The Symphony of Symmetry
Unlocking the Integral
Welcome, future engineer. Today, we are not just solving a problem; we are uncovering a hidden truth about the nature of functions.
When you first look at the integral
I=∫−2π2π[f(x)+f(−x)][g(x)−g(−x)]dx
your instinct might be to panic. You see generic functions f(x) and g(x), and you think, 'How can I integrate functions I don't even know?'
But here is the secret of JEE Advanced: whenever you see an integral with limits from −a to a, stop. Breathe. You are not meant to integrate; you are meant to observe.
Phase 1
The Symmetric Interval
The limits −2π to 2π are a massive clue. They are symmetric about the origin.
In the world of calculus, this is a giant neon sign pointing toward the properties of even and odd functions. If we can prove that the integrand—the entire expression inside the integral—is an odd function, the answer collapses to zero instantly.
Let us define our integrand as a single function, h(x):
h(x)=[f(x)+f(−x)][g(x)−g(−x)]
Our mission is simple: determine the parity of h(x). Is it even, where h(−x)=h(x)? Or is it odd, where h(−x)=−h(x)?
Phase 2
The Algebraic Dance
To test for parity, we perform the standard substitution: replace every x with −x. Let us watch the algebra unfold:
h(−x)=[f(−x)+f(−(−x))][g(−x)−g(−(−x))]
Simplifying the double negatives, we get:
h(−x)=[f(−x)+f(x)][g(−x)−g(x)]
Now, look closely at the first bracket: [f(−x)+f(x)]. Because addition is commutative, this is identical to [f(x)+f(−x)]. The first bracket is invariant!
But look at the second bracket: [g(−x)−g(x)]. This is the negative of our original second bracket, [g(x)−g(−x)]. If we factor out a −1, we get:
h(−x)=[f(x)+f(−x)]×(−1)[g(x)−g(−x)]
When we pull that negative sign to the front, the transformation is complete:
h(−x)=−[f(x)+f(−x)][g(x)−g(−x)]=−h(x)
Phase 3
The Geometric Revelation
We have proven that h(x) is an odd function. Geometrically, this means the graph of h(x) has rotational symmetry about the origin.
Imagine the area under the curve from 0 to 2π. Let us call this area A. Because the function is odd, the area from −2π to 0 is exactly −A.
When we integrate from −2π to 2π, we are summing these two regions:
∫−2π2πh(x)dx=∫−2π0h(x)dx+∫02πh(x)dx
Substituting our values:
Conclusion
There is no complex integration, no substitution, and no headache. Just pure, elegant logic.
The answer is 0.
This problem teaches us that in physics and mathematics, observation is often more powerful than calculation. Keep this perspective, and you will conquer the most difficult problems the JEE can throw at you.