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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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FOURIER SERIES12.21 Find the complex Fourier series <strong>for</strong> the periodic function of period 2π defined inthe range −π ≤ x ≤ π by y(x) =coshx. By setting x = 0 prove that∞∑ (−1) nn 2 +1 = 1 ( π)2 sinh π − 1 .n=112.22 The repeating output from an electronic oscillator takes the <strong>for</strong>m of a sine wavef(t) =sint <strong>for</strong> 0 ≤ t ≤ π/2; it then drops instantaneously to zero <strong>and</strong> startsagain. The output is to be represented by a complex Fourier series of the <strong>for</strong>m∞∑c n e 4nti .n=−∞Sketch the function <strong>and</strong> find an expression <strong>for</strong> c n .Verifythatc −n = c ∗ n.Demonstratethat setting t =0<strong>and</strong>t = π/2 produces differing values <strong>for</strong> the sum∞∑ 116n 2 − 1 .n=1Determine the correct value <strong>and</strong> check it using the result of exercise 12.20.12.23 Apply Parseval’s theorem to the series found in the previous exercise <strong>and</strong> soderive a value <strong>for</strong> the sum of the series17(15) + 652 (63) + 1452 (143) + ···+ 16n2 +12 (16n 2 − 1) + ··· .212.24 A string, anchored at x = ±L/2, has a fundamental vibration frequency of 2L/c,where c is the speed of transverse waves on the string. It is pulled aside at itscentre point by a distance y 0 <strong>and</strong> released at time t = 0. Its subsequent motioncan be described by the series∞∑y(x, t) = a n cos nπx nπctcosL L .n=1Find a general expression <strong>for</strong> a n <strong>and</strong> show that only the odd harmonics of thefundamental frequency are present in the sound generated by the released string.By applying Parseval’s theorem, find the sum S of the series ∑ ∞0 (2m +1)−4 .12.25 Show that Parseval’s theorem <strong>for</strong> two real functions whose Fourier expansionshave cosine <strong>and</strong> sine coefficients a n , b n <strong>and</strong> α n , β n takes the <strong>for</strong>m∫1 Lf(x)g ∗ (x) dx = 1 L 04 a 0α 0 + 1 ∞∑(a n α n + b n β n ).2n=1(a) Demonstrate that <strong>for</strong> g(x) =sinmx or cos mx this reduces to the definitionof the Fourier coefficients.(b) Explicitly verify the above result <strong>for</strong> the case in which f(x) =x <strong>and</strong> g(x) isthe square-wave function, both in the interval −1 ≤ x ≤ 1.12.26 An odd function f(x) ofperiod2π is to be approximated by a Fourier sine serieshaving only m terms. The error in this approximation is measured by the squaredeviation∫ [2 πm∑E m = f(x) − b n sin nx]dx.−πn=1By differentiating E m with respect to the coefficients b n , find the values of b n thatminimise E m .430

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