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Gibbs phenomenon
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Gibbs phenomenon

The Gibbs phenomenon (also known as ringing artefacts) is the peculiar mode in which the Fourier series of a piecewise differentiable periodic function f behaves at a jump discontinuity: the nth partial sum of the Fourier series has large oscillations near the jump, which might increase the maximum of the partial sum above that of the function itself.

First observed by Albert Michelson via a mechanical graphing machine. Albert Michelson developed a device in 1898 that could compute and re-synthesize the Fourier series. The machine had faults when dealing with discontinuous functionss. When a square wave was inputed into the machine, the graph would move to and from around the discontinuities. This would occur, and continue to occur, as the number of Fourier coefficients approached infinity.

The phenomenon was first explained by J. Willard Gibbs in 1899.

Table of contents
1 See also
2 Publication
3 External links and references

See also

Publication

External links and references

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