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Section 5.2 Evaluation of Double Integrals

In this section we will learn how to compute a double integral over some domains. The idea is to reduce the computation to the evaluation of two integrals over functions of one variable only. We consider special domains of the form
(5.3)D1={(x,y)R2:axb,φ(x)yΦ(x)},
or the same situation with x and y switched
(5.4)D2={(x,y)R2:ayb,φ(y)xΦ(y)},
where φ and Φ are continuous functions on the interval [a,b], and φ(x)Φ(x) for all x[a,b]. The domain D is the region between the graphs of φ and Φ. Both possibilities are shown in Figure 5.10
A domain of the form $D_1$.
A domain of the form $D_2$.
Figure 5.10. The two types of special domains.
Assume now that we have a domain of the type D1. Recall that, the double integral of a function f can be interpreted as the volume of the region under its graph. To get an approximation of that volume we can `cut’ the region parallel to the y-axis into thin slices, and then add the volumes of the slices up. More precisely, we choose a partition a=x0<x1<<xn=b. We then look at the slice between xi1 and xi as shown in Figure 5.11.
Figure 5.11. Cutting a domain into thin slices
Its thickness is Δxi:=xixi1. We next choose xi[xi1,xi]. The approximate surface area of one side of the slice is then
F(xi):=φ(xi)Φ(xi)f(xi,y)dy.
Hence the approximate volume of one of the slices is F(xi)Δxi. Adding up we conclude that
i=1nF(xi)Δxi
is an approximation of the volume under the graph of f. The last expression is a Riemann sum for F. Passing to the limit as maxΔxi0 the above suggests that
D1f(x,y)dxdy=ab(φ(x)Φ(x)f(x,y)dy)dx.
The integral
φ(x)Φ(x)f(x,y)dy
is usually called the inner integral, the integral over [a,b] the outer integral, and the full expression an iterated integral. The above is not a rigorous proof, but strong evidence that a formula like the above holds. One can show that the formula is true, at least if f,φ,Φ are all continuous. Similar arguments can be applied with x and y interchanged, leading to a formula for domains of the form D2. We state the result as a theorem.

Example 5.13.

Let D be the domain below y=2x and above y=x2. Write
Df(x)dx
as an iterated integral.
Solution.
We first determine where 2xx2. To do so we solve the equation 2x=x2. One solution certainly is x=0. If x0 we can divide by x and get 2=x, providing another solution. Hence we have 2xx2 for 0x2. Make a sketch of the domain to visualise the situation. We therefore have a=0, b=2, φ(x)=x2 and Φ(x)=2x. Hence, by Fubini’s Theorem
Df(x)dx=02(x22xf(x,y)dy)dx,
which is an iterated integral as required.

Example 5.14.

Compute
Dx2ydxdy,
where D is the domain from Example 5.13.
Solution.
By the result from the previous example we have
Df(x,y)dxdy=02(x22xx2ydy)dx.
We first evaluate the inner integral:
x22xx2ydy=x2x22xydy=x2y22|x22x=x22((2x)2(x2)2)=2x4x62.
Then we evaluate the outer integral:
Df(x,y)dxdy=02(x22xx2ydy)dx=022x4x62dx=2x55|02x727|02=26502727+0=72652635=22635=2735,
which is the required result.