espen180
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Homework Statement
Positive charge Q is uniformly distributed around a semicircle of radius a (See fig). Find the electric field (magnitude and direction) at the center of curvature P.
http://img132.imageshack.us/img132/8278/electricfield1.png
Homework Equations
Electric field of point charge:
\vec{E}=k\frac{Q}{r^2}
The Attempt at a Solution
Since I suspect the linear charge distribution \lambda=\frac{Q}{\pi a} will be troublesome to wirk with here, I will define the angular charge distribution \alpha=\frac{Q}{\pi}, divide the semicircle into infinitisimal pieces, calculate the electric field for each one and integrate.
Since each piece is a distance a away from point P, the electric field caused by each piece is dE=k\frac{dQ}{a^2}. dQ=\alpha d\theta=\frac{Q d\theta}{\pi}, so dE=k\frac{Qd\theta}{a^2\pi}.
By symmetry, the total electric field in the x-direction is zero, so I only have to find the field in the y-direction, which is given by dE_y=dE\cdot \sin \theta=\frac{kQ}{a^2\pi}\sin\theta d\theta.
Integrating from \theta=0 to \theta=\pi, the result is
E_y=\frac{kQ}{a^2\pi}\int_0^\pi \sin\theta d\theta=\frac{kQ}{a^2\pi}\left[-\cos\theta\right]_0^\pi=\frac{2kQ}{a^2\pi}.
Since Q is positive, the field is in the negative y-direction.
\vec{E_P}=-\frac{2kQ}{a^2\pi}\hat{j}
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