The method is applied to oscillatory definite integrals in the form:
where is a relatively slowly-varying function and is either sine or cosine or a complex exponential that causes the rapid oscillation of the integrand, particularly for high frequencies. In Filon quadrature, the is divided into subintervals of length , which are then interpolated by parabolas. Since each subinterval is now converted into a Fourier integral of quadratic polynomials, these can be evaluated in closed-form by integration by parts. For the case of , the integration formula is given as:[1][2]
where
Explicit Filon integration formulas for sine and complex exponential functions can be derived similarly.[2] The formulas above fail for small values due to catastrophic cancellation;[3]Taylor series approximations must be in such cases to mitigate numerical errors, with being recommended as a possible switchover point for 44-bit mantissa.[2]
^ abFilon, L. N. G. (1930). "III.—On a Quadrature Formula for Trigonometric Integrals". Proceedings of the Royal Society of Edinburgh. 49: 38–47. doi:10.1017/S0370164600026262.
^Domínguez, V.; Graham, I. G.; Smyshlyaev, V. P. (2011). "Stability and error estimates for Filon–Clenshaw–Curtis rules for highly oscillatory integrals". IMA Journal of Numerical Analysis. 31 (4): 1253–1280. doi:10.1093/imanum/drq036.
^Červený, Vlastislav; Ravindra, Ravi (1971). Theory of Seismic Head Waves. University of Toronto Press. pp. 287–289. ISBN9780802000491.
^Thouless, M. D.; Evans, A. G.; Ashby, M. F.; Hutchinson, J. W. (1987). "The edge cracking and spalling of brittle plates". Acta Metallurgica. 35 (6): 1333–1341. doi:10.1016/0001-6160(87)90015-0.