The box has two sides of area \(xz\text{,}\) two sides of area \(yz\) and a bottom of area \(xy\text{.}\) So the total surface area of material used is
\begin{equation*}
S = 2xz + 2yz + xy
\end{equation*}
However the three dimensions \(x\text{,}\) \(y\) and \(z\) are not independent. The requirement that the box have volume \(V\) imposes the constraint
\begin{equation*}
xyz = V
\end{equation*}
We can use this constraint to eliminate one variable. Since \(z\) is at the end of the alphabet (poor \(z\)), we eliminate \(z\) by substituting \(z=\frac{V}{xy}\text{.}\) So we have find the values of \(x\) and \(y\) that minimize the function
\begin{equation*}
S(x,y) = \frac{2V}{y} + \frac{2V}{x} + xy
\end{equation*}
Let’s start by finding the critical points of \(S\text{.}\) Since
\begin{align*}
S_x(x,y) &= -\frac{2V}{x^2} + y\\
S_y(x,y) &= -\frac{2V}{y^2} + x
\end{align*}
\((x,y)\) is a critical point if and only if
\begin{align*}
x^2y&=2V \tag{E1}\\
xy^2&=2V \tag{E2}
\end{align*}
Solving (E1) for \(y\) gives \(y=\frac{2V}{x^2}\text{.}\) Substituting this into (E2) gives
\begin{equation*}
x\frac{4V^2}{x^4}=2V \implies
x^3 = 2V \implies x = \root{3}\of{2V}\quad\text{and}\quad
y = \frac{2V}{(2V)^{2/3}} = \root{3}\of{2V}
\end{equation*}
As there is only one critical point, we would expect it to give the minimum. But let’s use the second derivative test to verify that at least the critical point is a local minimum. The various second partial derivatives are
\begin{align*}
S_{xx}(x,y)&=\frac{4V}{x^3} &
S_{xx}\big(\root{3}\of{2V}\,,\,\root{3}\of{2V}\big)&=2\\
S_{xy}(x,y)&=1&
S_{xy}\big(\root{3}\of{2V}\,,\,\root{3}\of{2V}\big)&=1\\
S_{yy}(x,y)&=\frac{4V}{y^3} &
S_{yy}\big(\root{3}\of{2V}\,,\,\root{3}\of{2V}\big)&=2
\end{align*}
So
\begin{align*}
S_{xx}\big(\root{3}\of{2V}\,,\,\root{3}\of{2V}\big)\
S_{yy}\big(\root{3}\of{2V}\,,\,\root{3}\of{2V}\big)
-S_{xy}\big(\root{3}\of{2V}\,,\,\root{3}\of{2V}\big)^2
&=3 \gt 0\\
S_{xx}\big(\root{3}\of{2V}\,,\,\root{3}\of{2V}\big)&=2 \gt 0
\end{align*}
and, by Theorem
2.9.16.b,
\(\big(\root{3}\of{2V}\,,\,\root{3}\of{2V}\big)\) is a local minimum and the desired dimensions are
\begin{equation*}
x=y=\root{3}\of{2V}\qquad
z=\root{3}\of{\frac{V}{4}}
\end{equation*}
Note that our solution has \(x=y\text{.}\) That’s a good thing — the function \(S(x,y)\) is symmetric in \(x\) and \(y\text{.}\) Because the box has no top, the symmetry does not extend to \(z\text{.}\)