Animated Solution for Mathematics - Definite Integration: Comprehension Passage
Let f:[0,2π]→[0,1] be the function defined by f(x)=sin2x and let g:[0,2π]→[0,∞) be the function defined by g(x)=2πx−x2.
Question 1:
The value of 2∫0π/2f(x)g(x)dx−∫0π/2g(x)dx is ________.
Enter Numerical Value:
Question 2:
The value of π316∫0π/2f(x)g(x)dx is ________.
Enter Numerical Value:
Visualized Solution
Define Expression E
Let the given expression be E.
E=2∫0π/2f(x)g(x)dx−∫0π/2g(x)dx
Substitute f(x)=sin2x:
E=2∫0π/2sin2x⋅g(x)dx−∫0π/2g(x)dx
Combine Integrals
Both integrals have the same limits: 0 to 2π.
Factor out g(x)dx:
E=∫0π/2(2sin2x−1)g(x)dx
Trigonometric Identity
Recall the double angle identity:
cos(2x)=1−2sin2x
Therefore, 2sin2x−1=−cos(2x)
E=∫0π/2−cos(2x)g(x)dx
Substitute g(x)
Given: g(x)=2πx−x2
Substitute g(x) into the integral:
E=−∫0π/2cos(2x)(2πx−x2)dx
Split the Integral
Distribute cos(2x) and split into two integrals:
E=−2π∫0π/2xcos(2x)dx+∫0π/2x2cos(2x)dx
First Integral: Setup
Evaluate I1=∫0π/2xcos(2x)dx
Use Integration by Parts: ∫udv=uv−∫vdu
Let u=x⟹du=dx
Let dv=cos(2x)dx⟹v=2sin(2x)
First Integral: Compute
I1=[x2sin(2x)]0π/2−∫0π/22sin(2x)dx
First term: 2π/2⋅sin(π)−0=0
Second term: −21[−2cos(2x)]0π/2=41(cos(π)−cos(0))
I1=41(−1−1)=−21
Second Integral: Setup
Evaluate I2=∫0π/2x2cos(2x)dx
Use Integration by Parts again.
Let u=x2⟹du=2xdx
Let dv=cos(2x)dx⟹v=2sin(2x)
Second Integral: Compute
I2=[x22sin(2x)]0π/2−∫0π/22x2sin(2x)dx
First term is 0 (since sin(π)=sin(0)=0).
I2=−∫0π/2xsin(2x)dx
Apply parts again: −([x2−cos(2x)]0π/2−∫0π/22−cos(2x)dx)
I2=−(4π+0)=−4π
Substitute Back into E
Recall: E=−2πI1+I2
Substitute I1=−21 and I2=−4π:
E=−2π(−21)+(−4π)
Final Calculation
E=22π−4π
Multiply numerator and denominator of first term by 2:
E=4π2−4π
E=4π(2−1)
Conclusion & Discrepancy
Calculated value: E=4π(2−1)
Key Takeaway: Always trust your rigorous mathematical steps.
Note: The official answer key states 0, which implies a possible typo in the original question's function g(x).
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The Sigma Insight: Fundamental Theorem & Properties of Definite Integrals
Solution Diagram
Analyzing the Setup
Welcome, my fellow traveler, to the beautiful world of JEE Advanced calculus. Today, we are not just solving a problem; we are embarking on a journey.
We are looking at a function f(x)=sin2x and a polynomial g(x)=2πx−x2. At first glance, they seem like strangers, but through the lens of integration, they are about to perform a perfect, synchronized dance.
The Art of Simplification
We begin with our expression:
E=2∫0π/2f(x)g(x)dx−∫0π/2g(x)dx
The first instinct of a novice is to jump straight into the calculation. But the master educator pauses. Look at the structure!
Both integrals share the same limits, from 0 to 2π. This is our invitation to combine them. By factoring out g(x)dx, we transform our expression into:
E=∫0π/2(2sin2x−1)g(x)dx
Suddenly, the fog clears. That term (2sin2x−1) is not just a random collection of symbols; it is the negative of the double-angle identity for cosine: −cos(2x).
Our integral is now:
E=−∫0π/2cos(2x)g(x)dx
This is the power of trigonometric intuition.
The Divide and Conquer Strategy
Now, we introduce g(x)=2πx−x2 into the mix. Our integral becomes:
E=−∫0π/2cos(2x)(2πx−x2)dx
We distribute the −cos(2x) and split this into two distinct integrals, I1 and I2. This is our 'Divide and Conquer' strategy.
We are breaking a complex problem into two manageable pieces:
I1=∫0π/2xcos(2x)dx
I2=∫0π/2x2cos(2x)dx
The Mastery of Integration by Parts
Let us tackle I1. We have an algebraic term x multiplied by a trigonometric term cos(2x).
We use Integration by Parts: ∫udv=uv−∫vdu. By choosing u=x and dv=cos(2x)dx, we ensure that the derivative of u simplifies the expression.
Now, for I2=∫0π/2x2cos(2x)dx. This requires a second round of Integration by Parts.
We set u=x2 and dv=cos(2x)dx. The process is repetitive, but the beauty lies in the precision.
As we evaluate the boundary conditions, we see the terms involving sin(2x) vanish at both 0 and 2π. This leaves us with:
I2=−4π
The Final Synthesis
We have conquered the integrals. Now, we bring them back to our original expression E.
Substituting our values, we get E=−2πI1+I2. Plugging in I1=0 and I2=−4π, we arrive at the final result.
The final answer is:
E=−4π
My dear student, remember this: the journey is more important than the destination. You have mastered the identity, the integration by parts, and the algebraic manipulation. That is the true victory.