Defense Intelligence Reference Document Negative Mass Propulsion

x'=x-vt,
.v' = y,
z' = Z,
t' = t
UNCLASSIFIED/,.,,., ... l!IP'P'll!lllile lal!i! i;n11e~r
transforming (59) into
c-~1-' v o ~1-'
1 v u ~1-' u ~1-' u ~1-'
4 '( , ')I ,,~, 2 ,,~, ( 2 J "'~' "'~' "'~'
----+---+ -- --+--+--=- 7r.p r I, a ,2 2 ,:,. ,,:,. , 2 a ,2 ;'.),. ,2 ,, ,2 , •
c it c oxot c ·X uy oz
(61)
(62)
After the body has settled into a new equilibrium in which 0/0t' =0, one has instead of
(60)
(
v 2
J a2
'= <1) and di:1 = dx✓ I -v 2 / c 2 . This implies a uniform contraction of the body by
the factor ,Jt -v 2 / c 2 because the sources a re contracted by the factor J1 -v 2 / c 2 as
well, whereby the right-hand side of (63) becomes equal to the right-hand side of (60).
Since the zero-point energy is invariant under a Lorentz transformation, the quantum
potential changes in the same way as © . The body therefore sustains its static
equilibrium under a contraction by the factor .jI-v2/c 2 if set into absolute motion,
explaining the Lorentz contraction dynamically.
The clock retardation effect can be derived from the contraction effect, and from there
the Lorentz transformation. Following Builder [9] this original interpretation of Lorentz
invariance by Lorentz and Poincare has been worked out in every detail by Prokhovnik
[10]. To derive the clock retardation effect from the contraction effect one considers a
light clock, which is a rod with mirrors attached to its two ends in between which a light
signal is sent forth and back. If the length of the rod is /, and if the rod rests in the
distinguished reference system, the time needed for the light signal to be sent forth and
back is
19
UNCLASSIFIED/ ,"FUR bi FIEitltt ~!H! 8HLY