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Section 3.2 Differentiability

Subsection 3.2.1 Differentiability on an Interval

Definition 3.2.1.

If a function is defined on an open interval \((a,b)\text{,}\) then \(f\) is differentiable on \((a,b)\) if \(f\) is differentiable for all \(x \in (a,b)\text{.}\)
Functions that are differentiable are intuitively “smooth”. Values of \(x\) in \(D(f)\) where \(f\) is non-differentiable and are not endpoints are called singular points of \(f\text{.}\)
Note that we used an open interval \((a,b)\) and did not include the endpoints. This is because if \(f\) is defined on a closed interval \([a,b]\text{,}\) then it cannot be differentiable at the endpoints \(x = a\) or \(x = b\text{,}\) because the (two-sided) limit cannot exist if the function is only defined on one side.

Subsection 3.2.2 Continuous But Not Differentiable

Consider the derivative of the absolute value function,
\begin{equation*} f(x) = \abs{x} = \begin{cases} x \amp x \geq 0 \\ -x \amp x \lt 0 \end{cases} \end{equation*}
For \(x \neq 0\text{,}\) \(f\) is differentiable. In particular, for \(x > 0\text{,}\) \(f'(x) = \frac{d}{dx} x = 1\text{,}\) and for \(x \lt 0\text{,}\) \(f'(x) = \frac{d}{dx} (-x) = -1\text{.}\) However, at \(x = 0\text{,}\)
\begin{align*} f'(0) \amp = \lim_{h \to 0} \frac{\abs{0 + h} - \abs{0}}{h}\\ \amp = \lim_{h \to 0} \frac{\abs{h}}{h} \end{align*}
  • From the right, as \(h \to 0+\text{,}\) \(\abs{h} = h\text{,}\) and so,
    \begin{equation*} \lim_{h \to 0+} \frac{\abs{h}}{h} = \lim_{h \to 0} \frac{h}{h} = \lim_{h \to 0} 1 = 1 \end{equation*}
    Thus, from the right, the slopes approach 1 (this can be confirmed graphically).
  • However, from the left, as \(h \to 0-\text{,}\) \(\abs{h} = -h\text{,}\) and so,
    \begin{equation*} \lim_{h \to 0-} \frac{\abs{h}}{h} = \lim_{h \to 0-} \frac{-h}{h} = \lim_{h \to 0} -1 = -1 \end{equation*}
    From the left, the slopes approach -1.
Since these one sided limits are unequal, \(\lim_{h \to 0} \frac{\abs{h}}{h}\) does not exist, and so \(f\) is not differentiable at \(x = 0\text{.}\) In summary,
\begin{equation*} \frac{d}{dx} \abs{x} = \begin{cases} 1 \amp x > 0 \\ -1 \amp x \lt 0 \end{cases} \end{equation*}
This can be summarized as,
\begin{equation*} \boxed{\frac{d}{dx} \abs{x} = \frac{\abs{x}}{x} \qquad x \neq 0} \end{equation*}

Subsection 3.2.3 Differentiability and Continuity

If a function \(f\) is continuous at \(x\text{,}\) it may or may not be differentiable at \(x\text{.}\) For example, \(f(x) = \abs{x}\) is continuous but not differentiable at \(x = 0\text{.}\) However, the converse is true, in that differentiability implies continuity.
Intuitively, this theorem says that if a function is smooth at a point \(a\text{,}\) then it can't have a discontinuity there. Alternatively, it is more intuitive to consider the contrapositive, that if \(x\) is not continuous at \(a\) (i.e. it has a break or jump), then it is not differentiable at \(a\) (the slope of a tangent line cannot be found).