From 5662d93f8d77941c3f604b86ebd0e9f5882483aa Mon Sep 17 00:00:00 2001
From: DorisReiter <132465655+DorisReiter@users.noreply.github.com>
Date: Tue, 8 Aug 2023 15:03:53 +0200
Subject: [PATCH] Update docs/math/maxwell.md

Co-authored-by: Helge Gehring <42973196+HelgeGehring@users.noreply.github.com>
---
 docs/math/maxwell.md | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

diff --git a/docs/math/maxwell.md b/docs/math/maxwell.md
index 61f8f404..96d0ae8d 100644
--- a/docs/math/maxwell.md
+++ b/docs/math/maxwell.md
@@ -97,7 +97,7 @@ $$\begin{aligned}
 \end{aligned}$$
 
 ### Piecewise constant materials and boundary conditions
-It is instructive to condsider the well-known case of an interface $I$ between two dielectric materials, which appear in many devices. We assume an interface between two materials called $1$ with dielectric constant $\varepsilon_1$ and $2$ with dielectric constant $\varepsilon_2$. The surface is defined by the normal vector of the interface $\mathbf{n}_{I}$ and there are no external surface charges or currents. For simplicity, we surpress the index  $\left(\mathbf{r},t\right)$ here. 
+It is instructive to condsider the well-known case of an interface $I$ between two dielectric materials, which appear in many devices. We assume an interface between two materials called $1$ with dielectric constant $\varepsilon_1$ and $2$ with dielectric constant $\varepsilon_2$. The surface is defined by the normal vector of the interface $\mathbf{n}_{I}$ and there are no external surface charges or currents. For simplicity, we surpress the arguments $\left(\mathbf{r},t\right)$ here. 
 
 All fields can then be split into the component parallel to the interface (hence perpendicular to the normal vector) and perpendicular to the interface (hence parallel to the normal vector). For example we consider the electric field: Define the normalized field vector $\hat{\mathbf{E}}=\mathbf{E}/E$ we split it into