Analyzing the Setup
Imagine you are standing before the graph of the Gaussian function, y=e−t2. It is a beautiful, symmetric bell curve, centered at the origin.
Now, consider the function f(x)=∫x2x2+1e−t2dt. Geometrically, this function represents the area under that bell curve, trapped between two vertical lines at t=x2 and t=x2+1.
As you vary x, this 'window' of integration slides along the t-axis. Because x2 is always non-negative, our window is forever confined to the right side of the y-axis. To determine if this area grows or shrinks as x increases, we must calculate the derivative f′(x).
The Magic of Leibniz
When we face an integral where the limits are functions of x, the Leibniz Rule provides a systematic way to differentiate under the integral sign:
f′(x)=dxd∫u(x)v(x)g(t)dt=g(v(x))⋅v′(x)−g(u(x))⋅u′(x)
Here, our integrand is g(t)=e−t2, our upper limit is v(x)=x2+1, and our lower limit is u(x)=x2. By applying this rule, we transform a daunting integral into a manageable algebraic expression.
The Algebraic Grind
For the upper limit, we have e−(x2+1)2 multiplied by the derivative of x2+1, which is 2x. For the lower limit, we have e−(x2)2 multiplied by the derivative of x2, which is 2x.
Putting it all together, we get:
f′(x)=2x⋅e−(x2+1)2−2x⋅e−x4
Factoring out the 2x, we arrive at:
This expression is the heartbeat of our problem. To find where the function increases, we need f′(x)>0.
The Conceptual Pivot
We must now determine the sign of the bracketed term by comparing e−(x2+1)2 and e−x4. For any real x, it is clear that x2+1>x2, which implies (x2+1)2>x4.
Since the function y=e−u is strictly decreasing, a larger input u results in a smaller output e−u. Because (x2+1)2 is the larger input, e−(x2+1)2 must be smaller than e−x4.
Consequently, the difference e−(x2+1)2−e−x4 is strictly negative for all x.
The Final Revelation
We are left with the inequality:
For this product to be positive, 2x must be negative. Dividing by 2, we find x<0.
Thus, the function f(x) increases precisely when x is in the interval (−∞,0). You have navigated the geometry, mastered the Leibniz Rule, and conquered the sign analysis to reach this conclusion.