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WHY    FOURIER     SERIES? THE      FOURIER
                                                                            SERIES    OF   A  FUNCTION SINE       AND
                                        CHAPTER 13                          COSINE    SERIES    INTEGRATION AND
                                                                            DIFFERENTIATION

                                        Fourier Series
























                                        In 1807, Joseph Fourier submitted a paper to the French Academy of Sciences in competition for
                                        a prize offered for the best mathematical treatment of heat conduction. In the course of this work
                                        Fourier shocked his contemporaries by asserting that “arbitrary” functions (such as might specify
                                        initial temperatures) could be expanded in series of sines and cosines. Consequences of Fourier’s
                                        work have had an enormous impact on such diverse areas as engineering, music, medicine, and
                                        the analysis of data.



                            13.1        Why Fourier Series?

                                        A Fourier series is a representation of a function as a series of constant multiples of sine and/or
                                        cosine functions of different frequencies. To see how such a series might arise, we will look at a
                                        problem of the type that concerned Fourier.
                                           Consider a thin homogeneous bar of metal of length π, constant density and uniform cross
                                        section. Let u(x,t) be the temperature in the bar at time t in the cross section at x. Then (see
                                        Section 12.8.2) u satisfies the heat equation
                                                                                 2
                                                                          ∂u    ∂ u
                                                                            = k
                                                                          ∂t    ∂x  2
                                        for 0 < x <π and t > 0. Here k is a constant depending on the material of the bar. If the left and
                                        right ends are kept at temperature zero, then
                                                                  u(0,t) = u(π,t) = 0for t > 0.

                                        These are the boundary conditions. Further, assume that the initial temperature has been
                                        specified, say

                                                                   u(x,0) = f (x) = x(π − x).
                                        This is the initial condition.

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