Analyzing the Setup
The problem presents an integral equation:
∫01f(λx)dλ=af(x)
We are given that
f is twice differentiable, with boundary conditions
f(1)=1 and
f(16)=81. Our objective is to determine the value of
16−f′(161).
Phase 1
The Transformation
To simplify the integral, we perform a substitution. Let u=λx, which implies du=xdλ or dλ=xdu.
Adjusting the limits of integration: when
λ=0,
u=0; when
λ=1,
u=x. Substituting these into the original equation yields:
x1∫0xf(u)du=af(x)
Multiplying both sides by
x, we obtain the simplified integral form:
∫0xf(u)du=axf(x)
Phase 2
The Calculus Bridge
We apply the Newton-Leibniz theorem by differentiating both sides with respect to x. The derivative of the left side is simply f(x).
Applying the product rule to the right side,
axf(x), we get:
f(x)=a[f(x)+xf′(x)]
Rearranging the terms to isolate the derivative, we arrive at:
(1−a)f(x)=axf′(x)
Phase 3
Solving the Differential Equation
We now have a first-order separable differential equation:
f(x)f′(x)=ax1−a
Integrating both sides with respect to
x gives:
lnf(x)=a1−alnx+C
Exponentiating both sides, we find the general form
f(x)=kxa1−a. Using the condition
f(1)=1, we determine
k=1, resulting in:
f(x)=xa1−a
Phase 4
Finding the Constants
We use the second condition,
f(16)=81, to solve for
a:
16a1−a=81
Expressing both sides as powers of
2:
(24)a1−a=2−3
Equating the exponents, we have
4(a1−a)=−3. Solving for
a:
4−4a=−3a⇒a=4
Substituting
a=4 back into our function, we get:
f(x)=x41−4=x−43
Phase 5
The Final Victory
We calculate the derivative
f′(x):
f′(x)=−43x−47
Evaluating this at
x=161:
f′(161)=−43(161)−47=−43(16)47=−43(24)47=−43(27)=−96
Finally, the requested value is:
16−f′(161)=16−(−96)=112