Ejemplos integrales dobles

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    17.3 THE EVALUATION OF DOUBLE INTEGRALS BY REPEATED INTEGRALS I 881

    evident, but actually it is quite difficult to prove. The result follows from what is known

    as Fubinis theorem. J

    Computations

    Example 1 Evaluate

    (x4 2y) dxdy with as in Figure 17.3.4. x

    y

    y=x2

    y=

    x2

    x = 1 x = 1

    x

    Figure 17.3.4

    SOLUTION By projectingonto thex-axis,we obtain theinterval [1, 1]. Theregion

    consists of all points (x, y) with

    1 x 1 and x2 y x2.

    This is a region of Type I. By (17.3.1),

    (x4 2y) dxdy =

    11

    x2x2

    [x4 2y] dy

    dx

    = 1

    1x4y y2

    x2

    x2dx

    =

    11

    (x6 x4) (x6 x4)

    dx

    =

    11

    2x6 dx =

    27x7

    11=

    47. J

    Example 2 Evaluate

    (xy y3) dxdy with as in Figure 17.3.5.

    y = 1

    y = 0

    x = 1

    x = y

    x = 1

    x

    y

    y

    Figure 17.3.5

    SOLUTION By projecting

    onto the y-axis, we obtain the interval [0,

    1]. The region consists of all points (x, y) with

    0 y 1 and 1 x y.

    After the Italian mathematician Guido Fubini (18791943).

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    882 I CHAPTER 17 DOUBLE AND TRIPLE INTEGRALS

    This is a region of Type II. By (17.3.2),

    (xy y3) dxdy =

    10

    y1

    (xy y3) dx

    dy

    =

    10

    12x2y x y3

    y1

    dy

    =

    10

    12y3 y4

    12y + y3

    dy

    =

    10 1

    2y3 y4 1

    2y

    dy

    =

    1

    8y4 1

    5y5 1

    4y2

    10= 23

    40.

    We can also project onto the x-axis and express as a region of Type I, but then the

    lower boundary is defined piecewise (see the figure) and the calculations are somewhat

    more complicated: setting

    (x) =

    0, 1 x 0

    x, 0 x 1,

    we have as the set of all points (x, y) with

    1 x 1 and (x) y 1;

    y

    x

    y = 1

    1 1

    y = x

    1

    1

    (0, 0)

    (1, 1)

    y = x2 (x = y1/2)

    y = x1/4

    (x = y4)

    x

    y

    x

    y

    Figure 17.3.6

    thus

    (xy y3) dxdy =

    11

    1(x)

    (xy y3) dy

    dx

    = 0

    1

    1

    (x)(xy y

    3

    ) dydx+

    1

    0

    1

    (x)(x y y

    3

    ) dydx

    =

    01

    10

    (xy y3) dy

    dx+

    10

    1x

    (xy y3) dy

    dx

    as you can check =

    1

    2

    + 3

    40

    = 23

    40.

    Repeated integrals

    ba

    2(x)1(x)

    f(x, y) dydx and

    dc

    2(y)1(y)

    f(x, y) dxdy

    can be written in more compact form by omitting the large parentheses. From now on

    we will simply writeba

    2(x)1(x)

    f(x, y) dydx and

    dc

    2(y)1(y)

    f(x, y) dxdy.

    Example 3 Evaluate

    (x1/2 y2) dxdy with as in Figure 17.3.6.

    SOLUTION The projection of onto the x-axis is the closed interval [0, 1], and

    can be characterized as the set of all (x, y) with

    0 x 1 and x2 y x1/4.

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    17.3 THE EVALUATION OF DOUBLE INTEGRALS BY REPEATED INTEGRALS I 883

    Therefore

    (x1/2 y2) dxdy =1

    0

    x1/4x2

    (x1/2 y2) dydx

    =

    10

    x1/2y 1

    3y3

    x1/4x2

    dx

    =

    10

    23x3/4 x5/2 + 1

    3x6

    dx

    =

    8

    21x7/4 2

    7x7/2 + 1

    21x7

    10=

    821 2

    7+

    121=

    17.

    We can also integrate in the other order. The projection of onto the y-axis is theclosed interval [0, 1], and can be characterized as the set of all (x, y) with

    0 y 1 and y4 x y1/2.This gives the same result:

    (x1/2 y2) dxdy =1

    0

    y1/2y4

    (x1/2 y2) dxdy

    =

    1

    0

    23x3/2 y2x

    y

    1/2

    y4dy

    =

    10

    23y3/4 y5/2 + 1

    3y6

    dy

    =

    8

    21y7/4 2

    7y7/2 + 1

    21y7

    10=

    821 2

    7+

    121=

    17. J

    x = y1/2

    x = y4

    y

    x

    y

    Example 4 Use double integration to calculate the area of the region encolsedby

    y = x2 and x + y = 2.

    SOLUTION The region is pictured in Figure 17.3.7. Its area is given by the double

    integral

    dxdy.

    We project onto the x-axis and write the boundaries as functions of x:

    y = x2, y = 2 x. is the set of all (x, y) with 2 x 1 and x2 y 2 x . Therefore

    dxdy =

    12

    2xx2

    dydx =

    12

    (2 x x2) dx =

    2x 12x2 1

    3x3

    12

    = (2 12 13 ) (4 2+ 83 ) = 92 .We can also project onto the y-axis and write the boundaries as functions of y, but

    then the calculations become more complicated. As illustrated in Figure 17.3.8, is

    the set of all (x, y) with

    0 y 4 and y x (y)

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    884 I CHAPTER 17 DOUBLE AND TRIPLE INTEGRALS

    12 1

    1

    4

    y = 2 x

    y = x2

    x

    y

    (1, 1)

    (2, 4)

    Figure 17.3.7

    12 1

    4

    x = 2 y

    x = y

    x

    y

    (1, 1)

    (2, 4)

    1

    x = y

    Figure 17.3.8

    where

    (y) =

    y, 0 y 1

    2 y, 1 y 4.Therefore

    dxdy =1

    0

    yy

    dxdy+4

    1

    2yy

    dxdy.

    As you can check, the sum of the integrals is 92

    .

    Symmetry in Double Integration

    First wego back to the one-variable case. (Section 5.8) Lets suppose that g is continuous

    on an interval which is symmetric about the origin, say [

    a,a].

    Ifg is odd, then

    aa

    g(x) dx = 0.

    Ifg is even, then

    aa

    g(x) dx = 2

    a0

    g(x) dx.

    We have similar results for double integrals.

    Suppose that is symmetric about the y-axis.

    If f is odd in x [ f(x, y) = f(x, y)], then

    f(x, y) dxdy = 0.

    If f is even in x [ f(x, y) = f(x, y)], then

    f(x, y) dxdy = 2

    right half

    of

    f(x, y) dxdy.

    Suppose that is symmetric about the x-axis.

    If f is odd in y [ f(x,y) = f(x, y)], then

    f(x, y) dxdy = 0.

    If f is even in y [ f(x,y) = f(x, y)], then

    f(x, y) dxdy = 2

    upper half

    of

    f(x, y) dxdy.

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    878 C H A P T E R 15 M U L T I P L E I N T E G R A T I O N

    E X A M P L E 4 Evaluate

    42

    91

    yex d y

    d x.

    Solution First evaluate the inner integral, treating x as a constant:

    S(x) =

    91

    yex d y = ex9

    1

    y d y = ex

    1

    2y2 9

    y=1

    = ex

    81 1

    2

    = 40ex

    Then integrate S(x) with respect to x:

    42

    91

    yex d y

    d x=

    42

    40ex d x= 40ex

    4

    2

    = 40(e4 e2)

    If an iterated integral is written with d x preceding d y, then we integrate first with

    respect to x: dc

    ba

    f(x, y) dx dy =

    dy=c

    bx=a

    f(x, y) d x

    d y

    Here, for clarity, we have included the variables in the limits of integration of the iterated

    integral on the right.

    We often omit the parentheses in the

    notation for an iterated integral:

    ba

    dc

    f(x, y) dy dx

    The order of the variables in dy dx tells us

    to integrate first with respect to y between

    the limits y = c and y = d.

    E X A M P L E 5 Evaluate

    /2

    0

    /2

    0

    sin(2x+ y) dx dy.

    Solution Compute the inner integral, treating y as a constant:

    /2

    0

    sin(2x+ y) d x= 1

    2cos(2x+ y)

    /2x=0

    = 1

    2cos(+ y)+

    1

    2cos y

    /2

    0

    /2

    0

    sin(2x+ y) dx dy = 1

    2

    /2

    0cos(+ y) cos y d y

    = 1

    2

    sin(+ y) sin(y)

    /2y=0

    = 1

    2

    sin

    3

    2 sin

    2

    +

    1

    2

    sin sin0

    = 1

    E X A M P L E 6 Reversing the Order of Integration Verify that1

    0

    4

    2

    x2y3 dy dx=

    4

    2

    1

    0

    x2y3 dx dy

    Solution Both integrals have the value 20:

    10

    42

    x2y3 dy dx=

    10

    1

    4x2y4

    4y=2

    d x=

    10

    64x2 4x2

    d x

    =1

    060x

    2

    d x= 20x31

    0= 20

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    S E C T I O N 15.1 Integration in Several Variables 879

    42

    10

    x2y3 dx dy =

    42

    1

    3x3y3

    1x=0

    d y =

    1

    3

    42

    y3 d y

    =1

    12y

    44

    2

    =1

    12(

    256

    16) =

    20

    The previous example illustrates a general fact: The value of an iterated integral does

    not depend on the order in which the integration is performed. This is part of Fubinis

    Theorem. Even more important, Fubinis Theorem states that a double integral over a

    rectangle can be evaluated as an iterated integral.

    CAUTIONWhen you reverse the order of

    integration in an iterated integral,

    remember to interchange the limits of

    integration (the inner limits become the

    outer limits).

    THEOREM3 Fubinis Theorem The double integral of a continuous function f(x, y)

    over a rectangle R = [a, b] [c, d] is equal to the iterated integral (in either order):R

    f(x, y) d A =

    ba

    dc

    f(x, y) dy dx =

    dc

    ba

    f(x, y) dx dy

    Proof We sketch the proof. Consider a Riemann sum SN,M for a regular partition. Then

    SN,M is the sum of values f(Pi j )xy, where

    x =b a

    Nand y =

    d c

    M

    Fubinis Theorem ultimately stems from the elementary fact that we may sum these val-

    ues in any order. Think of the values f(Pi j ) as listed in an N M array. For example,

    the values for S3,3 are listed in the array in the margin. If we first sum the columns and

    3 f(P13) f(P23) f(P33)

    2 f(P12) f(P22) f(P32)

    1 f(P11) f(P21) f(P31)

    ji 1 2 3

    then add up the column sums, we obtain

    SN,M =

    Ni =1

    Mj =1

    f(Pi j )xy

    Sum in any order=

    Ni=1

    M

    j =1

    f(Pi j )y

    x

    First sum the columns,then add up the column sumsLet us choose sample points of the form Pi j = (xi , yj ), where {xi } are sample points

    for the regular partition on [a, b] and {yj } are sample points for the regular partition of

    [c, d]. We observe thatx andy approach zero as M and N tend to infinity. Therefore,

    the limit of the sums SN,M as P 0 may be expressed as a limit as N, M:R

    f(x, y) d A = limN,M

    Ni =1

    M

    j =1

    f(xi , yj )y

    x

    The inner sum on the right is a Riemann sum that approaches the single integraldc

    f(xi , y) d y as M approaches:

    limM

    SN,M = limM

    Mj =1

    f(xi , yj ) =

    dc

    f(xi , y) d y

    To complete the proof, we take two facts for granted. First is the fact that the function

    S(x) = d

    c f(x, y) d y is continuous for a x b. Second, the limit limN,M SN,Mmay be computed by first taking the limit with respect to M and then with respect to N.