The Beauty of Functional Equations
Imagine you are standing at the edge of a vast, uncharted mathematical landscape. You are given two mysterious equations:
To the untrained eye, these are just abstract symbols. But to a JEE aspirant, they whisper secrets. They are the structural DNA of the sine and cosine addition formulas. While we won't blindly assume they are trigonometric functions, we will use that intuition to guide our journey. Our mission is to find the derivative of g(x) at x=0.
Phase 1
The Origin
In any functional equation, the origin is our best friend. It is the anchor point. Let us substitute x=0 and y=0 into our first equation:
The right side collapses into nothingness, leaving us with f(0)=0. This is a profound realization! It tells us that the function f(x) is pinned to the origin.
Now, let us apply the same logic to the second equation:
Since f(0)=0, this simplifies to g(0)=g(0)2. For a non-trivial solution, g(0) must be 1. We have our coordinates: f(0)=0 and g(0)=1.
Phase 2
The Hidden Geometry
Now, let us uncover the deeper relationship between these two functions. Substitute y=x into the second equation:
The left side becomes g(0), which we know is 1. The right side becomes g(x)2+f(x)2.
Thus, we arrive at the beautiful identity:
This is the fundamental trigonometric identity! It tells us that the values of f(x) and g(x) are bounded, living on a unit circle in the phase plane.
Phase 3
The Symmetry
Next, we must understand the symmetry of g(x). Let us substitute x=0 and y=x into the second equation:
Using our known values, this becomes g(−x)=(1)g(x)+(0)f(x), which simplifies to g(−x)=g(x).
This is the definition of an even function. Just like the cosine function, g(x) is perfectly symmetric across the y-axis.
Phase 4
The Calculus
We are now ready for the final act. We need to find g′(0). By the first principle of derivatives:
This looks daunting, but remember our symmetry property! Since g(x) is even, g(h)=g(−h). Let us substitute this into our limit:
g′(0)=h→0limhg(−h)−g(0)
Now, let us perform a change of variable. Let k=−h. As h→0, k also approaches 0. The expression becomes:
g′(0)=k→0lim−kg(k)−g(0)
We can pull that negative sign out:
g′(0)=−k→0limkg(k)−g(0)
Look closely—the limit on the right is exactly the definition of g′(0)! We have arrived at the elegant conclusion:
The Final Conclusion
What real number is equal to its own negative? Only zero. Thus, 2g′(0)=0, which forces g′(0)=0.
Visually, this makes perfect sense. The tangent line at the peak of an even, differentiable function must be horizontal. We have solved the mystery, not by guessing, but by peeling back the layers of the functional equations one by one.