logowanie

matematyka » forum » forum zadaniowe - uczelnie wyższe » zadanie

Analiza matematyczna, zadanie nr 3761

ostatnie wiadomości  |  regulamin  |  latex

AutorZadanie / Rozwiązanie

magda2219
postów: 19
2015-11-03 18:38:33

Wykazać, że równanie Laplace'a w R^2 postaci: (delta^2*u)/(delta*x^2)+(delta^2*u)/(delta*y^2)=0 we współrzednych biegunowych x=rcosfi y=rsinfi wyraza sie wzorem: (delta^2*u)/(delta*r^2)+(1/r^2)*(delta^2*u)/(delta*y^2)+(1/r)*(delta*u)/(delta*r)=0


janusz78
postów: 820
2015-11-04 22:00:20

$\frac{\partial^2 u}{\partial x^2}+ \frac{\partial^2 u}{\partial y^2}=0$

$ x =r\cos(\phi), y = r\sin(\phi)$

$ r^2 = x^2 +y^2, \ \ \tan(\phi) = \frac{y}{x}$

$ r = \sqrt{x^2+y^2},\ \ \phi = \arctan(\frac{y}{x}),$

$\frac{\partial r}{\partial x}= \frac{x}{\sqrt{x^2+y^2}}= \frac{r\cos(\phi)}{r}= \cos(\phi).$
$\frac{\partial^2 u}{\partial x^2}+ \frac{\partial^2 u}{\partial y^2}=0$

$ x =r\cos(\phi), y = r\sin(\phi)$

$ r^2 = x^2 +y^2, \ \ \tan(\phi) = \frac{y}{x}$

$ r = \sqrt{x^2+y^2},\ \ \phi = \arctan(\frac{y}{x}),$

$\frac{\partial r}{\partial x}= \frac{x}{\sqrt{x^2+y^2}}= \frac{r\cos(\phi)}{r}= \cos(\phi).$

$\frac{\partial r}{\partial y}= \frac{y}{\sqrt{x^2+y^2}}= \frac{r\cos(\phi)}{r}= \cos(\phi).$

$ \frac{\partial \phi}{\partial x}= \frac{1}{1+(\frac{y}{x})^2}(-\frac{y}{x^2})=\frac{-y}{x^2+y^2}= -\frac{\sin(\phi)}{r}.$

$ \frac{\partial \phi}{\partial y}= \frac{1}{1+(\frac{y}{x})^2}(\frac{1}{x})=\frac{x}{x^2+y^2}= \frac{\cos(\phi)}{r}.$

Ze wzorów na pochodne cząstkowe funkcji złożonej

$\frac{\partial u}{\partial x}= \frac{\partial u}{\partial r}\frac{\partial r}{\partial x}+ \frac{\partial u}{\partial \phi}\frac{\partial \phi}{\partial x},$

$\frac{\partial u}{\partial x}= \cos(\phi)\frac{\partial u}{\partial r} - \frac{\sin(\phi)}{r}\frac{\partial u}{\partial \phi}$ (1)

$\frac{\partial^2 u}{\partial x^2}= \frac{\partial}{\partial x}(\frac{\partial u}{\partial x})= $ $\cos(\phi)\frac{\partial}{\partial r}(\frac{\partial u}{\partial x})- \frac{\sin(\phi)}{r}\frac{\partial}{\partial \phi}(\frac{\partial u}{\partial x}).$

Stosując ponownie wzór (1)

$\frac{\partial^2 u}{\partial x^2}=\frac{\partial}{\partial r}\left(\cos(\phi)\frac{\partial u}{\partial r} - \frac{\sin(\phi)}{r}\frac{\partial u}{\partial \phi}\right)- \frac{\sin(\phi)}{r}\frac{\partial}{\partial \phi}\left(\cos(\phi)\frac{\partial u}{\partial r} - \frac{\sin(\phi)}{r}\frac{\partial u}{\partial \phi}\right)= cos^2(\phi) \frac{\partial^2 u}{\partial r^2}-cos(\phi)\left(-\frac{\sin(\phi)}{r^2}\frac{\partial u}{\partial \phi} +\frac{\sin(\phi)}{r}\frac{\partial^2 u}{\partial r \partial \phi}\right)+$
$-\frac{\sin(\phi)}{r} \left(-\sin(\phi)\frac{\partial u}{\partial r}+\cos(\phi)\frac{\partial^2 u}{\partial \phi \partial r}\right)+ \frac{\sin(\phi)}{r}\left(\frac{\cos(\phi)}{r}\frac{\partial u}{\partial \phi} +\frac{\sin(\phi)}{r}\frac{\partial^2 u}{\partial \phi^2}\right).$

Uwzględniając równość pochodnych cząstkowych mieszanych otrzymujemy

$\frac{\partial^2 u}{\partial x^2}= \cos^2(\phi)\frac{\partial^2 u}{\partial r^2}-\frac{2\sin(\phi)\cos(\phi)}{r}\frac{\partial^2 u}{\partial r \partial \phi}+ \frac{\sin^2(\phi)}{r^2}\frac{\partial u^2}{\partial \phi^2}+\frac{\sin^2(\phi)}{r}\frac{\partial u}{\partial r}+ \frac{2\sin(\phi)\cos(\phi)}{r^2}\frac{\partial u}{\partial \phi}$ (2)

Podobnie obliczamy pochodną cząstkową $\frac{\partial^2 u}{\partial y^2}.$

$\frac{\partial u}{\partial y}=\frac{\partial u}{\partial r}\frac{\partial r}{\partial y}+\frac{\partial u}{\partial \phi}\frac{\partial \phi}{\partial y}.$

$\frac{\partial u}{\partial y}=\sin(\phi)\frac{\partial u}{\partial r}+ \frac{\cos(\phi)}{r}\frac{\partial u}{\partial \phi}.$

Postepujemy tak jak wyżej tzn. podstawiamy w miejsce $u, \ \ \frac{\partial u}{\partial y}$

i po uporządkowaniu składników sumy otrzymujemy ostatecznie

$\frac{\partial^2 u}{\partial y^2}= \sin^2(\phi)\frac{\partial^2 u}{\partial r^2}+\frac{2\sin(\phi)\cos(\phi)}{r}\frac{\partial^2 u}{\partial r \partial \phi}+ \frac{\cos^2(\phi)}{r^2}\frac{\partial u^2}{\partial \phi^2}+\frac{\cos^2(\phi)}{r}\frac{\partial u}{\partial r}- \frac{2\sin(\phi)\cos(\phi)}{r^2}\frac{\partial u}{\partial \phi}$ (3)


Po dodaniu stronami (2) i (3)

$\frac{\partial^2 u}{\partial x^2}+ \frac{\partial^2 u}{\partial y^2}= (\cos^2(\phi)+\sin^2(\phi))\frac{\partial^2 u}{\partial r^2}+ \frac{\sin^2(\phi)+\cos^2(\phi)}{r^2}\frac{\partial^2 u}{\partial \phi^2}+ \frac{\sin^2(\phi)+\cos^2(\phi)}{r}\frac{\partial u}{\partial r}= \frac{\partial^2 u}{\partial r^2} + \frac{1}{r^2}\frac{\partial^2 u}{\partial \phi^2} + \frac{1}{r}\frac{\partial u}{\partial r} =0.$


strony: 1

Prawo do pisania przysługuje tylko zalogowanym użytkownikom. Zaloguj się lub zarejestruj





© 2019 Mariusz Śliwiński      o serwisie | kontakt   drukuj