The Beauty of Algebraic Symmetry
Welcome, future engineer! Today, we are going to peel back the layers of an inverse trigonometry problem that, at first glance, might seem like a tangled mess of functions.
But I want you to take a deep breath. In JEE Advanced, the most intimidating problems are often just simple identities wearing a disguise. Let's embark on this journey together.
Phase 1
The Algebraic Dance
We start with the equation (sin−1x)2−(cos−1x)2=a. Your intuition might scream, "Should I find x?" No! That is the trap.
Instead, look at the structure. It is a perfect difference of squares, A2−B2, which we know expands to (A+B)(A−B).
By treating A=sin−1x and B=cos−1x, we factorize our equation into:
(sin−1x+cos−1x)(sin−1x−cos−1x)=a
Suddenly, the complexity begins to dissolve.
Phase 2
The Bridge of Identities
Now, look at that first bracket: (sin−1x+cos−1x). Does it ring a bell? It is the bedrock of inverse trigonometry!
We know that for any x∈[−1,1], the following identity holds:
Since our constraint is 0<x<1, we are perfectly safe to use this. Substituting this into our equation, we get:
By multiplying both sides by π2, we isolate the difference:
We have successfully reduced a quadratic-looking equation into a linear one.
Phase 3
The Final Transformation
We are almost there, but we have two different functions. Let's unify them.
Using the identity sin−1x=2π−cos−1x, our equation becomes:
Combining the terms, we arrive at:
Rearranging this gives us:
The Grand Finale
Here is the masterstroke. We need to find 2x2−1. Recall the double angle property:
Substituting this in, we get:
To free our target expression, we take the cosine of both sides:
Using the allied angle identity cos(2π−θ)=sinθ, we finally arrive at the result:
See how the pieces fit? We didn't fight the math; we guided it. Keep this mindset, and you will conquer any problem the exam throws at you!