Electrical Potential of a Uniformly Charged Ring

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SUMMARY

The discussion focuses on calculating the electric potential of a uniformly charged disk with an inner radius \( R_{in} \) and an outer radius \( R_{out} \). The correct approach involves integrating the contributions from small rings of charge, leading to the final expression for the potential at a distance \( z \) from the center: \( V=\frac{Q*(\sqrt{R_{out}^2+z^2}-\sqrt{R_{in}^2+z^2})}{2*\pi*\epsilon_0*(R_{out}^2-R_{in}^2)} \). The initial incorrect assumptions about substituting the radii directly were clarified, emphasizing the need for integration to account for the varying radius of the disk.

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  • Understanding of electric potential and charge distributions
  • Familiarity with calculus, specifically integration techniques
  • Knowledge of the formula for electric potential due to a ring
  • Concept of surface charge density and its calculation
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Gramma2005
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I am stuck on this problem:

A disk with a hole has inner radius R_in and outer radius R_out. The disk is uniformly charged with total charge Q. Find an expression for the on-axis electric potential at distance z from the center of the disk.

I started this problem by looking at the electric potential of a ring, which is:
V=\frac{kQ}{\sqrt{R^2+z^2}}

So then if it varies in the thickness of the ring, would it be reasonable to have it be:
V=\frac{kQ}{\sqrt{(R_{out}-R_{in})^2+z^2}}

Or would I need to use the equation for the electric potential of a uniformly charged disk with radius R_out, then subtract the electric potential of the inner disk of radius R_in.

Thanks for your help!

P.S. Hope I did the LaTeX right
 
Last edited:
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Gramma2005 said:
I am stuck on this problem:

A disk with a hole has inner radius R_in and outer radius R_out. The disk is uniformly charged with total charge Q. Find an expression for the on-axis electric potential at distance z from the center of the disk.

I started this problem by looking at the electric potential of a ring, which is:
V=\frac{kQ}{\sqrt{R^2+z^2}}

So then if it varies in the thickness of the ring, would it be reasonable to have it be:
V=\frac{kQ}{\sqrt{(R_{out}-R_{in})^2+z^2}}

No, that is not correct. You can't just substitute R_in and R_out.
One way of doing this, is finding the contribution of a small ring and integrating to get the contribution of the disc.
 
Would it be something more like this?:

V=\frac{2Q}{(R_{out}-R_{in})^2}*\int_{R_{in}}^{R_{out}}\frac{dx}{2*\sqrt{x}}

I'm not sure if this is the right integral for the equation?
 
Last edited:
Gramma2005 said:
Would it be something more like this?:

V=\frac{2Q}{(R_{out}-R_{in})^2}*\int_{R_{in}}^{R_{out}}\frac{dx}{2*\sqrt{x}}

I'm not sure if this is the right integral for the equation?

No, that's not right.

First, consider a small ring of thickness dr with a radius of r.

Now, what is the potential due to this ring at point at a height 'z' at the axis? It is,

V=\frac{kdQ}{\sqrt{r^2+z^2}}

where, dQ is the small charge on the ring. How do you find this dQ?
You can find the uniform surface charge density \sigma from the question right? (Hint:Total charge/Total area). Since the ring has a small thickness dr, the small area will be 2 \pi r dr. From this, you can find the charge "dQ" on the small ring.

How do you find the potential of the disc? Notice that, if you sum the contributions of such small rings, you will get the potential of the disc. So you integrate the contribution the small ring where the radius varies from r_{in} to r_{out}

Can you put this in mathematical equations and post the answer here?
 
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Alright, I see how it works now, thanks so much for the help. The final solution is:

V=\frac{Q*(\sqrt{R_{out}^2+z^2}-\sqrt{R_{in}^2+z^2})}{2*\pi*\epsilon_0*(R_{out}^2-R_{in}^2)}
 
Last edited:

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