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authorNao Pross <np@0hm.ch>2022-09-02 02:55:59 +0200
committerNao Pross <np@0hm.ch>2022-09-02 02:55:59 +0200
commit42b455abe1308e7ffd69f1d4ca6a44fd48969acf (patch)
treef69673025e48af00c77fbd66f7644301250e9697 /buch/papers
parentkugel: Add references to other chapters (diff)
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kugel: Spelling
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-rw-r--r--buch/papers/kugel/applications.tex2
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diff --git a/buch/papers/kugel/applications.tex b/buch/papers/kugel/applications.tex
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--- 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.