Since fx and fy are functions of x and y, we can take
derivatives of these functions to get second derivatives. There are
four such second derivatives, since each time we can differentiate
with respect to x or y.
Notation for second partial derivatives (fx)x=fxx=f11=∂∂x(∂f∂x)=∂2f∂x2=∂2z∂x2
(fx)y=fxy=f12=∂∂y(∂f∂x)=∂2f∂y∂x=∂2z∂y∂x
(fy)x=fyx=f21=∂∂x(∂f∂y)=∂2f∂x∂y=∂2z∂x∂y
(fy)y=fyy=f22=∂∂y(∂f∂y)=∂2f∂y2=∂2z∂y2
The main result about higher derivatives is:
Clairaut's Theorem (or "mixed partials are equal"): If fxy and fyx are both defined and continuous in a region containing the point (a,b), then fxy(a,b)=fyx(a,b).
A consequence of this theorem is that we don't need to keep track of
the order in which we take derivatives. We just need to keep track of
how many times we differentiate with respect to each variable.
Higher partial derivatives and Clairaut's theorem are explained in the
following video.