Core Concept: Substitution followed by Integration by Parts.
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The Sigma Insight: Fundamental Theorem & Properties of Definite Integrals
Solution Diagram
The Beauty of Transformation
Solving the Integral of 1−x2xsin−1x
Welcome, fellow traveler of the mathematical landscape. Today, we stand before a problem that might seem daunting at first glance: the integral of 1−x2xsin−1x from 0 to 1.
It looks like a tangled mess, doesn't it? But in the world of JEE Advanced, complexity is often just a mask for elegance. Let's peel back the layers together.
Phase 1
The Detective Work
When you look at an integral, don't just see a collection of symbols. See the relationships. We have x, we have sin−1x, and we have 1−x21 hiding in the denominator.
A seasoned eye immediately spots the relationship: the derivative of sin−1x is exactly 1−x21. This is our golden ticket. It tells us that the integrand is not just a random collection of functions; it is a structured, solvable puzzle.
Phase 2
The Transformation
We are going to shift our entire problem from the x-world into the θ-world. We set θ=sin−1x, which immediately implies x=sinθ.
Now, we need to handle the differential dx. Differentiating x=sinθ with respect to θ gives us:
dx=cosθdθ
But wait! We must not forget the limits. When x=0, θ=sin−1(0)=0. When x=1, θ=sin−1(1)=2π. Our new boundaries are set from 0 to 2π.
Phase 3
The Simplification
Now, let's plug these values into our integral:
I=∫02π1−sin2θ(sinθ)⋅θ⋅cosθdθ
Look at the denominator. 1−sin2θ is simply cosθ. The cosθ in the denominator and the cosθ from our dx term cancel out beautifully!
We are left with the much simpler integral:
I=∫02πθsinθdθ
Phase 4
The Integration by Parts
We have arrived at a product of two functions: an algebraic function, θ, and a trigonometric function, sinθ. This is the perfect candidate for Integration by Parts. Using the ILATE rule, we choose u=θ and dv=sinθdθ.
Applying the formula ∫udv=uv−∫vdu, we get:
I=[θ(−cosθ)]02π−∫02π(1)(−cosθ)dθ
The two minus signs multiply to become a plus, giving us:
I=[−θcosθ]02π+∫02πcosθdθ
The integral of cosθ is sinθ. So, our final expression is:
[−θcosθ+sinθ]02π
Phase 5
The Final Evaluation
Now, we just need to plug in the limits. At the upper limit θ=2π:
−(2π)cos(2π)+sin(2π)=−(2π)(0)+1=1
At the lower limit θ=0:
−(0)cos(0)+sin(0)=0+0=0
Subtracting the lower limit from the upper limit, we get 1−0=1.
And there it is! The complexity vanishes, leaving behind a clean, elegant result. The final answer is 1.