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Integral Theorems and Distributions

In classical mechanics and electrod)mamics the integral theorems of Gauss and Stokes may often be employed beneficially. Given a sufficiently smooth (i.e., differentiable) and well-behaved vector field A, Gauss theorem may be expressed in its most elementary form as [Pg.635]

Here a again denotes the outer normal unit vector perpendicular to the surface S. Eq. (A.20) is sometimes also referred to as the curl theorem. [Pg.635]

In discussions of the Coulomb potential the following relations are often useful. The gradients of a distance between two positions, r and r, read [Pg.636]

The indices in Eq. (A.21) label the variable with respect to which the derivative is taken. We note that the proof of Eq. (A.24) is only trivial for r — r 0 for which the right-hand side becomes zero. In this case, where r /, we may simply differentiate the inverse distance and obtain this result right away. [Pg.636]


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