Move (1+tan2x) to the numerator and replace with sec2x:
I=π2∫04π1+3tan2xsec2xdx
Substitution Method
Let t=3tanx⟹dt=3sec2xdx⟹sec2xdx=3dt
Change of Limits:
When x=0, t=0
When x=4π, t=3
Transformed Integral
Substitute t, dt, and the new limits:
I=π2∫031+t23dt
Pull out the constant:
I=π32∫031+t2dt
Evaluating the Integral
Standard integral: ∫1+t21dt=tan−1t
I=π32[tan−1t]03
I=π32(tan−1(3)−tan−1(0))
I=π32(3π−0)=332
Final Calculation
We need to find the value of 27I2.
First, square I:
I2=(332)2=274
Now, multiply by 27:
27I2=27×274=4
Final Answer:4
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The Sigma Insight: Fundamental Theorem & Properties of Definite Integrals
Analyzing the Setup
Welcome, fellow traveler of the mathematical landscape. Today, we stand before an integral that looks, at first glance, like a chaotic mess of exponentials and trigonometric functions.
You might feel a slight tremor of hesitation—that is perfectly normal. But remember, in the world of JEE Advanced, complexity is often just a mask for hidden elegance. Let us peel back that mask together.
We begin with our integral:
I=π2∫−4π4π(1+esinx)(2−cos2x)dx
The Power of King's Rule
Whenever you see symmetric limits like [−4π,4π], your intuition should immediately scream 'King's Rule!' This property, ∫abf(x)dx=∫abf(a+b−x)dx, is the ultimate tool for simplifying symmetric integrands.
Since our sum of limits a+b is 0, replacing x with −x is our first move. As we substitute, we use the fact that sin(−x)=−sinx and cos(−2x)=cos2x.
The integral transforms into:
I=π2∫−4π4π(1+e−sinx)(2−cos2x)dx
The Beautiful Cancellation
Now, watch the magic happen. When we add our original integral to this new version, we get 2I. Look at the bracketed term:
1+esinx1+1+e−sinx1
If you multiply the second fraction by esinxesinx, it becomes esinx+1esinx. When you add this to the first term, the numerators and denominators match perfectly!
The entire exponential mess collapses into 1. We are left with the much cleaner:
2I=π2∫−4π4π2−cos2xdx
Exploiting Even Symmetry
Since f(x)=2−cos2x1 is an even function, we can simplify our work by integrating from 0 to 4π and doubling the result. This gives us:
I=π2∫04π2−cos2xdx
Now, how do we handle the trigonometric denominator? We use the half-angle identity:
cos2x=1+tan2x1−tan2x
Substituting this into our integral, we get:
I=π2∫04π2−1+tan2x1−tan2xdx
The Final Transformation
After simplifying the complex fraction, the 1+tan2x term jumps to the numerator, becoming sec2x. Our integral now looks like this:
I=π2∫04π1+3tan2xsec2xdx
This is the moment of truth. We set t=3tanx, which implies dt=3sec2xdx. Our limits change from [0,4π] to [0,3].
The integral becomes:
I=π32∫031+t2dt
The Grand Finale
This is a standard form! The integral of 1+t21 is simply tan−1t. Evaluating this from 0 to 3, we get tan−1(3)−tan−1(0)=3π.
Finally, we calculate I:
I=π32×3π=332
Squaring this gives I2=274. Therefore, 27I2=27×274=4.
Take a deep breath. You have navigated through symmetry, trigonometric identities, and substitution to reach the summit. The final answer is 4.