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Wednesday, June 15, 2016

Gravitational Constant At Last!

From the post "Pound To Rescue Permittivity" dated 30 May 2016,

q=m.4πa2ψ=dqdr|r=aψ

This points to surface property, that the behavior of q, dqdr at the surface boundary r=aψ determines the field extended by the particle.  But it leads to high values for gravity and the gravitational constant, when the particles are large gravity particles (because there was a mistake).

If we reformulate more clearly,

M=m.4πa2ψ=dMdr|r=aψ

Because,

FG14πa2ψ=GMa2ψ=2mc2.ln(cosh(π))

We note that GM takes the place of q4πεo.  We have

GMa2ψ=2mc2.ln(cosh(π))

Gm.4πa2ψa2ψ=2mc2.ln(cosh(π))

G=c2ln(cosh(π))2π

G=2997924582ln(cosh(π))2π

G=3.504958e16

To account for entanglement, we divide by the Durian constant.

G=2997924582ln(cosh(π))2π9.029022e26

G=3.88188e11

which is just a coincident.

Compare this with the quoted value of G=6.67259e(11), we missed by a factor of 3.

G3=6.7236e11

What happened?  It could be,


where one dimensional space along r is elevated to three dimensional space.  A particle in one dimension is now a body with extends in two other dimensions.  The body "feels" the force in these additional two dimensions and the result is a factor of 3 ( used to be called Boltzmann).

Good night.