Any real function with continuous second partial derivatives which satisfies Laplace's equation,
(1)
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is called a harmonic function. Harmonic functions are called potential functions in physics and engineering. Potential functions are extremely useful, for example, in electromagnetism, where they reduce the study of a 3-component vector field to a 1-component scalar function. A scalar harmonic function is called a scalar potential, and a vector harmonic function is called a vector potential.
To find a class of such functions in the plane, write the Laplace's equation in polar coordinates
(2)
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and consider only radial solutions
(3)
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This is integrable by quadrature, so define ,
(4)
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(5)
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(6)
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(7)
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(8)
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(9)
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so the solution is
(10)
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Ignoring the trivial additive and multiplicative constants, the general pure radial solution then becomes
(11)
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(12)
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Other solutions may be obtained by differentiation, such as
(13)
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(14)
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(15)
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(16)
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and
(17)
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Harmonic functions containing azimuthal dependence include
(18)
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(19)
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The Poisson kernel
(20)
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is another harmonic function.