One way to state the interior extremum theorem is that, if a function has a local
extremum at some point and is
differentiable there, then the function's derivative at that point must be zero. In precise mathematical language: :Let f\colon (a,b) \rightarrow \mathbb{R} be a function from an
open interval to , and suppose that x_0 \in (a,b) is a point where f has a local extremum. If f is differentiable at x_0, then f'(x_0) = 0. Another way to understand the theorem is via the
contrapositive statement: if the derivative of a function at any point is not zero, then there is not a local extremum at that point. Formally: :If f is differentiable at x_0 \in (a,b), and f'(x_0) \neq 0, then x_0 is not a local extremum of f.
Corollary The global extrema of a function
f on a
domain A occur only at
boundaries, non-differentiable points, and stationary points. If x_0 is a global extremum of
f, then one of the following is true: •
boundary: x_0 is in the boundary of
A •
non-differentiable: f is not differentiable at x_0 •
stationary point: x_0 is a stationary point of
f Extension A similar statement holds for the
partial derivatives of
multivariate functions. Suppose that some real-valued function of the real numbers f = f(t_1, t_2, \ldots,t_k) has an extremum at a point C, defined by C = (a_1, a_2,\ldots ,a_k). If f is differentiable at C, then:\frac{\partial}{\partial t_i}f(a_i)=0where i = 1, 2, \ldots ,k. The statement can also be extended to
differentiable manifolds. If f : M \to \mathbb{R} is a
differentiable function on a manifold M, then its local extrema must be
critical points of f, in particular points where the
exterior derivative df is zero. ==Applications==