Analyzing the Setup
Imagine you are standing on a vast, open field, and before you are two paths represented by the functions f and g. The problem provides a beautiful constraint: the range of f is (0,∞).
This means the graph of f(x) is like a bird that never lands; it always hovers strictly above the x-axis. It can never touch the ground, and it can never dive below it.
Meanwhile, g(x) is a more adventurous path, crossing the x-axis at x=2. This is our point of interest, the coordinate where the magic happens.
The Indeterminate Mystery
We are presented with a limit:
x→2limf′(x)g′(x)f(x)g(x)=1
Before we panic, let's test the waters. What happens at x=2? The numerator becomes f(2)g(2). Since g(2)=0, the numerator is zero.
The denominator is f′(2)g′(2). We are told f′(2)=0, so the denominator is also zero. We are staring at a 0/0 indeterminate form.
This is not a dead end; it is an invitation to use L'Hopital's Rule. We are essentially looking for the ratio of the rates of change of these functions as they approach the point x=2.
The Calculus of Change
To apply L'Hopital's Rule, we must differentiate the numerator and the denominator. This is where the Product Rule becomes our best friend.
The derivative of the numerator f(x)g(x) is f′(x)g(x)+f(x)g′(x). Similarly, the derivative of the denominator f′(x)g′(x) is f′′(x)g′(x)+f′(x)g′′(x).
Our limit now looks like this:
x→2limf′′(x)g′(x)+f′(x)g′′(x)f′(x)g(x)+f(x)g′(x)=1
This looks intimidating, but let's breathe and substitute x=2. We know f′(2)=0 and g(2)=0.
The numerator simplifies beautifully: 0⋅0+f(2)g′(2)=f(2)g′(2). The denominator simplifies to f′′(2)g′(2)+0⋅g′′(2)=f′′(2)g′(2).
The Elegant Cancellation
Now we have:
The problem explicitly states $g'(2)
eq 0$, which is our golden ticket to cancel g′(2) from both the numerator and the denominator.
We are left with the elegant relationship:
f′′(2)f(2)=1⇒f′′(2)=f(2)
This is the key that unlocks the entire problem.
The Final Revelation
We established that f(x)>0 for all x, so f(2)>0. Since f′′(2)=f(2), it must be that f′′(2)>0.
We have a point x=2 where the first derivative f′(2) is zero (a horizontal tangent) and the second derivative f′′(2) is positive (concave up). By the Second Derivative Test, this point is a local minimum.
Furthermore, since f′′(2)=f(2), the equation f(x)−f′′(x)=0 is satisfied at x=2. We have successfully navigated the landscape of this problem and uncovered its hidden truths.