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Following the same argument as in Problem 3.54, we can treat the infinite conducting plane as a plane mirror. Hence, for each charge and equal and opposite image charge appears at the other end of the conducting plane as shown in the figure.
a)
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There are three forces acting on the positive charge q as shown in the figure. The attactive forces F2 and F1 from the real and the image negative charges located at distances l each and the repulsive force F3 from the image charge located diagonally. The net force is given by,
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b)
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The electric field at the mid point of the two charges can be obtained by considering the electric field due to all the four charges - the two real charges and the two image charges. This is given by,
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