AAWSAP DIRD, Negative Mass Propulsion, January 2011

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UNCLASSIFIED//fOR. 8FFI61.t..k W&i QJsll,¥
(82)
leaving invariant the probability density If* lj/ .
To give gauge invariance a hydrodynamic interpretation, we compare (81) with the
force acting on a test body of mass m placed into the moving Planck aether. This force
follows Euler's equation and is
dv
[av
(v2)
]
F=m-=m -+grad -
- vxcurlv
(83)
dt
8t
c
•
Complete analogy between (81) and (83) is established if one sets
(84)
me
A :::: --v
e
According to (78) and (82), <I> and A shift the phase of a Schrodinger wave by
liq, = _ !!_ . A
ds .
(85)
C
The corresponding expressions for a gravitational field can be directly obtained from the
equivalence principle [3]. If 8v/8t is the acceleration and w the angular velocity of the
universe relative to a reference system assumed to be a rest, the inertial forces in this
system are
(86)
F::::m[: +c&xr-rox(roxr)-&<2rol
For (86) we write
UNCLASSIFIED//POlt orr1e11tt tt!II!! or~LY
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