Analyzing the Setup
Welcome, fellow traveler on the path to JEE excellence. Today, we are going to look at an integral that, at first glance, appears to be a nightmare of transcendental functions:
I=∫0πecosx+e−cosxecosxdx
I know what you are thinking—how on earth do we integrate an exponential function of a cosine? If you try to use standard substitution, you will quickly find yourself in a loop of frustration. But here is the secret: in mathematics, when a problem looks impossible, it is usually because we are looking at it from the wrong angle.
The King's Property
A Strategic Masterstroke
In the world of definite integrals, there is a legendary tool known as the 'King's Property.' It states that for any continuous function f(x) on the interval [0,a], the integral ∫0af(x)dx is identical to ∫0af(a−x)dx.
Why is this so powerful? Because it allows us to transform the variable x into something that interacts beautifully with the limits of integration. In our case, a=π. Let us apply this transformation by replacing x with (π−x).
The Transformation
When we substitute x=π−x, our integral becomes:
I=∫0πecos(π−x)+e−cos(π−x)ecos(π−x)dx
Now, pause for a moment and recall your trigonometry. We know that cos(π−x)=−cosx.
This is the moment of truth. By substituting this identity, our integral transforms into:
I=∫0πe−cosx+ecosxe−cosxdx
Look closely at this new expression. The denominator is identical to our original integral, just rearranged!
The Grand Cancellation
This is where the magic happens. We now have two expressions for the same value I. Let us add them together:
2I=∫0πecosx+e−cosxecosxdx+∫0πe−cosx+ecosxe−cosxdx
Because the denominators are the same, we can combine the integrands into a single fraction:
2I=∫0πecosx+e−cosxecosx+e−cosxdx
Take a deep breath and look at that fraction. The numerator and the denominator are exactly the same! They cancel out perfectly to leave us with the integral of 1. The terrifying exponential functions have vanished, leaving behind the simplest possible integrand:
The Final Victory
Now, the path is clear. The integral of 1 with respect to x is simply x. Evaluating this from 0 to π, we get:
So, we have 2I=π. Dividing by 2, we arrive at our final answer:
Isn't it beautiful? We started with a complex, intimidating expression and, through the clever application of symmetry, reduced it to a simple constant. This is the essence of JEE Advanced mathematics: it is not about brute force; it is about finding the elegant path that nature has hidden in plain sight.