Animated Solution for Mathematics - Indefinite Integration: Let I(x)=∫sin2x(1−cotx)26dx. If I(0)=3, then I(12π) is equal to
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Visualized Solution
Analyze the Integrand Structure
Given integral: I(x)=∫sin2x(1−cotx)26dx
Observe the trigonometric terms: sin2x1 and (1−cotx)
Goal: Simplify the integrand to find a suitable substitution.
Rewrite using csc2x
Using the identity: sin2x1=csc2x
Rewrite the integral: I(x)=∫(1−cotx)26csc2xdx
Apply Substitution Method
Let t=1−cotx
Differentiating both sides: dxdt=0−(−csc2x)
Therefore, dt=csc2xdx
Transform the Integral
Substitute t and dt into the integral:
I=∫t26dt=6∫t−2dt
Integrate with respect to t
Using power rule ∫tndt=n+1tn+1:
I=6(−1t−1)+C
I=−t6+C
Back-Substitution
Substitute t=1−cotx back:
I(x)=−1−cotx6+C
Analyze the Limit at x=0
Rewrite using cotx=sinxcosx:
I(x)=−1−sinxcosx6+C=−sinx−cosx6sinx+C
As x→0, I(0)=0−1−6(0)+C=0+C
Find the Constant C
Given I(0)=3, and we found I(0)=C
⟹C=3
The complete function is: I(x)=3−1−cotx6
Evaluate at x=12π
We need I(12π). Note: cot(12π)=2+3
Substitute into I(x):
I(12π)=3−1−(2+3)6
Simplify the Expression
Simplify denominator: 1−2−3=−1−3
I(12π)=3−−(1+3)6=3+3+16
Rationalize: 3+(3+1)(3−1)6(3−1)
Final Calculation
Denominator becomes: (3)2−12=3−1=2
I(12π)=3+26(3−1)
I(12π)=3+3(3−1)=3+33−3
Final Answer: 33
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The Sigma Insight: Integration by Substitution
Solution Diagram
Analyzing the Setup
Welcome, future engineers. Today, we are not just solving an integral; we are embarking on a journey of pattern recognition and mathematical elegance.
When you first look at the problem
I(x)=∫sin2x(1−cotx)26dx
it is natural to feel a slight hesitation. The expression looks cluttered, almost chaotic. But in the world of JEE Advanced, chaos is often just order in disguise.
The Anatomy of the Integrand
Every great integration begins with a moment of observation. We see a sin2x in the denominator and a (1−cotx)2 term. Your mathematical intuition should immediately scream: "Trigonometric Identity!"
We know that sin2x1 is the reciprocal of sin2x, which is csc2x. By rewriting the integral as
I(x)=∫(1−cotx)26csc2xdx
the problem suddenly shifts from a confusing mess to a beautiful, structured form.
We have created a relationship between the numerator and the denominator. We have a function, (1−cotx), and its derivative, csc2x, sitting right there in the numerator. This is the hallmark of a perfect substitution.
The Magic of Substitution
Now, let us perform the substitution. We set t=1−cotx.
When we differentiate both sides with respect to x, we get dxdt=0−(−csc2x), which simplifies beautifully to dxdt=csc2x. This means dt=csc2xdx.
Our integral transforms into
I=∫t26dt=6∫t−2dt
This is the moment where the tension breaks. We have moved from the realm of complex trigonometry into the realm of simple algebraic power rules.
The Power of Integration
Applying the power rule ∫tndt=n+1tn+1, we find that the integral of t−2 is −1t−1. Multiplying by our constant 6, we arrive at
I=−t6+C
Do not forget the constant of integration, C! It is the ghost in the machine, the piece of information that defines the specific curve among the family of curves. We then substitute back to get
I(x)=−1−cotx6+C
The Boundary Trap
The problem states I(0)=3. If you try to plug x=0 directly into cotx, you will find it is undefined. This is the "Trap" I warned you about.
We rewrite cotx as sinxcosx to get
I(x)=−1−sinxcosx6+C=−sinx−cosx6sinx+C
Now, as x→0, sinx→0 and cosx→1. The expression becomes 0−1−6(0)+C, which is simply 0+C. Since we are given I(0)=3, we immediately find that C=3.
The Final Victory
Our specific function is I(x)=3−1−cotx6. Finally, we evaluate at x=12π.
We know that cot(12π)=2+3. Substituting this in, we get
I(12π)=3−1−(2+3)6=3−−1−36=3+1+36
To finish, we rationalize the denominator by multiplying by the conjugate (3−1). The denominator becomes (3)2−12=2.
Thus, we have
3+26(3−1)=3+3(3−1)=3+33−3
The 3 and −3 cancel out, leaving us with the elegant final answer: 33.