We would now formulate an expression for the repulsion between hot particles. The simplest of which is to consider conservation of flux, as Gauss did
\(F_T=\cfrac{T_aT_b}{4\pi\tau_or^2}\)
where \(F_T\) is the repulsive thermal force between hot particles, \(\tau\) is a measure of the resistance in establishing a thermal gradient between the two particles, and \(r\) the distance between the hot particles and, \(T_a\) and \(T_b\) are temperature on particle \(a\) and \(b\).
Not bad for a first guess.
And so, for the post "Not This Way",
\(F_{ h }=Fsin(\theta )=\cfrac { q_{ p }q }{ 4\pi \varepsilon _{ o }r^{ 2 } } sin(\theta )\)
can instead be,
\(F_{ h }=Fsin(\theta )=\cfrac { T_{ p }T_e }{ 4\pi \tau _{ o }r^{ 2 } } sin(\theta )\)
and we are fine with diffraction on a straight flat edge. \(T_p\) is the temperature on the photon and \(T_e\) is the temperature on the electron.
Hurra! More importantly, the Universe now has a counter force to balance gravity. Hot Banana Mochi safe.
