Understanding the Charge Distribution in a Coaxial Cylinder System

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Homework Help Overview

The discussion revolves around the charge distribution in a coaxial cylinder system, specifically examining the validity of Gauss's law in this context. Participants explore the electric field behavior between a solid conducting cylinder and a cylindrical conducting shell, with a voltage applied across them.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants attempt to calculate the electric field and voltage in the system, questioning the uniformity of the electric field and the distribution of charge on the cylinders. There is discussion about the implications of the inner cylinder's charge on the electric field and the reasoning behind the observed behavior.

Discussion Status

Some participants have provided insights into the nature of the electric field and charge distribution, noting that the inner cylinder contributes to the field while the outer cylinder's charge is concentrated on its inner surface. There is an ongoing exploration of the implications of these observations, with no explicit consensus reached on all points raised.

Contextual Notes

Participants are working under the assumption that the system is conductive and that the net charge of the entire system is zero. There is a focus on understanding how charge polarization affects the electric field and the implications for applying Gauss's law.

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A group of students want to test if Gauss's law works or not in some real-life situations.

A solid conducting cylinder of radius a = 2cm and a cylindrical conducting shell of radius b = 8cm are arranged to concentric (coaxial), and a voltage of V_0 = 12volts is connected to the two conductors. The heights of the cylinders are h = 2cm.

Prediction:
Then they predict that, if Gauss's law is valid, the electric field on a Gaussian cylindrical surface must be uniform. Then the magnitude of the electric field at any point between a and b is:

(for uniform electric fields)

E = V / d = 12volts / 6cm = 200 volts / meter

Then they predict the voltage across the outside shell and a middle point P must be:

(where 'r' is the distance from the center to 'p')
V = E(r - a) = 200 volts / meter (5cm - 2cm) = 6 volts

Then they can measure the voltage across the outside shell and a middle point P. If it is 6 volts then Gauss's law is valid and works with the real life situation.

Identify the deficiencies in this line of reasoning.

First I set about to calculate the electric field:

E_cylinder = (2 Ke Q) / r^2
Solve for Q with the capacitance of two coaxial cylinders:

C_cylinders = l / (2*Ke*ln(b/a))

C*V = Q

Q = l*V / (2*Ke*ln(b/a))

substituting:

E_cylinder = (l*V) / (ln(b/a)*r^2)

Where 'r' is a distance measured from the center. Trying several distances (r = 5cm -> E = 69.2 Volts / meter, r = 2cm [on the internal cylinder] -> 432.8 Volts / meter) I discovered that the electric field varies with distance, therefore its not uniform.

The equation:

V = E/d

Cannot be applied to this situation.

This is (guess) because less charge from the power source settles on the inner cylinder because of its relative radius compared to the outer cylinder.

Am I correct?

Peter
 
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This is (guess) because less charge from the power source settles on the inner cylinder because of its relative radius compared to the outer cylinder.
You are correct that the field is not uniform but your reason is wrong. Both cylinders have the same quanta of charge but with opposite signs, i.e if the inner cylinder is positively charged by +q the outer cylinder is negatively charged by -q. The reason the electric field is not constant is because only the inner cylinder contributes to it, and the cylinder can be treated as a long line in which the charges are uniformly distributed. Therefore the electrid field near it is given by the formula:

[tex]E = 2Ke\frac{\lambda}{r}[/tex]

Where [tex]\lambda = \frac{dq}{dl}[/tex], i.e the amount of charge for a length unit. We assume it is constant here, even thought that closer to the ends of the cylinder it is not. But the height of the cylinders are so big compared to their radii that this doesn't matter.
 
Last edited:
You are correct that the field is not uniform but your reason is wrong. Both cylinders have the same quanta of charge but with opposite signs

Quanta? I'll assume it means amount. So my intuition was correct about the maximum available charge is spread between the cylinders.

Calculating the electric field at the outer cylinder:

E_cylinder = (l*V) / (ln(b/a)*r^2)
l = .02m
V = 12 volts
b = .08m
a = .02m
r = .08m

E_cylinder = 27.05 V / m

So you are correct, the electric field does extend beyond the outer cylinder and some distance beyond where it becomes negligible. The only way this could be if the electric field produced by the inner cylinder was stronger than the outer cylinder, or that there is no electric field internal to a cylinder?

Which would mean that the forces internal to the cylinder, the charges on the surface, exactly balance each other perpendicular to the surface. Which makes sense given the symmetry of a slice of the cylinder, a circle.

So given that line of reasoning, there is no electric field internal to the outer cylinder and only the inner cylinder contributes to the field inside the cylindrical shell. Which would explain why the field dissipates with distance as if it were alone.

Again, is there a flaw in my logic?

Peter
 
Before doing anything here you need to understand exactly how the charge is distributed. Do you know (and understand why) the charge of the outer cylinder is concentrated in its inner surface only, and there is no charge on the outer surface?

So given that line of reasoning, there is no electric field internal to the outer cylinder and only the inner cylinder contributes to the field inside the cylindrical shell.
That's correct. When you are in the space between the cylinders, only the inner cylinder contributes to the field (you can easily prove this and calculate the field with Gauss's law [tex]\oint E\cdot dA = \frac{q}{\epsilon _0}[/tex]). The field between the cylinders is anything but constant, and it weakens as you move away from the inner cylinder and towards the outer one.

So you are correct, the electric field does extend beyond the outer cylinder and some distance beyond where it becomes negligible.
I never said that (I hope). As I said above, there is no charge on the outer surface of the outer cylinder.* But more importantly, the net charge of the whole system is 0 (it was not charged to begin with, the cylinders were just 'polarized'). So if you look at it from the outside, both cylinders contribute the exact same field, but in opposite directions, making the net electric field outside the system 0.


*The reason for this is that the electric field inside the shell is 0, since it's conductive. So if you define a Gaussian space that includes the inside of the shell, the inner surface of it and the inner cylinder, the net charge of them should be zero. This means that the charge of the inner surface of the outer shell is equal (and opposite) to the charge of the inner cylinder, leaving no more charge to reside on the outer surface of the shell.
 

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