๐Ÿงฎ Brain Teaser

The Integral That Loops Back Around

Evaluate the definite integral

I=โˆซ0ฯ€/211+tanโก3xโ€‰dx.I = \int_0^{\pi/2} \frac{1}{1 + \tan^{\sqrt{3}} x}\, dx.

King's substitutionsymmetrytrigonometric integralcomplementary substitution

Answer: The Integral That Loops Back Around

Key Idea / Intuition

The trick is the King's substitution: replace xx with ฯ€/2โˆ’x\pi/2 - x. Under this swap, tanโกx\tan x and cotโกx=1/tanโกx\cot x = 1/\tan x exchange roles, and the two resulting integrands are complementary โ€” they add to 1 over the same interval. So I+I=ฯ€/2I + I = \pi/2, giving I=ฯ€/4I = \pi/4, regardless of the exponent 3\sqrt{3} (or any positive exponent!).


Formal Proof / Solution

Step 1: Apply the substitution xโ†ฆฯ€/2โˆ’xx \mapsto \pi/2 - x.

Let x=ฯ€/2โˆ’ux = \pi/2 - u, so dx=โˆ’dudx = -du; when x=0x = 0, u=ฯ€/2u = \pi/2; when x=ฯ€/2x = \pi/2, u=0u = 0. Thus

I=โˆซฯ€/2011+tanโก3(ฯ€/2โˆ’u)โ€‰(โˆ’du)=โˆซ0ฯ€/211+cotโก3uโ€‰du.I = \int_{\pi/2}^{0} \frac{1}{1 + \tan^{\sqrt{3}}(\pi/2 - u)}\,(-du) = \int_0^{\pi/2} \frac{1}{1 + \cot^{\sqrt{3}} u}\, du.

Step 2: Simplify the new integrand.

Since cotโกu=1/tanโกu\cot u = 1/\tan u,

11+cotโก3u=11+tanโกโˆ’3u=tanโก3u1+tanโก3u.\frac{1}{1 + \cot^{\sqrt{3}} u} = \frac{1}{1 + \tan^{-\sqrt{3}} u} = \frac{\tan^{\sqrt{3}} u}{1 + \tan^{\sqrt{3}} u}.

So we have

I=โˆซ0ฯ€/2tanโก3x1+tanโก3xโ€‰dx.I = \int_0^{\pi/2} \frac{\tan^{\sqrt{3}} x}{1 + \tan^{\sqrt{3}} x}\, dx.

Step 3: Add the two expressions for II.

2I=โˆซ0ฯ€/211+tanโก3xโ€‰dx+โˆซ0ฯ€/2tanโก3x1+tanโก3xโ€‰dx=โˆซ0ฯ€/21โ€‰dx=ฯ€2.2I = \int_0^{\pi/2} \frac{1}{1 + \tan^{\sqrt{3}} x}\, dx + \int_0^{\pi/2} \frac{\tan^{\sqrt{3}} x}{1 + \tan^{\sqrt{3}} x}\, dx = \int_0^{\pi/2} 1\, dx = \frac{\pi}{2}.

Step 4: Conclude.

I=ฯ€4.\boxed{I = \frac{\pi}{4}.}

Remark: The exponent 3\sqrt{3} is completely irrelevant. The same argument shows

โˆซ0ฯ€/211+tanโกฮฑxโ€‰dx=ฯ€4\int_0^{\pi/2} \frac{1}{1 + \tan^{\alpha} x}\, dx = \frac{\pi}{4}

for any ฮฑโˆˆR\alpha \in \mathbb{R} (with ฮฑ>0\alpha > 0 to ensure the integrand is well-behaved). This is a beautiful example of how symmetry collapses an apparently difficult integral.

Type: IntegrationEdit on GitHub โ†—