commit e0b02423e77ecbfcac3c286471d93684ec0364fb
parent 683e1f92b790dddd6f2a82af2ef43aff81057289
Author: Anders Damsgaard <anders@adamsgaard.dk>
Date: Tue, 3 Dec 2019 16:58:19 +0100
Remove unused abbreviation
Diffstat:
1 file changed, 1 insertion(+), 1 deletion(-)
diff --git a/si.tex b/si.tex
@@ -276,7 +276,7 @@ As for the granular flow solution, we also use operator splitting and finite dif
\label{eq:p_f_solution}
\end{equation}
\end{linenomath*}
-For each time step $\Delta t$, a solution to Eq.~\ref{eq:p_f_solution} is found by the Crank-Nicholson (CN) method \cite<e.g.,>[] {Patankar1980, Ferziger2002, Press2007}.
+For each time step $\Delta t$, a solution to Eq.~\ref{eq:p_f_solution} is found by the Crank-Nicholson method \cite<e.g.,>[] {Patankar1980, Ferziger2002, Press2007}.
In the procedure the pressure field at $t + \Delta t$ is found by mixing explicit and implicit solutions with equal weight.
The method is unconditionally stable and second-order accurate in time and space.
Our implementation of grain and fluid dynamics is highly efficient, and for the presented experiments each time step completes in less than 1 ms on a single CPU core.
