Analyzing the Setup
Imagine you are standing on a graph, looking at two distinct paths, f(x) and g(x), both winding their way from x=0 to x=1.
You are given the boundary conditions:
f(0)=2,g(0)=0,f(1)=6, and g(1)=2.
Your mission is to prove that at some point c between 0 and 1, the slope of f is exactly twice the slope of g. This is a beautiful dance of calculus.
The Spark of Insight
The equation f′(c)=2g′(c) is our North Star. If we rearrange it, we get f′(c)−2g′(c)=0.
This is the key! It looks exactly like the derivative of a combined function.
If we define a new function
h(x)=f(x)−2g(x), then its derivative is simply:
h′(x)=f′(x)−2g′(x)
Suddenly, the problem transforms from a complex relationship between two functions into a simple search for a root of the derivative of one auxiliary function.
Constructing the Bridge
Let us build this auxiliary function, h(x)=f(x)−2g(x). Since f(x) and g(x) are differentiable, h(x) inherits this smoothness.
Now, let us test the boundaries:
At
x=0, we have:
h(0)=f(0)−2g(0)=2−2(0)=2
At
x=1, we have:
h(1)=f(1)−2g(1)=6−2(2)=6−4=2
Look at that! h(0)=h(1)=2. This is the moment where the magic happens.
The Climax
Rolle's Theorem
We have a function h(x) that is continuous on [0,1], differentiable on (0,1), and satisfies h(0)=h(1). These are the exact conditions required for Rolle's Theorem.
Rolle's Theorem tells us that there must exist some c∈(0,1) such that h′(c)=0.
Since
h′(c)=f′(c)−2g′(c), this implies:
f′(c)−2g′(c)=0⇒f′(c)=2g′(c)
You have just proven that such a point c must exist. It is not just a coincidence; it is the inevitable consequence of the geometry of smooth functions.