From ea3927bb133e2da28c56fc0aadb4cba856d4e207 Mon Sep 17 00:00:00 2001 From: Laurent Rineau Date: Tue, 18 Dec 2018 12:12:20 +0100 Subject: [PATCH] Fix the naming of the divergence operator --- Heat_method_3/doc/Heat_method_3/Heat_method_3.txt | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/Heat_method_3/doc/Heat_method_3/Heat_method_3.txt b/Heat_method_3/doc/Heat_method_3/Heat_method_3.txt index 66234767034..6a5d487d2a6 100644 --- a/Heat_method_3/doc/Heat_method_3/Heat_method_3.txt +++ b/Heat_method_3/doc/Heat_method_3/Heat_method_3.txt @@ -104,7 +104,7 @@ For a detailed overview of the heat method, the reader may consult sequel, we introduce the basic notions so as to explain our algorithms. In general, the heat method is applicable to any setting if there exists a gradient operator \f$ \nabla\f$, a divergence -operator \f$\nabla\f$ and a Laplace operator \f$\Delta = \nabla \cdot +operator \f$\nabla \cdot\f$ and a Laplace operator \f$\Delta = \nabla \cdot \nabla\f$, which are standard derivatives from vector calculus. The Heat Method consists of three main steps: