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Note first that 1 + sin ( x ) 1 = 1 + sin ( x ) 1 × 1 − sin ( x ) 1 − sin ( x ) = 1 − sin 2 ( x ) 1 − sin ( x ) = cos 2 ( x ) 1 − sin ( x ) = sec 2 ( x ) − cos 2 ( x ) sin ( x ) .
Now the integral of sec 2 ( x ) is tan ( x ) , and for the cos 2 ( x ) sin ( x ) term we can use the substitution method with u = cos ( x ) ⟹ d u = − sin ( x ) d x , giving us that
∫ 0 π 1 + sin ( x ) 1 d x = ( tan ( x ) − cos ( x ) 1 ) 0 π = ( 0 − ( − 1 ) − ( 0 − 1 ) = 2 .
You should note that the discontinuity your antiderivative has at x = 2 π is removable, which is why you can still use the fundamental theorem of calculus there... Otherwise, it would be better to just remove it by rewriting the antiderivative as 1 + sin ( x ) − cos ( x )
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Using tangent half-angle substitution , t = tan ( 2 x ) , we get ∫ 0 π 1 + sin ( x ) 1 d x = = = = = = ∫ 0 ∞ 1 + 1 + t 2 2 t 1 1 + t 2 2 d t 2 ∫ 0 ∞ 1 + 2 t + t 2 1 d t 2 ∫ 0 ∞ ( 1 + t ) 2 1 d t − 1 + t 2 ∣ ∣ ∣ 0 ∞ t → ∞ lim 1 + t − 2 − ( 1 − 2 ) 2