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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/ ,'P81l 81'1'11!111it 1!1!11!! 811LY
The time needed for the liquid metal to pass through a ~ 20 m thick layer is then ~ 2 x
103 seconds~ 1 hour. The specific heat per unit volume of the coolant is pc, ~ 3 x 107
erg/cm 3K, and for T = 3 x 103 Kone has pcJ ~ 10 11 erg/cm 3 .
The heat per unit volume which has to be removed from the crushed rocks is of the
order p, where p is the rock pressure. In the center of the moon where p = 5 x 1010
dyn/cm 2 , this energy is 5 x 10 10 erg/cm 3 . It thus follows that the volume of the liquid
coolant must be about 1/2 of the rock volume to be cooled. For a rock volume of (20
cm) 3 ~ 104 m 3 , a coolant volume of about 5 x 10 3 cm 3 would be needed. The same
coolant can be used many times over after the heat is removed from it, which could be
done on the surface of the moon by radiation or perhaps better by heat exchangers
transferring the heat to lunar sand. Without a thick layer of shattered rocks surrounding
the tunnel, the pressure acting on the tunnel wall would be large, in particular in the
center of the moon. Because of friction between particles of the shattered rock, large
shear stresses can be sustained changing the pressure distribution in the rock and
reducing the pressure gradient and hence the pressure on the tunnel wall.
A more detailed calculation [15] for the pressure distribution in the shattered rock
tunnel wall gives
(113)
where ro is the radius of the tunnel.
Integrating eqn (108) one obtains for the pressure distribution in the moon
(114)
for which one can also write
p(r) ~ P,,,,, (,-(; )'J. (115)
35
UNCLASSIFIED/ ,'1'81l 81'1'11!111it 1!1!11!! 811LY

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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.