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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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/ ,'Flilll. lilFFllil_.,le lal!il!! 8111!¥
or
(52)
which is the continuity equation of the Planck aether. Variation with regard to n
according to
( aL)- a ( aL )=oen ar an/er (53)
leads to
as h' ( ') h' [l(V")' V'n]h-+U+-- vs-+-- - - -- =0
(}[ 2ml' 4m1, 2 n n (54)
or
as h" (Ds') h" v' ✓n 0h-+U+-- V +-----=
8t 2m1, 2m1, Fn • (55)
With the Madelung transformation
1/f = Fne1s, lj/• = Fne-,s, (56)
one obtains from (51) and (55) the Schr6dinger equation
(57)
In the Planck aether hypothesis all particles, save and except the Planck mass particles,
are quasi-particles of the Planck aether, like the phonons, rotons, excitons, etc., of
condensed matter physics, and by the wave structure of the Planck aether are Lorentz
invariant. In forming quantized vortices, the Planck aether also has vortex waves,
simulating Maxwell's and Einstein's electromagnetic and gravitational waves. Dirac
spinors are made possible by the negative masses of the Planck aether.
17
UNCLASSIFIED/ ,'F81l 81'1'1@1,_le tl!9E CIIE I

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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.