Since the numerator and denominator in the formula
(2.53) are both positive,
\(f\) has no zeros on its domain, and hence there is no
\(x\)-intercept. Since
\(f(0)=A/(1+ce^0)\text{,}\) the
\(y\)-intercept of the graph of
\(f\) is
\((0,A/(1+c)\text{.}\)
The value \(f(0)=A/(1+c)\) determines the left end behavior of \(f\text{.}\) For the right end behavior, we compute the limit
\begin{align*}
\lim\limits_{x\to \infty}f(x) \amp = \lim\limits_{x\to \infty}\frac{A}{1+ce^{-kx}}\\
\amp =\frac{A}{1+c\lim\limits_{x\to \infty}e^{-kx}}\\
\amp =\frac{A}{1+0}\\
\amp =A\text{.}
\end{align*}
Thus the graph of \(f\) has the horiztontal asymptote \(y=A\text{.}\)
Continuing with our analysis, we now look at the first and second derivatives of \(f\text{:}\)
\begin{align*}
f'(x) \amp =-A(1+ce^{-kx})^{-2}(1+ce^{-kx})'\\
\amp = \frac{ckAe^{-kx}}{(1+ce^{-kx})^2}\\
f''(x) \amp = ckA\frac{-ke^{-kx}(1+ce^{-kx})^2-2e^{-kx}(1+ce^{-kx})(-cke^{-kx})}{(1+ce^{-kx})^4}\\
\amp = \frac{ck^2Ae^{-kx}(1+ce^{-kx})(ce^{-kx}-1)}{(1+ce^{-kx})^4}\text{.}
\end{align*}
From since the numerator and denominator for \(f'\) are both easily seen to be positive for all \(x\in D\text{,}\) we see that \(f\) is increasing on its entire domain, and has no critical points.
Moving to \(f''\) we see that the denominator, as well as all of the terms in the numerator, with the exception of \((ce^{-kx}-1)\) are positive. Thus the sign of \(f''\) is equal to the sign of \(g(x)=ce^{-kx}-1\text{.}\) Performing a sign diagram for \(g\text{,}\) we first solve
\begin{align*}
g(x) \amp = 0\\
ce^{-kx} \amp =1\\
e^{-kx} \amp =\frac{1}{c}\\
-kx \amp = \ln(1/c)=-\ln c\\
x \amp = \ln(c)/k \text{.}
\end{align*}
Note that since we assume \(c> 1\text{,}\) we have \(\ln c> 0\text{,}\) whence \(x=\ln(c)/k> 0\text{.}\) Since \(g(0)=c-1> 0\) and \(g(x)\to -1 \) as \(x\to \infty\text{,}\) we conclude that \(f''\) has the following sign diagram.

We conclude that \(f''\) is concave up on \((0,\ln(c)/k)\) and concave down on \((\ln(c)/k,\infty)\text{,}\) and thus has an inflection point at
\begin{align*}
P= \amp (\ln(c)/k, f(\ln(c)/k))\\
\amp =(\ln(c)/k, A/(1+ce^{-\ln c}))\\
\amp =(\ln(c)/k, A/2)\text{.}
\end{align*}
Interestingly, we see that the unique inflection point of the graph of \(f\) occurs at the unique point where the \(y\)-coordinate is \(A/2\text{,}\) exactly half of the ceiling value of the function!
The graph in
Figureย 2.14.6 assembles all of the details of our analysis.