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both arctanx and 1+x2, since 1+tan2t simplifies to sec2t=1cos2t, as does tan′t.
Then try an integration by parts with regard to t (on one hand) and the trigonometric
part (on the other hand). This implies evaluating the anti-derivative oftan4tcost = sin4tcos5t = sin4t⋅costcos6t = sin4t⋅sin′t(1−sin2t)3,which is trivial, following a simple trigonometric substitution and some partial fraction
decomposition. The non-trivial part consists in integrating ln(1±sint),which, for all I
care, can be done by expanding the integrand into its Mercator series, and reversing the
order of summation and integration. Alternately, transform sint into cos2u using the
fact that sint=cos(π2−t), and then employ the well-known trigonometric formulas
for 1±cos2u, along with the properties of the natural logarithm. Now use the fact that
∫π40lncotu du = Catalan's constant, and we are left with expressing∫π80lncotu du = ∫π80lncosu du−∫
Step-by-step explanation:
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