Since fx and fy are functions of x and y, we can take derivatives of fx and fy to
get second derivatives. There are four such
second derivatives, since each time we can differentiate with
respect to x or y. Each of these second derivatives has
multiple notations, and we have listed some of them.
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
A nice result regarding second partial derivatives is Clairaut's Theorem, which tells us
that the mixed variable partial derivatives are equal.
Clairaut's Theorem
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.
Example 1: Let f(x,y)=3x2−4y3−7x2y3.
Previously, we determined that fx=6x−14xy3 and
fy=−12y2−21x2y2. We have four second derivatives, but
as Clairaut's Theorem tells us, fxy=fyx, so we really only
need to compute three of them (we do all four to illustrate the
theorem).