∫ 0 2 5 ( 1 + 4 x 2 ) 2 5 − 2 0 x 2 6 0 d x = π b a
The equation above holds true for square-free positive coprime integers a and b . Enter your answer as a b .
Note: I came across the integral above while solving a very interesting mechanics problem.
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Thank you for the solution! I just noticed an insignificant typo in the second line of the solution. It should be sin ( θ ) instead of sin ( x ) . Also, I really like the format in which you have documented your solution. If it is not too much trouble, would you mind sharing the latex code of the solution? If not share, some tips on how to document would be great. I am still in the process of learning and I will find your insights helpful.
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Thank you very much!
∫ 0 2 5 ( 4 x 2 + 1 ) 2 5 − 2 0 x 2 6 0 d x ⇒ 3 0 tan − 1 ( 5 − 4 x 2 2 6 x ) ∣ x = 0 x = 2 5
3 0 tan − 1 ( 5 − 4 x 2 2 6 x ) ∣ x = 0 ⇒ 0
x → ( 2 5 ) − lim 3 0 tan − 1 ( 5 − 4 x 2 2 6 x ) = 2 1 5 π
The limit has to be taken from below as the expression can not be evaluated from above in R and taking the limit from this direction is sufficient.
Taking the limit is necessary to the evaluation as the direct substitution is indeterminate.
I = 5 6 0 0 ∫ 2 5 1 + 4 x 2 5 − 4 x 2 d x . Let x = 2 5 y ,
= 6 5 0 ∫ 1 1 + 5 y 2 1 − y 2 d y . Let y = sin θ ,
= 6 5 0 ∫ 2 π 1 + 5 sin 2 θ d θ = 0 ∫ 2 π cos 2 θ + 6 sin 2 θ d θ = 0 ∫ 2 π 1 + 6 tan 2 θ sec 2 θ d θ . Let ϕ = 6 tan θ .
= 3 0 0 ∫ ∞ 1 + ϕ 2 d ϕ . Let ϕ = tan ζ .
= 3 0 0 ∫ 2 π d ζ = 2 1 5 π .
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I = ∫ 0 2 5 ( 1 + 4 x 2 ) 2 5 − 2 0 x 2 6 0 d x = ∫ 0 2 π ( 1 + 5 sin 2 θ ) 1 − sin 2 θ 6 5 cos θ d θ = ∫ 0 2 π 1 + 5 sin 2 θ 6 5 d θ = ∫ 0 2 π 7 − 5 cos 2 θ 1 2 5 d θ = ∫ 0 ∞ 7 − 5 ( 1 + t 2 1 − t 2 ) 1 2 5 × 1 + t 2 d t = ∫ 0 ∞ 1 + 6 t 2 6 5 d t = 3 0 ∫ 0 2 π 1 + tan 2 ϕ sec 2 ϕ d ϕ = 3 0 ∫ 0 2 π d ϕ = 3 0 ϕ ∣ ∣ ∣ ∣ 0 2 π = π 2 1 5 Let sin θ = 5 2 x ⟹ cos θ d θ = 5 2 d x Since cos 2 θ = 1 − 2 sin 2 θ Let t = tan θ ⟹ d t = sec 2 θ d θ Let 6 t = tan ϕ ⟹ 6 d t = sec 2 ϕ d ϕ
Therefore, a b = 1 5 × 2 = 3 0 .