neutrons is greatly increased with a reduced neutron kinetic energy. Both the boron and the hydrogen there simply become part of the propellant, reducing the specific impulse but increasing the thrust. Figure 3. Screening of the Spacecraft, SC, Against the Neutrons, n, By a Boron Diaphragm, b, With Solid 14 UNCLASSIFIED/ /@@8:@FESGitieWG EO bbiniee
UNCLASSIFIED /FPOReOPRPSCERE USE ONT? Hydrogen H2 as a Neutron Moderator to Increase the Neutron Absorption Cross Section of Boron, With the Neutrons Released From Deuterium Cylinder d. As noted earlier, in comets there is a large amount of deuterium readily available for mining. And we know comets also contain nitrogen and carbon. From this knowledge we can assume that very likely other light elements, such as boron, exist in relatively high concentrations in comets. Although the waste heat radiator remains a problem, it favors large explosions, because most of the waste heat accompanies the propellant into space. Droplet radiators, with the droplets slowly evaporating, are unlikely to work. Placing the neutron-absorbing radiators near the shock absorber, permitting them to get red-hot, and thermally insulating the rest of the spacecraft from the radiators may solve the problem. Delivery of a Gev Proton Beam Onto the Deuterium Fusion Explosive The spacecraft is inductively charged against an electron cloud surrounding the craft, and, with a magnetic field on the order of 10°G, easily reached by superconducting currents flowing in an azimuthal direction around the craft, is magnetically insulated against the electron cloud up to GeV potentials. The spacecraft and its surrounding electron cloud form a virtual diode with a GeV potential difference. To generate a proton beam, it is proposed to attach a miniature hydrogen-filled rocket chamber R to the deuterium bomb target at the position where the proton beam hits the fusion explosive (see Figure 2). A pulsed laser beam from the spacecraft is shot into the rocket chamber, vaporizing the hydrogen, which is emitted through the Laval nozzle as a supersonic plasma jet. If the nozzle is directed toward the spacecraft, a conducting bridge is established, rich in protons between the spacecraft and the fusion explosive, Protons in this bridge are then accelerated to GeV energies, hitting the deuterium explosive. Because of the spacecraft’s large dimensions, the jet does not have to be aimed at the Spacecraft very accurately. The original idea for the electrostatic energy storage on a magnetically Figure 4. Superconducting “Atomic” Spaceship, Positively Charged to GeV Potential, With Azimuthal Currents and Magnetic Mirror M By Magnetic Field B. F fusion minibomb in position to be ignited by intense [on beam I, SB storage space for the bombs, BS bioshield for the payload PL, C coils pulsed by current drawn from Induction ring IR. @ electron flow neutralizing space charge of the fusion explosion plasma. insulated conductor was to charge up a levitated superconducting ring to GeV 15 UNCLASSIFIED / 4bOP-@551GRAirU6rONe
UNCLASSIFIED / 2@R-@EEGEA=VSEONEY potentials, with the ring magnetically insulated against breakdown by the magnetic field of a large toroidal current flowing through the ring. It is here proposed to give the spacecraft a topologically equivalent shape, using the entire spacecraft for the electrostatic energy storage (see Figure 4). There toroidal currents flowing azimuthally around the outer shell of the spacecraft not only magnetically insulate the spacecraft against the surrounding electron cloud but also generate a magnetic mirror field that can reflect the plasma of the exploding fusion bomb. In addition, the expanding bomb plasma can induce large currents, and if these currents are directed to flow through magnetic field coils positioned on the upper side of the spacecraft, electrons from there can be emitted into space surrounding the spacecraft by thermionic emitters placed on the inner side of these coils, inductively charging (Reference 12) the spacecraft for subsequent proton beam ignition pulses. A small high-voltage generator driven by a small onboard fission reactor can make the initial charging, ejecting from the spacecraft negatively charged pellets. With the magnetic insulation criterion £< BCE,B,in electrostatic units, esu), where 8 is the magnetic field surrounding the spacecraft measured in gauss, then for B= 104G, FE =3x10°esu = 9x105 V/cm, one has E ~ (1/3)B, hence E < B. A spacecraft with the dimension 7 ~ 3x10*cm can then be charged to a potential £7 ~3x10° volts, with the stored electrostatic energy on the order of « ~ (e*/s7) is For E=3xIl0*esu and /=3x10'cm, ¢ is onthe order of 1 gigajoule. The discharge time is on the order of r ~ 7/c, where c =3x10'°cm/s is the velocity of light. In our example, we have zr ~10’sec. For a proton energy pulse of 1 gigajoule, the beam power is 3x10'°erg/s = 30 petawatts, large enough to ignite a pure deuterium explosion. Lifting of Large Payloads Into Earth Orbit To lift large payloads into Earth orbit remains the most difficult task. For a launch from the Earth’s surface, magnetic insulation inside the Earth’s atmosphere fails, and with it the proposed pure deuterium bomb configuration. A different technique is suggested here, one I had first proposed in a classified report dated January 1970 (Reference 9), declassified in July 2007, and thereafter published (Reference 17). A similar idea was proposed in a classified Los Alamos report, dated November 1970 (Reference 18) and declassified in July 1979. In both cases the idea is to use an expendable laser for the ignition of each nuclear explosion, with the laser material thereafter becoming part of the propellant. The Los Alamos scientists had proposed to use an infrared carbon dioxide (CO2) or chemical laser for this purpose, but this idea does not work, because the wavelength is too long and therefore unsuitable for inertial confinement fusion. I had suggested an ultraviolet argon ion laser instead. However, since argon ion lasers driven by an electric discharge have a small efficiency, I had suggested a quite different way of pumping it, illustrated in Figure 5. There the efficiency can be expected to be quite high. It was proposed to use a cylinder of solid argon, surrounding it by a thick cylindrical shell of high explosive. If simultaneously detonated from outside, a convergent cylindrical shockwave is launched into the argon. For the high explosive, one may choose hexogen with a detonation velocity of 8 km/s. In a convergent cylindrical shockwave, the temperature rises as r°-4, where r is the distance from axis 16 UNCLASSIFIED / SPOR" OFERCGHE esr one,
UNCLASSIFIED / -2@R-@557GRA=-U6E-ONE- of the cylindrical argon rod. If the shock is launched from a distance of ~1 m onto an argon rod with a radius equal to 10 cm, the temperature reaches 90,000 K, just right to excite the upper laser level of argon. Following its heating to 90,000 K, the argon cylinder radially expands and cools, with the upper laser level frozen into the argon. This is similar to a gas dynamic laser, where the upper laser level is frozen in the gas during its isentropic expansion in a Laval nozzle. To reduce depopulation of the upper laser level during the expansion by superradiance, one may dope to the argon with a saturable absorber, acting as an “antiknock” additive. In this way, megajoule laser pulses can be released within 10 nanoseconds. A laser pulse from a small Q-switched argon ion laser placed in the spacecraft can then launch a phicton avalanche in the argon rod, igniting a DT microexplosion. Figure 5. Argon Ion Laser Igniter, to Ignite a Staged DT —DD Fusion Explosion in a Mini-Teller-Ulam Configuration. A solid argon rod. HE cylindrical shell of high explosive, d detonators. Q Q-switched argon ion laser oscillator. Employing the Teller-Ulam configuration, by replacing the fission explosive with a DT microexplosion, one can then ignite a much larger DD explosion. As an alternative, one may generate a high current linear pinch discharge with a high- explosive-driven magnetic flux compression generator. If the current J is on the order of J= 107A, the laser can ignite a DT thermonuclear detonation wave propagating down the high current discharge channel, which in turn can ignite a much larger pure DD explosion. If the craft is launched from the Earth’s surface, one has to take into account the mass of the air entrained in the fireball. The situation resembles a hot-gas-driven gun, albeit one of rather poor efficiency. There the velocity gained by the craft with N explosions, each setting off the energy £,,is given by v = /2NE,/M, (27) i7 UNCLASSIFIED / £202-06-65G3R=8SPOnter
UNCLASSIFIED / POR" O2?20h=USE-Oi== For E, =5x10"erg, M,=10's, and setting for v= 10 km/s = 10° cm/s the escape velocity from Earth, one finds that AW > 10. Assuming an efficiency of 10 percent, about 100 1-kiloton explosions would therefore be needed. Neutron Entrapment in an Autocatalytic Thermonuclear Detonation Wave — a Means to Increase the Specific Impulse and to Solve the Large Radiator Problem The principal reason why neutrons released by thermonuclear reactions pose such a serious problem is that they cannot be repelled from the spacecraft by a magnetic field. However, choosing a neutron-absorbing target as shown in Figure 3, one can reduce the flux of neutrons hitting the spacecraft. Besides inflicting material damage on the spacecraft, the neutrons release heat that must be removed by a very large radiator. The idea of the autocatalytic thermonuclear detonation wave (Reference 13) presents a solution, which if feasible would very much reduce the magnitude of this problem. For its implementation, it requires very large bremsstrahlung flux densities in the burn zone behind the thermonuclear detonation front. Such large bremsstrahlung flux densities will occur in deuterium detonation burn, at the highest temperature for all the thermonuclear reactions. In an autocatalytic thermonuclear detonation, explained in Figure 6, soft X-rays generated through the burn of the thermonuclear plasma behind the detonation front compress the still unburned thermonuclear fuel ahead of the front. The increase in the fuel density, both in the Teller-Ulam configuration and in the autocatalytic thermonuclear detonation wave, is of crucial importance, with the reaction rate proportional to the square of the density. Figure 6. Autocatalytic Thermonuclear Detonation Using a Soft X-ray Precursor From the Burn Zone BZ to Precompress the Thermonuclear Fuel TF Ahead of the Detonation Front DF. The soft x-rays travel through the gap G between the tamp T and the liner L. 18 UNCLASSIFIED/ /
UNCLASSIFIED / (®@R°@FFtGE-U6E-ONE From the burning plasma behind the detonation front, energy flows into all spatial directions. Part is by bremsstrahlung and part by electronic heat conduction. Roughly half of the energy flows into the liner, one-quarter into the still unburned fuel ahead of the wave, and one-quarter into the opposite direction. The bremsstrahlung emission rate is given by €, =142x10 7" n?VT [erg/cm's] (28) For T = 10? K, one has ¢, = 3.2x 10°73 n@ [erg/cm3s]. The flux of the bremsstrahlung that goes into the liner is ¢,r/2, where r is the radius of the deuterium rod just behind the detonation front. About one-half of this radiation runs ahead of the detonation front, where it precompresses the deuterium. Its intensity is: “m0 nr [erg/cm?s] Ae?) with nr # 3x 1024cm-2 (corresponding pr * 10 g/cm), one has é.F ma x 30n [erg/cm2s] (30) We are aiming at a density where the neutrons are absorbed in the burning plasma cylinder of radius r. If the neutron-deuteron collision cross section is o, then the neutron path length An must be smaller than r: Ha Jey (31) tex or es =e (32) One typically has o + 10°24 cm2, hence nr 210" cm? (33) If r= 0.01 cm, then n > 102 cm3 = 5 x103 no, where mo = 5 x 1024 cmv}, the particle number density of liquid deuterium. With n=107° cm, one finds that é,r/4~3x10"' erg/cm?2s. The flux on a deuterium tube of radius r and length z, where for the burn zone r = z, one obtains onto its surface (¢, /4)2arz = 10" erg/s = 101” watts 19 UNCLASSIFIED / ,bO2- Ober SF ORnTT
UNCLASSIFIED / AB@R-@ERLGLALALSE.DAL ave = 100 petawatts, certainly powerful enough to compress the deuterium to more than thousandfold density. With the entrapment of the neutrons comes an increase of the specific impulse. With 38 percent of the energy going into the kinetic energy of the neutrons and 62 percent into charged fusion products, the specific impulse is increased by the factor ol +38/62 = 10/6.2 =1.275. This increases the maximum exhaust velocity from v=1.5x 10° cm/s to y =1.9x 10° cm/s = 0.063c. In the course of the thermalization in the supercompressed plasma, the neutron absorption cross section is greatly increased, both in the liner and tamp, with the liner also compressed to high densities. If the liner and tamp are made from boron, which has a large neutron-absorption cross section, the spacecraft is heated only by a greatly reduced thermal neutron flux, and only this much smaller amount of heat must be removed by a radiator. Testing the Deuterium Microdetonation Concept For the Orion bomb propulsion concept, testing was a serious problem. If tested on the Earth, it would have resulted in the large fallout of fission products. These tests would have been needed to study the survival of the pusher plate under the repeated exposure of kiloton fission explosions (or fusion-boosted explosions). Of course, the tests could have been carried out in space, but this would have been extremely expensive, because it would have required launch by chemical rockets of the huge Orion spaceship into space. Fortunately, this is not necessary for the deuterium microdetonation propulsion concept because there exists an alternative way to generate a 10’-ampere GeV proton beam: replacing the huge spaceship used as a large capacitor to be charged up to gigavolt potentials with a “Super Marx generator” (Reference 16). This Super Marx generator can achieve on Earth what the huge spaceship can achieve in space: the generation of gigavolt 10’-ampere proton beams. Since the realization of pure deuterium beams would obviously be a breakthrough in fusion, the expenditure for the development of a Super Marx generator would be well justified. Up until now nuclear fusion by inertial confinement has been achieved only using large fission explosives as a means (driver) for ignition. From this experience we know that the ignition is easy with sufficiently large driver energies, difficult to duplicate with lasers or electric pulse power by an ordinary Marx generator. The problem therefore is not the configuration of the thermonuclear explosive but the driver, be it for the ignition of pure deuterium (D) as in the Mike Test or for the ignition of deuterium-tritium (DT) as in the Centurion-Halite experiment, because for sufficiently large driver energies the target configuration is of secondary importance. Substantially larger driver energies can be reached with the “Super Marx generator.” It can be viewed as a two-stage Marx generator, where a bank of ordinary Marx generators assumes the role of a first stage. If the goal is the much more difficult ignition of a pure deuterium microexplosion, the Super Marx generator must in addition deliver a much larger amount of energy (compared with that of the most powerful lasers) and also generate a magnetic field in the thermonuclear target that is strong 20 UNCLASSIFIED / /®@ OPEC SsSronrrT
UNCLASSIFIED / / POfeOFFtGitie=J6G-OalL. enough to entrap the charged DD fusion products within the target. Only then is the condition for a propagating thermonuclear burn fulfilled. Figure 7, Ordinary Marx Generator. In an “ordinary” Marx generator n capacitors C charged up to the voltage v, and aré over.spark gaps switched into series, adding up their voltages to the voltage VY = nv. ‘es sun ae = any’ focebt Super HV gun Fusion Target Charmnber cali Fast Capacitors as } “Sf ft, i tt Coaxial Transmission Lines Su se / Sw SW $u SW : Marx Banks in Oil Tanks Figure 8. Super Marx Generator. In a Super Marx Figure 9. Artist's Conception of a 1.5-km-Long generator, Marx generators charge up NW fast Super Marx Generator. Composed of 100 x 15-meter- capacitors FC to the voltage Y, which switched into long high-voltage capacitors, each designed as a series add up thelr voltages to the voltage AV, magnetically insulated coaxial transmission line. The coaxial capaciters/ transmission lines are plated inside a high-vacuum vessel. Each capacitor/transmission line is charged up by two conventional Marx generators symmetrically to 10 MV (+ 5 MV), After charge-up is completed, the Marx generators are electrically decoupled from the capacitors/transmission lines. The individual capacitors/transmission lines are subsequently connected in series via spark gap switches (that is, the “Super Marx” generator), producing a potential of 1 GV. ~ KY Input 21 UNCLASSIFIED / /®O@ROFFECERE UST ONTrY
UNCLASSIFIED / /P@R"OPPPCER=VSECiet= Figure 7 shows the circuit of an ordinary Marx generator, and Figure 8 that of a Super Marx. An artist’s view of a mile-long Super Marx generator, charged up by about 100 ordinary Marx generators and connected to the chamber in which the thermonuclear target is placed, is shown in Figures 9-11. Coaxial Capacitars Vacuum Vessel tgrounded! Marx Banks Target Chamber Deuterium Target Marx Banks in Oil Tanks with High Yoltage Capacitors Figure 10. Detailed View of a Section ofthe Super Figure 11. Injection of GeV - 10 MA Proton Beam. Marx Generator. Two conventional Marx banks charge Drawn From Super Marx generator made up of up one coaxial capacitor/transmission line element to 10 magnetically insulated coaxial capacitors into chamber MV. with cylindrical deuterium target. As shown in Figure 12, the Super Marx is made up of a chain of co-axial capacitors with a dielectric that has to withstand the potential difference of 10’ volts between the inner and outer conductor, M aes Sas =e. S - Boe >. ane ee es. 1 NA NN AN _. ae a <a sae _ | a at XX KX XK KIX K KKK XK XK Figure 12. Showing a Few Elements of the Super Marx Generator Following their charging up of the Super Marx generator, the Marx generators are disconnected from the Super Marx. If the capacitors of the Super Marx can hold their charge lang enough, this can be done by mechanical switches. 22 UNCLASSIFIED / 4@2.02546041-2065-00ine=
UNCLASSIFIED / 50.2. 055160412 S= Oi To erect the Super Marx, its capacitors C are switched into series by circular spark gap switches S. The capacitors of the Super Marx are magnetically levitated inside an evacuated tunnel and magnetically insulated against the wall of the tunnel by an axial magnetic field B, generated by superconducting external magnetic field coils M. The magnetic insulation criterion requires that 8 > &, where B is measured in gauss and & in electrostatic cgs units. If B=3x10'G, for example, magnetic insulation is possible up to E=3x10'esu = 107 V/cm, at the limit of electron field emission. To withstand a voltage of 10° volts between the outer positively charged surface of the capacitors in series and the tunnel wall then requires a distance somewhat greater than 1 meter. The capacitance of one co-axial capacitor with the inner and outer radius Ro and R: of length / and filled with a dielectric of dielectric constant é is i «= "one R,) (34) Assuming a breakdown strength of the dielectric larger than 3x 104 V/cm and a potential difference of 10’ volts between the inner and outer conductor, the smallest distance of separation d between both conductors has to be d= R,—R, =3x10°cm. If, for example, /=1,6x10°cm, R, =1/2=8x 10°cm, andé £10, one finds that C =2x10'*cm. For these numbers, the energy e stored in the capacitor (V =10’ volts= 3x10" esu) is e=(I/2) CV? = 10" erg (35) which for the 100 capacitors of the Super Marx add up to e~ 10" erg. About 10 times more energy can be stored if the radius of the capacitor is about 3 times larger, if there is a larger dielectric constant, or if a combination of these conditions exists. This means that for about 100 capacitors, energy 101° erg = 1 GJ can be stored in the mile-long Super Marx. Another idea, proposed by Fuelling (Reference 19), is to place the ordinary Marx generators of the first stage inside the coaxial capacitors of the Super Marx. The advantage of this configuration is that it does not require disconnection of the Marx generators from the capacitors of the Super Marx prior to its firing. Because the charging and discharging of the Super Marx can be done very fast, one can use compact water capacitors where¢ = 80. And instead of magnetic insulation of the Capacitors of the Super Marx against the outer wall, one can perhaps use transformer oil for the insulation. Giving each inner segment of the Super Marx enough buoyancy, for example by adding air chambers, these segments can be suspended in the transformer oil. There the outer radius of the co-axial capacitors is much larger. This permits storage of gigajoule energies in the Super Marx. 23 UNCLASSIFIED / Gh@R-OEhbLGiAdeld GEO biiee
UNCLASSIFIED / /-@R-OFPPCREUSPOnt™ As shown in Figure 13, the last capacitor of the Super Marx is a superconducting ring with a large toroidal current. There the large azimuthal magnetic field set up by the toroidal current magnetically insulates the ring against breakdown to the wall. The load is the deuterium target shown in Figure 13. It consists of a solid deuterium rod covered with a thin ablator placed inside a cylindrical hohlraum. To the left of the hohlraum and the deuterium rod is a mini-rocket chamber filled with solid hydrogen. The method of discharging the energy from the Blumlein transmission line to the target then goes as follows (see Figure 13): e A short laser pulse is projected into the mini-rocket chamber through a hole of an electrode at the center of the ring. e By heating the hydrogen in the mini-rocket chamber to a high temperature, a supersonic hydrogen jet is emitted through the Laval nozzle toward the electrode at the center of the ring, forming a bridge to the target. e A second laser pulse then traces out an ionization trail inside the hydrogen jet, facilitating an electric discharge to the target, with the space charge neutralizing plasma pinching the proton beam down to a small diameter. e o a a of © 3 e o @ a Target —— oe Praton Beam ? eheaimaieaade. © Om ey, ey Ma Ce Cosette ee pacahad feaa, See ne stine Ey te neta ey e aoe (b) eto. Ww fe et XXXXxXKXXXXX AXE Figure 13. The Superconducting Teroidal Capaciter (a) and Its Discharge Onto the Target (b) 24 UNCLASSIFIED / /P@R-@FHtGE esr ontr
UNCLASSIFIED / ,5OR.OEELGrAla SiG ia The Super Marx generator therefore can accomplish on Earth what the spacecraft acting as a large capacitor can do in space. The testing of an Argon ion laser driven by high explosives can, of course, be done on Earth, and the same applies to the conjectured superexplosives. Conclusion If large-scale manned spaceflight has any future, a high-specific-impulse, high-thrust propulsion system is needed. The only known propulsion concept with this property is nuclear bomb propulsion. However, since large-yield nuclear explosions are for obvious reasons undesirable, the nuclear explosions should be comparatively small. But because of what Freeman Dyson described as the “tyranny of the critical mass,” small fission bombs or fission-triggered fusion bombs become extravagant, with only a fraction of the nuclear material consumed.! In the original Orion bomb propulsion concept, the propulsive power was through the ablation of a pusher plate. There the energy is delivered to the pusher plate by the black-body radiation of the exploding bomb. The propulsion by non-fission-triggered fusion bombs not only has the advantage that it is not subject to the “tyranny of the critical mass,” but the propulsive power is there delivered by the kinetic energy of the expanding hot plasma fireball repelled from the spacecraft by a magnetic mirror. This is particularly true for a pure deuterium bomb, where, compared with DT, more energy is released into charged fusion products (in a DT bomb, 80 percent of the energy goes into neutrons). Whereas in a fission explosion most of the energy is lost into space by the undirected black-body radiation, much more propulsive energy can be drawn from the plasma of a pure deuterium fusion bomb explosion, in conjunction with a magnetic mirror. Manned space flight requires lifting large masses into Earth orbit, where they are assembled into a large spacecraft. While this can be done with chemical rockets, it would be much more economical if it could be done with a chain of small nuclear explosions. Without radioactive fallout, this can be done with a chain of laser-ignited fusion bombs, with one laser for each bomb, where the lasers become part of the exhaust. Ignition can be done not by infrared chemical or CO2 lasers, as was suggested by the Los Alamos team (Reference 18), but rather by an ultraviolet laser driven by high explosives, as suggested by the author (Reference 9). Looking to the future, using deuterium—widely available on most planets of the solar system and in the Oort cloud outside the solar system—as the nuclear rocket fuel would make manned space flight to the Oort cloud possible, at a distance at about one-tenth of one light year. ' The same Is true for nuclear fission gas core rocket reactors, where much of the unburned fission fuel is lost in the exhaust. 25 UNCLASSIFIED / AP@-@ FECES E-ONEY
UNCLASSIFIED / / ®@R-@F52624.-065-02i2—-=—=0 Appendix: Conjectured Metastable Superexplosives Formed Under High Pressure for Thermonuclear Ignition Under normal pressure, the distance of separation between two atoms in condensed matter is typically on the order of 10°* cm, with the distance between molecules formed by the chemical binding of atoms of the same order of magnitude. As illustrated schematically in Figure 14, the electrons of the outer electron shells of two atoms undergaing a chemical binding form a “bridge” between the reacting atoms. The formation of the bridge is accompanied in a lowering of the electric potential well for the outer-shell electrons of the two reacting atoms, with the electrons feeling the attractive force of both atomic nuclei. Because of the lowering of the potential well, the electrons undergo under the emission of electronvolt (eV) photons a transition into lower energy molecular orbits. At higher pressures, bridges between the next inner shells are formed under the emission of soft X-rays. Going to still higher pressures, a situation can arise as shown in Figure 15, with the building of electron bridges between shells inside shells. i —~\ ({r rey —~©) © ordinary | explosive \ i, eV A; \. / ordinan ao Mb burning ae . a ordinary ‘An & >< Oar e IA AY. pe explosive { \ | \ | | Ly superesplosive Nerays releasen! ©> <(s) by kev ie eva \ an ones heat released by eV photons buming keV photons super- explosive iukils Figure 14. Explosives. In an ordinary explosive, the Figure 15. With Increasing Pressure, Electron outer-shell electrons of the reacting atoms form “eV” Bridges are Formed Between Shells Inside Shells molecules accompanied by the release of heat through Melting into Common Shells eV photons. In a superexplosive, the outer-shell electrons “melt” into a common outer shell with inner electron shells forming “keV” molecules accompanied by the release of X-ray keV photons. There the explosive power would be even larger. Now consider a situation where the condensed state of many closely spaced atoms is put under high pressure making the distance of separation between the atoms much smaller, and where the electrons from the outer shells coalesce into one shell surrounding both nuclei, with the electrons from inner shells forming a bridge. Because there the change in the potential energy is much larger, the change in the electron energy levels is also much larger, potentially on the order of keV. There then a very powerful explosive is formed, releasing its energy ina 26 UNCLASSIFIED / A®@R=@EE5GEA=-U6EOHEYUNCLASSIFIED / 42OR-@F6EGEALUSE-ONETE burst of keV X-rays. This powerful explosive is likely to be very unstable, but it can be produced by the sudden application of a high pressure at just the moment when it is needed. Because an intense burst of X-rays is needed for the ignition of a thermonuclear microexplosion, it could be used as an alternative to the argon ion laser for the ignition of a pure fusion bomb. The energy of an electron in the ground state of a nucleus with the charge Ze is Fi = —13.6 Z? [ev] (36) With the inclusion of all the Z electrons surrounding the nucleus of charge Ze, the energy is Fi* =» -13.6 22-2 [ev] (37) with the outer electrons less strongly bound to the nucleus. Now, assume that two nuclei are so strongly pushed together that they act like one nucleus with the charge 2Ze onto the 2Z electrons surrounding the 2Ze charge. In this case, the energy for the innermost electron is E2 = -13.6 (22)? [ev] (38) Or if the outer electrons are taken into account, Fo"s —13.6 (2Z)2-42 [eV] (39) For the difference, one obtains OF =F" — £2" = 13.62 244 (2242 -1) = 58.5Z2-42 [ev] (40) Using the example Z = 10, which is a neon nucleus, one obtains SOE ~15 keV. Of course, it would require a very high pressure to push two neon atoms that close to each other, but this example shows it is plausible that smaller pressures exerted on heavier nuclei with many more electrons may result in a substantial lowering of the potential well for their electrons. A pressure of p = 100 megabars (Mb) = 1014 dyn/cm? can be reached with existing technology in sufficiently large volumes, with at least three possibilities: e Bombardment of a solid target with an intense relativistic electron or ion beam. e Hypervelocity impact. 27 . UNCLASSIFIED / / F@R@FSGRAL GEOR
UNCLASSIFIED / -PO@R-@FFtGEEUSEONE- e Bombardment of a solid target with beams or by hypervelocity impact, followed by a convergent shock wave. BOMBARDMENT OF A SOLID TARGET WITH AN INTENSE RELATIVISTIC ELECTRON OR ION BEAM This possibility was considered by Kidder (Reference 20), who computes a pressure of 50 Mb, if an iron plate is bombarded with a 1-M] - 10-MeV - 10° A relativistic electron beam, focused down to an area of 0.1 cm?. Accordingly, a 2-MJ beam would produce 100 Mb. Instead of an intense relativistic electron beam, one may use an intense ion beam. It can be produced by the same high-voltage technique, replacing the electron beam diode by a magnetically insulated diode (Reference 21). Using intense ion beams has the additional benefit that the stopping of the ions in a target is determined by a Bragg curve, generating the maximum pressure inside the target, not on its surface. HYPERVELOCITY IMPACT A projectile with the density p * 20 g/cm® accelerated to a velocity v = 30 km/s would, upon impact, produce a pressure of p ~ 100 Mb. The acceleration of the projectile to these velocities can be done by a magnetic traveling wave accelerator. BOMBARDMENT OF A SOLID TARGET WITH BEAMS OR BY HYPERVELOCITY IMPACT, FOLLOWED BY A CONVERGENT SHOCK WAVE If, upon impact of either a particle beam or a projectile, the pressure is less than 100 Mb (for example, only on the order of 10 Mb) but is acting over a larger area, a tenfold increase in the pressure over a smaller area is possible by launching a convergent shock wave from the larger area on the surface of the target onto a smaller area inside. According to Guderley, the rise in pressure in a convergent spherical shock wave goes as r ~°-9, which means 100 Mb could be reached by a tenfold reduction in the radius of the convergent shock wave. While it is difficult to reach 30 km/s with a traveling magnetic wave accelerator, it is easy to reach a velocity of 10 km/s with a two-stage light gas gun. We assume an equation of state of the form p/p, =(n/n,)”. For a pressure of 100 Mb = 1014 dyn/cm?, we may set y= 3 and p,= 101! dyn/cm?, p, being the Fermi pressure of a solid at the atomic number density #,, with being the atomic number density at the elevated pressure p> p,. With d = n-/3, where d is the lattice constant, one has d/d, =(p/p.)"”" (41) Such a lowering of the inneratomic distance is sufficient for the formation of molecular states. 28 UNCLASSIFIED / #2@R@EEDGHiHUGE-ONEY
UNCLASSIFIED / SA RnDEELGiAHSE- ONE Calculations done by Muller, Rafelski, and Greiner (Reference 22) show that for molecular states 35Br- 35Br, s3l- 7oAu, and 92U- 92U, a twofold lowering of the distance of separation leads to a lowering of the electron orbit energy eigenvalues by ~ 0.35 keV and 1.4 keV, respectively. At a pressure of 100 Mb = 1014 dyn/cm? where d/do = 1/2, the result of these calculations can be summarized by (6E in keV) fog OE = 1.3 x10*%Z-1.4 (42) replacing equation (40), where Z is here the sum of the nuclear charge for both components of the molecule formed under the high pressure. The effect the pressure has on the change p in these quasi-molecular configurations is illustrated in Figure 16, showing a p - d (pressure-lattice distance) diagram. This diagram illustrates how the molecular state is reached during the compression along the adiabat a at the distance d = d; where the pressure attains the critical value p = pc. IN passing over this pressure, the electrons fall into the potential well of the two-center molecule, releasing their potential energy as a burst of X-rays. Following its decompression, the molecule disintegrates along the lower adiabat b. Figure 16. p-d, Pressure. Inneratomic distance diagram for the upper atomic and lower molecular If the conjectured superexplosive consists SAIGBAt. | of just one element, as in the case of the 35Br - asBr reaction or the 92U - 92U reaction, no special preparation for the superexplosive is needed. But as the example of Al-FeO thermite reaction shows, reactions with different atoms can release a much larger amount of energy compared with other chemical reactions. For the conjectured superexplosives, this means they have to be prepared as homogeneous mixtures of nano-particle powders, bringing the reacting atoms as close together as possible. For the ignition of a thermonuclear reaction, one may consider the following scenario illustrated in Figure 17. A convergent shock wave launched at the radius R = Ro into a spherical shell of outer and inner radius Ro, Ri reaches near the radius R = Ri ata pressure of 106 Mb. After the inward-moving convergent shock wave has reached the radius R = Ri, an outward-moving rarefaction wave is launched from the same radius R = Ri, from which an intense burst of X-rays is emitted. One can then place a thermonuclear DT target inside the cavity of the radius R = Rz, with the target bombarded, imploded, and ignited by the X-ray pulse. The ignited DT can there serve as a “hot spot” for the ignition of deuterium. 29 | UNCLASSIFIED / /#@R 6PFPtGH"SE-One
UNCLASSIFIED/ AN by o SS 8 S ies CS SS Aa a SENS . ay NN O *. sy MA e AOA, Pi ote Ssen cate Figure 17. Inertial Confinement Fast-Ignition Configuration References [1] F. Winterberg, Phys. Rev. 174, 212 (1968). [2] F. Winterberg, Raumfahrtforschung 15, 208-217 (1971). [3] Project Daedalus, A. Bond, A.R.Martin et al., J. British Interplanetary Society, Supplement, 1978. [4] R. Lewis, K. Meyer, G. Smith, S. Howe, http://www.engr.psu.edu/antimatter/papers/AIMStar_99.pdf. [5] G. Dyson, Project Orion, The True story of The Atomic Spaceship, Henry and Holt Company, New York, 2002. [6] H. Oberth, Die Rakete zu den Planetenraumen, R. Oldenbourg, Berlin 1923. [7] K. Clusius and K. Starke, Z. Naturforsch. 4a, 549 (1949). [8] F. Winterberg, J. Fusion Energy 2, 377 (1982). 30 UNCLASSIFIED / /®@?e OFC esr contr”
UNCLASSIFIED / -42@R-OEEEGR Rie Sein [9] F. Winterberg, "Can a Laser Beam ignite a Hydrogen Bomb?”, United States Atomic Energy Commission, classified January 27, 1970, declassified, July 11, 2007, S-RD-1 (NP — 18252). [10] F. Winterberg, J. Fusion Energy, DOI 10.1007/s10894-008-9143-4. [11] Y.K. Bae, Y.Y Chu, L. Friedman Phys. Rev. 54, R1742 (1995). [12] G.S. Janes, R.H. Levy, H.A. Bethe and B.T. Feld, Phys. Rev. 145, 925 (1966). [13] F. Winterberg, Atomkernenergie, 39, 265 (1981). [14] 0. Buneman, Phys. Rev. 115, 503 (1959). [15] L. Davis, R. List and A. Schliiter Z. Naturforsch. 13a, 916 (1958). [16] F. Winterberg, J. Fusion Energy, DOI 10.1007/s10894-008-9189-3. [17] F. Winterberg, Laser and Particle Beams, 26, 127 (2008). [18] 1.D. Balcomb et al. “Nuclear Pulse Space Propulsion System,” Los Alamos scientific Laboratory, classified November 1970, declassified July 10, 1979, LA - 4541 - MS. [19] S. Fuelling, private communication. [20] R. Kidder in the Proceedings “Physics of High Energy Density”, Academic Press, New York 1971. [21] F. Winterberg, in the same Proceeding p. 398. [22] B. Muller, J. Rafelski, W. Greiner, Phys. Lett. 47B(1), 5(1973). 31 UNCLASSIFIED / / P@"@FFtCGHL-UGE-ON