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Title: VECTOR%20CALCULUS


1
17
VECTOR CALCULUS
2
VECTOR CALCULUS
  • So far, we have considered special types of
    surfaces
  • Cylinders
  • Quadric surfaces
  • Graphs of functions of two variables
  • Level surfaces of functions of three variables

3
VECTOR CALCULUS
  • Here, we use vector functions to describe more
    general surfaces, called parametric surfaces, and
    compute their areas.

4
VECTOR CALCULUS
  • Then, we take the general surface area formula
    and see how it applies to special surfaces.

5
VECTOR CALCULUS
17.6 Parametric Surfaces and their Areas
In this section, we will learn about Various
types of parametric surfaces and computing their
areas using vector functions.
6
INTRODUCTION
  • We describe a space curve by a vector function
    r(t) of a single parameter t.
  • Similarly, we can describe a surface by a
    vector function r(u, v) of two parameters u and
    v.

7
INTRODUCTION
Equation 1
  • We suppose that r(u, v) x(u, v) i
    y(u, v) j z (u, v) kis a vector-valued
    function defined on a region D in the uv-plane.

8
INTRODUCTION
  • So x, y, and zthe component functions of rare
    functions of the two variables u and v with
    domain D.

9
PARAMETRIC SURFACE
Equations 2
  • The set of all points (x, y, z) in such that
    x x(u, v) y y(u, v) z
    z(u, v)and (u, v) varies throughout D, is
    called a parametric surface S.
  • Equations 2 are called parametric equations of S.

10
PARAMETRIC SURFACES
  • Each choice of u and v gives a point on S.
  • By making all choices, we get all of S.

11
PARAMETRIC SURFACES
  • In other words, the surface S is traced out by
    the tip of the position vector r(u, v) as (u, v)
    moves throughout the region D.

12
PARAMETRIC SURFACES
Example 1
  • Identify and sketch the surface with vector
    equation r(u, v) 2 cos u i v j 2 sin u k
  • The parametric equations for this surface are
    x 2 cos u y v z 2 sin
    u

13
PARAMETRIC SURFACES
Example 1
  • So, for any point (x, y, z) on the surface, we
    have x2 z2 4 cos2u 4 sin2u
    4
  • This means that vertical cross-sections parallel
    to the xz-plane (that is, with y constant) are
    all circles with radius 2.

14
PARAMETRIC SURFACES
Example 1
  • Since y v and no restriction is placed on v,
    the surface is a circular cylinder with radius 2
    whose axis is the y-axis.

15
PARAMETRIC SURFACES
  • In Example 1, we placed no restrictions on the
    parameters u and v.
  • So, we obtained the entire cylinder.

16
PARAMETRIC SURFACES
  • If, for instance, we restrict u and v by writing
    the parameter domain as 0
    u p/2 0 v 3then x 0
    z 0 0 y 3

17
PARAMETRIC SURFACES
  • In that case, we get the quarter-cylinder with
    length 3.

18
PARAMETRIC SURFACES
  • If a parametric surface S is given by a vector
    function r(u, v), then there are two useful
    families of curves that lie on Sone with u
    constant and the other with v constant.
  • These correspond to vertical and horizontal
    lines in the uv-plane.

19
PARAMETRIC SURFACES
  • Keeping u constant by putting u u0, r(u0, v)
    becomes a vector function of the single parameter
    v and defines a curve C1 lying on S.

20
GRID CURVES
  • Similarly, keeping v constant by putting v v0,
    we get a curve C2 given by r(u, v0) that lies on
    S.
  • We call these curves grid curves.

21
GRID CURVES
  • In Example 1, for instance, the grid curves
    obtained by
  • Letting u be constant are horizontal lines.
  • Letting v be constant are circles.

22
GRID CURVES
  • In fact, when a computer graphs a parametric
    surface, it usually depicts the surface by
    plotting these grid curvesas we see in the
    following example.

23
GRID CURVES
Example 2
  • Use a computer algebra system to graph the
    surface
  • r(u, v) lt(2 sin v) cos u, (2 sin v)
    sin u, u cos vgt
  • Which grid curves have u constant?
  • Which have v constant?

24
GRID CURVES
Example 2
  • We graph the portion of the surface with
    parameter domain 0 u 4p, 0 v 2p
  • It has the appearance of a spiral tube.

25
GRID CURVES
Example 2
  • To identify the grid curves, we write the
    corresponding parametric equations
    x (2 sin v) cos u y (2 sin v) sin
    u z u cos v

26
GRID CURVES
Example 2
  • If v is constant, then sin v and cos v are
    constant.
  • So, the parametric equations resemble those of
    the helix in Example 4 in Section 13.1

27
GRID CURVES
Example 2
  • So, the grid curves with v constant are the
    spiral curves.
  • We deduce that the grid curves with u constant
    must be the curves that look like circles.

28
GRID CURVES
Example 2
  • Further evidence for this assertion is that, if
    u is kept constant, u u0, then the equation
    z u0
    cos v shows that the z-values vary from u0
    1 to u0 1.

29
PARAMETRIC REPRESENTATION
  • In Examples 1 and 2 we were given a vector
    equation and asked to graph the corresponding
    parametric surface.
  • In the following examples, however, we are given
    the more challenging problem of finding a vector
    function to represent a given surface.
  • In the rest of the chapter, we will often need
    to do exactly that.

30
PARAMETRIC REPRESENTATIONS
Example 3
  • Find a vector function that represents the plane
    that
  • Passes through the point P0 with position vector
    r0.
  • Contains two nonparallel vectors a and b.

31
PARAMETRIC REPRESENTATIONS
Example 3
  • If P is any point in the plane, we can get from
    P0 to P by moving a certain distance in the
    direction of a and another distance in the
    direction of b.
  • So, there are scalars u and v such that
    ua vb

32
PARAMETRIC REPRESENTATIONS
Example 3
  • The figure illustrates how this works, by means
    of the Parallelogram Law, for the case where u
    and v are positive.
  • See also Exercise 40 in Section 12.2

33
PARAMETRIC REPRESENTATIONS
Example 3
  • If r is the position vector of P, then
  • So, the vector equation of the plane can be
    written as r(u, v) r0 ua
    vb where u and v are real numbers.

34
PARAMETRIC REPRESENTATIONS
Example 3
  • If we write r ltx, y, zgt r0 ltx0, y0, z0gt
    a lta1, a2, a3gt b ltb1, b2, b3gt we can
    write the parametric equations of the plane
    through the point (x0, y0, z0) as
  • x x0 ua1 vb1
    y y0 ua2 vb2 z z0
    ua3 vb3

35
PARAMETRIC REPRESENTATIONS
Example 4
  • Find a parametric representation of the sphere
    x2 y2 z2 a2
  • The sphere has a simple representation ? a in
    spherical coordinates.
  • So, lets choose the angles F and ? in spherical
    coordinates as the parameters (Section 15.8).

36
PARAMETRIC REPRESENTATIONS
Example 4
  • Then, putting ? a in the equations for
    conversion from spherical to rectangular
    coordinates (Equations 1 in Section 15.8), we
    obtain
  • x a sin F cos ? y a sin F sin ?
  • z a cos F
  • as the parametric equations of the sphere.

37
PARAMETRIC REPRESENTATIONS
Example 4
  • The corresponding vector equation is r(F, ?)
    a sin F cos ? i a sin F sin ? j a cos F k
  • We have 0 F p and 0 ? 2p.
  • So, the parameter domain is the rectangle
    D 0, p x 0,
    2p

38
PARAMETRIC REPRESENTATIONS
Example 4
  • The grid curves with
  • F constant are the circles of constant latitude
    (including the equator).
  • ? constant are the meridians (semicircles), which
    connect the north and south poles.

39
APPLICATIONSCOMPUTER GRAPHICS
  • One of the uses of parametric surfaces is in
    computer graphics.

40
COMPUTER GRAPHICS
  • The figure shows the result of trying to graph
    the sphere x2 y2 z2 1 by
  • Solving the equation for z.
  • Graphing the top and bottom hemispheres
    separately.

41
COMPUTER GRAPHICS
  • Part of the sphere appears to be missing because
    of the rectangular grid system used by the
    computer.

42
COMPUTER GRAPHICS
  • The much better picture here was produced by a
    computer using the parametric equations found in
    Example 4.

43
PARAMETRIC REPRESENTATIONS
Example 5
  • Find a parametric representation for the
    cylinder x2 y2 4 0
    z 1
  • The cylinder has a simple representation r 2
    in cylindrical coordinates.
  • So, we choose as parameters ? and z in
    cylindrical coordinates.

44
PARAMETRIC REPRESENTATIONS
Example 5
  • Then the parametric equations of the cylinder
    are x 2 cos ? y 2 sin ? z
    z
  • where
  • 0 ? 2p
  • 0 z 1

45
PARAMETRIC REPRESENTATIONS
Example 6
  • Find a vector function that represents the
    elliptic paraboloid z x2 2y2
  • If we regard x and y as parameters, then the
    parametric equations are simply x x
    y y z x2 2y2and
    the vector equation is r(x, y) x i
    y j (x2 2y2) k

46
PARAMETRIC REPRESENTATIONS
  • In general, a surface given as the graph of a
    function of x and yan equation of the form z
    f(x, y)can always be regarded as a parametric
    surface by
  • Taking x and y as parameters.
  • Writing the parametric equations as x x
    y y z f(x, y)

47
PARAMETRIZATIONS
  • Parametric representations (also called
    parametrizations) of surfaces are not unique.
  • The next example shows two ways to parametrize a
    cone.

48
PARAMETRIZATIONS
Example 7
  • Find a parametric representation for the surface

    that is, the top half of
    the cone z2 4x2 4y2

49
PARAMETRIZATIONS
E. g. 7Solution 1
  • One possible representation is obtained by
    choosing x and y as parameters x x
    y y
  • So, the vector equation is

50
PARAMETRIZATIONS
E. g. 7Solution 2
  • Another representation results from choosing as
    parameters the polar coordinates r and ?.
  • A point (x, y, z) on the cone satisfies x r
    cos ? y r sin ?

51
PARAMETRIZATIONS
E. g. 7Solution 2
  • So, a vector equation for the cone is
    r(r, ?) r cos ? i r sin ? j 2r kwhere
  • r 0
  • 0 ? 2p

52
PARAMETRIZATIONS
  • For some purposes, the parametric representations
    in Solutions 1 and 2 are equally good.
  • In certain situations, though, Solution 2 might
    be preferable.

53
PARAMETRIZATIONS
  • For instance, if we are interested only in the
    part of the cone that lies below the plane z
    1, all we have to do in Solution 2 is change the
    parameter domain to 0 r ½ 0 ? 2p

54
SURFACES OF REVOLUTION
  • Surfaces of revolution can be represented
    parametrically and thus graphed using a computer.

55
SURFACES OF REVOLUTION
  • For instance, lets consider the surface S
    obtained by rotating the curve
    y f(x) a x b about the x-axis,
    where f(x) 0.

56
SURFACES OF REVOLUTION
  • Let ? be the angle of rotation as shown.

57
SURFACES OF REVOLUTION
Equations 3
  • If (x, y, z) is a point on S, then x x y
    f(x) cos ? z f(x) sin ?

58
SURFACES OF REVOLUTION
  • Thus, we take x and ? as parameters and regard
    Equations 3 as parametric equations of S.
  • The parameter domain is given by a x b
    0 ? 2p

59
SURFACES OF REVOLUTION
Example 8
  • Find parametric equations for the surface
    generated by rotating the curve y sin x, 0 x
    2p, about the x-axis.
  • Use these equations to graph the surface of
    revolution.

60
SURFACES OF REVOLUTION
Example 8
  • From Equations 3,
  • The parametric equations are x x y
    sin x cos ? z sin x sin ?
  • The parameter domain is 0 x 2p 0 ?
    2p

61
SURFACES OF REVOLUTION
Example 8
  • Using a computer to plot these equations and
    rotate the image, we obtain this graph.

62
SURFACES OF REVOLUTION
  • We can adapt Equations 3 to represent a surface
    obtained through revolution about the y- or
    z-axis.
  • See Exercise 30.

63
TANGENT PLANES
  • We now find the tangent plane to a parametric
    surface S traced out by a vector function
    r(u, v) x(u, v) i y(u, v) j z(u, v) k
    at a point P0 with position vector r(u0, v0).

64
TANGENT PLANES
  • Keeping u constant by putting u u0, r(u0, v)
    becomes a vector function of the single parameter
    v and defines a grid curve C1 lying on S.

65
TANGENT PLANES
Equation 4
  • The tangent vector to C1 at P0 is obtained by
    taking the partial derivative of r with respect
    to v

66
TANGENT PLANES
  • Similarly, keeping v constant by putting v v0,
    we get a grid curve C2 given by r(u, v0) that
    lies on S.

67
TANGENT PLANES
Equation 5
  • Its tangent vector at P0 is

68
SMOOTH SURFACE
  • If ru x rv is not 0, then the surface is called
    smooth (it has no corners).
  • For a smooth surface, the tangent plane is the
    plane that contains the tangent vectors ru and
    rv , and the vector ru x rv is a normal vector
    to the tangent plane.

69
TANGENT PLANES
Example 9
  • Find the tangent plane to the surface with
    parametric equations x u2
    y v2 z u 2v at the point
    (1, 1, 3).

70
TANGENT PLANES
Example 9
  • We first compute the tangent vectors

71
TANGENT PLANES
Example 9
  • Thus, a normal vector to the tangent plane is

72
TANGENT PLANES
Example 9
  • Notice that the point (1, 1, 3) corresponds to
    the parameter values u 1 and v 1.
  • So, the normal vector there is
    2 i 4 j 4 k

73
TANGENT PLANES
Example 9
  • Therefore, an equation of the tangent plane at
    (1, 1, 3) is 2(x 1) 4(y 1)
    4(z 3) 0or x 2y 2z
    3 0

74
TANGENT PLANES
  • The figure shows the self-intersecting surface in
    Example 9 and its tangent plane at (1, 1, 3).

75
SURFACE AREA
  • Now, we define the surface area of a general
    parametric surface given by Equation 1.

76
SURFACE AREAS
  • For simplicity, we start by considering a
    surface whose parameter domain D is a rectangle,
    and we divide it into subrectangles Rij.

77
SURFACE AREAS
  • Lets choose (ui, vj) to be the lower left
    corner of Rij.

78
PATCH
  • The part Sij of the surface S that corresponds to
    Rij is called a patch and has the point Pij with
    position vector r(ui, vj) as one of its corners.

79
SURFACE AREAS
  • Let ru ru(ui, vj) and rv
    rv(ui, vj) be the tangent vectors at Pij as
    given by Equations 5 and 4.

80
SURFACE AREAS
  • The figure shows how the two edges of the patch
    that meet at Pij can be approximated by vectors.

81
SURFACE AREAS
  • These vectors, in turn, can be approximated by
    the vectors ?u ru and ?v rv because partial
    derivatives can be approximated by difference
    quotients.
  • So, we approximate Sij by the parallelogram
    determined by the vectors ?u ru and ?v rv.

82
SURFACE AREAS
  • This parallelogram is shown here.
  • It lies in the tangent plane to S at Pij.

83
SURFACE AREAS
  • The area of this parallelogram is So, an
    approximation to the area of S is

84
SURFACE AREAS
  • Our intuition tells us that this approximation
    gets better as we increase the number of
    subrectangles.
  • Also, we recognize the double sum as a Riemann
    sum for the double integral
  • This motivates the following definition.

85
SURFACE AREAS
Definition 6
  • Suppose a smooth parametric surface S is
  • Given by r(u, v) x(u, v) i y(u, v) j
    z(u, v) k
    (u, v) D
  • Covered just once as (u, v) ranges throughout
    the parameter domain D.

86
SURFACE AREAS
Definition 6
  • Then, the surface area of S iswhere

87
SURFACE AREAS
Example 10
  • Find the surface area of a sphere of radius a.
  • In Example 4, we found x a sin F cos ?, y
    a sin F sin ?, z a cos F where the
    parameter domain is D (F, ?) 0
    F p, 0 ? 2p)

88
SURFACE AREAS
Example 10
  • We first compute the cross product of the
    tangent vectors

89
SURFACE AREAS
Example 10

90
SURFACE AREAS
Example 10
  • Thus,
  • since sin F 0 for 0 F p.

91
SURFACE AREAS
Example 10
  • Hence, by Definition 6, the area of the sphere is

92
SURFACE AREA OF THE GRAPH OF A FUNCTION
  • Now, consider the special case of a surface S
    with equation z f(x, y), where (x, y) lies in D
    and f has continuous partial derivatives.
  • Here, we take x and y as parameters.
  • The parametric equations are x x
    y y z f(x, y)

93
GRAPH OF A FUNCTION
Equation 7
  • Thus,and

94
GRAPH OF A FUNCTION
Equation 8
  • Thus, we have

95
GRAPH OF A FUNCTION
Formula 9
  • Then, the surface area formula in Definition 6
    becomes

96
GRAPH OF A FUNCTION
Example 11
  • Find the area of the part of the paraboloid z
    x2 y2 that lies under the plane z 9.
  • The plane intersects the paraboloid in the
    circle x2 y2 9, z 9

97
GRAPH OF A FUNCTION
Example 11
  • Therefore, the given surface lies above the disk
    D with center the origin and radius 3.

98
GRAPH OF A FUNCTION
Example 11
  • Using Formula 9, we have

99
GRAPH OF A FUNCTION
Example 11
  • Converting to polar coordinates, we obtain

100
SURFACE AREA
  • The question remains
  • Is our definition of surface area (Definition 6)
    consistent with the surface area formula from
    single-variable calculus (Formula 4 in Section
    8.2)?

101
SURFACE AREA
  • We consider the surface S obtained by rotating
    the curve y f(x), a x b about the
    x-axis, where
  • f(x) 0.
  • f is continuous.

102
SURFACE AREA
  • From Equations 3, we know that parametric
    equations of S are
  • x x y f(x) cos ? z f(x)
    sin ? a x b 0
    ? 2p

103
SURFACE AREA
  • To compute the surface area of S, we need the
    tangent vectors

104
SURFACE AREA
  • Thus,

105
SURFACE AREA
  • Hence,because f(x) 0.

106
SURFACE AREA
  • Thus, the area of S is

107
SURFACE AREA
  • This is precisely the formula that was used to
    define the area of a surface of revolution in
    single-variable calculus (Formula 4 in Section
    8.2).
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