AAWSAP DIRD, Negative Mass Propulsion, January 2011

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UNCLASSIFIED/ /P'OR. 8FFIEil1'1.k lellii Ql'II.¥
or </J =-,
my
r
the same as in Newton's theory.
For a sphere of constant density p one obtains the solution
If/ = sinh kr k2 = 4,ryp
kr
'
c2
Hence,
<P = c2 ln [ sin:, kr] _
For small values of r one has
with the force per unit mass
lgl= -IV </JI= (41r/3) ypr,
as in Newton's theory.
In general one has
(27)
(28)
(29)
(30)
(31)
(32)
which in the limit r -
oo becomes a constant:
(33)
which implies the self-shielding of a large mass by the negative mass of its own
gravitational field surrounding the mass. The shielding becomes important at the
distance
UNCLASSIFIED/fFOA OFFI&il.t.k lellii OJi,k¥
9