flat ring

logistic_guy

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A flat ring of inner radius \(\displaystyle R_1\) and outer radius \(\displaystyle R_2\), carries a uniform surface charge density \(\displaystyle \sigma\). Determine the electric potential at points along the axis (the \(\displaystyle x\) axis).
 
The formula for the electric potential is \(\displaystyle V = k\frac{Q}{r}\).

Or

\(\displaystyle V = \int dV = \int k\frac{dQ}{r}\)

In the next post, we'll try to write \(\displaystyle dQ\) in terms of \(\displaystyle \sigma\).
 
Let us revisit our last integral.

\(\displaystyle \int k\frac{dQ}{r}\)

Here \(\displaystyle r\) is the distance from a point on the flat ring to a point on the \(\displaystyle x\)-axis (not along the radius of the ring, except at \(\displaystyle x = 0\)). I'll make a sketch to show you the idea.

flat_ring.png

If the blue color is a point on the flat ring, then \(\displaystyle r\) is the purple distance \(\displaystyle (h)\). I should have called it \(\displaystyle h\) (hypotenuse) instead.

So, the integral should be:

\(\displaystyle \int k\frac{dQ}{h}\)

From the sketch, \(\displaystyle h = \sqrt{x^2 + r^2}\), where \(\displaystyle r\) is the distance from the center of the ring to the blue point

Then, the integral becomes:

\(\displaystyle \int k\frac{dQ}{\sqrt{x^2 + r^2}}\)

\(\displaystyle \sigma = \frac{Q}{A} = \frac{dQ}{dA} = \frac{dQ}{2\pi r \ dr}\)

\(\displaystyle dQ = \sigma 2\pi r \ dr\)

Then,

\(\displaystyle \int k\frac{dQ}{\sqrt{x^2 + r^2}} = \int_{R_1}^{R_2} k\frac{\sigma 2\pi r \ dr}{\sqrt{x^2 + r^2}}\)

We are ready to integrate, and that's what we'll do in the next post.

💪😈
 
Last edited:
Let us continue.

\(\displaystyle \int_{R_1}^{R_2} k\frac{\sigma 2\pi r \ dr}{\sqrt{x^2 + r^2}} = k\sigma\pi\int_{x^2+R_1^2}^{x^2+R_2^2}\frac{1}{\sqrt{u}} \ du\)

Then,

\(\displaystyle V = 2k\sigma\pi\sqrt{u}\bigg|_{x^2+R_1^2}^{x^2+R_2^2} = 2k\sigma\pi\left(\sqrt{x^2+R_2^2} - \sqrt{x^2+R_1^2}\right)\)
 
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