Fourier series serve many useful purposes, as manipulation and conceptualization of the modal coefficients are often easier than with the original function. Areas of application include electrical engineering, vibration analysis, acoustics, optics, signal and image processing, and data compression. Using the tools and techniques of spectroscopy, for example, astronomers can deduce the chemical composition of a star by analyzing the frequency components, or spectrum, of the star's emitted light. Similarly, engineers can optimize the design of a telecommunications system using information about the spectral components of the data signal that the system will carry. See alsospectrum analyzer.
The Fourier series is named after the French scientist and mathematician Joseph Fourier, who used them in his influential work on heat conduction, Théorie Analytique de la Chaleur (The Analytical Theory of Heat), published in 1822.
The form for period T can be easily derived from the canonical one with the change of variable defined by . Therefore, both formulations are equivalent. However, the form for period T is used in most practical cases because it is directly applicable. For the theory, the canonical form is preferred because it is more elegant and easier to interpret mathematically, as will later be seen.
Modern derivation of the Fourier coefficients
The method used by Fourier to derive the coefficients of the series is very practical and well-suited to the problem he was dealing with (heat propagation). However, this method has since been generalized to a much wider class of problems: writing a function as a sum of periodic functions.
More precisely, if f:R → C is a function, we would like to write this function as a sum of trigonometric functions, i.e. . We have to restrict our choice of functions in order for this to make sense. First of all, if f has period T, then by changing variables, can study which has period 2π. This simplifies notations a lot and allows us to use a canonical (standard) form. We can restrict the study of to any interval of length 2π, [-π,π], say.
We will take the functions f:R → C in the set of piecewise continuous, 2π periodic functions with . Technically speaking, we are in fact taking functions from the Lp spaceL2(μ), where μ is the normalized Lebesgue measure of the interval [-π,π] (i.e. such that .
Fourier series take advantage of the periodicity of a function f but what if f is periodic in more than one variable, or for that matter, what if f is not periodic? These problems led mathematicians and theoretical physicists to try to define Fourier series on any group G. The advantage of this is that it allows us, for example, to define Fourier series for functions of several variables. Fourier series and Fourier transforms usually used in signal processing then become special cases of this theory and are easier to interpret.
If G is a locally compact Abelian group and T is the unit circle, we can define the dual of G by . This is the set of rotations on the unit circle and its elements are called characters. We can define a scalar product on C[G] by: . is then an orthonormal basis of C[G] with respect to this scalar product. Let f :G → C. The Fourier coefficients of f are defined by: and we have . If the group is discrete, then the integral reduces to an ordinary sum.
For example, the Fourier series of this article are obtained by taking G=R/2πZ. We get
Periodic functions in n dimensions can be defined on an n-dimensional torus (the function taking a value at each point on the torus). Such a torus is defined by Tn=Rn/(2πZ)n. For n=1 we get a circle, for n=2 the cartesian product of two circles, i.e. a torus in the usual sense. Choosing G=Tn gives the corresponding Fourier series.
Approximation and convergence of Fourier series
It is clear that this expression is minimum for and for this value only.
This means that there is one and only one such that
it is given by
This means that the best approximation of f we can make using only the functions for n from to N is precisely the Nth partial sum of the Fourier series. An illustration of this is given on the animated plot of example 1.
While the Fourier coefficientsan and bn can be formally defined for any function for which the integrals make sense, whether the series so defined actually converges to f(x) depends on the properties of f.
This is convergence in the norm of the space L2. The proof of this result is simple, unlike Lennart Carleson's much stronger result that the series actually converges almost everywhere.
There are many known tests that ensure that the series converges at a given point x, for example, if the function is differentiable at x. Even a jump discontinuity does not pose a problem: if the function has left and right derivatives at x, then the Fourier series will converge to the average of the left and right limits (but see Gibbs phenomenon). However, a fact that many find surprising, is that the Fourier series of a continuous function need not converge pointwise.
This unpleasant situation is counter-balanced by a theorem by Dirichlet which states that if f is -periodic and piecewise continuously differentiable function, then its Fourier series converges pointwise and , where and . If f is continuous as well as piecewise continuously differentiable, then the Fourier series converges uniformly.
Joseph Fourier, translated by Alexander Freeman (published 1822, translated 1878, re-released 2003). The Analytical Theory of Heat. Dover Publications. ISBN0-486-49531-0. Check date values in: |year= (help) 2003 unabridged republication of the 1878 English translation by Alexander Freeman of Fourier's work Théorie Analytique de la Chaleur, originally published in 1822.
Yitzhak Katznelson, An introduction to harmonic analysis, Second corrected edition. Dover Publications, Inc., New York, 1976. ISBN0-486-63331-4
Felix Klein, Development of mathematics in the 19th century. Mathsci Press Brookline, Mass, 1979. Translated by M. Ackerman from Vorlesungen über die Entwicklung der Mathematik im 19 Jahrhundert, Springer, Berlin, 1928.
Walter Rudin, Principles of mathematical analysis, Third edition. McGraw-Hill, Inc., New York, 1976. ISBN0-07-054235-X
William E. Boyce and Richard C. DiPrima, Elementary Differential Equations and Boundary Value Problems, Eighth edition. John Wiley & Sons, Inc., New Jersey, 2005. ISBN0-471-43338-1