Space Density Under Temperature

From the post "Possibilities, Possibilities, And God Created More Possibilities",

${ d }_{ s }(T)=\cfrac { ({ d }_{ T_{ max } }-{ d }_{ n }) }{ -ln({ T_{ max }^{ 2 } } ) }( ln(x )-ln(A^2))+{ d }_{ n }$

${ d }_{ s }(T)=A.ln(x )+B$

A plot of log( x ) + 1 is shown below

When  $T=T_{max}$  space density is  $d_{Tmax}$  when  $T=0$,  $d_s=d_n$  at normal space density.  The derivative of  space density,

$\cfrac{d(d_s(x))}{dx}$  gives thermal gravity.

This is assuming that  $g_T=\cfrac{G_{To}}{x}$.