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Defense Intelligence Reference Document Negative Mass Propulsion

Defense Intelligence Agency · 43 pages · text from the file's own layer

This Defense Intelligence Reference Document from the Defense Intelligence Agency is dated 3 January 2011. It was produced under the Advanced Aerospace Weapon System Applications (AAWSA) Program as part of a series of advanced technology reports. The report asks whether negative mass exists and whether it could be used for propulsion. It concludes that one route might be an ultra-light form of matter that could have gathered at the Moon's center. Reaching it would take a tunnel dug with thermonuclear shape charges.

  • p. 1 …Wliii 8111.'f Defense Intelligence Reference Document Defense Futures Negative Mass Propulsion UNCLASSIFIED/ /FOIi. QFFiliil,jl…
  • p. 2 …8FFHil.t.k Wfili 8HkY Negative Mass Propulsion The Defense Intelligence Reference Document provides non-substantive…
  • p. 3 …Negative Mass Interpretation of the Aharonov-Bohm Effect ................................ 23 9. Negative Masses in Cosmology ....................................................................... 29 10…
  • p. 5 UNCLASSIFIED//FOR QFFISil.ltk W!ilE 8HLY Negative Mass Propulsion Summary It is easy to prove…
  • p. 6 …A somewhat different situation arises if both masses, the field producing mass and the mass of…
  • p. 7 …With both forming a mass dipole, the system becomes self-accelerating, because one mass is repelled…
  • p. 8 …The Theory of Bondi The first attempt to introduce negative masses into general relativity to describe…
  • p. 9 …Making this assumption, Bondi can reproduce the uniform acceleration of the mass dipole, as it is…
  • p. 10 …Hund begins with the force F acting on a mass m in a "merry-go-round…
  • p. 11 UNCLASSIFIED/ ,'P81l 8PPll!lllit tl!II!! t!IHLY The mass density (14) is not fictitious but…
  • p. 12 …2c (21) According to (21) the positive mass as the source of the Newtonian potential is…
  • p. 13 …large mass by the negative mass of its own gravitational field surrounding the mass. The shielding…
  • p. 14 …The negative gravitational mass of the universe there shields its positive mass. 4. The Theory of…
  • p. 15 …Since the overall mass of the electron is positive, the occurrence of negative masses in the…
  • p. 16 …s constant and m as the electron mass h 2mc' (37) whereby the circular motion around…
  • p. 17 …If the positive and negative masses are m+, m-, with m+ -lm.-1 << m+ _ and with…
  • p. 18 …We therefore see that there are huge amounts of negative masses bound to positive masses in…
  • p. 19 …While Newton's action-reaction remains valid for the interaction of equal Planck mass particles, it…
  • p. 20 …Therefore, a Planck-mass particle immersed in the Planck aether makes a stochastic quivering motion (Zitterbewegung…
  • p. 21 …Dirac spinors are made possible by the negative masses of the Planck aether. 17 UNCLASSIFIED/ ,'F81l…
  • p. 27 …Negative Mass Interpretation of the Aharonov-Bohm Effect 11 In Maxwell's equations the electric and…
  • p. 28 …force acting on a test body of mass m placed into the moving Planck aether. This…
  • p. 33 …The Planck aether consists of two superfluid components, one composed of positive Planck masses and the…
  • p. 34 …This is certainly true if the negative mass is equal to the negative mass of the…
  • p. 35 …Finally, with the negative entropy of the negative Planck masses playing the role of a kind…
  • p. 37 …This would not lead to a negative-positive mass self-chasing mass dipole as envisioned by…
  • p. 42 …Conclusion The purpose of this study is the question as to whether negative mass might exist…
  • p. 43 …Holmlid, International Journal of Mass Spectroscopy 282, 70 (2009). 17. F. Winterberg, 40 th Congress of…
UNCLASSIFIED/)'P9R: 9PPll!ltllt W!ilE 1n•tY
make a critical assembly) released. For a 10 kiloton fission explosion the shatter radius
computed from (110) is ~ 20 m. With a tunnel radius ro ~ 10 m one would have
(rj1;,)- 2and from (118) that
(121)
Putting for the depth of the tunnel (if measured from the surface of the moon)
8 = R- r, with
(122)
or that 5eal0km.
For a depth < 10 km the nuclear explosion with a yield < 10 kiloton would suffice, a
yield which is uneconomical. It is for this reason suggested that one uses altogether
thermonuclear explosive devices where the cost per yield is much lower. To penetrate
and shatter the rocks more efficiently, jet-generating thermonuclear explosive lenses
could be used. The thermonuclear detonation wave ignited at one point is there shaped
into a jet-producing conical explosion by placing obstacles in the path of the wave. The
ignition can be done by a fission explosive, but conceivably also by a powerful laser
beam, with the laser beam projected down the tunnel shaft, triggering the
thermonuclear explosive positioned at the lower end.
With the above-given estimate of ~ 50 Megaton needed to dig the tunnel shaft, the
number of thermonuclear explosive devices making use of the detonation wave lens
technique could for this reason be quite reasonable, and certainly much less than the
number of required fission explosives.
After nuclear explosions have crushed the rocks and the heat is removed, the tunnel
wall has to be made from some kind of ceramic material, since water with which to
make concrete is only sparsely available on the moon. But for the wall to last, its
temperature must be kept low. The low heat conductivity of rocks, requiring little
cooling, is there of considerable help. For the crushed rocks the heat conduction
coefficient should not be very different than for solid rocks. According to eqn (112) the
37
UNCLASSIFIED/ ;CFQA: QFFI&I.«1L W!ilE 8HLI/

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Report, from the dia collection. The PDF is mirrored here; the original link is under it. 43 pages are in the text index: search them above, or from the library's search.