AAWSAP DIRD, Negative Mass Propulsion, January 2011

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3. Hund's Nonlinear Newtonian Theory of Gravity
As explained by Hund [3], already Newton's theory of gravity, in conjunction with the
postulates of special relativity, leads to a nonlinear theory of gravity. With this model
theory of gravity the nonlinearity of the gravitational field can be much better explained
than with Einstein's theory.
Hund begins with the force F acting on a mass m in a "merry-go-round":
mv
F=mg +-x G .
(11)
C
If g is the gravitational acceleration by real masses with the density p, one has in
Newton's theory
divg =--4.nyp .
(12)
In the merry-go-round g has a vertical component from the earth's gravitational field,
but also a radial component by the radial centrifugal acceleration which is not source­
free. With lgl = alr, where m= 2TC/T, with T the time of revolution, and r the radial
distance from the center of the merry-go-round, one has
divg =2m2 .
(13)
Comparing (13) with (12) one sees that the centrifugal force corresponds to a
gravitational repulsion of a homogeneous mass density
(14)
For a typical "merry-go-round" one has T = 10 sec, and hence, w =0.6s-1 • For this
example one obtains from (14), µ = -106 glcm3 , taken as an absolute value about
equal to the mass density of a white dwarf.
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