If the equation above holds true for positive integers and , find .
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First I will rewrite the integral as ∫ 0 2 π x 2 csc 2 x d x . The form looks naturally vulnerable to integration by parts so the obvious course of action is letting u = x 2 , d u = 2 x , d v = csc 2 x , v = − cot x to get − x 2 cot x ∣ ∣ 0 2 π + ∫ 0 2 π 2 x cot x d x .
Before tackling the new integral, I will prove that the expression outside of the integral evaluates to 0. We know that cot ( 2 π ) = 0 so that part goes to 0 so we only need to check lim x → 0 − x 2 cot x = lim x → 0 tan x − x 2 = lim x → 0 sec 2 x − 2 x = 1 2 × 0 = 0 by applying L'hopital's rule.
For the new integral I will do integration by parts again, applying the property that ∫ cot x d x = lo g sin x let u = 2 x , d u = 2 , d v = cot x , v = lo g sin x . Then the integral is equal to 2 x lo g sin x ∣ ∣ 0 2 π − ∫ 0 2 π 2 lo g sin x d x .
Again, I will prove that the bit outside of the integral evaluates to 0. First notice that lo g sin 2 π = lo g 1 = 0 . And lim x → 0 2 x lo g sin x = lim x → 0 2 x − 1 lo g sin x = lim x → 0 2 − x − 2 cot x d x = lim x → 0 − 2 x 2 cot x = lim x → 0 − 2 x 2 ( x − 1 + O ( x ) ) = lim x → 0 − 2 x + O ( x 3 ) = 0 by applying L'hopital's rule first and then using the Laurent series for the cotangent function.
So after all that the integral is actually equal to − 2 ∫ 0 2 π lo g sin x d x . Now, the integral for lo g sin x over this interval is a familiar one so I will assume that the reader knows, can deduce, or look up on the internet that it evaluates to − 2 1 π lo g 2 so by multiplying the outside factor our integral evaluates to precisely π lo g 2 .