In this section, we introduce the concept of a one-sided derivative.
Definition 1. If the function \(y=f(x)\) is defined for \(x=x_{0}\), then the derivative from the right of \(f\) at \(x_{0}\), denoted by \(f’_{+}(x_{0})\), is defined by
\[f’_{+}(x_{0})=\lim_{\Delta x\to0^{+}}\frac{f(x_{0}+\Delta x)-f(x_{0})}{\Delta x},\]
if the limit exists. Similarly, the derivative from the left of \(f\) at \(x_{0}\), denoted by \(f’_{-}(x_{0})\), is defined by
\[f’_{-}(x_{0})=\lim_{\Delta x\to0^{-}}\frac{f(x_{0}+\Delta x)-f(x_{0})}{\Delta x}.\]
\[f’_{+}(x_{0})=\lim_{\Delta x\to0^{+}}\frac{f(x_{0}+\Delta x)-f(x_{0})}{\Delta x},\]
if the limit exists. Similarly, the derivative from the left of \(f\) at \(x_{0}\), denoted by \(f’_{-}(x_{0})\), is defined by
\[f’_{-}(x_{0})=\lim_{\Delta x\to0^{-}}\frac{f(x_{0}+\Delta x)-f(x_{0})}{\Delta x}.\]
The geometric interpretation of one-sided derivatives is illustrated in Figure 1.
- The Theorem of the Uniquness of a Limit that we learned in the previous chapter, states that \(\lim_{x\to a}f(x)=L\) if and only if \(\lim_{x\to a^{+}}f(x)=\lim_{x\to a^{-}}f(x)=L\). It follows from this theorem that \(f'(x_{0})\) exists if and only if \(f’_{+}(x_{0})=f’_{-}(x_{0})\).