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1) For a point charge, the E-field is proportional to the charge q and inversely proportional to the distance r squared. The potential V is proportional to q and inversely proportional to r. 2) For a uniformly charged rod, the E-field is proportional to the linear charge density λ and inversely proportional to the distance. The potential is proportional to λ and the logarithm of the distance. 3) For a uniformly charged thin disk, the E-field is proportional to the surface charge density σ and inversely

Author

Michael Barker

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