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So, I'm trying to solve this problem for my assignment,

A point of charge, Q = 3 nC, is located at the origin of a cartesian coordinate system. What flux crosses the portion of the z=2 m plane for which -4 $\le$ x $\le$ 4 m and -4 $\le$ y $\le$ 4 m

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I'm thinking this question can be solved by using this equation $$\Psi = \oint \mathbf{D} \cdot d\mathbf{S}$$ because the limits of the integration are already known from the problem

but I don't understand how I can get the D of this question. Am I using the wrong formula? can someone clear this out for me? Thanks.

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  • $\begingroup$ There are two things that need sorting out. Are you looking for electric field flux or displacement field flux? By context I think you are looking for displacement field flux. If you can't think of a way to calculate ${\bf D}$ directly, perhaps you can find it another way. You would have to make the reasonable assumption that the problem lies in a vacuum. $\endgroup$
    – garyp
    Commented Sep 14, 2021 at 17:35
  • $\begingroup$ Say you considered vacuum. Then the equation would be $\Psi = \oint \vec{E}\cdot \vec{da}$. Assume small area $dxdy$ on the plane. This area points in the $z$ direction. Calculate $\vec{E}$ for some general point $(x, y, z_0)$. Evaluate the flux $\oint Eda\cos\theta$ involving double integrals with the limits for $x$ and $y$ given. $\endgroup$ Commented Sep 14, 2021 at 17:41
  • $\begingroup$ If it were the $z=4$ m plane it would be so easy! $\endgroup$ Commented Sep 14, 2021 at 18:49

1 Answer 1

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Consider some point $(x,y)$ on the surface of interest. The distance of that point to the origin is $R=\sqrt{x^2+y^2+2^2}$. The angle of elevation for the vector that connects the point $(x, y)$ to the origin is $\theta=\cos^{-1}(\frac{2}{R})$

We know the Electric Field at the point $(x,y)$ will given by:

$$\vec{E}=\frac{kQ}{|\vec{R}|^2}\frac{\vec{R}}{|\vec{R}|}$$

And so:

$$\vec{E} \cdot \hat{n}=\frac{kQ}{|\vec{R}|^2}\Big(\frac{\vec{R}}{|\vec{R}|} \cdot \hat{n}\Big)=\frac{kQ}{|\vec{R}|^2}\cos(\theta)=\frac{kQ}{|\vec{R}|^2}\frac{2}{|\vec{R}|}=\frac{2kQ}{(x^2+y^2+2^2)^{3/2}}$$

From there we find the value of flux through the surface to be:

$$\Phi_E=\int_{-4}^4 \int_{-4}^4 \frac{2kQ}{(x^2+y^2+2^2)^{3/2}} dxdy$$

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