hitemup
- 81
- 2
Homework Statement
[/B]
Charge is distributed uniformly over a large square plane of side l, as shown in the figure. The charge per unit area (C/m^2) is [itex]\sigma[/itex]. Determine the electric field at a point P a distance z above the center of the plane, in the limit [itex]l \to \infty[/itex].
[Hint: Divide the plane into long narrow strips of width dy, and use the result of Example 11]
Homework Equations
[/B]
Result of Example 11: [itex]\frac{2k\lambda }{x}[/itex] (electric field at a distance x due to an infinitely long wire)(that point is symmetric about the x-axis, so there is no y component of the electric field.)
[tex]k = \frac{1}{4\pi\epsilon_0}[/tex]
The Attempt at a Solution
Charge densities:
[tex]\sigma = \frac{dq}{dy*l}[/tex] (an infinitely small q over an infinitely small surface)
[tex]\lambda = \frac{dq}{l}[/tex] (total charge of the strip / total length)
[tex]dE = \frac{2k\lambda}{\sqrt{y^2+z^2}}[/tex]
(electric field due to a long strip)
[tex]dE_z = dE sin\theta = \frac{2k\lambda y}{{(y^2+z^2)}^{3/2}}[/tex]
(its z component is what we need)
[tex]dE_z = dE sin\theta = \frac{2k\sigma y}{{(y^2+z^2)}^{3/2}}dy[/tex]
(dy is necessary, so replace lambda with sigma)
The following is what I get after the integration,
[tex]{-2\sigma k} \frac{1}{\sqrt {y^2+z^2}}[/tex]
The limits are zero and infinity, so I end up with;
[tex]\frac{2\sigma k}{z}[/tex]
There is an example of uniformly charged disk in my textbook. The formula for electric field for that disk does not depend on the distance. That's why I believe I've done this question wrong. What do you think about my solution? I am not sure if I wrote charge densities correct, so that may be the mistake.
Last edited: