∫ 0 ∞ 1 + x 6 1 d x = a π
If the equation above holds true for some constant a , find a .
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I = ∫ 0 ∞ 1 + x 6 1 d x Let tan θ = x 3 ⇒ sec 2 θ d θ = 3 x 2 d x = ∫ 0 2 π 3 tan 3 2 θ ( 1 + tan 2 θ ) sec 2 θ d θ = 3 1 ∫ 0 2 π sin − 3 2 cos 3 2 d θ = 6 1 ⋅ B ( 6 1 , 6 5 ) B ( m , n ) is Beta function. = 6 Γ ( 1 ) Γ ( 6 1 ) Γ ( 6 5 ) Γ ( n ) is Gamma function. = 6 ( 0 ! ) Γ ( 6 1 ) Γ ( 1 − 6 1 ) Γ ( n ) = ( n − 1 ) ! = 6 1 ⋅ sin ( 6 π ) π Γ ( x ) Γ ( 1 − x ) = sin ( x π ) π = 3 π
⇒ a = 3
Best way is by beta function!
Using the Residue Theorem which states κ ∮ f ( z ) d z = 2 π i ∑ R e s ( f ( z ) , z 0 )
κ ∮ f ( z ) d z = ∫ − R R f ( z ) d z + κ ∫ f ( z ) d z
R → ∞ lim κ ∫ f ( z ) d z = 0
Using a semicircle contour, κ , in the 1 s t and 2 n d quadrants of radius R allows only the usage of the poles in this region which are e 6 π i , e 2 π i , and e 6 5 π i .
α = e 6 π i
The residue of f ( z ) = z 6 + 1 1 at a pole is, z → β lim ( z − β ) f ( z ) , where β is a pole, to find the a − 1 term in the Laurent series.
lim z → α z 6 + 1 z − α = 6 e 6 1 1 π i and repeating for α 3 and α 5 produces the sum of the residues in κ :
6 e 6 1 1 π i + 6 e 2 3 π i + 6 e 6 5 π i = 6 − i , but there are 3 more poles on another semi-circle contour on the 3 r d and 4 t h quadrants. They are obtainable by rotating κ by 1 8 0 ˚ but multiplying the sum by 2 would do. Therefore the sum of all residues is 3 − i
2 π i × 3 − i = 3 2 π
The function is even so ∫ − a a f ( x ) d x = 2 ∫ 0 a f ( x ) d x .
∫ 0 ∞ f ( x ) d x = 3 π
Did it the same way!
can you tell me any good resource from where i can learn about this theorem
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@kalpa roy Here is a good youtube video explaining it. https://goo.gl/297pNN
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I = ∫ 0 ∞ 1 + x 6 1 d x = ∫ 0 1 1 + x 6 1 d x + ∫ 1 ∞ 1 + x 6 1 d x
Let I ′ = ∫ 1 ∞ 1 + x 6 1 d x
Now substituting x = p 1 and then replacing p by x we get:
I ′ = ∫ 0 1 1 + x 6 x 4 d x
Therefore now we can write I as :
I = ∫ 0 1 1 + x 6 1 d x + ∫ 0 1 1 + x 6 x 4 d x = ∫ 0 1 1 + x 6 1 + x 4 d x
I = ∫ 0 1 1 + x 6 ( 1 + x 2 ) 2 d x − ∫ 0 1 1 + x 6 2 x 2 d x
I = ∫ 0 1 1 − x + x 2 1 + x 2 d x − 3 2 ∫ 0 1 1 + ( x 3 ) 2 3 x 2 d x
I = ∫ 0 1 ( x − x 1 ) 2 + 1 x 2 1 + 1 d x − 3 2 [ t a n − 1 ( x 3 ) ] 0 1
I = [ t a n − 1 ( x − x 1 ) ] 0 1 − 3 2 [ t a n − 1 ( x 3 ) ] 0 1
I = ( 0 − ( − 2 π ) ) − 3 2 ( 4 π )
I = 3 π
Therefore a = 3