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Derivative and Differentiability

Definition

Let X⊆R,X\subseteq \mathbb{R}\text{,} let x0x_0 be an interior point of X,X\text{,} that is, (x0−r,x0+r)⊆X(x_0-r,x_0+r)\subseteq X for some r>0,r>0\text{,} and let f ⁣:X→Rf \colon X \to \mathbb{R} be a function. We say that ff is differentiable at x=x0x=x_0 with derivative L,L\text{,} and write f′(x0)=L,f'(x_0) = L\text{,} if the two-sided limit

lim⁡x→x0f(x)−f(x0)x−x0\lim_{x\to x_0}\frac{f(x)-f(x_0)}{x-x_0}

exists and equals the real number L.L\text{.} If the limit does not exist, we leave f′(x0)f'(x_0) undefined and say that ff is not differentiable at x=x0.x=x_0\text{.} At a boundary point the corresponding one-sided derivative is treated separately.

The derivative can be written using either a moving point xx or an increment h:h\text{:}

f′(x0)=lim⁡x→x0f(x)−f(x0)x−x0=lim⁡h→0f(x0+h)−f(x0)h,f'(x_0)=\lim_{x\to x_0}\frac{f(x)-f(x_0)}{x-x_0} =\lim_{h\to 0}\frac{f(x_0+h)-f(x_0)}{h},

and the substitution h=x−x0h=x-x_0 shows the two forms are equivalent.

Finally, if every point of XX is an interior point of XX (for example, XX an open interval), ff is differentiable on XX if it is differentiable at every x0∈X;x_0\in X\text{;} at the endpoints of a closed interval one uses the one-sided derivative instead.


Interpretation

The derivative measures the instantaneous rate of change of a function at a point. The difference quotient f(x)−f(x0)x−x0\frac{f(x)-f(x_0)}{x-x_0} is the average rate of change between x0x_0 and xx, the slope of a secant line, and the derivative is its limit as x→x0x\to x_0. Differentiability means that this limit exists as a finite number.

A curve with its tangent line at a point x0; near x0 the curve stays close to the tangent, whose slope is the derivative.

Near the marked point (x0,f(x0))(x_0,f(x_0)) the curve and the tangent line are hard to tell apart, and the slope of the tangent is f′(x0)f'(x_0). Here the curve is falling at x0x_0, so f′(x0)<0f'(x_0)<0.

Let hh shrink towards 00 from either side: the secant turns into the tangent and the difference quotient approaches f′(x0)f'(x_0). For ∣x∣|x| at x0=0x_0=0 the two sides disagree.

Differentiability at x0x_0 can be read in two equivalent ways. Geometrically, the graph has a non-vertical tangent line at (x0,f(x0))(x_0,f(x_0)), with slope f′(x0)f'(x_0). Analytically, in a small neighbourhood of x0x_0 the function is approximated by the tangent line: f(x)=f(x0)+f′(x0)(x−x0)+r(x)f(x)=f(x_0)+f'(x_0)(x-x_0)+r(x) with an error r(x)r(x) that is small even relative to x−x0x-x_0, that is, r(x)/(x−x0)→0r(x)/(x-x_0)\to0. The second reading is the one behind the differential.

Differentiability is stronger than continuity: letting x→x0x\to x_0 in f(x)−f(x0)=f(x)−f(x0)x−x0 (x−x0)f(x)-f(x_0)=\frac{f(x)-f(x_0)}{x-x_0}\,(x-x_0) gives f(x)→f(x0)f(x)\to f(x_0). The converse fails at a corner, where the one-sided derivatives differ, and at a vertical tangent: for x3\sqrt[3]{x} at 00 the difference quotient is 1/x231/\sqrt[3]{x^2}, which tends to +∞+\infty.

The approximation reading returns in Math III as the total derivative of a function of several variables.


Key Results

  • Differentiability implies continuity.
  • The derivative is unique when it exists.
  • Non-differentiability often signals sharp changes in behaviour.

Examples

  • The function f(x)=x2f(x)=x^2 is differentiable everywhere.
  • The function f(x)=∣x∣f(x)=|x| is not differentiable at x=0.x=0\text{.}

Prerequisites

Sources

Keywords: derivative, differentiable function, difference quotient Symbols: element of, infinity, real numbers, square root, subset

Last updated: 22 October 2026 19:04