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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. 7 …sign, the total energy and momentum of the combined system remains zero for all times, leaving…
  • p. 8 …of special relativity, being the expression of a Minkowskian space-time structure, there is an older…
  • p. 10 …With lxl = (1/r, where OJ= 2tr/T, with T the time of revolution, and r…
  • p. 11 …time before their fields propagating with the velocity of light would reach the earth. Adding the…
  • p. 16 …Even though its time-averaged velocity is always less than the velocity of light, this means…
  • p. 18 …0~ m· =12r ~6X1Q-13g, ( 45) larger by a factor 3.6x10 11 times the mass…
  • p. 22 …by saying that the zero-point vacuum energy "generates" the Minkowski space-time. 7. Dynamic Interpretation…
  • p. 23 …the rod is /, and if the rod rests in the distinguished reference system, the time needed…
  • p. 24 …c -v Slll-1// -VCOSlf/ (67) with the time t' for a to and fro signal…
  • p. 25 …If tR is the absolute reflection time of the light signal at clock B, one has…
  • p. 26 …using a rod to measure the distance and the time it takes a light signal in…
  • p. 34 …The time needed to bring back the universe to its original low entropy state, is the…
  • p. 37 …times more dense than water 16. Suppose that in the center of the moon the accumulation…
  • p. 38 …the heat diffusion equation given by (109) where Xis the heat diffusion coefficient, the diffusion time…
  • p. 39 UNCLASSIFIED/ ,'P81l 81'1'11!111it 1!1!11!! 811LY The time needed for the liquid…
  • p. 42 …This means that a small, continuous removal of the heat through the injection and circulation of…
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To make a tunnel, a cylindrical, rather than spherical, volume of crushed rocks is
desired. For this reason a thermonuclear shape charge or an explosive lens is better
suited to shatter the rocks.
In the center of the moon the temperature is several thousand degrees centigrade.
With the heat diffusion equation given by
(109)
where Xis the heat diffusion coefficient, the diffusion time for a layer of thickness xis
(110)
For lunar rocks one has x~4x10-3cm2/s. Taking the example x;:::2Qm;:::2x103cm,
one finds that r=l0 9 s~30yr, and at the high rock temperatures the heat diffusion
time would be uncomfortably long.
The situation is drastically changed for a layer of crushed rocks, because there it is
possible to remove heat by a coolant pumped through the porous medium of the
crushed rocks. At the high temperatures of several thousand degrees centigrade, a
liquid alkali metal, for example lithium, abundantly available on the moon, could be
used as a coolant. The velocity the coolant diffuses into the crushed rocks is determined
by Darcy's law
v~-Dgradp, (111)
where p is the pressure, D = Kj pg, with K ~ 1 cm/s a typical value. If the pressure
gradient is provided by the gravitational force one has gradp = pg and hence
lvl ~ IC~ 1 cm/s. (112)
34
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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.