I ( a ) = ∫ 0 ∞ x 2 ( x 2 + a ) ln ( x 2 + 1 ) d x
Define I ( a ) as above, where a > 0 . Then
I ( 1 ) + I ( 2 ) = x 4 π ( x 1 ⋅ x 3 − x 1 ln ( x 1 + x 2 ) − x 1 2 ln ( x 1 ) )
where x 1 , x 2 , x 3 , and x 4 are positive integers. Find x 1 + x 2 + x 3 + x 4 .
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Wow....so simple.
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This method was invented by Prof Richard Feynman.
Wow..its great.The best thing is how such a complex problem wields a simple answer!
The solution was good. Can you tell me how did you decide where to assume the second variable t?
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It is a trick used in [differentiation under the integration sign}(https://brilliant.org/wiki/differentiate-through-the-integral/). Basically try and error and based on experience.
I ( a ) = ∫ 0 ∞ x 2 ( x 2 + a ) ln ( x 2 + 1 ) d x
Let's define a new integral:
I ( a , t ) = ∫ 0 ∞ x 2 ( x 2 + a ) ln ( t x 2 + 1 ) d x
Let's use differentiation under the integral sign
⇒ d t d I ( a , t ) = d t d ∫ 0 ∞ x 2 ( x 2 + a ) ln ( t x 2 + 1 ) d x = ∫ 0 ∞ ∂ t ∂ x 2 ( x 2 + a ) ln ( t x 2 + 1 ) d x = ∫ 0 ∞ t x 2 + 1 1 ⋅ x 2 + a 1 d x
Then we have to use partial fraction decomposition and get integral in the form:
d t d I ( a , t ) = ∫ 0 ∞ a t − 1 t ⋅ ( x t ) 2 + 1 1 − a t − 1 1 ⋅ x 2 + a 1 d x
Let's use the integration formula ∫ ( a x ) 2 + 1 1 d x = a 1 arctan ( a x ) + C
Then we are going to end up with
d t d I ( a , t ) = a t − 1 t ⋅ 2 t π − a t − 1 1 ⋅ 2 a π
We notice that I ( a , 0 ) = 0 ∧ I ( a , 1 ) = I ( a )
∫ 0 1 d t d I ( a , t ) d t = I ( a , 1 ) = I ( a ) = 2 π ∫ 0 1 a t − 1 t ⋅ t 1 − a t − 1 1 ⋅ a 1 d t
Solving this trivial integral (you can use u sub to solve both integrals) we are going to end up with
I ( a ) = π ⋅ a − 2 3 ( a − ln ( a + 1 ) )
Then we calculate the sum of the first two values:
I ( 1 ) = π ⋅ 1 − 2 3 ⋅ ( 1 − ln ( 1 + 1 ) ) = π ⋅ ( 1 − ln ( 2 ) )
I ( 2 ) = π ⋅ 2 − 2 3 ⋅ ( 2 − ln ( 2 + 1 ) ) = 2 2 π ( 2 − ln ( 2 + 1 ) )
I ( 1 ) + I ( 2 ) = π ⋅ ( 1 − ln ( 2 ) ) + 2 2 π ( 2 − ln ( 2 + 1 ) )
= 4 π ( 6 − 4 ln ( 2 ) − 2 ln ( 2 + 1 ) ) = − 4 π ( 2 ln ( 2 + 1 ) + 4 ln ( 2 ) − 6 )
= − ( 2 ⋅ ln ( 2 + 1 ) + 2 2 ⋅ ln ( 2 ) − 3 ⋅ 2 ) ⋅ 4 π
Finally, we get
⇒ x 1 = 2 ∧ x 2 = 1 ∧ x 3 = 3 ∧ x 4 = 4 ⇒ ∑ 1 ≤ i ≤ 4 x i = 1 0
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Similar solution as @Henri Kärpijoki 's, presented as follows:
Using differentiation under the integration sign , define I ( a , t ) as follows:
I ( a , t ) ∂ t ∂ I ( a , t ) ⟹ I ( a , t ) ⟹ I ( a ) = ∫ 0 ∞ x 2 ( x 2 + a ) ln ( t x 2 + 1 ) d x = ∫ 0 ∞ ( x 2 + a ) ( t x 2 + 1 ) 1 d x = 1 − a t 1 ∫ 0 ∞ ( x 2 + a 1 − t x 2 + 1 t ) d x = 1 − a t 1 ⎣ ⎡ a tan − 1 ( a x ) − t tan − 1 ( t x ) ⎦ ⎤ 0 ∞ = 2 a ( 1 − a t ) π ( 1 − a t ) = 2 a ( 1 + a t ) π = ∫ 2 a ( 1 + a t ) π d t = a a π ∫ 1 + u u d u = a a π ∫ ( 1 − 1 + u 1 ) d u = a a π ( u − ln ( 1 + u ) ) + C = a a π ( a t − ln ( 1 + a t ) ) = a a π ( a − ln ( 1 + a ) ) Since 1 − a t = ( 1 − a t ) ( 1 + a t ) Let u 2 = a t ⟹ 2 u d u = a d t where C is the constant of integration. Since I ( a , 0 ) = 0 ⟹ C = 0 Putting t = 1
Therefore,
I ( 1 ) + I ( 2 ) = π ( 1 − ln 2 ) + 2 2 π ( 2 − ln ( 2 + 1 ) ) = 4 π ( 6 − 2 ln ( 2 + 1 ) − 4 ln 2 )
Then we have x 1 + x 2 + x 3 + x 4 = 2 + 1 + 3 + 4 = 1 0 .