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Clairaut's Theorem




:f \colon \mathbb{R}^n o \mathbb{R}

has Continuous second Partial Derivatives at any given point in \mathbb{R}^n , say, (a_1, \dots, a_n), then for 1 \leq i,j \leq n,

: rac{\partial^2 f}{\partial x_i\, \partial x_j}(a_1, \dots, a_n) = rac{\partial^2 f}{\partial x_j\, \partial x_i}(a_1, \dots, a_n).

In words, the partial derivatives of this function Commute at that point. This theorem is named after the French mathematician Alexis Clairaut .


CLAIRAUT'S CONSTANT

A byproduct of this theorem is Clairaut's constant (alternatively known as "Clairaut's formula" and "Clairaut's parameter"), which relates the Latitude (Lat) and Azimuth (Az) of points on a Sphere's Great Circle .
The identification of a particular great circle equals its azimuth at the Equator , or arc path (AP):
:\sin\!\left\{AP ight\}=\cos\!\left\{Lat ight\}\sin\!\left\{Az ight\}.\,\!


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