From 29fd344738894593ae434a271613815d1aa563ac Mon Sep 17 00:00:00 2001 From: =?UTF-8?q?Erik=20L=C3=B6ffler?= Date: Thu, 28 Jul 2022 12:56:49 +0200 Subject: Added solutions for heat conduction. --- .../sturmliouville/waermeleitung_beispiel.tex | 32 ++++++++++++++++++++++ 1 file changed, 32 insertions(+) (limited to 'buch/papers/sturmliouville') diff --git a/buch/papers/sturmliouville/waermeleitung_beispiel.tex b/buch/papers/sturmliouville/waermeleitung_beispiel.tex index cd7a620..a493749 100644 --- a/buch/papers/sturmliouville/waermeleitung_beispiel.tex +++ b/buch/papers/sturmliouville/waermeleitung_beispiel.tex @@ -106,3 +106,35 @@ Differenzialgleichungen aufgeteilt werden: = 0 \] + +% TODO: Rechenweg +TODO: Rechenweg... Enden auf konstanter Temperatur: +\[ + u(t,x) + = + \sum_{n=1}^{\infty}a_{n}e^{-\frac{n^{2}\pi^{2}\kappa}{l^{2}}t} + \sin\left(\frac{n\pi}{l}x\right) +\] +\[ + a_{n} + = + \frac{2}{l}\int_{0}^{l}u(0,x)sin\left(\frac{n\pi}{l}x\right) dx +\] + +TODO: Rechenweg... Enden isoliert: +\[ + u(t,x) + = + a_{0} + \sum_{n=1}^{\infty}a_{n}e^{-\frac{n^{2}\pi^{2}\kappa}{l^{2}}t} + \cos\left(\frac{n\pi}{l}x\right) +\] +\[ + a_{0} + = + \frac{1}{l}\int_{0}^{l}u(0,x) dx +\] +\[ + a_{n} + = + \frac{2}{l}\int_{0}^{l}u(0,x)sin\left(\frac{n\pi}{l}x\right) dx +\] -- cgit v1.2.1