Numerical PDE's II - Circular Domain

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SUMMARY

The discussion focuses on solving a numerical partial differential equation (PDE) defined in a circular domain, specifically the equation \(\frac{\partial^{2}u }{{\partial r^{2} }} + \frac{1}{r}\frac{\partial u}{\partial r} + \frac{1}{r^{2}}\frac{\partial^{2}u}{\partial \theta^{2}} = 0\) with boundary conditions \(u(1,\theta) = 1-\cos(\theta)\), \(u(2,\theta)=0\), \(u(r,0)=0\), and \(u(r,\pi)=4-2r\). The solution approach involves discretizing the domain using \(\delta r\) and \(\delta \theta\) and applying finite difference methods. The discussion also raises questions about the applicability of such models in real-world scenarios involving circular annuli.

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Homework Statement


Approximate the solution of:
[tex] <br /> \frac{\partial^{2}u }{{\partial r^{2} }} + \frac{1}{r}\frac{\partial u}{\partial r} + \frac{1}{r^{2}}\frac{\partial^{2}u}{\partial \theta^{2}} = 0, 1<r<3, 0<\theta<\pi,<br /> <br /> u(1,\theta) = 1-\cos(\theta),u(2,\theta)=u(r,0)=0 u(r,\pi)=4-2r<br /> [/tex]

Homework Equations


[tex] <br /> \delta r = \frac{r_{outer} - r_{inner}}{N}<br /> \delta \theta = \frac{\theta_{end} - \theta_{start}}{M}<br /> [/tex]
n,m are positve integers

[tex] \delta r_i = r_{inner} + i\delta r[/tex]
[tex] \delta theta_j = \theta_{start} + j\delta \theta[/tex]

The Attempt at a Solution


[tex] \frac{u_{i+1,j} - 2U_{i,j} + U_{i-1,j}}{(\delta r)^2} + \frac{1}{r_i}\frac{u_{i+1,j}-u_{i-1,j}}{2\delta r} +\frac{u_{i,j+1} - 2U_{i,j} + U_{i,j-1}}{(\delta \theta)^2} = f_{i,j}[/tex]

Multiply this equation by [tex](\delta r)^2[/tex]
[tex] u_{i+1,j} - 2u_{i,j} + u_{i-1,j} + \frac{1}{r_i}\frac{u_{i+1,j}-u_{i-1,j}}{2}\delta r + \frac{1}{r_i}\frac{\delta r}{\delta \theta}(u_{i+1,j}-2u{i,j}+u{i,j-1} = f_{i,j}(\delta r)^2<br /> [/tex]

What do I do next>
 
Last edited:
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And the question is?
 
Nevermind, I got it.

But does anyone know if such a problem with those given BC's can be applied elsewhere?
When would you model something with a circular annulus?
 

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