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authorNao Pross <np@0hm.ch>2022-08-30 22:42:54 +0200
committerNao Pross <np@0hm.ch>2022-08-30 22:42:54 +0200
commit1bdb803ced744bcfe7cf81c89a740fcbcf6bdc70 (patch)
treee2ce322601e737494626056741174ff5acf11e07 /buch/papers/kugel/applications.tex
parentkugel: Minor changes and fix proofs (remove enumerate) (diff)
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kugel: Minor corrections
Diffstat (limited to '')
-rw-r--r--buch/papers/kugel/applications.tex7
1 files changed, 3 insertions, 4 deletions
diff --git a/buch/papers/kugel/applications.tex b/buch/papers/kugel/applications.tex
index 15a57d5..10bf153 100644
--- a/buch/papers/kugel/applications.tex
+++ b/buch/papers/kugel/applications.tex
@@ -32,7 +32,6 @@ at their location (figure \ref{kugel:fig:eeg-electrodes}). To see how this will
relate to the spherical harmonics, we will first quickly recap a bit of physics,
electrodynamics to be precise.
-
\subsubsection{Electrodynamics}
In section \ref{kugel:sec:construction:eigenvalue} we have shown that the
@@ -88,7 +87,7 @@ using the spherical harmonics.
To solve this new interpolation problem, we will start with a blatantly
engineering assumption: the human head is a sphere of radius $R$, with the value
-of $R$ begin the average radius of a human head (which is around 11 cm). So, we
+of $R$ being the average radius of a human head (which is around 11 cm). So, we
will assume that the potential distribution on the head can be written as a
finite linear combination of spherical harmonics:
\begin{equation*}
@@ -110,7 +109,7 @@ minimization problem:
\sin \vartheta \, d\vartheta d\varphi,
\label{kugel:eqn:eeg-min} \\
&\text{under the constraints} \quad V(p_j) = \phi_j
- \quad \text{ for } \quad 1 < j < M.
+ \quad \text{ for } \quad 1 \leq j \leq M.
\label{kugel:eqn:eeg-min-constraints}
\end{align}
\end{subequations}
@@ -203,4 +202,4 @@ quite unwieldy.
\subsection{Measuring Gravitational Fields}
-\subsection{Quantisation of Angular Momentum}
+% \subsection{Quantisation of Angular Momentum}