From 42b455abe1308e7ffd69f1d4ca6a44fd48969acf Mon Sep 17 00:00:00 2001
From: Nao Pross <np@0hm.ch>
Date: Fri, 2 Sep 2022 02:55:59 +0200
Subject: kugel: Spelling

---
 buch/papers/kugel/applications.tex | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

(limited to 'buch/papers/kugel/applications.tex')

diff --git a/buch/papers/kugel/applications.tex b/buch/papers/kugel/applications.tex
index f8f3edd..868d738 100644
--- a/buch/papers/kugel/applications.tex
+++ b/buch/papers/kugel/applications.tex
@@ -62,7 +62,7 @@ electric field is proportional to the charge density $\rho$. So, the Laplacian
 of the electric potential is proportional to the charge density! For those that
 are more familiar with the integral form of Maxwell's equation, we have also
 included an additional step using the divergence theorem, which brings us to the
-electric Flux $\Phi$, which by Gauss' law (shown in the iconic\footnote{Every
+electric flux $\Phi$, which by Gauss' law (shown in the iconic\footnote{Every
 electrical engineer has seen this picture so many times that is probably burnt
 in their eyes.} figure \ref{kugel:fig:eeg-flux}) equals the net electric charge.
 
-- 
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