Electric Flux question [Surface integral]

AI Thread Summary
To find the electric flux through a non-conducting square plate with a charge 'Q' positioned above it, the discussion highlights the use of Gauss's law, which simplifies the calculation to φ = q/(6ε₀) for one surface of a cube. An alternative approach using surface integrals is explored, with the electric field expressed as a function of coordinates on the plate. The integral for flux is set up as φ = ∫ E·dS, but challenges arise in correctly accounting for the angle between the electric field and the differential area element dS. The discussion emphasizes the need to treat variables as constants during integration and to consider the varying angle of E relative to dS across the surface. The conversation concludes with the acknowledgment that this complexity complicates the integration process.
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Homework Statement


Q] A charge 'Q' is kept over a non-conducting square plate of side 'l' at a height l/2 over the center of the plate. Find the electric flux through the square plate surface. Neglect any induction that may occur.

Homework Equations



<br /> \phi = \int \overrightarrow{E}\cdot \overrightarrow{dS}<br />

The Attempt at a Solution



Well.. it was pretty simple to do using Gauss law. Just take a cube as the surface and then the flux will be equal from all surfaces.. so the flux through one surface would be \frac{q}{6\varepsilon_o}..

but i wanted to actually try a surface integral.. so I found out the Electric field as a function of the coordinates (x, y) on the square plate. Here, one of the corners is taken as the origin (0, 0):

<br /> E(x, y) = \frac{2Q\sqrt{(l - x)^2 + (l - y)^2}}{\pi \varepsilon_o \left[4(l - x)^2 + 4(l - y)^2 + l^2\right]^\frac{3}{2}}<br />

Also..

<br /> \phi = \int \overrightarrow{E}\cdot \overrightarrow{dS} = \int EdS\cos{\theta}<br />

and
<br /> dS = d(xy) = xdy + ydx<br />

so..

<br /> \phi = \int \overrightarrow{E}\cdot \overrightarrow{dS} = \int E(xdy + ydx)<br />

I have no idea how to go from here.

Any help will be appreciated. Thanks...
 
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Well you have two integrals there at the end, the integral of E*x*dy and the integral of E*y*dx, and you have that big expression for E in terms of x and y(which I only assume you did correctly)

Go nuts
 
blochwave said:
Well you have two integrals there at the end, the integral of E*x*dy and the integral of E*y*dx, and you have that big expression for E in terms of x and y(which I only assume you did correctly)

Go nuts

I get that.. but how do I solve E*x*dy? I mean.. while integrating the term with 'dy' do I take 'x' to be constant and vice versa for dx?
 
Yes...

Except the whole affair is going to be a little fishier than that because you have to take into account the angle between E and dS at every point. You smartly wrote E dot dS then ignored that in writing E(xdy+ydx), which would imply that the electric field and dS are always parallel, which is only true at one point; the one directly beneath the charge
 
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