Resistance between coaxial cylinders

[Reshma]

Two coaxial cylinders, inner radius a and outer radius b are separated by a material of conductivity given by \sigma (r) = k/r for some constant 'k'. Find the resistance between the cylinders.

Here the conductivity is a function of position and the charge density is not zero in the resistive medium, and the electric field \vec E does not go as 1/r. So how is this problem solved?

 

[Meir Achuz]

Two coaxial cylinders, inner radius a and outer radius b are separated by a material of conductivity given by \sigma (r) = k/r for some constant 'k'. Find the resistance between the cylinders.

Here the conductivity is a function of position and the charge density is not zero in the resistive medium, and the electric field \vec E does not go as 1/r. So how is this problem solved?

Assuming steady state, div j=0 so j=j_0/r and E=j/\sigma=constant.

 

[Reshma]

Assuming steady state, div j=0 so j=j_0/r and E=j/\sigma=constant.

The charge density is not zero here, so \vec \nabla \cdot \vec E = {1\over \sigma}\vec \nabla \cdot \vec J = 0 will not hold good.

 

[Meir Achuz]

The charge density is not zero here, so \vec \nabla \cdot \vec E = {1\over \sigma}\vec \nabla \cdot \vec J = 0 will not hold good.

Div E is NOT zero. Div j is zero because rho is constant in time.
Your equation above should be
\vec \nabla \cdot \vec E = \vec \nabla \cdot [\vec J/\sigma] ,
but Div j does =0.
Do you want to argue or to do the problem?

 

[Reshma]

Div E is NOT zero. Div j is zero because rho is constant in time.
Your equation above should be
\vec \nabla \cdot \vec E = \vec \nabla \cdot [\vec J/\sigma] ,
but Div j does =0.
Do you want to argue or to do the problem?

Ok, here goes...
I need to evaluate the current and the voltage in order to find the resistance.
\vec \nabla \cdot \vec E = \vec \nabla \cdot [\vec J/\sigma]

Integrating over a volume dV.
\int \vec \nabla \cdot \vec E dV= \int \vec \nabla \cdot [\vec J/\sigma] dV

By Divergence theorem,

\int \vec E \cdot d\vec a = \int (\vec J /\sigma)\cdot d\vec a

{Q_{enc}\over \epsilon_0} = \int (\vec J /\sigma)\cdot d\vec a

I'm getting stuck here. I don't know how to proceed.

Anyway, I found the current.
But by Ohm's law, \vec J = \sigma \vec E
Current I is given by;
I = \int \vec J \cdot d\vec a = \int {k\over r}\vec E \cdot d\vec a

But, I need \vec E to compute the voltage. How do I do that?

 

[Meir Achuz]

Read my first post.

 

[Reshma]

Assuming steady state, div j=0 so j=j_0/r and E=j/\sigma=constant.

\vec \nabla \cdot \vec J = 0
J = {J_0\over r}
E = {J\over \sigma} = {J_0\over r} {r\over k} = {J_0\over k}

I_{enc} = \int \vec J \cdot d\vec a = \int_a^b {J_0\over r} 2\pi r dr = J_0 2\pi (b-a)

V_a - V_b = -\int_b^a \vec E \cdot d\vec r = {J_0\over k}(b-a)

Resistance R will be:
R = \frac{V_a - V_b}{I} = \left({J_0\over k}(b-a)\right)\left({1\over (J_0 2\pi (b-a)}\right)
R = {1\over 2\pi k}

Thank you for your time!