Any real function with continuous second partial
derivatives which satisfies Laplace's equation,
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(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
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(2)
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and consider only radial solutions
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(3)
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This is integrable by quadrature, so define ,
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(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
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(10)
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Ignoring the trivial additive and multiplicative constants, the general pure radial solution then becomes
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(11)
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(12)
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Other solutions may be obtained by differentiation, such as
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(13)
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(14)
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(15)
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(16)
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and
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(17)
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Harmonic functions containing azimuthal dependence include
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(18)
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(19)
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The Poisson kernel
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(20)
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is another harmonic function.