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maxverywell
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Homework Statement
We have a sphere of radius [itex]a [/itex] with permanent magnetization [itex]\mathbf{M}=M\hat{e}_{\mathbf{r}}[/itex].
Find the magnetic scalar potential.
Homework Equations
$$\Phi_M(\mathbf{x})=-\frac{1}{4\pi}\int_V \frac{\mathbf{\nabla}'\cdot\mathbf{M}(\mathbf{x}')}{|\mathbf{x}-\mathbf{x}'|}d^3 x' +\frac{1}{4\pi}\int_S \frac{\mathbf{n}'\cdot\mathbf{M}(\mathbf{x}')}{|\mathbf{x}-\mathbf{x}'|}da'$$
The Attempt at a Solution
$$\mathbf{\nabla}'\cdot\mathbf{M}(\mathbf{x}')=\frac{2M}{r'}$$
$$\mathbf{n}'\cdot\mathbf{M}(\mathbf{x}')=M$$
$$\Phi_M(\mathbf{x})=-\frac{M}{2\pi}\int_{0}^{a} r'dr'\int\int\frac{1}{|\mathbf{x}-\mathbf{x}'|}d\Omega' +\frac{Ma^2}{4\pi}\int \int\frac{1}{|\mathbf{x}-\mathbf{x}'|}d\Omega'$$
I expanded the [itex]1/|\mathbf{x}-\mathbf{x}'| [/itex] in terms of spherical harmonics (and because of the spherical symmetry we have [itex]m=0,\ell=0 [/itex]) and solved the integrals. What I got is:
$$\Phi_M(\mathbf{x})=-2M\int_{0}^{a}\frac{r'}{r_{>}}dr'+\frac{Ma^2}{r_{>}}$$
where [itex]r_{>}=max(r,a)[/itex]
Inside the sphere we have [itex]r_{>}=a[/itex], therefore:
$$\Phi_M(r)=\frac{-2M}{a}\int_{0}^{a}r'dr'+Ma=0$$
This is constant. However the [itex]\Phi_M(r)[/itex] inside the sphere has to satisfy the Poisson equation:
$$\nabla^2 \Phi_M(r)=\nabla\cdot \mathbf{M}=\frac{2M}{r}$$
This is not true for the potential that I found..
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