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Defense Intelligence Reference Document Advanced Nuclear Propulsion For Manned Deep Space Missions

Defense Intelligence Agency · 37 pages · text from the file's own layer

This Defense Intelligence Reference Document from the Defense Intelligence Agency, dated 11 March 2010, was produced under the Advanced Aerospace Weapon System Applications (AAWSA) Program. It argues that spaceships powered by deuterium thermonuclear reactions could be built with current science and technology. The paper covers ignition by GeV proton beams, magnetic insulation, the Super Marx generator and conjectured chemical superexplosives, and it concludes that such craft could make manned exploration of the entire solar system possible.

  • p. 6 …He remains convinced that small, clean bombs could propel Orion - but he still fears more than…
  • p. 8 …The comparatively small amount of energy needed for the separation can ideally be drawn from a…
  • p. 9 …laser level can then be removed from the rod by a small Q-switched laser, the…
  • p. 10 …For the newly formed electron cloud to be stable, its maximum electron number density must be…
  • p. 13 …for a small DT sphere. A configuration of this kind can still be used to burn…
  • p. 14 …The energy required would be about 10 4 times larger, or about 104 MJ-for all…
  • p. 16 …There the thrust and specific impulse are comparatively huge, but a comparatively small explosive yield is…
  • p. 17 …This problem can be overcome through the nonfission ignition of small fusion explosions. A first step…
  • p. 19 …There the driver energy, but not the driver, may be rather small. A direct way requires…
  • p. 20 …Therefore, the yield of the deuterium fusion explosions can be made much smaller, eliminating the need…
  • p. 22 …A small high-voltage generator driven by a small onboard fission reactor can make the initial…
  • p. 23 …pulses can be released within 10 nanoseconds. A laser pulse from a small Q-switched argon…
  • p. 31 …would be much more economical if it could be done with a chain of small nuclear…
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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 -10 7-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 -
107-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 (MH proton mass)
(19)
For n1,-='= 2x J010 cm- 3 , one obtains p1 :::: 3x 101.1 dyn/cm 3 . For the electron return current,
one has (m electron mass)
(20)
With the return current condition nJ:i\, = np'1 , where for GeV protons i\ :::: c, one has
v,./c=n,/n,, (21)
Taking the value n" =5xl0 22 cm- 3 , valid for uncompressed solid deuterium, one obtains
v,. :::: 104 cm/sand hence Pe :::: 5 x 103 dyn/cm 2 . This is negligible against p1, 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
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Report, from the dia collection. The PDF is mirrored here; the original link is under it. 37 pages are in the text index: search them above, or from the library's search.