∫ 0 ∞ x 2 3 + 1 1 d x = b d c a π
The equation above holds true for coprime positive integers a , b , c , and d .
What is the minimum possible value of a + b + c + d ?
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The subsitution u = x 2 3 gives ∫ 0 ∞ x 2 3 + 1 1 d x = 3 2 ∫ 0 ∞ u + 1 u − 3 1 d u = 3 2 B ( 3 1 , 3 2 ) = 3 2 Γ ( 3 1 ) Γ ( 3 2 ) = 3 2 × sin 3 1 π π = 3 3 4 π = 3 2 3 4 π making the answer 4 + 3 + 3 + 2 = 1 2 .
4 and 2 are not coprime though
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True, but 4 , 3 , 3 , 2 are coprime, since they have no common factor other than ± 1 . There is a difference between coprime and pairwise coprime .
My solution is based on Contour integral. First, we do a substitution u = x such that the integral becomes
I = ∫ 0 ∞ x 3 / 2 + 1 1 d x = ∫ 0 ∞ u 3 + 1 2 u d u
Let ρ be a very small positive number and R a very large positive number, ρ < R . Let C be the positively oriented contour consists of four parts: C = C 1 ∪ C 2 ∪ C 3 ∪ C 4 , where C 1 = { x ∈ R ∣ ρ ≤ x ≤ R } , C 2 = { R e i θ ∣ θ ∈ [ 0 , 2 π / 3 ] } , C 3 = { x e 2 π i / 3 ∣ ρ ≤ x ≤ R } , C 4 = { ρ e i θ ∣ θ ∈ [ 0 , 2 π / 3 ] } .
Since the function 2 u / ( u 3 + 1 ) only has one simple pole at u = e i π / 3 , by residue theorem, the contour integral is I C = ∫ C u 3 + 1 2 u d u = 2 π i u = e π i / 3 R e s u 3 + 1 2 u = 3 4 π e π i / 6 .
Taking ρ → 0 + and R → ∞ , the paths C 2 , C 4 converges to zero, hence I C = ∫ C 1 u 3 + 1 2 u d u − ∫ − C 3 u 3 + 1 2 u d u = ∫ 0 ∞ u 3 + 1 2 u d u − ∫ 0 ∞ u 3 + 1 2 e 2 π i / 3 u ⋅ e 2 π i / 3 d u (Crucial role of C 3 here) = ( 1 − e 4 π i / 3 ) I = 3 e π i / 6 I . Comparing two expression of I C we see I = 3 3 4 π .
$$ x=tan^{4/3} \theta$$ just makes it the same old cuberoot(tan) integral
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Lets start by substituting x = u and finding the antiderivative The integral becomes ∫ 1 + u 3 2 u d u
Note that ( 1 + u ) ( 1 − u + u 2 ) = 1 + u 3 ,which gives the integral as ∫ ( 1 + u ) ( 1 − u + u 2 ) 2 u d u
Now 1 − u + u 2 1 − 1 + u 1 = ( 1 + u ) ( 1 − u + u 2 ) 2 u − u 2 = ( 1 + u ) ( 1 − u + u 2 ) 2 u − ( 1 + u ) ( 1 − u + u 2 ) u 2 = 1 + u 3 2 u − 1 + u 3 u 2
We have 1 − u + u 2 1 − 1 + u 1 = 1 + u 3 2 u − 1 + u 3 u 2
1 − u + u 2 1 − 1 + u 1 + 1 + u 3 u 2 = 1 + u 3 2 u
∫ ( 1 − u + u 2 1 − 1 + u 1 + 1 + u 3 u 2 ) d u = ∫ 1 + u 3 2 u d u
We can find anti-derivative for each one separately, the second and third ones are :
∫ 1 + u 1 d u = ln ( 1 + u )
∫ 1 + u 3 u 2 d u = 3 ln ( 1 + u 3 )
Now 1 − u + u 2 = ( u − 2 1 ) 2 + 4 3
∫ 1 − u + u 2 1 = ∫ ( u − 2 1 ) 2 + 4 3 1 d u = ∫ 3 ( 1 + ( 3 2 u − 1 ) 2 ) 4 d u , by substituting 3 2 u − 1 = tan θ we can find the antiderivative.
The final form of the antiderivative after reverting to original variable and simplifying will be 3 2 arctan ( 3 2 x − 1 ) + ln ⎝ ⎜ ⎛ 1 + x ( 1 + x 2 3 ) 3 1 ⎠ ⎟ ⎞
For the x = ∞ limit we can factor out the x inside logarithm and in both limits expression inside logarithm evaluates to 1, which evaluates to 0. Evaluating 3 2 arctan ( 3 2 x − 1 ) at limits will give 3 π + 3 3 π which simplifies to 3 3 4 π = 3 2 3 4 π