# Electrostatic potential energy - dielectric between concentric spheres

Saitama

## Homework Statement

A conducting sphere of radius ##a## carries an initial charge ##q_o##. It is surrounded by another concentric sphere of radius ##b##. The space between the two spheres is filled with a dielectric of permittivity ##\epsilon## and conductivity ##\sigma##. Find the electrostatic potential energy stored in the system at time ##t##.

## The Attempt at a Solution

The electric field at a distance ##r## from the centre of smaller sphere is ##\frac{q_0}{4\pi \epsilon r^2}##. The electrostatic potential energy stored can be calculated by the following integral:
$$U=\int \frac{1}{2}\epsilon E^2dV$$
Replacing dV with ##4\pi r^2dr## and solving, I don't get the right answer. Also, I don't see how can I express U in terms of t and ##\sigma##. Any help is appreciated. Thanks!

## Answers and Replies

Homework Helper
That conductivity allows charge to flow from one plate to the other. It is the same as if a resistor was connected across the capacitor.

ehild

Saitama
That conductivity allows charge to flow from one plate to the other. It is the same as if a resistor was connected across the capacitor.

ehild

What if there was no conductivity given in the question? Would my approach be correct then?

And I still don't know how to begin with this question. :(

Gold Member
You have HCV Part II? There's a formula given for finding out Capacitance of Spherical Capacitor. That's ought to help.

Saitama
You have HCV Part II? There's a formula given for finding out Capacitance of Spherical Capacitor. That's ought to help.

I don't think that formula would help. A current flows here so I think a good equation to start with would be ##J=\sigma E## (that's the only equation I remember which involves conductivity), where J is current density and E is the electric field but I am not sure if it would work though.

Gold Member
The charge will be conducted from Inner Sphere to outer Sphere. The instantaneous charge can be found out by the help of current. Then we can find the energy of the system. Let's see if that helps.

BTW, is your D-Day this year or next? (You know what I mean)

Homework Helper
I don't think that formula would help. A current flows here so I think a good equation to start with would be ##J=\sigma E## (that's the only equation I remember which involves conductivity), where J is current density and E is the electric field but I am not sure if it would work though.

You are on the right track. J=σE and JE is the power dissipated in unit volume in unit time.

You also can find both the capacitance and the resistance of the spherical shell, and treat the problem as discharging a capacitor.

ehild

Saitama
You also can find both the capacitance and the resistance of the spherical shell, and treat the problem as discharging a capacitor.
How can I calculate the resistance here? Can I have a few hints to start with? Gold Member
Use conductivity as inverse of resistivity to find resistance. Take an elemental spherical shell of thickness dx and radius x. Now use integral calculus to find the overall resistance.

Saitama
Use conductivity as inverse of resistivity to find resistance. Take an elemental spherical shell of thickness dx and radius x. Now use integral calculus to find the overall resistance.

That's the first thought that came to my mind but what should I use as cross-section area?
We have
$$R=\frac{1}{\sigma}\cdot \frac{\ell}{A}$$
What should be A for the differential element?

Gold Member
$$dR=\frac{1}{\sigma}\times \frac{dx}{4\pi x^2}$$

Saitama
$$dR=\frac{1}{\sigma}\times \frac{dx}{4\pi x^2}$$

That gives me,
$$R=\frac{1}{4\pi \sigma}\cdot \left(\frac{1}{a}-\frac{1}{b}\right)$$

The capacitance is
$$4\pi \epsilon\left(\frac{ab}{b-a}\right)$$

From ehild's suggestion,
$$I=I_oe^{-t/RC}$$
where ##RC=\epsilon/\sigma## and how can I find ##I_o##? Gold Member
This is what I am coming to$$E=\frac{Q_0^2}{8C}\times (1 - e^{-t/RC})^2$$

It really helps if you have some solution to reach to... Saitama
This is what I am coming to$$E=\frac{Q_0^2}{8C}\times (1 - e^{-t/RC})^2$$

It really helps if you have some solution to reach to... That's wrong and I am still clueless about what should be ##I_o##. :(

Gold Member
How about finding the potential at the inner sphere and the outer sphere due to the charge on inner sphere, find their difference and divide by resistance?

Homework Helper
From ehild's suggestion,
$$I=I_oe^{-t/RC}$$
where ##RC=\epsilon/\sigma## and how can I find ##I_o##? ehild

Homework Helper
This is what I am coming to$$E=\frac{Q_0^2}{8C}\times (1 - e^{-t/RC})^2$$

It really helps if you have some solution to reach to... Conduction means dissipation, loss of electric energy. The energy of the electric field has to decrease.

ehild

• 1 person
Saitama
How about finding the potential at the inner sphere and the outer sphere due to the charge on inner sphere, find their difference and divide by resistance?

ehild

Thank you both, I have reached close to the answer but it is still not correct.
$$U=\frac{Q_o^2}{2C}e^{-\frac{2t}{RC}}$$
Substituting RC and C,
$$U=\frac{Q_o^2(b-a)}{8\pi \epsilon ab}e^{-\frac{2\sigma t}{\epsilon}}$$
But the given answer is:
$$U=\frac{q_o^2(b-a)e^{-2\sigma \epsilon t}}{4\pi \epsilon ab}$$
I am sure that my exponential term is correct. ##2\sigma \epsilon t## is not dimensionless so the given answer is wrong but what about the factor of 1/2?

Thanks!

Last edited:
Homework Helper
Thank you both, I have reached close to the answer but it is still not correct.
$$U=\frac{Q_o^2}{2C}e^{-\frac{t}{RC}}$$
Substituting RC and C,
$$U=\frac{Q_o^2(b-a)}{8\pi \epsilon ab}e^{-\frac{2\sigma t}{\epsilon}}$$
But the given answer is:
$$U=\frac{q_o^2(b-a)e^{-2\sigma \epsilon t}}{4\pi \epsilon ab}$$
I am sure that my exponential term is correct. ##2\sigma \epsilon t## is not dimensionless so the given answer is wrong but what about the factor of 1/2?

Thanks!

The given answer is wrong. Yours is correct (at least the same, I got) :)

ehild

• 1 person
Saitama
The given answer is wrong. Yours is correct (at least the same, I got) :)

ehild

Thanks a lot ehild! • 1 person
Homework Helper
Thanks a lot ehild! Thanks for the thanks ehild

Saitama
Thanks for the thanks ehild

One thanks isn't enough. You deserve a lot more of them. Gold Member
Asking ehild whether or not he's willing to help tomorrow too in real time!? :p

Saitama
Asking ehild whether or not he's willing to help tomorrow too in real time!? :p

Don't you know they don't allow other gadgets in the examination hall? Gold Member
This IS India my son! There's always a way or two around!

Saitama
This IS India my son! There's always a way or two around!

Yes, you are correct. But let's not talk about that stuff publicly, Dad. 