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authorNao Pross <np@0hm.ch>2022-08-28 14:20:31 +0200
committerNao Pross <np@0hm.ch>2022-08-28 14:20:31 +0200
commit53c3b1227a2433eac5a3ab32a6937607d5cd8e3d (patch)
tree69e316589fa148c575ed69f6ed0a9c4e34a2ee42 /buch
parentkugel: Add figure and minor corrections (diff)
downloadSeminarSpezielleFunktionen-53c3b1227a2433eac5a3ab32a6937607d5cd8e3d.tar.gz
SeminarSpezielleFunktionen-53c3b1227a2433eac5a3ab32a6937607d5cd8e3d.zip
kugel: Re-add usecase reference, minor corrections
Diffstat (limited to 'buch')
-rw-r--r--buch/papers/kugel/references.bib16
-rw-r--r--buch/papers/kugel/spherical-harmonics.tex21
2 files changed, 31 insertions, 6 deletions
diff --git a/buch/papers/kugel/references.bib b/buch/papers/kugel/references.bib
index e13b67c..7603f2f 100644
--- a/buch/papers/kugel/references.bib
+++ b/buch/papers/kugel/references.bib
@@ -275,4 +275,20 @@ This photo was taken during studies that resulted in the publication: Hope, C, S
urldate = {2022-08-27},
date = {2022-04-27},
doi = {10.5281/ZENODO.6497293},
+}
+
+@article{davari_new_2013,
+ title = {New Implementation of Legendre Polynomials for Solving Partial Differential Equations},
+ volume = {04},
+ issn = {2152-7385, 2152-7393},
+ url = {http://www.scirp.org/journal/doi.aspx?DOI=10.4236/am.2013.412224},
+ doi = {10.4236/am.2013.412224},
+ pages = {1647--1650},
+ number = {12},
+ journaltitle = {Applied Mathematics},
+ shortjournal = {{AM}},
+ author = {Davari, Ali and Ahmadi, Abozar},
+ urldate = {2022-08-28},
+ date = {2013},
+ file = {Full Text:/Users/npross/Zotero/storage/A8XM56WK/Davari and Ahmadi - 2013 - New Implementation of Legendre Polynomials for Sol.pdf:application/pdf},
} \ No newline at end of file
diff --git a/buch/papers/kugel/spherical-harmonics.tex b/buch/papers/kugel/spherical-harmonics.tex
index 02d93e9..0fb6557 100644
--- a/buch/papers/kugel/spherical-harmonics.tex
+++ b/buch/papers/kugel/spherical-harmonics.tex
@@ -190,7 +190,6 @@ require a dedicated section of its own.
\begin{figure}
\centering
- % \kugelplaceholderfig{.8\textwidth}{5cm}
\includegraphics[
scale = 1.2,
trim = 0 40 0 0, clip,
@@ -327,7 +326,14 @@ obtain the \emph{associated Legendre functions}.
\end{equation}
are known as Ferrers or associated Legendre functions.
\end{definition}
-The constraint $|m|<n$, can be justified by considering eq.\eqref{kugel:eq:associated_leg_func}, where we differentiate $m+n$ times. We all know that a differentiation, to be well defined, must have an order that is greater than zero \kugeltodo{is that always true?}. Furthermore, it can be seen that this derivative is applied on a polynomial of degree $2n$. As is known from Calculus 1, if you derive a polynomial of degree $2n$ more than $2n$ times, you get zero, that would be a trivial solution. This is the power of zero: It is almost always a (boring) solution.
+The constraint $|m|<n$, can be justified by considering equation
+\eqref{kugel:eq:associated_leg_func}, where we differentiate $m+n$ times. We all
+know that a differentiation, to be well defined, must have an order that is
+greater than zero. Furthermore, it can be seen that this derivative is applied
+on a polynomial of degree $2n$. As is known from Calculus 1, if you derive a
+polynomial of degree $2n$ more than $2n$ times, you get zero, that would be a
+trivial solution. This is the power of zero: It is almost always a (boring)
+solution.
We can thus summarize these two conditions by writing:
\begin{equation*}
@@ -344,8 +350,8 @@ section \ref{kugel:sec:construction:eigenvalue}. We had left off in the middle
of the separation, were we had used the Ansatz $f(\vartheta, \varphi) =
\Theta(\vartheta) \Phi(\varphi)$ to find that $\Phi(\varphi) = e^{im\varphi}$,
and we were solving for $\Theta(\vartheta)$. As you may recall, previously we
-performed the substitution $z = \cos \vartheta$. Now we can finally bring back the
-solution to the associated Legendre equation $P^m_n(z)$ into the $\vartheta$
+performed the substitution $z = \cos \vartheta$. Now we can finally bring back
+the solution to the associated Legendre equation $P^m_n(z)$ into the $\vartheta$
domain and combine it with $\Phi(\varphi)$ to get the full result:
\begin{equation*}
f(\vartheta, \varphi)
@@ -709,8 +715,11 @@ To start this journey, we can first write the following equations, which relate
\end{subequations}
Much of the effort will be proving this bunch of equalities. Then, in the second part, where we will derive the recursion equations for $Y^m_n(\vartheta,\varphi)$, we will basically reuse the ones presented above.
-Maybe it is worth mentioning at least one use case for these relations: In some software implementations (that include lighting computations in computer graphics, antenna modelling softwares, 3-D modelling in medical applications, etc.)
-they are widely used, as they lead to better numerical accuracy and computational cost lower by a factor of six\cite{usecase_recursion_paper}.
+Maybe it is worth mentioning at least one use case for these relations: In some
+software implementations (that include lighting computations in computer
+graphics, antenna modelling software, 3-D modelling in medical applications,
+etc.) they are widely used, as they lead to better numerical accuracy and
+computational cost lower by a factor of six \cite{davari_new_2013}.
\begin{enumerate}[(i)]
\item
\begin{proof}