Analyzing the Setup
We are given the differential equation f′(x)=b2+x2f(x) with the initial condition f(0)=1. This is a classic setup where the rate of change of a function is proportional to the function itself, scaled by a geometric factor.
To solve this, we separate the variables by grouping all terms involving f on one side and all terms involving x on the other. By dividing both sides by f(x) and multiplying by dx, we obtain:
The Integration Journey
Now, we integrate both sides of the equation:
The left side yields ln∣f(x)∣, while the right side is the standard integral of the inverse tangent function. This gives us:
We use the initial condition f(0)=1 to determine the constant C. Substituting x=0 and f(0)=1 into the equation:
Since ln(1)=0 and tan−1(0)=0, we find that C=0. Our function simplifies to:
Exponentiating both sides and removing the absolute value bars (as the exponential function is always positive), we arrive at the final expression:
Analyzing the Behavior
To determine monotonicity, we examine f′(x)=b2+x2f(x). Since f(x)>0 and b2+x2>0 for all x, f′(x) is strictly positive. This confirms that the function is always increasing.
Finally, we check for symmetry by evaluating f(−x):
f(−x)=eb1tan−1(b−x)=e−b1tan−1(bx)
Multiplying f(x) and f(−x) yields:
f(x)⋅f(−x)=eb1tan−1(bx)⋅e−b1tan−1(bx)=e0=1
This confirms the property f(x)f(−x)=1. You have successfully navigated the logic of this function; keep this analytical rigor in your toolkit to conquer any problem.