Q. Electric field at the centre of a uniformly charged semicircle of radius a is
Solution:
Electric field intensity at $O$ due to small elemental length $d l$ of charged ring,
$d E=\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{\lambda d l}{a^{2}}=\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{\lambda a d \theta}{a^{2}}$
$d E=\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{\lambda}{a} d \theta$
$\therefore $ Net electric field at centre $O$ is
$E=\int d E \sin \theta =\int_\limits{0}^{\pi} \frac{1}{4 \pi \varepsilon_{0}} \frac{\lambda}{a} \sin \theta d \theta$
$=\frac{\lambda}{4 \pi \varepsilon_{0} a}[-\cos \theta]_{0}^{\pi}$
$\therefore E=\frac{\lambda}{2 \pi \varepsilon_{0} a}$
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