
22 Double Integrals I
22.1 Introduction
If \(f(x,y)\) is a function defined over a planar region \(R\), we can write \[ \iint_R f(x,y) \mathop{}\!\mathrm{d}A \] for the volume of the solid under the graph of \(f\) and above \(R\): the double integral of \(f(x,y)\) over \(R\).
To define such a quantity, we need to partition \(R\) into small rectangles, then consider the limit of Riemann sums as the partition becomes finer—see (Stewart et al. 2020, figs. 15.1.4–5).
As with a single variable, integrals have some nice properties that help us compute them. In particular:
If \(f(x,y)\) and \(g(x,y)\) are continuous on a region \(R\) and \(a\) and \(b\) are constants, then \[ \iint_R \left( a f(x,y) + b g(x,y) \right) \mathop{}\!\mathrm{d}A = a \iint_R f(x,y)\ \mathop{}\!\mathrm{d}A + b \iint_R g(x,y) \mathop{}\!\mathrm{d}A. \]
22.2 Main results
If \(f(x,y)\) is continuous on a rectangular region \(R = [a,b] \times [c,d]\), then \[ \iint_R f(x,y) \mathop{}\!\mathrm{d}A = \int_a^b \left( \int_c^d f(x,y) \mathop{}\!\mathrm{d}y \right) \mathop{}\!\mathrm{d}x = \int_c^d \left( \int_a^b f(x,y) \mathop{}\!\mathrm{d}x \right) \mathop{}\!\mathrm{d}y. \]
By Fubini’s theorem, we can compute this integral in two ways:
\[ \begin{split} \iint_R x^2 y \mathop{}\!\mathrm{d}A & = \int_0^1 \int_2^3 x^2 y \mathop{}\!\mathrm{d}y \mathop{}\!\mathrm{d}x = \int_0^1 \tfrac{5}{2} x^2 \mathop{}\!\mathrm{d}x = \tfrac{5}{6} \\ & = \int_2^3 \int_0^1 x^2 y \mathop{}\!\mathrm{d}x \mathop{}\!\mathrm{d}y = \int_2^3 \tfrac{1}{3} y \mathop{}\!\mathrm{d}y = \tfrac{5}{6}. \end{split} \]
The first of these—where we hold \(x\) constant, integrate along \(y\), and then add up these slices in \(x\)—is shown in the first figure below; the second is the last figure.


We emphasize that the integrands in the penultimate step of each calculation above—\(\frac{5}{2} x^2\) and \(\frac{1}{3} y\), respectively—represent the area of each slice being integrated to compute the final volume, as shown below:
Each slice has area \(\frac{5}{2} x^2\).