A total charge q is distributed uniformly along a straight rod of length l the potential at point p
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see figure, seperation between straight rod and point P is h.
cut an elementary length of straight rod of thickness dx at x distance from the midpoint of it.
so, charge on element, dq = (q/L)dx
potential at point P , V = Kdq/√(x² + h²)
= K(q/L)
we know, ∫dx/(x² + a²) = ln(x + √(x² + a²) + C
so, V = k(q/L)
= k(q/L)[ln{L/2 + √(L² + 4h²)/2 } - ln{-L/2 + √(L² + 4h²)/2}]
= kq/L ln[ {L + √(L² + 4h²)}/{-L+√(L² + 4h²)}]
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A total charge Q is distributed uniformly along a straight rod of Length L. The potential at a point P at a distance h from the midpoint of the rod is (Hint: ∫x2+a2 1dx=ln(x+x2+a2 ))
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