Combine both parts: I=(Boundary Term)+(Integral Term)
I=loge2+2π−1
Key Takeaways:
1. Always check for Even/Odd symmetry with limits [−a,a].
2. IBP is powerful for logarithmic integrands.
3. Simplify derivatives before re-integrating.
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The Sigma Insight: Fundamental Theorem & Properties of Definite Integrals
Solution Diagram
The Symmetry of the Logarithmic Integral
A Journey Through Calculus
Welcome, fellow traveler on the road to JEE Advanced excellence. Today, we are going to dissect a problem that, at first glance, might seem like a daunting thicket of square roots and logarithms.
But as we peel back the layers, you will see that this problem is a masterclass in elegance and strategic thinking. Let us begin with the integral:
I=∫−11loge(1−x+1+x)dx
When you see limits of the form [−a,a], your mathematical spider-sense should immediately tingle. This is the universe whispering to you: "Check for symmetry."
Phase 1
The Mirror Image
Let f(x)=loge(1−x+1+x). To check for symmetry, we perform the substitution x→−x.
As we calculate f(−x)=loge(1−(−x)+1+(−x)), we see the terms inside the square roots simply swap places:
f(−x)=loge(1+x+1−x)
Because addition is commutative, f(−x)=f(x). Our function is perfectly even, meaning its graph is a mirror image across the y-axis.
This allows us to invoke the property ∫−aaf(x)dx=2∫0af(x)dx. Our integral now becomes:
I=2∫01loge(1−x+1+x)dx
We have successfully cut our work in half and anchored our lower limit at zero. This is the first victory.
Phase 2
The Tool of Integration by Parts
Now, we face the challenge of integrating a lone logarithmic function. The standard tool in our arsenal is Integration by Parts (IBP), guided by the ILATE rule.
We set u=loge(1−x+1+x) and dv=dx. Consequently, v=x.
The real test lies in finding du. We must use the chain rule:
du=1−x+1+x1⋅dxd(1−x+1+x)dx
This yields:
du=1−x+1+x1⋅(21−x−1+21+x1)dx
I know this looks terrifying, but take a breath. We are about to perform an algebraic dance to simplify this.
Phase 3
The Algebraic Masterstroke
To simplify du, we take the lowest common multiple inside the bracket:
du=1−x+1+x1⋅(21−x21−x−1+x)dx
Now, we rationalize the expression by multiplying the numerator and denominator by the conjugate (1−x−1+x). After expanding and canceling, we arrive at the much neater:
du=2x1−x21−x2−1dx
This simplification is the heart of the problem. When we plug this into the IBP formula I=2[uv]01−2∫01vdu, the x in our v term and the x in the denominator of du cancel out perfectly!
We are left with:
I=2[xloge(1−x+1+x)]01+∫011−x21−1−x2dx
Phase 4
The Final Integration
Evaluating the boundary term is straightforward. At x=1, we get 2loge(2)=loge2. At x=0, the term vanishes.
Now, for the remaining integral:
∫01(1−x21−1)dx
These are standard, elementary integrals. The first part is sin−1x, and the second is x.
Evaluating from 0 to 1, we get (sin−1(1)−1)−(0−0)=2π−1.
Combining our boundary term and our integral, we reach the final answer:
I=loge2+2π−1
You have navigated the symmetry, mastered the IBP, and conquered the algebra. This is the essence of JEE Advanced mathematics—not just calculation, but the art of simplification.