Analyzing the Setup
Welcome, fellow traveler, to the elegant world of differential inequalities. We are given a function P(x) with two key pieces of information: P(1)=0 and P′(x)>P(x) for all x≥1.
Our mission is to prove that P(x)>0 for all x>1. Imagine you are standing at the point x=1 on a graph; you know the function is currently touching the x-axis, and its rate of change is "pushing" it upwards faster than the function itself.
The 'Aha!' Moment
The Integrating Factor
When we look at the inequality P′(x)>P(x), it is helpful to bring everything to one side: P′(x)−P(x)>0. This structure is a classic signature in calculus that suggests the use of an integrating factor.
To make the left side a perfect derivative, we multiply the entire inequality by e−x. This yields:
Since the derivative of e−x is −e−x, this expression is exactly the derivative of the product e−xP(x).
Constructing the Auxiliary Function
Let us define a new, auxiliary function to simplify our analysis: f(x)=e−xP(x). We find its derivative, f′(x), using the product rule:
f′(x)=dxd(e−x)⋅P(x)+e−x⋅dxd(P(x))
This expands to:
f′(x)=−e−xP(x)+e−xP′(x)=e−x(P′(x)−P(x))
Because e−x>0 for all real x and we are given P′(x)−P(x)>0, it follows that f′(x)>0 for all x≥1.
The Climax
Monotonicity and the Boundary
Because f′(x)>0, we have proven that f(x) is a strictly increasing function. This means that as x moves to the right, f(x) must increase.
We look back at our boundary condition: P(1)=0. Substituting this into our definition of f(x), we get:
Since the function starts at zero at x=1 and is strictly increasing, it must be that f(x)>f(1) for all x>1. Therefore, f(x)>0 for all x>1.
The Victory
We have established that e−xP(x)>0. Since the exponential function e−x is always strictly positive, we can divide both sides by it without changing the direction of the inequality.
This leaves us with the final result: P(x)>0 for all x>1. We have successfully navigated the differential inequality by leveraging the integrating factor and the boundary condition.