# Thread: Most General solution of Laplace's equation

1. ## Most General solution of Laplace's equation

Laplace's equation written in plane polar coordinates $(r,\theta)$ is

$T_{rr} + \frac{1}{r}T_r + \frac{1}{r^2}T_{\theta \theta} = 0$

I need to find the most general solution $T(r)$ which is a function of $r$ only.

Can anyone see what this would be?

2. Originally Posted by Jason Bourne
Laplace's equation written in plane polar coordinates $(r,\theta)$ is

$T_{rr} + \frac{1}{r}T_r + \frac{1}{r^2}T_{\theta \theta} = 0$

I need to find the most general solution $T(r)$ which is a function of $r$ only.

Can anyone see what this would be?
If T is a function of r only, then $T_{\theta\theta}= 0$ so the equation becomes the ordinary differential equation $T_{rr}+ \frac{1}{r}T_r= 0$. Let $u= T_r$ and we have $u_r+ \frac{1}{r}u= 0$ which is a separable first order differential equation. $\frac{du}{u}= -\frac{dr}{r}$. Can you finish it from there?

3. Originally Posted by HallsofIvy
If T is a function of r only, then $T_{\theta\theta}= 0$ so the equation becomes the ordinary differential equation $T_{rr}+ \frac{1}{r}T_r= 0$. Let $u= T_r$ and we have $u_r+ \frac{1}{r}u= 0$ which is a separable first order differential equation. $\frac{du}{u}= -\frac{dr}{r}$. Can you finish it from there?
Thanks. So $T = Aln(r) + B$

A,B constants?

4. Yes, that is correct.