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3. Basic Principles of Electrostatics
Electrostatics is concerned with three functions, (x), E(x), and V(x). To proceed to the next few chapters one must comprehend the six relations among these three functions. For each pair of functions there is an integral formula and a partial differential equation. (In the integrals for E and V, r is the distance from the source point x’ to the field point x, and dV’= d3x’ is the elemental volume at the source point.) G L Pollack and D R Stump Electromagnetism
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Use of Gauss’s Theorem (Figure 3.8)
By Gauss’s theorem, the flux of E through a closed surface S is equal to Q/0 where Q is the charge enclosed. For a charge distribution with spherical, cylindrical or planar symmetry, E(x) can be determined. For spherical symmetry, apply Gauss’s theorem to a spherical surface around the center of symmetry; the flux of E is Er(r)4 r2. For cylindrical symmetry use a cylindrical gaussian surface around the line of symmetry; the flux of E is Er(R)2 Rh. For planar symmetry use a cylindrical gaussian surface with the end-caps at equal distances above and below the plane of symmetry; the flux of E is 2Ez(z) A. G L Pollack and D R Stump Electromagnetism
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