Analyzing the Setup
My dear student, welcome to the arena. Today, we are going to dissect a problem that, at first glance, looks like a nightmare. You see an exponential term ex sitting in the denominator, coupled with a high-power trigonometric expression sin6x+cos6x.
It is natural to feel a moment of hesitation. But in the world of JEE Advanced, intimidation is just a sign that you are about to learn something profound. Let us peel back the layers of this problem together.
The King's Property - The Magic Key
Imagine you are standing before a locked door. You have the key, but you have to know how to turn it. In definite integration, when you see symmetric limits like [−2π,2π], that key is almost always the King's Property:
∫abf(x)dx=∫abf(a+b−x)dx
Here, a+b=−2π+2π=0. So, we replace x with −x. Our integral becomes:
I=∫−2π2π(1+e−x)(sin6(−x)+cos6(−x))d(−x)
Because sin6(−x)=sin6x and cos6(−x)=cos6x, the trigonometric part remains unchanged. But look at the exponential part! e−x is just ex1.
When we simplify the denominator (1+ex1), we get exex+1. This ex jumps to the numerator. Now, we have two versions of I.
When we add them, the 1+ex terms cancel out perfectly. It is like watching a complex machine suddenly click into place. We are left with:
2I=∫−2π2πsin6x+cos6xdx
The Trigonometric Transformation
Now that the exponential term is gone, we are left with a purely trigonometric integral. Because sin6x+cos6x is an even function, we can simplify the limits from [−2π,2π] to [0,2π] by multiplying by 2.
The 2 on both sides cancels out, leaving us with:
To solve this, we use the standard technique of dividing the numerator and denominator by cos6x. This transforms the expression into:
We can rewrite sec6x as (sec2x)2⋅sec2x, which is (1+tan2x)2⋅sec2x. This is the perfect setup for a substitution.
The Algebraic Pivot
Let t=tanx. Then dt=sec2xdx. As x goes from 0 to 2π, t goes from 0 to ∞. Our integral becomes:
Using the sum of cubes formula, t6+1=(t2)3+13=(t2+1)(t4−t2+1). One factor of (t2+1) cancels out, leaving us with:
This is a classic biquadratic form. We divide the numerator and denominator by t2:
The Final Integration
We are almost there. Let u=t−t1. Then du=(1+t21)dt.
Also, u2=t2+t21−2, so t2+t21=u2+2. The denominator becomes u2+2−1=u2+1. The limits change from 0 to ∞ for t to −∞ to ∞ for u.
This is the standard integral for tan−1u. Evaluating this from −∞ to ∞ gives us:
I=[tan−1u]−∞∞=2π−(−2π)=π
And there it is. The complexity dissolves into a simple, elegant π. Remember, in JEE Advanced, the path is rarely a straight line, but if you trust the properties and keep your algebraic steps clean, the solution will always reveal itself.