Animated Solution for Mathematics - Definite Integration: If f:R→R be a continuous function satisfying ∫0π/2f(sin2x)sinxdx+α∫0π/4f(cos2x)cosxdx=0, then the value of α is
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Visualized Solution
Defining the First Integral I
Let I=∫0π/2f(sin2x)sinxdx
Given: I+α∫0π/4f(cos2x)cosxdx=0
Splitting the Integral at 4π
Split the integral at x=4π:
I=∫0π/4f(sin2x)sinxdx+∫π/4π/2f(sin2x)sinxdx
Applying Substitution x=2π−t
In the second integral, let x=2π−t
Differentiating both sides: dx=−dt
Limits: x=4π⟹t=4π
Limits: x=2π⟹t=0
Transforming the Integrand
Substitute x in the functions:
sin2x=sin(2(2π−t))=sin(π−2t)=sin2t
sinx=sin(2π−t)=cost
Simplifying the Second Integral
The second integral becomes:
∫π/40f(sin2t)cost(−dt)
Using ∫ab=−∫ba, flip the limits:
∫0π/4f(sin2x)cosxdx
Combining the Two Parts
Combine both parts of I:
I=∫0π/4f(sin2x)sinxdx+∫0π/4f(sin2x)cosxdx
I=∫0π/4f(sin2x)(sinx+cosx)dx
Substitution x=4π−t
To match f(cos2x), let x=4π−t
Then dx=−dt
Limits swap: 0→4π and 4π→0
sin2x=sin(2(4π−t))=sin(2π−2t)=cos2t
Transforming the Trigonometric Sum
Transform the sum sinx+cosx:
=sin(4π−t)+cos(4π−t)
=(21cost−21sint)+(21cost+21sint)
=2cost
Final Form of I
Substitute everything back into I:
I=∫π/40f(cos2t)(2cost)(−dt)
Flip the limits using the negative sign:
I=2∫0π/4f(cos2x)cosxdx
Solving for α
Substitute I into the original equation:
2∫0π/4f(cos2x)cosxdx+α∫0π/4f(cos2x)cosxdx=0
(2+α)∫0π/4f(cos2x)cosxdx=0
⟹2+α=0⟹α=−2
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The Sigma Insight: Fundamental Theorem & Properties of Definite Integrals
Solution Diagram
Analyzing the Setup
Welcome, future engineer. Today, we are not just solving a math problem; we are embarking on a journey through the elegance of calculus.
When you first look at the equation
∫0π/2f(sin2x)sinxdx+α∫0π/4f(cos2x)cosxdx=0
it is natural to feel a bit overwhelmed. You see an arbitrary function f, two different limits, and a mysterious constant α. But take a deep breath; in the world of JEE Advanced, complexity is often just a mask for symmetry.
Phase 1
The Divide and Conquer
Our first objective is to make the two integrals speak the same language. The first integral, let us call it I, spans from 0 to π/2.
The second integral spans from 0 to π/4. The discrepancy in limits is our first clue. We must split I at the point x=π/4.
By the fundamental properties of definite integrals, we can write I as:
I=∫0π/4f(sin2x)sinxdx+∫π/4π/2f(sin2x)sinxdx
Now, the first part is already aligned with our target. The second part, however, is the one that needs our attention.
Phase 2
The Mirroring Principle
Look at the second integral: ∫π/4π/2f(sin2x)sinxdx. We want the limits to be 0 to π/4.
We use the substitution x=π/2−t. This is the 'Reflection Principle.' When x=π/4, t=π/4. When x=π/2, t=0. The differential dx becomes −dt.
As we substitute, sin2x becomes sin(2(π/2−t))=sin(π−2t)=sin2t. Similarly, sinx becomes sin(π/2−t)=cost.
After accounting for the negative sign from the differential, the limits flip back to 0 to π/4. We have successfully transformed the second part into:
∫0π/4f(sin2t)costdt
Now, both parts of I share the same limits.
Phase 3
The Elegant Cancellation
We combine the parts:
I=∫0π/4f(sin2x)(sinx+cosx)dx
We are close, but our target involves f(cos2x), not f(sin2x). We need one final, powerful substitution: x=π/4−t. This is our 'Symmetry Bridge.'
Watch what happens to the argument: sin2x becomes sin(2(π/4−t))=sin(π/2−2t)=cos2t. This is exactly what we need.
Now, what about the term (sinx+cosx)? Substituting x=π/4−t gives us sin(π/4−t)+cos(π/4−t).
Using the compound angle formulas, this expands to:
(21cost−21sint)+(21cost+21sint)=2cost
The sint terms vanish into thin air, leaving us with 2cost.
The Endgame
Putting it all together, our integral I transforms into:
I=2∫0π/4f(cos2t)costdt
Substituting this back into our original equation, we get:
2∫0π/4f(cos2x)cosxdx+α∫0π/4f(cos2x)cosxdx=0
Factoring out the integral, we see that (2+α)×Integral=0. For this to hold for any continuous function f, the coefficient must be zero.
Thus, α=−2. You did it! You navigated the substitution, respected the symmetry, and emerged victorious.