Question

2 SPHERICAL CONDUCTORS Two concentric spherical conductors or radii a, b (with b> a) have an Ohmic material with conductivity

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Answer #1

Let Q be the charge on the inner shell. Then

\overrightarrow{E}=\frac{1}{4\pi \epsilon_{o}}\frac{Q}{r^2}\hat{r}

in the space between them, and

V_{a}-V_{b}=-\int_{b}^{a}\overrightarrow{E}.\overrightarrow{dr}

or,

V_{a}-V_{b}=-\int_{b}^{a}\frac{1}{4\pi \epsilon_{o}}\frac{dr}{r^2}

or,

V_{a}-V_{b}=\frac{Q}{4\pi \epsilon_{o}}(\frac{1}{a}-\frac{1}{b})

now

I=\sigma \frac{Q}{\epsilon_{o}}=\frac{\sigma}{\epsilon_{o}}\frac{4\pi \epsilon_{o}(V_{a}-V_{b})}{\frac{1}{a}-\frac{1}{b}}

so, the resistance between the shell is given by

R=\frac{V_{a}-V_{b}}{I}=\frac{1}{4\pi \sigma}(\frac{1}{a}-\frac{1}{b})

Now if b is very large the

R=\frac{1}{4\pi \sigma a}

Essentially all of the resistance is in the region right around the inner sphere. Successive shells contribute less and less because the cross-section area  4\pi r^2 gets large and large. For the two submerged spheres

R=\frac{2}{4\pi \sigma a}=\frac{1}{2\pi \sigma a}

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