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Distortion (mathematics)

In mathematics, the distortion is a measure of the amount by which a function from the Euclidean plane to itself distorts circles to ellipses. If the distortion of a function is equal to one, then it is conformal; if the distortion is bounded and the function is a homeomorphism, then it is quasiconformal. The distortion of a function ƒ of the plane is given by

which is the limiting eccentricity of the ellipse produced by applying ƒ to small circles centered at&nbsp;z. This geometrical definition is often very difficult to work with, and the necessary analytical features can be extrapolated to the following definition. A mapping ƒ&nbsp;:&nbsp;Ω&nbsp;→&nbsp;R<sup>2</sup> from an open domain in the plane to the plane has finite distortion at a point x&nbsp;∈&nbsp;Ω if ƒ is in the Sobolev space W(Ω,&nbsp;R<sup>2</sup>), the Jacobian determinant J(x,ƒ) is locally integrable and does not change sign in Ω, and there is a measurable function K(x)&nbsp;≥&nbsp;1 such that

almost everywhere. Here Df is the weak derivative of ƒ, and |Df| is the Hilbert–Schmidt norm.

For functions on a higher-dimensional Euclidean space R<sup>n</sup>, there are more measures of distortion because there are more than two principal axes of a symmetric tensor. The pointwise information is contained in the distortion tensor

The outer distortion K<sub>O</sub> and inner distortion K<sub>I</sub> are defined via the Rayleigh quotients

The outer distortion can also be characterized by means of an inequality similar to that given in the two-dimensional case. If Ω is an open set in R<sup>n</sup>, then a function has finite distortion if its Jacobian is locally integrable and does not change sign, and there is a measurable function K<sub>O</sub> (the outer distortion) such that

almost everywhere.

See also

References

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