From 65c31eca1c29a0e3c19a0c24dfe4c25ee980f898 Mon Sep 17 00:00:00 2001 From: Alberto Botto Poala Date: Mon, 20 Jan 2025 11:34:17 +0100 Subject: [PATCH] =?UTF-8?q?fix=20ref=20to=20eq=20adv:eq:fvadv,=20was=20eq:?= =?UTF-8?q?adv:fvadv=20=C2=A7=205.3?= MIME-Version: 1.0 Content-Type: text/plain; charset=UTF-8 Content-Transfer-Encoding: 8bit --- advection/advection-higherorder.tex | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/advection/advection-higherorder.tex b/advection/advection-higherorder.tex index 1be6d9c..5b55fc0 100644 --- a/advection/advection-higherorder.tex +++ b/advection/advection-higherorder.tex @@ -508,7 +508,7 @@ \section{Method of lines approach} In the above constructions, we computed a time-centered flux by predicting the interface state to the half-time (by Taylor-expanding in time through $\Delta t /2$). Instead, we can recognize that with -the spatial discretization done in Eq.~\ref{eq:adv:fvadv}, we are left +the spatial discretization done in Eq.~\ref{adv:eq:fvadv}, we are left with an ordinary differential equation in time that can then be solved using standard ODE techniques.