Animated Solution for Mathematics - Indefinite Integration: If I(x)=∫esin2x(cosxsin2x−sinx)dx and I(0)=1, then I(3π) is equal to
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Visualized Solution
The Integral I(x)
Given: I(x)=∫esin2x(cosxsin2x−sinx)dx
Initial condition: I(0)=1
Objective: Find I(3π)
Substitution for Exponent
The term esin2x suggests substituting the exponent.
Let t=sin2x
Finding dt
Differentiate t=sin2x with respect to x:
dxdt=2sinxcosx
Using the double angle identity: 2sinxcosx=sin2x
Therefore, dt=sin2xdx
Extracting sin2x
We need sin2x in the integrand to replace with dt.
Original term: (cosxsin2x−sinx)
Multiply and divide sinx by 2cosx:
sinx=2cosx2sinxcosx=2cosxsin2x
Factor out sin2x: sin2x(cosx−2cosx1)
Converting to t
We have: ∫et(cosx−2cosx1)sin2xdx
Replace sin2xdx with dt.
Since t=sin2x, we know cos2x=1−t.
Therefore, cosx=1−t.
The integral becomes: ∫et(1−t−21−t1)dt
The Classic Integral Form
Notice the structure: ∫et(f(t)+f′(t))dt
Let f(t)=1−t
Differentiate f(t) using the chain rule:
f′(t)=21−t1⋅dtd(1−t)=−21−t1
Integrating and Reverting to x
The standard result is: ∫et(f(t)+f′(t))dt=etf(t)+C
Applying this: I(x)=et1−t+C
Back-substitute t=sin2x and 1−t=cosx:
I(x)=esin2xcosx+C
Evaluating C
Use the given initial condition: I(0)=1
Substitute x=0 into I(x):
I(0)=esin20cos0+C
Since sin0=0 and cos0=1:
1=e0⋅1+C⟹1=1+C⟹C=0
Thus, I(x)=esin2xcosx
Calculating I(π/3)
We need to find I(3π).
Substitute x=3π:
sin3π=23⟹sin23π=43
cos3π=21
I(3π)=e43⋅21=21e43
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The Sigma Insight: Evaluation of Special Integral Forms
Analyzing the Setup
Imagine you are standing before a complex, intimidating integral:
I(x)=∫esin2x(cosxsin2x−sinx)dx
It looks like a tangled mess of trigonometric functions and exponential growth. In the world of JEE Advanced, intimidation is just a sign that you haven't yet seen the underlying symmetry. Let's embark on a journey to uncover it.
The Power of Substitution
The first thing that should catch your eye is the exponent: sin2x. Whenever you see a function in the exponent of e, your mathematical intuition should immediately suggest a substitution.
Let us set t=sin2x. Now, we need to find dt. Differentiating t with respect to x, we get:
dxdt=2sinxcosx
Using the double angle identity, this is simply sin2x. Thus, dt=sin2xdx. This is our golden ticket.
The Algebraic Puzzle
Now, look at the integrand: (cosxsin2x−sinx). We have a sin2x term, but we also have a pesky −sinx.
To make this work with our dt=sin2xdx, we need to express everything in terms of sin2x. We can rewrite sinx as:
sinx=2cosx2sinxcosx=2cosxsin2x
Now, our integrand becomes:
sin2x(cosx−2cosx1)
This is the breakthrough! We have successfully factored out the sin2x that we need for our dt.
The Elegant Form
With t=sin2x, we know that cos2x=1−t, so cosx=1−t. Substituting this into our integral, we get:
∫et(1−t−21−t1)dt
Does this look familiar? It is the classic form ∫et(f(t)+f′(t))dt.
If we let f(t)=1−t, then its derivative f′(t) is indeed:
f′(t)=−21−t1
The integral of this form is simply etf(t)+C.
The Final Victory
Applying this, we get I(x)=et1−t+C. Substituting back t=sin2x and 1−t=cosx, we arrive at:
I(x)=esin2xcosx+C
Using the initial condition I(0)=1, we find C=0. Finally, evaluating at x=3π, we have sin2(3π)=43 and cos(3π)=21.
The final result is:
21e43
You see? What started as a terrifying expression was just a beautiful, hidden structure waiting for you to reveal it. Keep practicing, and you will start seeing these patterns everywhere!