Analyzing the Setup
Imagine you are standing before a massive, complex-looking function:
f(x)=7tan8x+7tan6x−3tan4x−3tan2x
It looks like a monster, doesn't it? A chaotic collection of high-power trigonometric terms that seem designed to make your head spin.
But here is the secret of JEE Advanced physics and mathematics: the most intimidating problems are often the ones that hide the most elegant solutions. Today, we are going to dismantle this monster, piece by piece, and find the beauty hidden within.
The Art of Factoring
When you first see an expression like this, your instinct might be to panic or to try some brute-force integration. Resist that urge! Instead, take a deep breath and look for patterns.
Mathematics is the study of patterns, and this function is practically screaming for us to group its terms. Look at the first two terms: 7tan8x+7tan6x. We can factor out 7tan6x to get 7tan6x(tan2x+1).
Now look at the last two terms: −3tan4x−3tan2x. We can factor out −3tan2x to get −3tan2x(tan2x+1).
Do you see it now? The common factor
(tan2x+1) has emerged like a lighthouse in the fog! Our function is simply:
f(x)=(7tan6x−3tan2x)(tan2x+1)
The Substitution Magic
Now, we invoke one of the most powerful tools in our trigonometric arsenal: the identity
1+tan2x=sec2x. By substituting this into our factored expression, the function transforms into:
f(x)=(7tan6x−3tan2x)sec2x
Suddenly, the integration becomes a walk in the park. We want to evaluate ∫f(x)dx. With the sec2x term sitting there, we know that if we let u=tanx, then du=sec2xdx.
The integral becomes ∫(7u6−3u2)du. This is just a simple polynomial! Integrating this gives us u7−u3.
Substituting back, we get tan7x−tan3x. When we evaluate this from 0 to 4π, we get (1−1)−(0−0)=0. The net area is zero!
The Integration by Parts Journey
But we are not done yet. The problem also asks us to evaluate ∫04πxf(x)dx. Now we have a product of two functions: x and f(x).
This is the classic setup for Integration by Parts. We choose u=x and dv=f(x)dx. The formula ∫udv=uv−∫vdu becomes our roadmap.
We already know
v=∫f(x)dx=tan7x−tan3x. So, our integral is:
[x(tan7x−tan3x)]04π−∫04π(tan7x−tan3x)dx
As we discussed, the boundary term vanishes completely because tan(4π)=1. We are left with −∫04π(tan7x−tan3x)dx, which is ∫04π(tan3x−tan7x)dx.
The Final Victory
We are in the home stretch now. We can factor this as:
∫04πtan3x(1−tan4x)dx
Using the difference of squares, this becomes:
∫04πtan3x(1−tan2x)(1+tan2x)dx
Again, we see that
1+tan2x term, which is
sec2x. With another substitution
t=tanx, the integral becomes:
∫01t3(1−t2)dt=∫01(t3−t5)dt
Evaluating this, we get:
[4t4−6t6]01=41−61=121
We have tamed the monster! We have navigated the complexity, used our tools wisely, and arrived at the elegant answer of 121. Remember, in JEE Advanced, it is not about memorizing formulas; it is about seeing the structure and trusting the process.