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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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APPLICATIONS OF COMPLEX VARIABLES25.17 Use the binomial theorem to exp<strong>and</strong>, in inverse powers of z, both the squareroot in the exponent <strong>and</strong> the fourth root in the multiplier, working to O(z −2 ).The leading terms are y 1 (z) =Ce −z2 /4 z ν <strong>and</strong> y 2 (z) =De z2 /4 z −(ν+1) . Stokes lines:arg z =0,π/2,π,3π/2; anti-Stokes lines: arg z =(2n +1)π/4 <strong>for</strong>n =0, 1, 2, 3. y 1is dominant on arg z = π/2 or3π/2.25.19 (a) i √ πe −z2 , valid <strong>for</strong> all z, including i √ π exp(β 2 ) in case (iii).(b) The same values as in (a). The (only) saddle point, at t 0 = z, is traversed inthe direction θ =+ 1 π in all cases, though the path in the complex t-plane varies2with each case.(c) The same values as in (a). The level lines are v = ±u. In cases (i) <strong>and</strong> (ii) thecontour turns through a right angle at the saddle point.All three methods give exact answers in this case of a quadratic exponent.25.21 Saddle points at t 1 = −z <strong>and</strong> t 2 =2z with f 1 ′′ = −18z <strong>and</strong> f′′ 2 =18z.Approximation is[( π) 1/2 cos(7νz 3 − 1 π) 4+ cos(20νz3 − 1 π)]4.9zν 1+z 2 1+4z 225.23 Saddle point at t 0 =cos −1 (ν/z) is traversed in the direction θ = − 1 4 π. F ν(z) ≈(2π/z) 1/2 exp [ i(z − 1 2 νπ − 1 4 π)]. 926

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