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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.
“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/ ff81il 8ffll1Ak Wfili IH.k\f
or
(93)
'
A =-cv
Apart from the factor m/e, this is same as (84).
For weak gravitational fields produced by slowly moving matter, Einstein's linearized
gravitational field equations permit the gauge condition (replacing the Lorentz gauge)
4 il ,
--+divA =0
C Ct
With the gauge transformation for ct> and A
~ ---y • ds
"' A
26
UNCLASSIFIED/ /1"91t 91"1"1!111it 1!191!! 9HLY
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About this file
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.