Biot–Tolstoy–Medwin diffraction model

In applied mathematics, the Biot–Tolstoy–Medwin (BTM) diffraction model describes edge diffraction. Unlike the uniform theory of diffraction (UTD), BTM does not make the high frequency assumption (in which edge lengths and distances from source and receiver are much larger than the wavelength). BTM sees use in acoustic simulations.[1]

Impulse response

The impulse response according to BTM is given as follows:[2]

The general expression for sound pressure is given by the convolution integral

where represents the source signal, and represents the impulse response at the receiver position. The BTM gives the latter in terms of

as an integral over edge positions

where the summation is over the four possible choices of the two signs, and are the distances from the point to the source and receiver respectively, and is the Dirac delta function.

where

See also

Notes

  1. Calamia 2007, p. 182.
  2. Calamia 2007, p. 183.

References


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