From 1bdb803ced744bcfe7cf81c89a740fcbcf6bdc70 Mon Sep 17 00:00:00 2001
From: Nao Pross <np@0hm.ch>
Date: Tue, 30 Aug 2022 22:42:54 +0200
Subject: kugel: Minor corrections

---
 buch/papers/kugel/applications.tex | 7 +++----
 1 file changed, 3 insertions(+), 4 deletions(-)

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

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}
-- 
cgit v1.2.1

