Subtract lower limit from upper limit:
B−(−π2A)=B+π2A
Equate to the given condition:
B+π2A=π2A
Subtract π2A from both sides:
B=0
Final Conclusion
We found A=π4 from the derivative condition.
We found B=0 from the integral condition.
The constants are π4 and 0.
This matches Option 4.
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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 problem; we are peeling back the layers of a function to reveal its hidden identity.
We are given a function f(x)=Asin(2πx)+B, and we are tasked with finding the constants A and B. This is a classic JEE Advanced scenario where the problem provides two distinct 'keys'—the derivative and the integral—to unlock the two 'locks'—the constants A and B.
The Slope of the Curve
Our first key is the derivative condition: f′(21)=2. In the language of geometry, the derivative f′(x) is the slope of the tangent line to the curve at any point x.
To use this, we must first find the general expression for the derivative. We apply the differentiation operator to our function:
f′(x)=dxd[Asin(2πx)+B]
Using the linearity of the derivative, we treat the terms separately. The derivative of the constant B is 0. For the sine term, we invoke the Chain Rule:
f′(x)=A⋅2πcos(2πx)
Now, we substitute x=21 into this expression. The argument of the cosine becomes 2π⋅21=4π. Since cos(4π)=21, we equate this to our given condition:
A⋅2π⋅21=2
With a bit of algebraic finesse, we multiply both sides by 22. Since 2⋅2=2, the right side becomes 2⋅2=4. We are left with Aπ=4, which gives us our first constant:
A=π4
The Area Under the Curve
Now, let us turn our attention to the second key: the integral condition ∫01f(x)dx=π2A. This integral represents the net area bounded by the curve f(x) and the x-axis from x=0 to x=1.
We substitute our function into the integral:
∫01(Asin(2πx)+B)dx=π2A
Using the linearity of the integral, we split this into two parts:
A∫01sin(2πx)dx+∫01Bdx=π2A
Integrating the sine term, where the integral of sin(kx) is −k1cos(kx), we set k=2π. The integral becomes:
[−A⋅π2cos(2πx)+Bx]01=π2A
The Final Synthesis
Let us evaluate the limits with precision. At the upper limit x=1, we have −A⋅π2cos(2π)+B(1). Since cos(2π)=0, this simplifies to B.
At the lower limit x=0, we have −A⋅π2cos(0)+B(0). Since cos(0)=1, this simplifies to −A⋅π2.
According to the Fundamental Theorem of Calculus, we subtract the lower limit from the upper limit:
B−(−A⋅π2)=B+π2A
We equate this to the given condition π2A:
B+π2A=π2A
The terms π2A appear on both sides and cancel out, leaving us with B=0. We have successfully found our constants: A=π4 and B=0.