2. Consider a charged cylindrical conducting surface of arbitrary (not necessarily circu- lar) cross section. Use Gauss'

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2. Consider a charged cylindrical conducting surface of arbitrary (not necessarily circu- lar) cross section. Use Gauss'

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2 Consider A Charged Cylindrical Conducting Surface Of Arbitrary Not Necessarily Circu Lar Cross Section Use Gauss 1
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2. Consider a charged cylindrical conducting surface of arbitrary (not necessarily circu- lar) cross section. Use Gauss' law to show that, at the surface of the cylinder, the derivative of the electric field in the normal direction is JE E == al R where R is the (local) radius of curvature of the surface.
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