Analyzing the Setup
Welcome, fellow traveler of the mathematical landscape. Today, we are not just solving a problem; we are peeling back the layers of a beautiful functional equation.
We are given two functions,
f and
g, linked by the relationship:
f(x+y)=f(x)+f(y)+f(x)f(y)
We are also given the definition f(x)=xg(x) and the condition limx→0g(x)=1. This is our compass. Let us begin.
The Zero Insight
In any functional equation, the point x=0 is our anchor. Let us substitute x=0 into our relation f(x)=xg(x).
The right side becomes
0⋅g(0), which is zero. Thus, we have our first solid ground:
f(0)=0
This simple fact is the key that will unlock the derivative at the origin.
The First Principle
Now, let us find
f′(0). We use the first principle of derivatives:
f′(0)=h→0limhf(h)−f(0)
Since
f(0)=0, this simplifies to
limh→0hf(h). Substituting
f(h)=hg(h), we get:
h→0limhhg(h)=h→0limg(h)
The problem explicitly told us this limit is 1. Therefore, f′(0)=1. This confirms that Statement (D) is true.
The General Derivative
To find the derivative at any point
x, we again turn to the first principle:
f′(x)=h→0limhf(x+h)−f(x)
Here, we invoke the functional equation
f(x+h)=f(x)+f(h)+f(x)f(h). Substituting this into our limit, we get:
f′(x)=h→0limhf(x)+f(h)+f(x)f(h)−f(x)=h→0limhf(h)(1+f(x))
Since
(1+f(x)) does not depend on
h, we pull it out:
f′(x)=(1+f(x))⋅h→0limhf(h)
We already know limh→0hf(h)=f′(0)=1. Thus, f′(x)=1+f(x). This derivative exists for all x, so Statement (A) is true.
Solving the Differential Equation
We have arrived at a first-order differential equation: f′(x)=1+f(x). This is a classic separable equation.
Integrating both sides with respect to x, we obtain ln∣1+f(x)∣=x+C. Using our initial condition f(0)=0, we find C=0.
Exponentiating both sides, we get
1+f(x)=ex, or:
f(x)=ex−1
With this, we can check Statement (C). Since f′(1)=1+f(1)=1+(e1−1)=e, and $e
eq 1$, Statement (C) is false.
The Taylor Series Magic
Finally, let us examine g(x). Since f(x)=xg(x), for $x
eq 0$, we have g(x)=xex−1.
To check if
g is differentiable at
x=0, we calculate:
g′(0)=x→0limxg(x)−g(0)=x→0limxxex−1−1=x→0limx2ex−1−x
Using the Taylor series ex=1+x+2!x2+…, the numerator becomes 2x2+…. Dividing by x2 gives 1/2.
The limit exists, so g is differentiable. Statement (B) is true. We have successfully navigated the problem!