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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. 3 UNCLASSIFIED/ /F8A 8FFIGl1l1k WI>& Qtlk':C Contents 1. Introduction ................................................................................................. 2 2. The Theory by Bondi ...................................................................................... 4…
  • p. 9 …partial differential equations ( K = 8;r y / c 4 ) given by ' 'o 2, 1 ,_,,-, 2 2…
  • p. 10 …merry-go-round": mv F=mg+-xG. C (11) If g is the gravitational acceleration by…
  • p. 12 UNCLASSIFIED/ /F81il 8fFllil.t.k WE&i Si'llk>C In one further step one should…
  • p. 17 …velocity of circular motion with f',.(J} ➔ c): + = m r;.rm =m+rc ( 41) Comparing (40…
  • p. 18 …Newton's constant, h Planck's constant, c the velocity of light): 14 UNCLASSIFIED//r;Oll…
  • p. 19 …But since & = r1, and because ml'rl'c = h, one obtains Heisenberg's uncertainty relation .6…
  • p. 20 …leads to a velocity fluctuation ~ a,,t,, = c with a displacement of the particle equal to…
  • p. 23 …l!IP'P'll!lllile lal!i! i;n11e~r transforming (59) into c-~1-' v…
  • p. 24 …and fro directions given by ✓ 2 2 • 'c_ =c -v Slll-1// -VCOSlf/ (67) with the…
  • p. 25 …y(1R-1'.,)=d/c y(t,;-tR)=d/c (70) where dis the distance between…
  • p. 26 …The impossibility is expressed in the Lorentz transformations themselves, containing the scalar c 2 rather than…
  • p. 27 …C Of C (79) (80) (81) By making a gauge transformation of the Hamilton operator in…
  • p. 28 …dt Gt C Complete analogy between (81) and (83) is established if one sets m • =--v…
  • p. 29 …1,1lii s,11.~r where A av E = -+ c&xr-w x(wxr) a, -H…
  • p. 30 …the Lorentz gauge) 4 il , --+divA =0 C Ct With the gauge transformation for ct> and…
  • p. 31 …v · ds c- . ~ 2 2;rv b(f) = 20Jrrr -,- c the same as predicted by quantum…
  • p. 32 …For H = 104 G, this would mean that vmax 2 c for R > 0.3 cm…
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.