Introduction to the Theory of Fouriers Series And Integrals
Introduction to the Theory of Fouriers Series And Integrals
H S Horatio Scott Carslaw
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I / I X] : ' (I, ''. Jo sin x Jo SIII. T Jo sin. ' 1 Using (i), the result follows, (iii) If f(x) is bounded and monotonic increasing, but not positive all the time, by adding a constant we can make it positive, and proceed as in (ii) ; and a similar remark applies to the case of the monotonic decreasing function, (iv) When f(x) is bounded and the interval can be broken up into a finite number of open partial intervals in which it is monotonic, the result follows from (i)-(iii). (v) And if f(x)... has a finite number of points of infinite discontinuity, as stated in the second of Dirichlet's Conditions, so far as these points are concerned the proof is similar to that given above. 95. Proof of the Convergence of Fourier's Series. In the opening sections of this chapter we have given the usual elementary, but quite incomplete, argument, by means of which the coefficients in the expansion f(x) = a + (a l cos x + ^ sin x) + (a 2 cos % x + b 2 sin 2x) + . . . Are obtained. We now return to this question, which we approach in quite a different way.
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