Let f ( t ) = 0 ∫ π sin ( t sin ( 4 π ) sin x ) sinh ( t sin ( 4 π ) sin x ) d x
Then, L { f ( t ) } ( s ) = ( s B + C ) D / E A π K sin ( G F tan − 1 ( s J H ) )
Evaluate A + B + C + D + E + F + G + H + J + K
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damn goood ... salute !!!!
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Salute isn't good enough. Mark Hennings is the best user in Brilliant, you need to print and frame this solution!
In your working in fifth line, For your integral of … = ∫ 0 π s 4 + sin 4 x sin 2 x d x = … how do you know when to use contour integration? I tried hacking it through various integration tricks like geometric series, Half tangent substitution, and many others, and I gave up. WolframAlpha also gave a seemingly wonky answer, so I thought there's no closed form.
Is there an indication on when to know it's suitable/easiest to use contour integration? (Treat me like I'm bad in contour integrals, hence my reluctance to use it)
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It is difficult to give a general rule about that. If an integral can be expressed as the integral over R of a rational function, then the "sum of residues in the upper half plane" trick works well, provided that you can factorise the denominator.
There are a variety of standard tricks for converting integrals of rational expressions of trigonometric functions into the above form. One is a t = tan 2 1 x substitution, but this would have created an order 8 polynomial in the denominator, and that was too big for me! After a bit of playing around, I came up with the t = cot x substitution.
Another approach to this sort of integral is to try the complex substitution z = e i x , which converts integrals of rational functions of trigonometric functions between 0 and 2 π into integrals of rational functions around the unit circle (in which case we need to add the residues at poles of modulus less than 1 ).
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Since cosh ( x + i y ) = cosh x cos y + sinh x sin y , we see that f ( t ) = I m ( ∫ 0 π cosh ( 2 1 + i t sin x ) d x ) and hence ( L f ) ( s ) = = = = = = ∫ 0 ∞ I m ( ∫ 0 π cosh ( 2 1 + i t sin x ) d x ) e − s t d t 2 1 I m ( ∫ 0 π ∫ 0 ∞ ( e 2 1 + i t sin x + e − 2 1 + i t sin x ) e − s t d t d x ) 2 1 I m ( ∫ 0 π ( s − 2 1 + i sin x 1 + s + 2 1 + i sin x 1 ) d x ) I m ∫ 0 π s 2 − i sin 2 x s d x = s ∫ 0 π s 4 + sin 4 x sin 2 x d x = s ∫ 0 π s 4 c o s e c 4 x + 1 c o s e c 2 x d x s ∫ R s 4 ( t 2 + 1 ) 2 + 1 1 d t = s 3 1 ∫ R ( t 2 + 1 + i s − 2 ) ( t 2 + 1 − i s − 2 ) 1 d t s 3 1 ∫ R ( t 2 + sec θ e i θ ) ( t 2 + sec θ e − i θ ) 1 d t where θ = tan − 1 s − 2 and we are using the substitution t = cot x .
By standard contour integration, we need to evaluate the residues of this integrand at the poles with positive imaginary part. These are i sec θ e ± 2 1 i θ , and so ( L f ) ( s ) = = = s 3 2 π i ( R e s z = i sec θ e 2 1 i θ + R e s z = i sec θ e − 2 1 i θ ) ( z 2 + sec θ e i θ ) ( z 2 + sec θ e − i θ ) 1 s 3 2 π i { − sec θ ( e i θ − e − i θ ) 1 2 i sec θ e 2 1 i θ 1 + sec θ ( e i θ − e − i θ ) 1 2 i sec θ e − 2 1 i θ 1 } 2 s 3 π cos 2 1 θ ( cos θ ) 2 3 So much for the integration. Now to get the result in the right shape to answer the question. Since tan θ = s − 2 , we have sec 2 θ = s 4 s 4 + 1 , and so cos θ = s 4 + 1 s 2 . Thus ( L f ) ( s ) = 2 ( s 4 + 1 ) 4 3 π sec 2 1 θ . Finally we have sin θ = s 4 + 1 1 , and hence ( L f ) ( s ) = 2 ( s 4 + 1 ) 4 1 π sin θ sec 2 1 θ = ( s 4 + 1 ) 4 1 π sin 2 1 θ = ( s 4 + 1 ) 4 1 π sin [ 2 1 tan − 1 ( s − 2 ) ] . Thus the answer is 1 + 4 + 1 + 1 + 4 + 1 + 2 + 1 + 2 + 1 = 1 8 .