Analyzing the Setup
Imagine you are standing before a massive, intimidating wall of symbols. You see an integral, a product of polynomials, and an exponential function all tangled together:
f(x)=∫−1xt(et−1)(t−1)(t−2)3(t−3)5dt
Your instinct might be to panic, to reach for a pen and try to integrate this expression. But stop. Take a deep breath. In the world of JEE Advanced, the most complex-looking problems often hide the most elegant, simple solutions. We don't need to solve the integral; we only need to understand its behavior.
The Leibniz Key
To find the local minima of f(x), we need to know where the function stops decreasing and starts increasing. This is the domain of the derivative, f′(x). How do we differentiate an integral with a variable upper limit?
We use the Leibniz Rule. It tells us that the derivative of the integral is simply the integrand itself, evaluated at the upper limit. It is as if the integral sign and the derivative operator cancel each other out, leaving us with the core of the problem:
f′(x)=x(ex−1)(x−1)(x−2)3(x−3)5
Suddenly, the "monster" has been tamed. We are no longer looking at an integral; we are looking at a polynomial-like function whose roots are easy to identify: x=0,1,2,3.
The Hidden Trap
The Sign of x(ex−1)
Now, we must determine where f′(x) changes sign. This is where most students stumble. Look closely at the term x(ex−1).
If you test a positive value, say x=1, you get 1(e1−1)>0. If you test a negative value, say x=−1, you get (−1)(e−1−1). Since e−1≈0.36, the term (e−1−1) is negative.
A negative times a negative is a positive! This means x(ex−1) is always non-negative. It never crosses the x-axis to become negative; it just touches it at x=0 and bounces back. Therefore, x=0 is not a point where the sign of f′(x) changes. It is a point of inflection, not a local extremum.
The Wavy Curve Dance
With that trap neutralized, we focus on the remaining factors: (x−1)(x−2)3(x−3)5. We use the Wavy Curve Method, starting from the rightmost interval (x>3). Here, all factors are positive, so f′(x)>0.
As we move left and cross each root, we check the power of the factor. Since the powers of (x−1), (x−2), and (x−3) are all odd (1, 3, and 5 respectively), the sign of f′(x) will flip at each of these points:
For x>3, f′(x)>0.
At x=3, we cross into the interval (2,3), and the sign flips to f′(x)<0.
At x=2, we cross into (1,2), and the sign flips to f′(x)>0.
At x=1, we cross into (0,1), and the sign flips to f′(x)<0.
The Moment of Truth
A local minimum occurs when the slope changes from negative to positive—the function goes down, hits a bottom, and starts climbing back up. Looking at our sign analysis:
1. At x=1, the sign changes from negative to positive. This is a local minimum.
2. At x=2, the sign changes from positive to negative. This is a local maximum.
3. At x=3, the sign changes from negative to positive. This is another local minimum.
And there you have it. By refusing to be intimidated by the integral and carefully analyzing the sign changes of the derivative, we have navigated the trap and arrived at the solution: x=1 and x=3. Physics and math are not about brute force; they are about seeing the structure beneath the surface.