Interior Extremum

Basis
Last updated: Tags: Calculus, Extrema

When you sketch the graph of a function and mark the “peaks” and “valleys”, you are locating its local extrema. Before you can prove any theorem about them — such as Fermat’s Lemma — you need precise definitions that distinguish local from global, interior from boundary, and strict from non-strict.

Local maximum and minimum

Let ff be defined on a set DRD \subseteq \mathbb{R} and let x0Dx_0 \in D.

Definition. x0x_0 is a local maximum of ff if there exists δ>0\delta > 0 such that

f(x)f(x0)for all xD with xx0<δ.f(x) \leq f(x_0) \quad \text{for all } x \in D \text{ with } |x - x_0| < \delta.

If the inequality is strict (f(x)<f(x0)f(x) < f(x_0) for xx0x \neq x_0), x0x_0 is a strict local maximum.

A local minimum and strict local minimum are defined symmetrically by reversing the inequality. The term local extremum covers both cases.

Interior vs. boundary extrema

The definitions above apply equally to interior points and boundary points of DD. However, most theorems about extrema — including Fermat’s Lemma — require x0x_0 to be in the interior of DD, meaning there exists δ>0\delta > 0 such that (x0δ,x0+δ)D(x_0 - \delta, x_0 + \delta) \subseteq D.

Why the distinction matters. At a boundary point, the function is only compared with values on one side. For example, f(x)=xf(x) = x on [0,1][0, 1] has a local minimum at x0=0x_0 = 0 and a local maximum at x0=1x_0 = 1, even though f=10f' = 1 \neq 0 at both endpoints. A stationarity condition like f(x0)=0f'(x_0) = 0 can only hold at interior points.

Local vs. global extrema

A global maximum (also called an absolute maximum) is a point x0Dx_0 \in D where f(x0)f(x)f(x_0) \geq f(x) for all xDx \in D — not just nearby. Every global extremum is a local extremum, but not conversely.

Example. For f(x)=sinxf(x) = \sin x on R\mathbb{R}: every point where sinx=1\sin x = 1 is both a local and a global maximum, while points where sinx=1\sin x = -1 are both local and global minima. There is no other local extremum because sinx\sin x oscillates to arbitrarily large values of xx in each direction.

Example. For f(x)=x33xf(x) = x^3 - 3x on R\mathbb{R}: x=1x = -1 is a local maximum with f(1)=2f(-1) = 2, and x=1x = 1 is a local minimum with f(1)=2f(1) = -2. Neither is a global extremum since f(x)±f(x) \to \pm\infty as x±x \to \pm\infty.

Characterisation via local properties

A point x0int(D)x_0 \in \operatorname{int}(D) is a local maximum of ff if and only if ff(x0)f - f(x_0) is non-positive in some neighbourhood of x0x_0. This reformulation connects directly to the sign-analysis of the difference quotient used in Fermat’s Lemma.

Summary

  • x0x_0 is a local maximum if f(x)f(x0)f(x) \leq f(x_0) for all xx near x0x_0 (within DD); strict if the inequality is sharp for xx0x \neq x_0.
  • Interior extrema lie in the open interior of the domain; boundary extrema do not.
  • Every global extremum is a local extremum; the converse fails.
  • Theorems that derive conditions from f(x0)=0f'(x_0) = 0 require the extremum to be interior and ff to be differentiable there.