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=2997924582∗ln(cosh(π))2π
G=3.504958e16
To account for entanglement, we divide by the Durian constant.
G=2997924582∗ln(cosh(π))2π∗9.029022e26
G=3.88188e−11
which is just a coincident.
Compare this with the quoted value of G=6.67259e(−11), we missed by a factor of √3.
G∗√3=6.7236e−11
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.