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E14M.2 Consider a conductor with excess charge on its surface, and consider a patch of that conductors surface that is small enough so that we can approximate it as being flat (a) Argue using the results of chapter E3 the conductors surface must be perpendicular to that surface Use Gausss law in integral form to prove that l E-σ eo Just outside the conductor, where σ is the local charge per unit area. (Hint: Consider a small gaussian surface with two faces parallel to the surface, one just barely inside and one just barely outside.) that the electric field E produced by the conductors surface charge at points just barely outside (b)

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no Not ct l た Co

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