Analyzing the Setup
We are given the equation:
6∫1xf(t)dt=3xf(x)−x3
Imagine this equation as a locked room. The function f(x) is inside, hidden behind the integral sign. To extract it, we use the Newton-Leibniz Theorem, which acts as the bridge between integration and differentiation.
Phase 1
The Newton-Leibniz Liberation
We differentiate both sides with respect to x. On the left side, the constant 6 remains, and the derivative of the integral ∫1xf(t)dt is simply f(x).
Thus, the left side becomes 6f(x).
On the right side, we apply the Product Rule: dxd(uv)=udxdv+vdxdu. The derivative of 3xf(x) is 3f(x)+3xf′(x), and the derivative of −x3 is −3x2.
Equating the two sides, we obtain:
6f(x)=3f(x)+3xf′(x)−3x2
Phase 2
Transformation into a Linear Differential Equation
We have successfully moved from an integral equation to a differential equation. Subtracting
3f(x) from both sides yields:
3f(x)=3xf′(x)−3x2
Dividing the entire equation by
3 simplifies it to:
f(x)=xf′(x)−x2
Rearranging to standard form, we get:
xf′(x)−f(x)=x2
To reach the standard
Linear Differential Equation (LDE) form,
dxdy+P(x)y=Q(x), we divide by
x:
f′(x)−x1f(x)=x
Here, our P(x)=−x1 and our Q(x)=x.
Phase 3
The Integrating Factor (I.F.)
Every LDE is solved using an Integrating Factor, defined as I.F.=e∫P(x)dx.
Calculating this, we find:
I.F.=e∫−x1dx=e−lnx=eln(x−1)=x1
Multiplying our differential equation by this factor, we get:
x1f′(x)−x21f(x)=1
The left side is now the derivative of the product xf(x). This is the magic of the Integrating Factor—it collapses the expression into a perfect derivative.
Phase 4
The Final Reveal
Integrating both sides with respect to
x:
∫dxd(xf(x))dx=∫1dx
xf(x)=x+C
Multiplying by
x, we find the general solution:
f(x)=x2+Cx
We use the initial condition
f(1)=2 to find
C:
2=(1)2+C(1)⇒C=1
Our specific function is f(x)=x2+x.
Finally, calculating
f(2):
f(2)=(2)2+2=4+2=6
The final answer is 6.