Answer: Integral of 1/(1+tan^√2 x)
Key Idea / Intuition
The exponent 2 \sqrt{2} 2 looks frightening, but it's a red herring. The trick is to pair the integral with itself under the substitution x ↦ π 2 − x x \mapsto \frac{\pi}{2} - x x ↦ 2 π − x , which swaps tan \tan tan and cot \cot cot . The two integrals add to give exactly π / 2 \pi/2 π /2 , so each equals π / 4 \pi/4 π /4 — regardless of the exponent.
Formal Proof / Solution
Let α = 2 \alpha = \sqrt{2} α = 2 (the argument works for any α > 0 \alpha > 0 α > 0 ). Define
I = ∫ 0 π / 2 1 1 + tan α x d x . I = \int_0^{\pi/2} \frac{1}{1 + \tan^\alpha x}\, dx. I = ∫ 0 π /2 1 + t a n α x 1 d x .
Step 1: Apply the substitution x ↦ π 2 − x x \mapsto \frac{\pi}{2} - x x ↦ 2 π − x .
Under this substitution d x ↦ − d x dx \mapsto -dx d x ↦ − d x , and the limits swap (then flip back), giving:
I = ∫ 0 π / 2 1 1 + tan α ( π 2 − x ) d x . I = \int_0^{\pi/2} \frac{1}{1 + \tan^\alpha\!\left(\frac{\pi}{2}-x\right)}\, dx. I = ∫ 0 π /2 1 + t a n α ( 2 π − x ) 1 d x .
Step 2: Use the identity tan ( π 2 − x ) = cot x = 1 tan x \tan\!\left(\frac{\pi}{2} - x\right) = \cot x = \frac{1}{\tan x} tan ( 2 π − x ) = cot x = t a n x 1 .
I = ∫ 0 π / 2 1 1 + cot α x d x = ∫ 0 π / 2 1 1 + tan − α x d x = ∫ 0 π / 2 tan α x 1 + tan α x d x . I = \int_0^{\pi/2} \frac{1}{1 + \cot^\alpha x}\, dx = \int_0^{\pi/2} \frac{1}{1 + \tan^{-\alpha} x}\, dx = \int_0^{\pi/2} \frac{\tan^\alpha x}{1 + \tan^\alpha x}\, dx. I = ∫ 0 π /2 1 + c o t α x 1 d x = ∫ 0 π /2 1 + t a n − α x 1 d x = ∫ 0 π /2 1 + t a n α x t a n α x d x .
Step 3: Add the two expressions for I I I .
2 I = ∫ 0 π / 2 1 1 + tan α x d x + ∫ 0 π / 2 tan α x 1 + tan α x d x = ∫ 0 π / 2 1 + tan α x 1 + tan α x d x = ∫ 0 π / 2 1 d x = π 2 . 2I = \int_0^{\pi/2} \frac{1}{1+\tan^\alpha x}\, dx + \int_0^{\pi/2} \frac{\tan^\alpha x}{1+\tan^\alpha x}\, dx = \int_0^{\pi/2} \frac{1 + \tan^\alpha x}{1 + \tan^\alpha x}\, dx = \int_0^{\pi/2} 1\, dx = \frac{\pi}{2}. 2 I = ∫ 0 π /2 1 + t a n α x 1 d x + ∫ 0 π /2 1 + t a n α x t a n α x d x = ∫ 0 π /2 1 + t a n α x 1 + t a n α x d x = ∫ 0 π /2 1 d x = 2 π .
Conclusion:
I = π 4 \boxed{I = \frac{\pi}{4}} I = 4 π
The value is completely independent of the exponent α \alpha α — so 2 \sqrt{2} 2 was there purely as a distraction.