How Do You Calculate the Electric Potential of a Square Plate?

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Homework Help Overview

The discussion revolves around calculating the electric potential of a square plate using integrals. Participants are exploring the mathematical formulation and integration techniques relevant to the problem, which falls under the subject area of electrostatics.

Discussion Character

  • Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to set up a double integral for electric potential but struggles with the calculation. Some participants suggest using polar coordinates, while others argue for the appropriateness of Cartesian coordinates given the square region of integration. There are also discussions about simplifying the integral and references to related problems involving line charges.

Discussion Status

Participants are actively engaging with the mathematical aspects of the problem, questioning the use of coordinate systems, and exploring different integration techniques. Some have provided partial results and insights, but there is no explicit consensus on the best approach yet.

Contextual Notes

There are mentions of specific integrals and potential simplifications, as well as references to known problems in introductory physics that may relate to the current problem. The complexity of the integrals involved and the nature of the square plate's geometry are noted as potential challenges.

Hamal_Arietis
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Homework Statement
Find the electric potential at a height d above the center of a square sheet
(side 2a) carrying a uniform surface charge σ.
Relevant Equations
[tex] σdS=σdxdy[/tex]
[tex] V=\int \frac{\sigma dS}{r}[/tex]
I found out the equation of electric potential, that is
V=\int_{-a}^a \int_{-a}^{a} \frac{σdxdy}{4 \pi \epsilon_0\sqrt{x^2+y^2+d^2}}=\int_{0}^a \int_{0}^{a} \frac{σdxdy}{\pi \epsilon_0\sqrt{x^2+y^2+d^2}}

but I couldn't calculate the integral.

It seems convenient if we use the polar coordinate, that is, assume that
x=rcos\theta, y=rsin\theta
then
\frac{\pi\epsilon_0 V}{\sigma}=\int_{0}^{\pi/4} \int_{0}^{\frac{a}{cos\theta}} \frac{rdrd\theta}{\sqrt{r^2+d^2}}+\int_{\pi/4}^{\pi/2} \int_{0}^{\frac{a}{sin\theta}} \frac{rdrd\theta}{\sqrt{r^2+d^2}}

But I find it difficult to calculate.
I also think another method that is find the electric field $$\vec E$$ then
V=\int \vec E \vec dl

but it seems hard to integrate too .
 
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Perhaps the double integral is obscuring it.
Could you solve ##\int\frac{dx}{\sqrt{x^2+c^2}}##?
 
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haruspex said:
Perhaps the double integral is obscuring it.
Could you solve ##\int\frac{dx}{\sqrt{x^2+d^2}}##?
$$\int\frac{dx}{\sqrt{x^2+d^2}}=log |x+\sqrt{x^2+d^2}|+C$$

but my fomular is
$$ \int\frac{rdr}{\sqrt{r^2+d^2}}=\sqrt{r^2+d^2} +C$$

the problem is when I replace ##r=\frac{a}{cos\theta}##, the integral became more complicated.
the double integral became
$$\int_0^{\frac{\pi}4} (\sqrt{\frac{a^2}{cos^2\theta}+d^2}-d)d\theta$$
 
I don't think its good idea to involve polar coordinates because the region of integration is a square ##[0,a]\times[0,a]## in the plane z=0 (xy plane). So i believe cartesian coordinates are just fine.

However when i tried this integral at wolfram i get a not so simple expression
https://www.wolframalpha.com/input/?i=integral+1/sqrt(x^2+y^2+d^2)dxdy

The first step (integration with respect to x or y) should be easy and I see haruspex post is toward this direction.

$$\int \frac{dx}{\sqrt{x^2+y^2+d^2}}=\ln {|x+\sqrt{x^2+y^2+d^2}|}+c=f(y)$$

The second step $$\int f(y) dy$$ is where I guess difficulties rise and it doesn't have a nice simplified expression.
 
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Have you solved for the potential a distance ##d## above the center of a line of charge of length ##L##? It's a pretty commonly covered problem in intro physics. You can use that result and reduce this problem to a one-dimensional integral.
 
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vela said:
Have you solved for the potential a distance ##d## above the center of a line of charge of length ##L##? It's a pretty commonly covered problem in intro physics. You can use that result and reduce this problem to a one-dimensional integral.
Hasn't that been achieved in the first line of post #3?
 
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I tried it. And I found the answer. by considering ##d=d_0## as the potential origin. The potential is
$$V=\frac{\sigma}{\pi\epsilon_0}(a\log{(\frac{d_0^2+a^2}{d^2+a^2}})^\frac{1}{2}+d_0\tan^{-1}(\frac{a}{d_0})-d\tan^{-1}(\frac{a}{d}))$$

It seems correct because when I calculate the limit of V when ##a## into infinite, then
$$V=\frac{\sigma}{2\epsilon_0}(d_0-d)$$

Thanks for helping
vela said:
Have you solved for the potential a distance ##d## above the center of a line of charge of length ##L##? It's a pretty commonly covered problem in intro physics. You can use that result and reduce this problem to a one-dimensional integral.
 
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