Analyzing the Setup
Imagine you are standing before a complex differential equation, a puzzle that seems to weave two different worlds—the world of f(x) and the world of g(x)—into a single, tangled expression:
It looks intimidating, but in the realm of JEE Advanced, intimidation is often just a mask for elegance. Let us peel back that mask together.
The Art of Separation
Our first instinct, and our most powerful tool, is the art of separation. We see that exponential term ef(x)−g(x). By the laws of exponents, we know this is simply:
Now, look at the equation again: f′(x)=eg(x)ef(x)g′(x). If we multiply both sides by e−f(x) and rearrange, we get a beautiful, clean separation:
We have effectively divorced the two functions, allowing them to exist in their own independent integrals.
The Integration Dance
Now, we prepare for the integration. We are looking at:
∫e−f(x)f′(x)dx=∫e−g(x)g′(x)dx
This is where the chain rule becomes our best friend. Recall that the derivative of e−h(x) is −e−h(x)h′(x). Our integrals are almost perfect matches for this!
By integrating both sides, we get:
Multiplying by −1 gives us the elegant relation:
This constant C is the bridge between our two functions, the hidden link that connects the behavior of f at x=1 to the behavior of g at x=2.
The Constant of Mystery
We are given f(1)=1 and g(2)=1. Let us use these keys to unlock the value of C. Substituting x=1 into our equation, we find:
e−f(1)=e−g(1)+C⇒e−1=e−g(1)+C
Thus, C=e−1−e−g(1). Now, let us look at x=2. Substituting this into our main equation, we get:
Since g(2)=1, this becomes e−f(2)=e−1+C. Substituting our expression for C, we arrive at:
e−f(2)=e−1+(e−1−e−g(1))⇒e−f(2)+e−g(1)=e2
The Final Inequality
We have arrived at the heart of the problem. We know that e−f(2)+e−g(1)=e2. Because the exponential function ey is always strictly positive for any real y, we know that e−g(1)>0.
This implies that e−f(2)<e2. Taking the natural logarithm of both sides, we get:
−f(2)<ln(e2)⇒−f(2)<ln2−1
Multiplying by −1 flips the inequality, giving us f(2)>1−ln2. By symmetry, the same logic applies to g(1), leading us to g(1)>1−ln2.
We have navigated the complexity, solved the differential equation, and bounded the functions with precision. This is the power of mathematical reasoning—turning a terrifying equation into a clear, logical truth.