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Section 4.4 Logarithmic functions
Objectives
Use inverse relationships to understand how logarithms and exponentials change.
Differentiate expressions involving real exponents, other bases, and logarithmic combinations.
Apply logarithmic differentiation and relative rates to analyze more complex models.
Differentiating \(\ln x\text{,}\) the inverse of the exponential function:
\begin{align*}
y \amp = \ln x \\
\ee^y \amp = x \\
\dd(\ee^y) \amp = \dd{x} \\
\ee^y \dd{y} \amp = \dd{x} \\
\dd{y} \amp = \frac{1}{\ee^y} \dd{x} \\
\dv{y}{x} \amp = \frac{1}{x}
\end{align*}
In general, derivatives of inverse functions:
\begin{align*}
y \amp = f\inv(x)\\
f(y) \amp = x\\
\dd(f(y)) \amp = \dd{x}\\
f'(y)\dd{y} \amp = \dd{x}\\
\dd{y} \amp = \frac{1}{f'(y)}\dd{x}\\
\dv{x} f\inv(x) \amp = \frac{1}{f'(f\inv(x))}
\end{align*}
Logarithmic differentiation:
\begin{equation*}
\dd(\ln y) = \frac{\dd{y}}{y}
\end{equation*}
Good for complicated derivatives or derivatives involving exponents.
Reminder of logarithm rules as opposites of exponent rules:
\begin{align*}
\ln(uv) \amp = \ln u + \ln v\\
\ln\left(\frac{u}{v}\right) \amp = \ln u - \ln v\\
\ln(u^r) \amp = r \ln u
\end{align*}
Differentiating \(x^r\) for any real exponent \(r\text{:}\)
\begin{align*}
y \amp = x^r \\
\ln y \amp = r \ln x \\
\dd(\ln y) \amp = \dd(r \ln x) \\
\frac{1}{y}\dd{y} \amp = r \frac{1}{x} \dd{x} \\
\dd{y} \amp = r x^{r-1} \dd{x} \\
\dv{y}{x} \amp = r x^{r-1}
\end{align*}
Differentiating \(b^x\) for any base \(b>0\text{:}\)
\begin{align*}
y \amp = b^x \\
\ln y \amp = x \ln b \\
\dd(\ln y) \amp = \dd(x \ln b) \\
\frac{1}{y}\dd{y} \amp = \ln b \dd{x} \\
\dd{y} \amp = y \ln b \dd{x} \\
\dv{y}{x} \amp = b^x \ln b
\end{align*}
Differentiating \(\log_b{x}\) for any base \(b>0\text{:}\)
\begin{align*}
y \amp = \log_b{x} \\
b^y \amp = x \\
\dd(b^y) \amp = \dd{x} \\
b^y \ln b \dd{y} \amp = \dd{x} \\
\dd{y} \amp = \frac{1}{x \ln b} \dd{x} \\
\dv{y}{x} \amp = \frac{1}{x \ln b}
\end{align*}
New way of looking at elasticity:
\begin{equation*}
\DS\rdv{y}{x}=\dv{(\ln y)}{(\ln x)}\text{.}
\end{equation*}
This for example shows that the elasticity of
\(uv\) is the sum of the elasticities of
\(u\) and
\(v\text{.}\)