The Art of the Telescoping Series
Welcome, future engineer. Today, we are not just solving a problem; we are peeling back the layers of a beautiful trigonometric structure. In the JEE Advanced arena, you will often encounter expressions that look intimidating at first glance—like sinxsin2kx—but hide a simple, elegant truth.
Let us embark on this journey together.
Phase 1
The Identity
Imagine you are staring at the right-hand side of our identity: 2[cosx+cos3x+⋯+cos(2k−1)x]. It looks like a long, tedious sum.
But what if we could collapse it? The secret weapon here is the denominator on the left-hand side: sinx. If we multiply our sum by sinxsinx, we introduce the term 2sinxcos(nx) into every single part of the sum.
Why is this powerful? Because of the product-to-sum identity:
2sinAcosB=sin(A+B)−sin(A−B)
Let us apply this to the first term:
2sinxcosx=sin2x. Now the second term:
2sinxcos3x=sin(3x+x)−sin(3x−x)=sin4x−sin2x
Do you see the pattern emerging? The positive sin2x from the second term is about to meet the negative sin2x from the first term. This is the telescoping effect.
Phase 2
The Telescoping Magic
When we write out the full numerator, we get:
sin2x+(sin4x−sin2x)+(sin6x−sin4x)+⋯+(sin2kx−sin(2k−2)x)
It is like a row of dominoes falling. The sin2x cancels, the sin4x cancels, and so on.
Every intermediate term vanishes into thin air, leaving only the very last term: sin2kx. Thus, we have proven that the sum is exactly sinxsin2kx. We have tamed the beast.
Phase 3
The Integration
Now, we turn our attention to the integral:
I=∫0π/2sin2kxcotxdx
At first, this looks like a nightmare. How do you integrate cotx multiplied by a high-frequency sine wave?
But wait—we just proved that sin2kxcotx=sin2kxsinxcosx=(sinxsin2kx)cosx. And we know exactly what that fraction is!
Substituting our identity, the integral becomes:
I=∫0π/22[cosx+cos3x+⋯+cos(2k−1)x]cosxdx
Distributing the
cosx, we get terms like
2cos2x and
2cos(nx)cosx. Using the identity
2cosAcosB=cos(A+B)+cos(A−B), we transform the integrand into a simple sum of cosines:
1+cos2x+cos4x+⋯+cos2kx
Phase 4
The Final Victory
Integrating this is straightforward. The integral of 1 is x, and the integral of cos(nx) is nsin(nx).
When we evaluate this from 0 to π/2, something magical happens. Every single sine term, sin(2x),sin(4x),…,sin(2kx), becomes sin(π),sin(2π),…,sin(kπ) at the upper limit.
And what is the sine of any integer multiple of π? It is zero!
So, all those complex cosine terms vanish, leaving us with only the integral of the constant term
1. The result is simply:
2π−0=2π
This, my friend, is the essence of JEE Advanced physics and mathematics. It is not about brute force; it is about finding the hidden pattern, simplifying the complex, and watching the chaos resolve into order. Keep practicing, keep visualizing, and keep falling in love with the process.