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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/ ,'1"81l 81"1"!!!11it tl!!E 811E I
t = 21/c0 • (64)
If prior to being set into motion the rod is inclined against the x-axis by the angle cp, it
appears to be inclined against the x-axis by the different angle 'f after set into motion,
with \If expressed through cp by
tan vi = r tan q,, (65)
(
, ')-112
r = I - v· I c· .
The absolute motion then contracts the rod from ! to (:
(66)
Relative to the moving rod the velocity of light is anisotropic, and for the to and fro
directions given by
✓ 2 2 • 'c_ =c -v Slll-1// -VCOSlf/
(67)
with the time t' for a to and fro signal given by
(68)
Therefore, as seen from an observer at rest in the distinguished reference system the
clock goes slower by the factor r = 1/,/1- v2 I c 2 , independent of the inclination of the
rod making up the clock. With solid bodies held together by electromagnetic forces,
clocks made from solid matter should behave like light clocks. As it was claimed by
Poincare, it should for this reason be possible to obtain the Lorentz transformations
solely from the contraction effect with a proper convention about the synchronization of
clocks.
According to Einstein, two clocks, A and B, are synchronized if
20
UNCLASSIFIED/ /P&tl err1e1111t ~:!I! 8HLY

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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.