Multivariable calculus

Partial Derivatives of x^3 - 3xy^2 (Monkey Saddle)

For f(x, y) = x^3 - 3xy^2 the partial with respect to x is 3x^2 - 3y^2, and the partial with respect to y is -6xy. This is the monkey saddle. Its second partials are 6x and -6x, which sum to zero, so the function satisfies Laplace's equation and is harmonic everywhere.

f(x,y)=x3−3xy2f(x,y) = x^3 - 3xy^2
∂f∂x=3x2−3y2\frac{\partial f}{\partial x} = 3x^2 - 3y^2
∂f∂y=−6xy\frac{\partial f}{\partial y} = -6xy

Both terms contain x, only one contains y

For ∂f∂x\frac{\partial f}{\partial x}, both terms are in play. The first gives 3x23x^2; in the second, −3y2-3y^2 is the constant multiplier on xx, so it contributes −3y2-3y^2.

∂f∂x=3x2−3y2\frac{\partial f}{\partial x} = 3x^2 - 3y^2

For ∂f∂y\frac{\partial f}{\partial y}, the term x3x^3 has no yy in it and contributes nothing. Only −3xy2-3xy^2 survives, with −3x-3x as the constant multiplier.

∂f∂y=−3x⋅2y=−6xy\frac{\partial f}{\partial y} = -3x \cdot 2y = -6xy

At (2,1)(2,1) the partials are 12−3=912 - 3 = 9 and −6(2)(1)=−12-6(2)(1) = -12, so the surface climbs in xx and drops in yy.

The mistake: giving x^3 a y derivative

Writing ∂f∂y=3x2−6xy\frac{\partial f}{\partial y} = 3x^2 - 6xy is the standard slip. It differentiates x3x^3 as though xx were the active variable, in the middle of a yy derivative.

Reset before each partial. Say out loud which letter is moving, then scan the terms once and cross out anything without that letter.

  • For ∂f∂y\frac{\partial f}{\partial y}: cross out x3x^3 entirely, since ∂∂y(x3)=0\frac{\partial}{\partial y}\left(x^3\right) = 0.
  • What remains is −3xy2-3xy^2, and only the y2y^2 is differentiated.
  • The coefficient −3-3 and the factor xx both ride along unchanged.

A second trap is the exponent on yy: ∂∂y(y2)=2y\frac{\partial}{\partial y}\left(y^2\right) = 2y, so the coefficient becomes −6-6, not −3-3.

Why this surface is called the monkey saddle

Setting both partials to zero gives −6xy=0-6xy = 0 and 3x2=3y23x^2 = 3y^2, whose only solution is the origin. There the surface has three directions going down and three going up, room for two legs and a tail, which is where the name comes from.

The second partials are worth computing here.

fxx=6x,fyy=−6x,fxx+fyy=0f_{xx} = 6x, \qquad f_{yy} = -6x, \qquad f_{xx} + f_{yy} = 0

A function whose second partials cancel like this satisfies Laplace's equation and is called harmonic. This one is the real part of the complex cube (x+iy)3(x + iy)^3, which is why the cancellation is exact at every point rather than a coincidence at one.

Frequently asked questions

Why does the second derivative test fail at the origin?

At (0,0)(0,0) every second partial is zero, so the discriminant fxxfyy−fxy2f_{xx}f_{yy} - f_{xy}^2 is 00 and the test is inconclusive. Restricting to the line y=0y = 0 gives x3x^3, which changes sign through the origin, so the point is neither a maximum nor a minimum.

Where does f_x vanish?

Setting 3x2−3y2=03x^2 - 3y^2 = 0 gives y=±xy = \pm x, the two diagonal lines. Along those lines the surface is momentarily flat in the xx direction, though it is still changing in yy unless you are at the origin.