Analyzing the Setup
Imagine you are standing before a mirror, and that mirror is reflecting another mirror. That is exactly what we have here with f(x) and g(x). They are intertwined, each defined by the other's behavior.
We are given:
f(x)=x2+g′(1)x+g′′(2)
g(x)=f(1)x2+xf′(x)+f′′(x)
The secret to solving this is to stop seeing g′(1) and g′′(2) as scary symbols and start seeing them as what they truly are: constants. Let us define A=g′(1) and B=g′′(2). Suddenly, the problem becomes a puzzle of finding two numbers.
Phase 1
The Power of Differentiation
We need to know what
f′(x) and
f′′(x) look like to understand
g(x). Given
f(x)=x2+Ax+B, the derivatives are:
f′(x)=2x+A
f′′(x)=2
This is the breakthrough! The second derivative of f is just a constant, 2. This simplifies our expression for g(x) immensely.
Substituting these into the definition of
g(x):
g(x)=f(1)x2+x(2x+A)+2
g(x)=(f(1)+2)x2+Ax+2
Phase 2
The Unraveling
To find our constants, we differentiate
g(x):
g′(x)=2(f(1)+2)x+A
Now, evaluate this at
x=1. Since we defined
g′(1)=A, we have:
A=2(f(1)+2)(1)+A
The A on both sides cancels out perfectly, leaving 0=2(f(1)+2). This tells us that f(1)=−2.
Next, we find
g′′(2). From our expression for
g′(x), we know
g′′(x)=2(f(1)+2). Substituting
f(1)=−2:
g′′(x)=2(−2+2)=0
Thus,
g′′(2)=0.
Phase 3
The Final Construction
We have
f(1)=−2 and
g′′(2)=0. Returning to our original definition of
f(x):
f(1)=12+A(1)+0
−2=1+A⇒A=−3
Now we have the complete functions:
f(x)=x2−3x
g(x)=(−2+2)x2−3x+2=−3x+2
Finally, we calculate the values at
x=4:
f(4)=42−3(4)=16−12=4
g(4)=−3(4)+2=−12+2=−10
The difference is:
f(4)−g(4)=4−(−10)=14
You untangled the system, navigated the calculus, and arrived at the elegant solution of 14.