Analyzing the Setup
The function is defined as:
At first glance, the integrand g(t)=te−(t+1/t) appears complex, and the limits are functions of x. However, in JEE Advanced, complexity is often a mask for elegance. Let us strip away that mask.
The Newton-Leibniz Revelation
To understand the monotonicity of f(x), we must determine its derivative f′(x). We invoke the Newton-Leibniz rule:
dxd∫u(x)v(x)g(t)dt=g(v(x))⋅v′(x)−g(u(x))⋅u′(x)
Here, our upper limit is v(x)=x (so v′(x)=1) and our lower limit is u(x)=1/x (so u′(x)=−1/x2). Substituting these into the formula, we obtain:
f′(x)=g(x)⋅(1)−g(1/x)⋅(−x21)
Substituting the integrand g(t)=te−(t+1/t), the first term becomes xe−(x+1/x). The second term becomes:
Notice the beauty here: the exponents x+1/x and 1/x+x are identical. When we simplify the second term, the 1/x in the denominator flips to the numerator, and the negative signs cancel out. We are left with:
f′(x)=xe−(x+1/x)+xe−(x+1/x)=x2e−(x+1/x)
Since x>0, this derivative is always positive. Therefore, the function is strictly increasing.
The Symmetry of the Integral
Now, let us evaluate the property f(x)+f(1/x)=0. If we define f(x)=∫1/xxg(t)dt, then f(1/x) is the integral with the limits swapped:
Recall the fundamental property of definite integrals: ∫abg(t)dt=−∫bag(t)dt. By swapping the limits, we introduce a negative sign:
f(1/x)=−∫1/xxg(t)dt=−f(x)
Rearranging this yields f(x)+f(1/x)=0. This is a perfect, symmetric cancellation.
The Parity of the Composition
Finally, let us tackle the parity of h(x)=f(2x). To check if a function is odd, we must verify if h(−x)=−h(x).
We compute:
Using our result from the previous section, we know that f(1/y)=−f(y). Letting y=2x, we find:
Thus, the function h(x) is odd. We have successfully navigated the derivative, the symmetry, and the parity of the function.