AAWSAP DIRD, Negative Mass Propulsion, January 2011

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In one further step one should have
divF-~(F 2 + G2) = -4,ryp
(20)
2c
or if G =0 and F =-'v¢, where ¢ is the Newtonian gravitational potential, one obtains
for Poisson's equation:
(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
(23)
transforms (22) into
y7 2
- 4;ryp
1//-
2
1/f .
(24)
C
If pis a delta function at r = 0, where
m = f4;rrr\5(r)pdr,
(25)
then one obtains from (24):
(26)
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