Analyzing the Setup
Welcome, fellow traveler on the path to JEE Advanced mastery. Today, we are not just solving a problem; we are witnessing a dance of symmetry and transformation. We are going to evaluate the integral:
where 0<α<π. At first glance, this integral looks intimidating. The x in the numerator is a classic 'distractor'—it makes the standard antiderivative formulas impossible to apply directly.
But in the world of JEE calculus, whenever you see a variable x in the numerator of a definite integral, your intuition should immediately scream: King's Property!
Phase 1
The King's Property Transformation
The King's Property, or the property of definite integrals, states that ∫abf(x)dx=∫abf(a+b−x)dx. This is our secret weapon. By replacing x with (π−x), we are essentially 'flipping' the function.
Let's see what happens:
I=∫0π1+cosαsin(π−x)(π−x)dx
Recall your trigonometric identities: sin(π−x)=sinx. The denominator remains perfectly unchanged! This is the moment of magic. Our new integral is:
Now, watch what happens when we add our original integral I to this new version. We get 2I on the left, and on the right, the x and −x in the numerators cancel out completely:
2I=∫0π1+cosαsinxx+π−xdx=π∫0π1+cosαsinxdx
We have successfully banished the x from the numerator. The problem is now reduced to a standard trigonometric integral.
Phase 2
Exploiting Symmetry
We can simplify this further. The function f(x)=1+cosαsinx1 is symmetric about x=π/2. Because of this, the integral from 0 to π is exactly twice the integral from 0 to π/2.
Dividing both sides by 2, we arrive at a much cleaner form:
Phase 3
The Half-Angle Substitution
Now, we enter the realm of algebraic substitution. To handle the sinx in the denominator, we use the Weierstrass substitution: t=tan(x/2). This implies dx=1+t22dt and sinx=1+t22t.
When x=0, t=0. When x=π/2, t=tan(π/4)=1. Our limits are now 0 to 1. Substituting these into our integral:
I=π∫011+cosα(1+t22t)1+t22dt
Multiplying the numerator and denominator by (1+t2), we get:
Phase 4
Completing the Square
We are almost there. The denominator t2+2tcosα+1 is a quadratic. To integrate this, we complete the square:
t2+2tcosα+1=(t+cosα)2+(1−cos2α)=(t+cosα)2+sin2α
Our integral becomes:
I=2π∫01(t+cosα)2+sin2αdt
This is the standard form ∫u2+a2du=a1tan−1(au). Here, u=t+cosα and a=sinα. Applying the formula:
I=sinα2π[tan−1(sinαt+cosα)]01
Phase 5
The Final Trigonometric Simplification
Evaluating at the limits 1 and 0:
I=sinα2π[tan−1(sinα1+cosα)−tan−1(sinαcosα)]
Using half-angle identities, sinα1+cosα=2sin(α/2)cos(α/2)2cos2(α/2)=cot(α/2). And sinαcosα=cotα.
So we have:
I=sinα2π[tan−1(cot(α/2))−tan−1(cotα)]
Using tan−1(cotθ)=π/2−θ, the expression becomes:
I=sinα2π[(π/2−α/2)−(π/2−α)]
Simplifying the bracket: (π/2−α/2−π/2+α)=α/2. Finally:
And there it is! The final result is: