Animated Solution for Mathematics - Definite Integration: The value of ∫−1/21/2((x−1x+1)2+(x+1x−1)2−2)1/2dx is:
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Visualized Solution
Analyze Integrand I
Given integral: I=∫−2121((x−1x+1)2+(x+1x−1)2−2)21dx
Let a=x−1x+1 and b=x+1x−1
Identify Perfect Square (a−b)2
Notice that a⋅b=x−1x+1⋅x+1x−1=1
The expression is a2+b2−2ab=(a−b)2
Integrand becomes (a−b)2=∣a−b∣
Simplify a−b
Simplify a−b:
x−1x+1−x+1x−1=(x−1)(x+1)(x+1)2−(x−1)2
=x2−1(x2+2x+1)−(x2−2x+1)=x2−14x
Simplified Integral I
I=∫−2121x2−14xdx
Let f(x)=x2−14x
Since f(−x)=f(x), f(x) is an even function.
Apply Symmetry ∫−aaf(x)dx
Using property: ∫−aaf(x)dx=2∫0af(x)dx for even functions.
I=2∫021x2−14xdx
Analyze Modulus ∣x∣
For x∈[0,21], x2<21<1
So, x2−1<0 and 4x≥0
Thus, x2−14x=−x2−14x=1−x24x
Set up Final Integral
I=2∫0211−x24xdx
I=4∫0211−x22xdx
Substitute u=1−x2
Let u=1−x2⟹du=−2xdx
When x=0,u=1; when x=21,u=21
I=4∫121u−du=4∫211udu
Evaluate ∫udu
I=4[lnu]211
=4(ln1−ln(21))
=4(0−(−ln2))=4ln2
Final Answer loge16
I=ln(24)=ln16
Final Answer: loge16
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The Sigma Insight: Fundamental Theorem & Properties of Definite Integrals
Solution Diagram
The Beauty of Hidden Symmetry
Welcome, fellow traveler on the path to JEE excellence. Today, we are going to dismantle a problem that, at first glance, looks like a chaotic mess of fractions and square roots.
You see an integral like:
I=∫−1/21/2((x−1x+1)2+(x+1x−1)2−2)1/2dx
Your instinct might be to panic. But I want you to take a deep breath. In mathematics, complexity is often just a mask for a simple, elegant truth waiting to be revealed.
Phase 1
Unmasking the Integrand
Let us look at the expression inside the square root. It is a classic algebraic structure.
Let us define A=x−1x+1 and B=x+1x−1. Notice the beautiful relationship between them:
A⋅B=(x−1x+1)⋅(x+1x−1)=1
This is not a coincidence; it is the key to the entire problem. The expression inside the root is A2+B2−2.
Since A⋅B=1, we can rewrite this as A2+B2−2AB. Does that look familiar? It is the expansion of (A−B)2!
So, our integrand simplifies to (A−B)2, which is simply ∣A−B∣. We have already tamed the monster.
Phase 2
The Power of Symmetry
Now, let us simplify A−B. We have:
x−1x+1−x+1x−1
Finding a common denominator, we get:
x2−1(x+1)2−(x−1)2=x2−14x
Our integral is now I=∫−1/21/2x2−14xdx.
Here is where we use the symmetry of the function. Because f(x)=x2−14x is an even function, the area under the curve from −1/2 to 0 is identical to the area from 0 to 1/2.
We can rewrite our integral as:
I=2∫01/2x2−14xdx
This is the kind of strategic thinking that wins exams.
Phase 3
The Modulus Trap
We must be careful. In the interval [0,1/2], x2 is less than 1/2, which means x2−1 is negative.
To remove the modulus, we must flip the sign: ∣x2−1∣=1−x2. Our integral becomes:
I=2∫01/21−x24xdx
To make this even cleaner, let us pull a 2 out of the 4x to get:
I=4∫01/21−x22xdx
Why did we do this? Because 2x is the derivative of x2, and by extension, −2x is the derivative of 1−x2. This is a perfect setup for substitution.
Phase 4
The Final Integration
Let u=1−x2. Then du=−2xdx.
When x=0, u=1. When x=1/2, u=1−1/2=1/2. Substituting these into our integral, we get:
I=4∫11/2u−du
The negative sign allows us to flip the limits:
I=4∫1/21udu
The integral of 1/u is ln∣u∣. Evaluating this, we get 4[ln(1)−ln(1/2)].
Since ln(1)=0 and −ln(1/2)=ln(2), we are left with 4ln(2). Using the logarithmic power rule, 4ln(2)=ln(24)=ln(16).
We started with a terrifying expression and ended with a clean, elegant ln(16). This is the joy of mathematics—taking the complex and finding the simple, logical path through it.