The Symphony of Functional Equations
Welcome, fellow traveler of the mathematical landscape. Today, we are not just solving a problem; we are decoding a hidden law of nature.
Functional equations are the 'DNA' of mathematics. They don't tell us what a function is explicitly; they tell us how a function behaves.
When we see an equation like f(yx)=f(y)f(x), we are looking at a fundamental symmetry. Our mission is to translate this symmetry into the language of calculus—the language of change.
Phase 1
Finding the Anchor
Before we rush into the complex machinery of derivatives, we must find our footing. Every function has a 'base state,' a point of reference. In this problem, that point is x=1.
Imagine we substitute x=1 and y=1 into our given equation:
Since the problem guarantees $f(y)
eq 0$, we can safely cancel the terms. This leaves us with the elegant result: f(1)=1.
This is our anchor. It is the solid ground upon which we will build the rest of our derivation. Never underestimate the power of testing simple values; they often reveal the secrets that complex algebra hides.
Phase 2
The Calculus Hammer
Now, we need to bridge the gap between the function f(x) and its derivative f′(x). We have an algebraic relation, but we need a differential one. The tool for this job is partial differentiation.
We treat y as a constant—a fixed number, like 5 or π—and we differentiate both sides of the equation with respect to x.
On the left-hand side, we have f(yx). Applying the chain rule, the derivative becomes:
On the right-hand side, since f(y) is treated as a constant, we simply differentiate f(x):
∂x∂[f(y)f(x)]=f(y)f′(x)
Equating these two, we arrive at our golden key:
Take a moment to appreciate this. We have successfully transformed a static relationship into a dynamic one. We are now looking at how the rate of change of the function at one point relates to the rate of change at another.
Phase 3
The Strategic Substitution
We are almost at the finish line. We know that f′(1)=2024. Looking at our equation, we have a term f′(yx).
To utilize our known value, we need the argument yx to become 1. This is the 'Aha!' moment. By setting y=x, we force the argument to be 1.
Let us substitute y=x into our equation:
This simplifies beautifully to:
Substituting our known value f′(1)=2024, we get:
The Final Elegance
We have arrived at a first-order differential equation. To match the options provided, we simply rearrange the terms. Cross-multiplying gives us:
Or, moving everything to one side:
And there it is. We started with a mysterious functional equation and, through the systematic application of calculus, we uncovered the differential law governing the function.
This is the essence of JEE Advanced physics and mathematics: taking a complex, abstract problem and breaking it down into logical, manageable steps. You have mastered the technique; now, go forth and apply this logic to the next challenge!