A conductor of resistivity ρ and resistance R, as shown in the figure, is connected across a battery of mf V. Its radius varies from 'a' at left end to 'b' at right end. The electric field at a point P at distance x from left end of it is:
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E = jr [j = current density]
j = [r = radius of c.s. at distance 'x' from left end]
Hence,
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