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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…
UNCLASSIFIED/ ,'P81il 8PPl!ltltt ".JI! Gilt I
' [ ,e 1·]W =v,exp he ' (82)
leaving invariant the probability density lf/*f//.
To give gauge invariance a hydrodynamic interpretation, we compare (81) with the
force acting on a test body of mass m placed into the moving Planck aether. This force
follows Euler's equation and is
d
[ ' ( 'J ]V CV v-
F = m- = m -+grad - -vxcurlv.
dt Gt C
Complete analogy between (81) and (83) is established if one sets
m •
=--v·
2e
According to (78) and (82), <ti and A shift the phase of a Schrbdinger wave by
e f ,.OlfJ = - <Pdt
h ,,
oq,~--'--pA• ds.,,
(83)
(84)
(85)
The corresponding expressions for a gravitational field can be directly obtained from the
equivalence principle [3]. If 8v/8t is the acceleration and w the angular velocity of the
universe relative to a reference system assumed to be a rest, the inertial forces in this
system are
F =m[: +<&xr-wx(wxr)-&<2wl (86)
For ( 86) we write
24
UNCLASSIFIED/ /f81il 8ffl@Itlll::: 1!181! &••1:::Y

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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.