RA Iterated integrals and Fubini theorem

Section 10.2 Iterated integrals and Fubini theorem

Note: 1–2 lectures

The Riemann integral in several variables is hard to compute via the definition. For one-dimensional Riemann integral, we have the fundamental theorem of calculus, which allows computing many integrals without having to appeal to the definition of the integral. We will rewrite a Riemann integral in several variables into several one-dimensional Riemann integrals by iterating. However, if

f : [0, 1]^{2} \to R

is a Riemann integrable function, it is not immediately clear if the three expressions

\int_{[0, 1]^{2}} f, \int_{0}^{1} \int_{0}^{1} f (x, y) d x d y, and \int_{0}^{1} \int_{0}^{1} f (x, y) d y d x

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are equal, or if the last two are even well-defined.

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Example 10.2.1.

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Define

f (x, y) := {\begin{cases} 1 & if x =^{1} /_{2} and y \in Q, \\ 0 & otherwise. \end{cases}

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Then

f

is Riemann integrable on

R := [0, 1]^{2}

and

\int_{R} f = 0 .

Moreover,

\int_{0}^{1} \int_{0}^{1} f (x, y) d x d y = 0 .

However,

\int_{0}^{1} f (^{1} /_{2}, y) d y

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does not exist, so strictly speaking,

\int_{0}^{1} \int_{0}^{1} f (x, y) d y d x

does not make sense. See Figure 10.5.

Figure 10.5. Left:

[0, 1]^{2}

with the line

x =^{1} /_{2}

marked dotted and

\int_{0}^{1} f (x, y) d x

marked as gray solid line for a generic

y .

Center: Similar picture but

\int_{0}^{1} f (x, y) d y

marked for some

x \neq^{1} /_{2} .

Right: The three different rectangles in the partition used to integrate

f

in different grays.

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Proof: We start with integrability of

f .

Consider the partition of

[0, 1]^{2}

where the partition in the

x

direction is

{0,^{1} /_{2} - ϵ,^{1} /_{2} + ϵ, 1}

and in the

y

direction

{0, 1} .

The corresponding subrectangles are

R_{1} := [0,^{1} /_{2} - ϵ] \times [0, 1], R_{2} := [^{1} /_{2} - ϵ,^{1} /_{2} + ϵ] \times [0, 1], R_{3} := [^{1} /_{2} + ϵ, 1] \times [0, 1] .

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We have

m_{1} = M_{1} = 0,

m_{2} = 0,

M_{2} = 1,

and

m_{3} = M_{3} = 0 .

Therefore,

L (P, f) = m_{1} V (R_{1}) + m_{2} V (R_{2}) + m_{3} V (R_{3}) = 0 (^{1} /_{2} - ϵ) + 0 (2 ϵ) + 0 (^{1} /_{2} - ϵ) = 0,

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and

U (P, f) = M_{1} V (R_{1}) + M_{2} V (R_{2}) + M_{3} V (R_{3}) = 0 (^{1} /_{2} - ϵ) + 1 (2 ϵ) + 0 (^{1} /_{2} - ϵ) = 2 ϵ .

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The upper and lower sums are arbitrarily close and the lower sum is always zero, so the function is integrable and

\int_{R} f = 0 .

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For every fixed

y,

the function that takes

x

f (x, y)

is zero except perhaps at a single point

x =^{1} /_{2} .

Such a function is integrable and

\int_{0}^{1} f (x, y) d x = 0 .

Therefore,

\int_{0}^{1} \int_{0}^{1} f (x, y) d x d y = 0 .

However, if

x =^{1} /_{2},

the function that takes

y

f (^{1} /_{2}, y)

is the nonintegrable function that is 1 on the rationals and 0 on the irrationals. See Example 5.1.4.

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We solve this problem of undefined inside integrals by using the upper and lower integrals, which are always defined for any bounded function.

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Split the coordinates of

R^{n + m}

into two parts: Write the coordinates on

R^{n + m} = R^{n} \times R^{m}

(x, y)

where

x \in R^{n}

and

y \in R^{m} .

For a function

f (x, y),

write

f_{x} (y) := f (x, y)

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when

x

is fixed and we want a function of

y .

Write

f^{y} (x) := f (x, y)

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when

y

is fixed and we want a function of

x .

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Theorem 10.2.2. Fubini version A.

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Named after the Italian mathematician Guido Fubini (1879–1943).

Let

R \times S \subset R^{n} \times R^{m}

be a closed rectangle and

f : R \times S \to R

be integrable. The functions

g : R \to R

and

h : R \to R

defined by

g (x) := \underset{―}{\int_{S}} f_{x} and h (x) := \overset{―}{\int_{S}} f_{x}

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are integrable on

R

and

\int_{R} g = \int_{R} h = \int_{R \times S} f .

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In other words,

\int_{R \times S} f = \int_{R} (\underset{―}{\int_{S}} f (x, y) d y) d x = \int_{R} (\overset{―}{\int_{S}} f (x, y) d y) d x .

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f_{x}

is integrable for all

x,

for example when

f

is continuous, we obtain the more familiar

\int_{R \times S} f = \int_{R} \int_{S} f (x, y) d y d x .

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Proof.

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A partition of

R \times S

is a concatenation of a partition of

R

and a partition of

S .

That is, write a partition of

R \times S

(P, P^{'}) = (P_{1}, P_{2}, \dots, P_{n}, P_{1}^{'}, P_{2}^{'}, \dots, P_{m}^{'}),

where

P = (P_{1}, P_{2}, \dots, P_{n})

and

P^{'} = (P_{1}^{'}, P_{2}^{'}, \dots, P_{m}^{'})

are partitions of

R

and

S

respectively. Let

R_{1}, R_{2}, \dots, R_{N}

be the subrectangles of

P

and

R_{1}^{'}, R_{2}^{'}, \dots, R_{K}^{'}

be the subrectangles of

P^{'} .

The subrectangles of

(P, P^{'})

are

R_{i} \times R_{j}^{'}

where

1 \leq i \leq N

and

1 \leq j \leq K .

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Let

m_{i, j} := inf_{(x, y) \in R_{i} \times R_{j}^{'}} f (x, y) .

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Notice that

V (R_{i} \times R_{j}^{'}) = V (R_{i}) V (R_{j}^{'})

and hence

L ((P, P^{'}), f) = \sum_{i = 1}^{N} \sum_{j = 1}^{K} m_{i, j} V (R_{i} \times R_{j}^{'}) = \sum_{i = 1}^{N} (\sum_{j = 1}^{K} m_{i, j} V (R_{j}^{'})) V (R_{i}) .

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Define

m_{j} (x) := inf_{y \in R_{j}^{'}} f (x, y) = inf_{y \in R_{j}^{'}} f_{x} (y) .

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For

x \in R_{i},

we have

m_{i, j} \leq m_{j} (x),

and therefore,

\sum_{j = 1}^{K} m_{i, j} V (R_{j}^{'}) \leq \sum_{j = 1}^{K} m_{j} (x) V (R_{j}^{'}) = L (P^{'}, f_{x}) \leq \underset{―}{\int_{S}} f_{x} = g (x) .

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The inequality holds for all

x \in R_{i},

and so

\sum_{j = 1}^{K} m_{i, j} V (R_{j}^{'}) \leq inf_{x \in R_{i}} g (x) .

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We obtain

L ((P, P^{'}), f) \leq \sum_{j = 1}^{N} (inf_{x \in R_{j}} g (x)) V (R_{j}) = L (P, g) .

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Similarly,

U ((P, P^{'}), f) \geq U (P, h),

and the proof of this inequality is left as an exercise. Putting the two inequalities together with the fact that

g (x) \leq h (x)

for all

x,

L ((P, P^{'}), f) \leq L (P, g) \leq U (P, g) \leq U (P, h) \leq U ((P, P^{'}), f) .

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Since

f

is integrable, it must be that

g

is integrable as

U (P, g) - L (P, g) \leq U ((P, P^{'}), f) - L ((P, P^{'}), f),

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and we can make the right-hand side arbitrarily small. As for any partition we have

L ((P, P^{'}), f) \leq L (P, g) \leq U ((P, P^{'}), f),

we have

\int_{R} g = \int_{R \times S} f .

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Likewise,

L ((P, P^{'}), f) \leq L (P, g) \leq L (P, h) \leq U (P, h) \leq U ((P, P^{'}), f),

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and hence

U (P, h) - L (P, h) \leq U ((P, P^{'}), f) - L ((P, P^{'}), f) .

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f

is integrable, so is

h .

Moreover,

L ((P, P^{'}), f) \leq L (P, h) \leq U ((P, P^{'}), f)

implies

\int_{R} h = \int_{R \times S} f .

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We can also do the iterated integration in the opposite order. The proof of this version is almost identical to version A (or follows quickly from version A). We leave it as an exercise.

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Theorem 10.2.3. Fubini version B.

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Let

R \times S \subset R^{n} \times R^{m}

be a closed rectangle and

f : R \times S \to R

be integrable. The functions

g : S \to R

and

h : S \to R

defined by

g (y) := \underset{―}{\int_{R}} f^{y} and h (y) := \overset{―}{\int_{R}} f^{y}

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are integrable on

S

and

\int_{S} g = \int_{S} h = \int_{R \times S} f .

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That is,

\int_{R \times S} f = \int_{S} (\underset{―}{\int_{R}} f (x, y) d x) d y = \int_{S} (\overset{―}{\int_{R}} f (x, y) d x) d y .

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Next suppose

f_{x}

and

f^{y}

are integrable. For example, suppose

f

is continuous. By putting the two versions together we obtain the familiar

\int_{R \times S} f = \int_{R} \int_{S} f (x, y) d y d x = \int_{S} \int_{R} f (x, y) d x d y .

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Often the Fubini theorem is stated in two dimensions for a continuous function

f : R \to R

on a rectangle

R = [a, b] \times [c, d] .

Then the Fubini theorem states that

\int_{R} f = \int_{a}^{b} \int_{c}^{d} f (x, y) d y d x = \int_{c}^{d} \int_{a}^{b} f (x, y) d x d y .

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The Fubini theorem is commonly thought of as the theorem that allows us to swap the order of iterated integrals, although there are many variations on Fubini, and we have seen but two of them.

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Repeatedly applying Fubini theorem gets us the following corollary: Let

R := [a_{1}, b_{1}] \times [a_{2}, b_{2}] \times \dots \times [a_{n}, b_{n}] \subset R^{n}

be a closed rectangle and let

f : R \to R

be continuous. Then

\int_{R} f = \int_{a_{1}}^{b_{1}} \int_{a_{2}}^{b_{2}} \dots \int_{a_{n}}^{b_{n}} f (x_{1}, x_{2}, \dots, x_{n}) d x_{n} d x_{n - 1} \dots d x_{1} .

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We may switch the order of integration to any order we please. We may relax the continuity requirement by making sure that all the intermediate functions are integrable, or by using upper or lower integrals appropriately.

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Exercises Exercises

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10.2.1.

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Compute

\int_{0}^{1} \int_{- 1}^{1} x e^{x y} d x d y

in a simple way.

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10.2.2.

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Prove the assertion

U ((P, P^{'}), f) \geq U (P, h)

from the proof of Theorem 10.2.2.

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10.2.3.

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(Easy) Prove Theorem 10.2.3.

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10.2.4.

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Let

R := [a, b] \times [c, d]

and

f (x, y)

is an integrable function on

R

such that for every fixed

y,

the function that takes

x

f (x, y)

is zero except at finitely many points. Show

\int_{R} f = 0 .

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10.2.5.

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Let

R := [a, b] \times [c, d]

and

f (x, y) := g (x) h (y)

for continuous functions

g : [a, b] \to R

and

h : [c, d] \to R .

Prove

\int_{R} f = (\int_{a}^{b} g) (\int_{c}^{d} h) .

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10.2.6.

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Compute (using calculus)

\int_{0}^{1} \int_{0}^{1} \frac{x^{2} - y^{2}}{{(x^{2} + y^{2})}^{2}} d x d y and \int_{0}^{1} \int_{0}^{1} \frac{x^{2} - y^{2}}{{(x^{2} + y^{2})}^{2}} d y d x .

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You will need to interpret the integrals as improper, that is, the limit of

\int_{ϵ}^{1}

ϵ \to 0^{+} .

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10.2.7.

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Suppose

f (x, y) := g (x)

where

g : [a, b] \to R

is Riemann integrable. Show that

f

is Riemann integrable for every

R = [a, b] \times [c, d]

and

\int_{R} f = (d - c) \int_{a}^{b} g .

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10.2.8.

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Define

f : [- 1, 1] \times [0, 1] \to R

f (x, y) := {\begin{cases} x & if y \in Q, \\ 0 & else. \end{cases}

Show $\int_{0}^{1} \int_{- 1}^{1} f (x, y) d x d y$ exists, but $\int_{- 1}^{1} \int_{0}^{1} f (x, y) d y d x$ does not.
Compute $\int_{- 1}^{1} \overset{―}{\int_{0}^{1}} f (x, y) d y d x$ and $\int_{- 1}^{1} \underset{―}{\int_{0}^{1}} f (x, y) d y d x .$
Show $f$ is not Riemann integrable on $[- 1, 1] \times [0, 1]$ (use Fubini).

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10.2.9.

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Define

f : [0, 1] \times [0, 1] \to R

f (x, y) := {\begin{cases} ^{1} /_{q} & if x \in Q, y \in Q, and y =^{p} /_{q} in lowest terms, \\ 0 & else. \end{cases}

Show $f$ is Riemann integrable on $[0, 1] \times [0, 1] .$
Find $\overset{―}{\int_{0}^{1}} f (x, y) d x$ and $\underset{―}{\int_{0}^{1}} f (x, y) d x$ for all $y \in [0, 1],$ and show they are unequal for all $y \in Q .$
Show $\int_{0}^{1} \int_{0}^{1} f (x, y) d y d x$ exists, but $\int_{0}^{1} \int_{0}^{1} f (x, y) d x d y$ does not.

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Note: By Fubini,

\int_{0}^{1} \overset{―}{\int_{0}^{1}} f (x, y) d y d x

and

\int_{0}^{1} \underset{―}{\int_{0}^{1}} f (x, y) d y d x

do exist and equal the integral of

f

R .

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