Dirichlet Integral

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Dirichlet Integral


(named for P. G. L. Dirichlet), the name of several types of integrals.

(1) The integral

This Dirichlet integral is also called the Dirichlet discontinous factor and is equal to π/2 for β < a, to β/4 for β = α, and to 0 for β > α. Thus, Dirichlet integral (1) is a discontinous function of parameters α and β. Dirichlet used the integral (1) in his studies of the attraction of ellipsoids. However, this integral appeared earlier in the works of J. Fourier, S. Poisson, and A. M. Legendre.

(2) The integral


is the so-called Dirichlet kernel. This Dirichlet integral is equal to the nth partial sum

of a Fourier series of the function f(x). Formula (2) is one of the most important formulas in the theory of Fourier series; in particular, it enabled Dirichlet to show that the Fourier series of a function with a finite number of maxima and minima converges at every point.

(3) The integral

References in periodicals archive ?
1) holds at every point, the boundary conditions are satisfied and the Dirichlet integral [[integral].
We have used as the velocity field of a fluid the functional form derived in Casuso (2007), obtained by studying the origin of turbulence as a consequence of a new description of the density distribution of matter as a modified discontinuous Dirichlet integral.
Sobel, Uppuluri, and Frankowski [77] tabulated, to 10D, the incomplete Dirichlet integral of Type 1:
Sobel, Uppuluri, and Frankowski [78] tabulated the incomplete Dirichlet integrals of Type 2:
Modulus of a quadrilateral and Dirichlet integrals.
begin with an introductory and comprehensive account of the theory of (symmetric) Dirichlet forms, which they explain as an axiomatic extension of the classical Dirichlet integrals in the direction of Markovian semigroups.