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Although the denominator may look simplified, in reality there is a negative exponent in it. Our first step should be to remove that:
∫ 0 ∞ e x + e − x 1 d x = ∫ 0 ∞ e x + e x 1 1 d x = ∫ 0 ∞ e 2 x + 1 e x d x .
Now, it looks like we can group the numerator with the differential d x and use a clever u -substitution to simplify the problem. Choosing u = e x (and d u = e x d x ), the problem continues:
∫ 0 ∞ e 2 x + 1 e x d x = ∫ 0 ∞ e 2 x + 1 1 ⋅ e x d x = ∫ 1 ∞ u 2 + 1 1 d u .
Now, the trigonometric substitution u = tan θ (and d u = sec 2 θ d θ ) allows us to finish the problem:
∫ 1 ∞ u 2 + 1 1 d u = ∫ π / 4 π / 2 tan 2 θ + 1 1 ⋅ sec 2 θ d θ = ∫ π / 4 π / 2 s e c 2 θ 1 ⋅ sec 2 θ d θ = ∫ π / 4 π / 2 1 d θ = 4 π .