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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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NUMERICAL METHODSother exact expressions are possible, e.g. the integral of f(x i + y) over the range0 ≤ y ≤ h, but we will find (27.35) the most useful <strong>for</strong> our purposes.Although the preceding discussion has implicitly assumed that both of thelimits a <strong>and</strong> b are finite, with the consequence that N is finite, the general methodcan be adapted to treat some cases in which one of the limits is infinite. It issufficient to consider one infinite limit, as an integral with limits −∞ <strong>and</strong> ∞ canbe considered as the sum of two integrals, each with one infinite limit.Consider the integralI =∫ ∞af(x) dx,where a is chosen large enough that the integr<strong>and</strong> is monotonically decreasing<strong>for</strong> x>a<strong>and</strong> falls off more quickly than x −2 . The change of variable t =1/xconverts this integral into∫ 1/a( )1 1I =0 t 2 f dt.tIt is now an integral over a finite range <strong>and</strong> the methods indicated earlier can beapplied to it. The value of the integr<strong>and</strong> at the lower end of the t-range is zero.In a similar vein, integrals with an upper limit of ∞ <strong>and</strong> an integr<strong>and</strong> that isknown to behave asymptotically as g(x)e −αx ,whereg(x) is a smooth function, canbe converted into an integral over a finite range by setting x = −α −1 ln αt. Again,the lower limit, a, <strong>for</strong> this part of the integral should be positive <strong>and</strong> chosenbeyond the last turning point of g(x). The part of the integral <strong>for</strong> x

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