🧮 Brain Teaser

The Integral That Completes Itself

Evaluate:

I=∫0π/211+tan⁡2(x) dxI = \int_0^{\pi/2} \frac{1}{1 + \tan^{\sqrt{2}}(x)}\, dx

symmetry substitutionking's propertyintegration beeelegant cancellation

Answer: Integral of 1/(1+tan^√2 x)

Key Idea / Intuition

The exponent 2\sqrt{2} looks frightening, but it's a red herring. The trick is to pair the integral with itself under the substitution x↦π2−xx \mapsto \frac{\pi}{2} - x, which swaps tan⁡\tan and cot⁡\cot. The two integrals add to give exactly π/2\pi/2, so each equals π/4\pi/4 — regardless of the exponent.


Formal Proof / Solution

Let α=2\alpha = \sqrt{2} (the argument works for any α>0\alpha > 0). Define

I=∫0π/211+tan⁡αx dx.I = \int_0^{\pi/2} \frac{1}{1 + \tan^\alpha x}\, dx.

Step 1: Apply the substitution x↦π2−xx \mapsto \frac{\pi}{2} - x.

Under this substitution dx↦−dxdx \mapsto -dx, and the limits swap (then flip back), giving:

I=∫0π/211+tan⁡α ⁣(π2−x) dx.I = \int_0^{\pi/2} \frac{1}{1 + \tan^\alpha\!\left(\frac{\pi}{2}-x\right)}\, dx.

Step 2: Use the identity tan⁡ ⁣(π2−x)=cot⁡x=1tan⁡x\tan\!\left(\frac{\pi}{2} - x\right) = \cot x = \frac{1}{\tan x}.

I=∫0π/211+cot⁡αx dx=∫0π/211+tan⁡−αx dx=∫0π/2tan⁡αx1+tan⁡αx dx.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.

Step 3: Add the two expressions for II.

2I=∫0π/211+tan⁡αx dx+∫0π/2tan⁡αx1+tan⁡αx dx=∫0π/21+tan⁡αx1+tan⁡αx dx=∫0π/21 dx=π2.2I = \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}.

Conclusion:

I=π4\boxed{I = \frac{\pi}{4}}

The value is completely independent of the exponent α\alpha — so 2\sqrt{2} was there purely as a distraction.

Type: IntegrationEdit on GitHub ↗