Today I’m running run16_ken_fixedgradient so I can compare with our old method of doing things. Previously I was calculating the density gradient of the entire particle and using that for h:
\begin{equation*}
h=\frac{\rho}{|\nabla \rho|}
\end{equation*}
but now It’s changing to:
\begin{equation*}
h=\frac{\rho_{\rm{HI}}}{|\nabla \rho_{\rm{HI}}|}
\end{equation*}
which may not make much a difference at all, but will be nice to compare. Run is currently at $$z\sim4.8$$.
Have a SPLOTCH picture!
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