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

AI Thread Summary
The discussion focuses on calculating the electric potential of a square plate using integrals. The initial approach involves a double integral in Cartesian coordinates, but participants find it complex and consider switching to polar coordinates for simplification. However, the polar coordinate method complicates the integration further, leading to difficulties in solving the integral. A suggestion is made to reduce the problem to a one-dimensional integral by referencing a known solution for the potential above a line of charge. Ultimately, a potential expression is derived, which appears to be correct based on limits evaluated.
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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