thenewbosco
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A rod of length L lies along the x-axis with the left end at the origin. It has non-uniform charge density given by \lambda = \alpha x. where \alpha is a positive constant. Calculate the potential at a position A, which is a distance d to the left of the origin.
Here is what i did:
we have dV = \frac{k_e dq}{r}
then i made use of the \lambda = \alpha x
and we have V=\int\frac{k_e\lambda dx}{x} = \int\frac{k_e\alpha x dx}{x} = k_e\alpha (d+L-d) where my limits of integration were L to d+L in the second integral
however the answer provided says that V=k_e\alpha (L-d ln(1 + \frac{L}{d}).
where did i go wrong?
thanks
Here is what i did:
we have dV = \frac{k_e dq}{r}
then i made use of the \lambda = \alpha x
and we have V=\int\frac{k_e\lambda dx}{x} = \int\frac{k_e\alpha x dx}{x} = k_e\alpha (d+L-d) where my limits of integration were L to d+L in the second integral
however the answer provided says that V=k_e\alpha (L-d ln(1 + \frac{L}{d}).
where did i go wrong?
thanks
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