Animated Solution for Mathematics - Definite Integration: Let F(x)=∫xx2+6π2cos2t(dt) for all x∈R and f:[0,1/2]→[0,∞) be a continuous function. For α∈[0,1/2], if F′(α)+2 is the area of the region bounded by x=0,y=0,y=f(x) and x=α, then f(0) is
Enter Numerical Value:
Visualized Solution
A(α)=∫0αf(x)dx
Let A(α) be the area bounded by x=0, y=0, y=f(x), and x=α.
A(α)=∫0αf(x)dx
Given condition: A(α)=F′(α)+2
dαdA(α)=f(α)
Differentiating A(α) using the Fundamental Theorem of Calculus:
dαdA(α)=f(α)
Differentiating the given relation: f(α)=F′′(α)
Conclusion: To find f(0), we need F′′(0).
The Leibniz Rule
The Leibniz Rule for differentiating under the integral sign:
dxd∫g(x)h(x)w(t)dt=w(h(x))⋅h′(x)−w(g(x))⋅g′(x)
Applying Leibniz Rule
F(x)=∫xx2+6π2cos2tdt
Here, w(t)=2cos2t, g(x)=x, and h(x)=x2+6π
F′(x)
F′(x)=2cos2(x2+6π)⋅dxd(x2+6π)−2cos2(x)⋅dxd(x)
F′(x)=2cos2(x2+6π)⋅(2x)−2cos2(x)⋅(1)
F′(x)=4xcos2(x2+6π)−2cos2x
Differentiating F′(x)
We need F′′(x), so we differentiate F′(x) again.
Let T1=4xcos2(x2+6π)
Let T2=−2cos2x
F′′(x)=dxdT1+dxdT2
dxdT1
Using the product rule on T1=4xcos2(x2+6π):
dxdT1=4cos2(x2+6π)+4x⋅dxd[cos2(x2+6π)]
Note: We don't need to fully expand the second part because it has a factor of x, which will become zero at x=0.
dxdT2
Differentiating T2=−2cos2x:
dxdT2=−2⋅[2cosx⋅(−sinx)]
dxdT2=4sinxcosx=2sin2x
F′′(x)
F′′(x)=4cos2(x2+6π)+4x⋅dxd[cos2(x2+6π)]+2sin2x
This is our f(x) function.
f(0)=F′′(0)
Substitute x=0 into F′′(x):
f(0)=4cos2(02+6π)+4(0)⋅(…)+2sin(2⋅0)
The second and third terms become zero.
f(0)=4cos2(6π)
Final Calculation
We know that cos(6π)=23
cos2(6π)=(23)2=43
f(0)=4⋅43=3
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The Sigma Insight: Newton-Leibniz & Reduction Formulas
Solution Diagram
Analyzing the Setup
Welcome, fellow explorer of the mathematical universe. Today, we are going to unravel a problem that might look like a tangled mess of integrals and derivatives, but beneath the surface, it is a beautifully choreographed dance between geometry and analysis.
We are tasked with finding f(0), given a complex integral definition for F(x) and a relationship involving the area under f(x). Let us break this down, step by step, and see how the pieces fall into place.
The Area Connection
Imagine a curve representing the function f(x). We are interested in the area bounded by this curve, the x-axis, the y-axis, and a vertical line at x=α.
Mathematically, we define this area as:
A(α)=∫0αf(x)dx
The problem provides the relationship A(α)=F′(α)+2. To find f(0), we need to connect f to F.
If we differentiate both sides of this equation with respect to α, the Fundamental Theorem of Calculus tells us that the derivative of the integral is simply f(α). On the right side, the derivative of F′(α)+2 is F′′(α) (since the derivative of the constant 2 is zero).
Thus, we arrive at our target:
f(α)=F′′(α)
To find f(0), we simply need to calculate F′′(0).
The Leibniz Rule
Now, we turn our attention to the definition of F(x):
F(x)=∫xx2+6π2cos2tdt
This is where we invoke the Leibniz Rule for differentiating under the integral sign. This rule is our secret weapon:
dxd∫g(x)h(x)w(t)dt=w(h(x))⋅h′(x)−w(g(x))⋅g′(x)
Here, our integrand w(t) is 2cos2t, our lower limit g(x) is x, and our upper limit h(x) is x2+6π.
The Differentiation
Let us apply the rule. First, we evaluate the integrand at the upper limit and multiply by the derivative of the upper limit:
2cos2(x2+6π)⋅dxd(x2+6π)=2cos2(x2+6π)⋅(2x)
Next, we subtract the integrand evaluated at the lower limit, multiplied by the derivative of the lower limit:
2cos2(x)⋅dxd(x)=2cos2(x)⋅(1)
Putting it together, we get:
F′(x)=4xcos2(x2+6π)−2cos2x
The Second Derivative and the Elegant Collapse
We need F′′(x), so we differentiate F′(x) again. Let us split F′(x) into two terms: T1=4xcos2(x2+6π) and T2=−2cos2x.
For T1, we use the product rule:
dxdT1=4cos2(x2+6π)+4x⋅dxd[cos2(x2+6π)]
For T2, we use the chain rule:
dxdT2=−2⋅[2cosx⋅(−sinx)]=4sinxcosx=2sin2x
Now, we combine them:
F′′(x)=4cos2(x2+6π)+4x⋅dxd[cos2(x2+6π)]+2sin2x
Finally, we evaluate at x=0. The term with 4x vanishes, and 2sin(2⋅0) is also zero. We are left with:
f(0)=4cos2(6π)
Since cos(6π)=23, then cos2(6π)=43. Thus:
f(0)=4⋅43=3
The complexity dissolves, leaving us with a clean, elegant integer. The final answer is 3.