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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/ /F81il 8fFllil.t.k WE&i Si'llk>C
In one further step one should have
(20)
or if G =0 and F=-V¢, where¢ is the Newtonian gravitational potential, one obtains
for Poisson's equation:
' 1 2
v-¢ = 4n:yp- - 2 (V ¢) .
2c (21)
According to (21) the positive mass as the source of the Newtonian potential is reduced
by the negative mass of its field. (Einstein's theory leads to almost the same, except
that there the negative gravitational mass density is twice as large.) One can then write
(22)
The earth is therefore embedded in a sea of negative mass. Making the substitution
transforms (22) into
If pis a delta function at r = 0, where
m =f4ffr 2o(r)pdr,
then one obtains from (24):
d ( , dlf/ J- mrlf/- r - ---
dr Jr c-,_
8
UNCLASSIFIED//P9Pl err1e1At 652 one,
(23)
(24)
(25)
(26)

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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.