The Relay Race of Functions
Imagine you are standing at the starting line of a relay race. In mathematics, a composite function g(f(x)) is exactly that—a relay race. The function f(x) runs the first leg, and its output is handed off as the input to g(x).
To master this problem, we must understand not just the functions themselves, but the hand-off point. The function g(x) is a bit temperamental; it changes its behavior entirely depending on whether its input is negative or non-negative.
This means the composite function g(f(x)) will change its behavior whenever f(x) crosses the threshold of zero. Let us peel back the layers of this problem together.
Navigating the Negative Domain
We begin by looking at the region where x<0. In this territory, f(x)=x+a. But remember, g(x) changes its rule at 0.
So, we must ask: when is f(x)<0 and when is f(x)≥0? If x+a<0, which simplifies to x<−a, we must use the first branch of g(y), which is y+1.
Substituting
f(x) for
y, we get:
g(f(x))=(x+a)+1
However, if
x+a≥0, which means
−a≤x<0, we must switch to the second branch of
g(y), which is
(y−1)2+b. Substituting
f(x) here, we get:
g(f(x))=(x+a−1)2+b
We have successfully mapped the behavior of our composite function for all x<0. It is a piecewise function within a piecewise function—a beautiful, nested structure.
The Absolute Value Simplification
Now, let us shift our gaze to the right side of the y-axis, where x≥0. Here, f(x)=∣x−1∣.
A wonderful property of the absolute value function is that it is always non-negative. Since f(x)≥0 for all x≥0, we never have to worry about the first branch of g(y).
We can confidently use the second branch,
(y−1)2+b, for the entire region. Substituting
f(x)=∣x−1∣, our composite function becomes:
g(f(x))=(∣x−1∣−1)2+b
The complexity melts away, leaving us with a clear definition for the entire real line.
The Continuity Puzzle
For g(f(x)) to be continuous everywhere, it must be 'glued' together perfectly at its transition points. We have two critical points to check: x=−a and x=0.
At
x=−a, we equate the limits from the left and right. The left-hand limit is:
x→−a−lim(x+a+1)=1
The right-hand limit is:
x→−a+lim((x+a−1)2+b)=(−a+a−1)2+b=1+b
Setting these equal, we find 1=1+b, which immediately gives us b=0.
With
b=0 in hand, we move to
x=0. The left-hand limit is:
x→0−lim((x+a−1)2+0)=(a−1)2
The right-hand limit is:
x→0+lim((∣x−1∣−1)2+0)=(∣0−1∣−1)2=0
Equating these, we get (a−1)2=0, which tells us a=1. We have solved the mystery of the constants!
The Final Smoothness Test
Finally, we test for differentiability at x=0. With a=1 and b=0, our function h(x)=g(f(x)) simplifies beautifully.
For
x near
0, the left-hand side becomes
(x+1−1)2=x2. For the right-hand side, since
x is small and positive,
∣x−1∣=1−x, so:
h(x)=(1−x−1)2=(−x)2=x2
Since h(x)=x2 on both sides of zero, the function is not just continuous; it is smooth. The derivative h′(x)=2x exists at x=0 and is equal to 0.
The relay race is complete, and the transition is seamless. You have navigated the piecewise logic, enforced the continuity constraints, and verified the smoothness of the result. Well done!