Analyzing the Setup
The integral provided is I=∫01xcot−1(1−x2+x4)dx. At first glance, the quartic polynomial inside the inverse cotangent function appears intimidating.
However, in the context of JEE Advanced, such complexity is often a mask for a hidden, elegant structure. Our goal is to peel back this mask using trigonometric identities and algebraic manipulation.
The Architect's Blueprint
Working with cot−1 is rarely the most efficient path in calculus. We recall the identity cot−1(z)=tan−1(z1) for z>0.
Since our limits of integration are from 0 to 1, the argument 1−x2+x4 is always positive. We rewrite the integral as:
I=∫01xtan−1(1−x2+x41)dx
Next, we perform algebraic surgery on the denominator. We rewrite 1−x2+x4 as 1+x2(x2−1).
This creates a structure resembling 1+AB, where A=x2 and B=x2−1. Note that A−B=x2−(x2−1)=1.
Using the identity tan−1(A)−tan−1(B)=tan−1(1+ABA−B), our integral transforms into:
I=∫01x[tan−1(x2)−tan−1(x2−1)]dx
The King's Gambit
With the expression simplified, we use the substitution t=x2, which implies dt=2xdx, or xdx=21dt. The limits remain 0 to 1.
The integral becomes:
I=21∫01[tan−1(t)−tan−1(t−1)]dt
We split this into two parts:
I=21∫01tan−1(t)dt−21∫01tan−1(t−1)dt
We now invoke the King's Property: ∫0af(t)dt=∫0af(a−t)dt. Applying this to the second integral, we replace t with 1−t:
tan−1((1−t)−1)=tan−1(−t)=−tan−1(t)
Substituting this back, the two negative signs cancel out. We are left with:
I=21∫01tan−1(t)dt+21∫01tan−1(t)dt=∫01tan−1(t)dt
The Final Descent
We have reduced the quartic integral to the simple task of integrating tan−1(t). We use integration by parts, where u=tan−1(t) and dv=dt.
The formula ∫udv=uv−∫vdu yields:
I=[ttan−1(t)−∫1+t2tdt]01
The integral of 1+t2t is 21ln(1+t2). Thus, our result is:
I=[ttan−1(t)−21ln(1+t2)]01
Evaluating at the limits, we obtain:
I=(1⋅tan−1(1)−21ln(2))−(0−0)
The final result is: