Analyzing the Setup
Imagine you are standing before a graph, looking at a curve defined by a positive function f(x). You are told that the area under this curve, from x=0 to x=a, is given by the expression e−a+4a2+a−1.
This is not just a random collection of terms; it is the accumulated history of the function f(x). To find the function itself, we need to reverse the process of integration.
This is where the Newton-Leibniz Rule becomes our most powerful tool. By differentiating the integral ∫0af(x)dx with respect to the upper limit a, we are essentially asking, "How does the area change as the boundary moves?"
The answer, as the Fundamental Theorem of Calculus tells us, is simply the value of the function at that boundary: f(a).
The Function Revealed
Let us perform this differentiation with precision. We differentiate the expression e−a+4a2+a−1 with respect to a.
The derivative of e−a is −e−a. The derivative of 4a2 is 8a. The derivative of a is 1, and the constant −1 vanishes into zero.
Thus, we find:
Since a is just a placeholder for our variable, we can confidently state that f(x)=−e−x+8x+1. We have successfully unmasked the function!
The General Solution and the Elimination Game
Now, we turn our attention to the second part of our journey. We are given the general solution y=c1f(x)+c2. This equation describes a family of curves, and our goal is to find the differential equation that governs them.
Because we have two arbitrary constants, c1 and c2, we know we need a second-order differential equation. We must differentiate y twice.
First, we find the first derivative:
dxdy=c1f′(x)=c1(e−x+8)
Next, we differentiate again to find the second derivative:
Now, we face the challenge of eliminating the constant c1. The most elegant way to do this is to take the ratio of the second derivative to the first derivative.
This causes c1 to cancel out entirely, leaving us with a relationship between the derivatives:
The Final Polish
We are almost at the finish line. Cross-multiplying gives us:
Rearranging this, we get:
(e−x+8)dx2d2y+e−xdxdy=0
To match the clean, professional form, we multiply the entire equation by ex. This transforms e−x⋅ex into 1, and 8⋅ex into 8ex.
The result is the beautiful, final differential equation:
You have navigated the path from an area integral to a differential equation, mastering the Leibniz Rule and the art of constant elimination along the way. Keep this logical flow in your toolkit, and no differential equation will ever intimidate you again.