∫ − ∞ ∞ x 4 + 1 x sin 3 x d x = π a e − c b sin ( e d )
If the above equation is true for positive integers a , b , c , d and e ,where c and e are square free numbers, find the value of a + b + c + d + e .
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Define the contour C R given by the upper semicircle of radius R > 1 oriented counterclockwise and consider the contour integral ∮ C R z 4 + 1 z e 3 i z d z = ∫ − R R x 4 + 1 x e 3 i x d x + ∫ C R z 4 + 1 z e 3 i z d z , where C R is the upper half circle of radius R . We will prove that R → ∞ lim ∫ C R z 4 + 1 z e 3 i z d z = 0 . Note that by the reverse triangle inequality, ∣ ∣ ∣ ∣ ∫ C R z 4 + 1 z e 3 i z d z ∣ ∣ ∣ ∣ ≤ π R ⋅ z ∈ C R max ∣ ∣ ∣ ∣ z 4 + 1 z e 3 i z ∣ ∣ ∣ ∣ ≤ π R ⋅ z ∈ C R max ∣ z ∣ 4 − 1 ∣ z ∣ ∣ e 3 i z ∣ = R 4 − 1 π R 2 ⋅ z ∈ C R max ∣ e 3 i z ∣ R → ∞ 0 , as ∣ e 3 i z ∣ is bounded by 1 in the upper half plane. Therefore, by the Residue theorem, ∫ − ∞ ∞ x 4 + 1 x e 3 i x d x = R → ∞ lim ∮ C R z 4 + 1 z e 3 i z d z = 2 π i ( Res z = e π i / 4 z 4 + 1 z e 3 i z + Res z = e 3 π i / 4 z 4 + 1 z e 3 i z ) . Since the poles are simple, for a residue at z = z 0 we have that Res z = z 0 z 4 + 1 z e 3 i z = z → z 0 lim z 4 + 1 ( z − z 0 ) z e 3 i z = 4 z 0 3 z 0 e 3 i z 0 = 4 z 0 2 e 3 i z 0 , by l'Hôpital's rule. By doing some algebraic stuff we find that ∫ − ∞ ∞ x 4 + 1 x sin ( 3 x ) d x = I m ( ∫ − ∞ ∞ x 4 + 1 x e 3 i x d x ) = π e − 3 / 2 sin ( 3 / 2 ) . Therefore a = 1 , b = 3 , c = 2 , d = 3 and e = 2 and a + b + c + d + e = 1 1 .
Is this in jee main range
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It doesn't look like it (I'm not familiar with the program). I think this course is typical for 2nd/3rd year bachelor students at university if they are interested in the topic.
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We can consider ∫ − ∞ ∞ x 4 + 1 x sin 3 x d x = ℑ ( ∫ − ∞ ∞ x 4 + 1 x e 3 i x d x ) and apply contour integration using a semicircle with radius R → ∞ in the upper complex plane as the contour as follows:
∮ z 4 + 1 z e 3 i z d z = ∫ − ∞ ∞ x 4 + 1 x e 3 i x d x + ∫ arc z 4 + 1 z e 3 i z d z
The imaginary part of first integral on the right hand side is twice the integral we are solving for. The last integral on the right and side approaches to 0 when R → ∞ by Jordan's lemma. Then we have:
I = ∫ − ∞ ∞ x 4 + 1 x e 3 i x d x = ∮ z 4 + 1 z e 3 i z d z = ∮ ( z − e 4 π i ) ( z − e 4 3 π i ) ( z + e 4 π i ) ( z + e 4 3 π i ) z e 3 i z d z = ∮ 2 1 ( z − e 4 π i 1 − z − e 4 3 π i 1 ) ( z + e 4 π i ) ( z + e 4 3 π i ) z e 3 i z d z = 2 ( z + e 4 π i ) ( z + e 4 3 π i ) 2 π i z e 3 i z ∣ ∣ ∣ ∣ e 4 3 π i e 4 π i = 2 π ( e − 2 3 ( 1 − i ) − e − 2 3 ( 1 + i ) ) = i π e − 2 3 sin ( 2 3 ) Only 2 of the 4 poles are in the contour By Cauchy integral formula
Therefore, ℑ ( I ) = π e − 2 3 sin ( 2 3 ) and a + b + c + d + e = 1 + 3 + 2 + 3 + 2 = 1 1 .