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/ ,'F811. 8FFll!l*L 1!1!11! t!IIU:!Y
According to Newtonian mechanics and Planck's conjecture, the interaction of a positive
with a negative Planck-mass particle leads to a velocity fluctuation ~ a,,t,, = c with a
displacement of the particle equal to t5=(1/2)a/~ =r1,l2, where aP=~,/mP .
Therefore, a Planck-mass particle immersed in the Planck aether makes a stochastic
quivering motion (Zitterbewegung) with the velocity
( 46)
where n = 1/ r,~ is the average number density of positive or negative Planck mass
particles. The kinetic energy of this diffusion process is given by
( 47)
Putting
(48)
where S is the Hamilton action function and v is the velocity of the Planck aether, the
Lagrange density for the Planck aether is
L=n he: +--(vs")+U+-- _11_ .
[
"S h' h' (\7 )']
ct 2m1, 8m1, n (49)
Variation of (49) with regard to 5 according to
(50)
leads to
On h ,
-+-\7(n\7S)~O
Gt m,, (51)
16
UNCLASSIFIED//FQA: arrI&I.«11! 1!181! ·••1:v

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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.