释义 |
Fourier SeriesFourier series are expansions of Periodic Functions in terms of an infinite sum ofSines and Cosines
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Fourier series make use of the Orthogonality relationships of the Sine andCosine functions, which can be used to calculate the coefficients and in the sum. The computation andstudy of Fourier series is known as Harmonic Analysis.
To compute a Fourier series, use the integral identities
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where is the Kronecker Delta. Now, expand your function as an infinite series of the form
where we have relabeled the term for future convenience but set and left for . Assumethe function is periodic in the interval . Now use the orthogonality conditions to obtainandso
Plugging back into the original series then gives
for , 2, 3, .... The series expansion converges to the function (equal to the original function atpoints of continuity or to the average of the two limits at points of discontinuity)
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if the function satisfies the Dirichlet Conditions.
Near points of discontinuity, a ``ringing'' known as the Gibbs Phenomenon, illustrated above, occurs.For a function periodic on an interval , use a change of variables to transform the interval of integrationto . Let
Solving for , . Plugging this in gives
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If a function is Even so that , then is Odd. (This follows since is Odd and an Even Function times an OddFunction is an Odd Function.) Therefore, for all . Similarly, if a function is Odd so that , then is Odd. (This follows since isEven and an Even Function times an Odd Function is an Odd Function.) Therefore, for all .
Because the Sines and Cosines form a CompleteOrthogonal Basis, the Superposition Principle holds, and the Fourier series of alinear combination of two functions is the same as the linear combination of the corresponding two series. TheCoefficients for Fourier series expansions for a few common functions are given in Beyer (1987,pp. 411-412) and Byerly (1959, p. 51).
The notion of a Fourier series can also be extended to Complex Coefficients. Consider a real-valued function . Write
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Now examineso
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The Coefficients can be expressed in terms of those in the Fourier Series
For a function periodic in , these become
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These equations are the basis for the extremely important Fourier Transform, which is obtained by transforming froma discrete variable to a continuous one as the length .See also Dirichlet Fourier Series Conditions, Fourier Cosine Series, Fourier Sine Series, FourierTransform, Gibbs Phenomenon, Lebesgue Constants (Fourier Series), Legendre Series, Riesz-FischerTheorem References
Fourier TransformsArfken, G. ``Fourier Series.'' Ch. 14 in Mathematical Methods for Physicists, 3rd ed. Orlando, FL: Academic Press, pp. 760-793, 1985. Beyer, W. H. (Ed.). CRC Standard Mathematical Tables, 28th ed. Boca Raton, FL: CRC Press, 1987. Brown, J. W. and Churchill, R. V. Fourier Series and Boundary Value Problems, 5th ed. New York: McGraw-Hill, 1993. Byerly, W. E. An Elementary Treatise on Fourier's Series, and Spherical, Cylindrical, and Ellipsoidal Harmonics, with Applications to Problems in Mathematical Physics. New York: Dover, 1959. Carslaw, H. S. Introduction to the Theory of Fourier's Series and Integrals, 3rd ed., rev. and enl. New York: Dover, 1950. Davis, H. F. Fourier Series and Orthogonal Functions. New York: Dover, 1963. Dym, H. and McKean, H. P. Fourier Series and Integrals. New York: Academic Press, 1972. Folland, G. B. Fourier Analysis and Its Applications. Pacific Grove, CA: Brooks/Cole, 1992. Groemer, H. Geometric Applications of Fourier Series and Spherical Harmonics. New York: Cambridge University Press, 1996. Körner, T. W. Fourier Analysis. Cambridge, England: Cambridge University Press, 1988. Körner, T. W. Exercises for Fourier Analysis. New York: Cambridge University Press, 1993. Lighthill, M. J. Introduction to Fourier Analysis and Generalised Functions. Cambridge, England: Cambridge University Press, 1958. Morrison, N. Introduction to Fourier Analysis. New York: Wiley, 1994. Sansone, G. ``Expansions in Fourier Series.'' Ch. 2 in Orthogonal Functions, rev. English ed. New York: Dover, pp. 39-168, 1991.
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