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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.

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“Ç.”18 pages

  • 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 8FFI1il.t.k Wfili &,.kY
8. Negative Mass Interpretation of the Aharonov-Bohm
Effect [11]
In Maxwell's equations the electric and magnetic fields can be expressed through a
scalar potential and a vector potential A:
1 OA
E=---,--irad and A the Lorentz gauge condition,
1 i)(J)
--+divA=O
C C't
the gauge function must satisfy the wave equation
In an electromagnetic field the force on a charge e is
[ 1 oA 1 ]=e ---,--gradcD+-vxcurlA.
C Of C
(79)
(80)
(81)
By making a gauge transformation of the Hamilton operator in the SchrOdinger wave
equation, the wave function transforms as
23
UNCLASSIFIED/ ,'f81l 81'1'181*1. lal!ii e,11,~1

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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.