1. SECTION 13.7 SURFACE INTEGRALS

2. P2P213.7 SURFACE INTEGRALS  The relationship between surface integrals and surface area is much the same as the relationship between line integrals and arc length.

3. P3P313.7 SURFACE INTEGRALS  Suppose f is a function of three variables whose domain includes a surface S. We will define the surface integral of f over S such that, in the case where f(x, y, z) = 1, the value of the surface integral is equal to the surface area of S.  We start with parametric surfaces.  Then, we deal with the special case where S is the graph of a function of two variables.

4. P4P413.7 PARAMETRIC SURFACES  Suppose a surface S has a vector equation r(u, v) = x(u, v) i + y(u, v) j + z(u, v) k (u, v)  D  We first assume that the parameter domain D is a rectangle and we divide it into subrectangles R ij with dimensions ∆u and ∆v.

5. P5P513.7 PARAMETRIC SURFACES  Then, the surface S is divided into corresponding patches S ij.  We evaluate f at a point P ij * in each patch, multiply by the area ∆S ij of the patch, and form the Riemann sum

6. P6P613.7 SURFACE INTEGRAL  Then, we take the limit as the number of patches increases and define the surface integral of f over the surface S as:

7. P7P713.7 SURFACE INTEGRALS  Notice the analogy with: The definition of a line integral (Definition 2 in Section 13.2) The definition of a double integral (Definition 5 in Section 12.1)

8. P8P813.7 SURFACE INTEGRALS  To evaluate the surface integral in Equation 1, we approximate the patch area ∆S ij by the area of an approximating parallelogram in the tangent plane.

9. P9P913.7 SURFACE INTEGRALS  In our discussion of surface area in Section 13.6, we made the approximation ∆S ij ≈ |r u × r v | ∆u ∆v where: are the tangent vectors at a corner of S ij.

10. P1013.7 SURFACE INTEGRALS  If the components are continuous and r u and r v are nonzero and nonparallel in the interior of D, it can be shown from Definition 1 — even when D is not a rectangle — that:

11. P1113.7 SURFACE INTEGRALS  This should be compared with the formula for a line integral:  Observe also that:

12. P1213.7 SURFACE INTEGRALS  Formula 2 allows us to compute a surface integral by converting it into a double integral over the parameter domain D. When using this formula, remember that f(r(u, v) is evaluated by writing x = x(u, v), y = y(u, v), z = z(u, v) in the formula for f(x, y, z)

13. P1313.7 Example 1  Compute the surface integral, where S is the unit sphere x 2 + y 2 + z 2 = 1.

14. P1413.7 Example 1 SOLUTION  As in Example 4 in Section 13.6, we use the parametric representation x = sin  cos , y = sin  sin , z = cos  0 ≤  ≤ , 0 ≤  ≤ 2  That is, r( ,  ) = sin  cos  i + sin  sin  j + cos  k

15. P1513.7 Example 1 SOLUTION  As in Example 9 in Section 13.6, we can compute that: |r  × r  | = sin 

16. P1613.7 Example 1 SOLUTION  Therefore, by Formula 2,

17. P1713.7 APPLICATIONS  Surface integrals have applications similar to those for the integrals we have previously considered.  For example, suppose a thin sheet (say, of aluminum foil) has: The shape of a surface S. The density (mass per unit area) at the point (x, y, z) as  (x, y, z).

18. P1813.7 MASS  Then, the total mass of the sheet is:

19. P1913.7 CENTER OF MASS  The center of mass is, where  Moments of inertia can also be defined as before. See Exercise 35.

20. P2013.7 GRAPHS  Any surface S with equation z = g(x, y) can be regarded as a parametric surface with parametric equations x = x y = y z = g(x, y) So, we have:

21. P2113.7 GRAPHS  Thus,  and

22. P2213.7 GRAPHS  Therefore, in this case, Formula 2 becomes:

23. P2313.7 GRAPHS  Similar formulas apply when it is more convenient to project S onto the yz-plane or xy- plane.

24. P2413.7 GRAPHS  For instance, if S is a surface with equation y = h(x, z) and D is its projection on the xz-plane, then

25. P2513.7 Example 2  Evaluate where S is the surface z = x + y 2, 0 ≤ x ≤ 1, 0 ≤ y ≤ 2  See Figure 2.  SOLUTION

26. P2613.7 Example 2 SOLUTION  So, Formula 4 gives:

27. P2713.7 GRAPHS  If S is a piecewise-smooth surface — a finite union of smooth surfaces S 1, S 2, …, S n that intersect only along their boundaries — then the surface integral of f over S is defined by:

28. P2813.7 Example 3  Evaluate, where S is the surface whose: Sides S 1 are given by the cylinder x 2 + y 2 = 1. Bottom S 2 is the disk x 2 + y 2 ≤ 1 in the plane z = 0. Top S 3 is the part of the plane z = 1 + x that lies above S 2.

29. P2913.7 Example 3 SOLUTION  The surface S is shown in Figure 3. We have changed the usual position of the axes to get a better look at S.

30. P3013.7 Example 3 SOLUTION  For S 1, we use  and z as parameters (Example 5 in Section 13.6) and write its parametric equations as: x = cos  y = sin  z = z where: 0 ≤  ≤ 2  0 ≤ z ≤ 1 + x = 1 + cos 

31. P3113.7 Example 3 SOLUTION  Therefore, and

32. P3213.7 Example 3 SOLUTION  Thus, the surface integral over S 1 is:

33. P3313.7 Example 3 SOLUTION  Since S 2 lies in the plane z = 0, we have:  S 3 lies above the unit disk D and is part of the plane z = 1 + x. So, taking g(x, y) = 1 + x in Formula 4 and converting to polar coordinates, we have the following result.

34. P3413.7 Example 3 SOLUTION

35. P3513.7 Example 3 SOLUTION  Therefore,

36. P3613.7 ORIENTED SURFACES  To define surface integrals of vector fields, we need to rule out nonorientable surfaces such as the M ö bius strip shown in Figure 4. It is named after the German geometer August M ö bius (1790 – 1868).

37. P3713.7 MOBIUS STRIP  You can construct one for yourself by: 1.Taking a long rectangular strip of paper. 2.Giving it a half-twist. 3.Taping the short edges together.

38. P3813.7 MOBIUS STRIP  If an ant were to crawl along the M ö bius strip starting at a point P, it would end up on the “ other side ” of the strip — that is, with its upper side pointing in the opposite direction.

39. P3913.7 MOBIUS STRIP  Then, if it continued to crawl in the same direction, it would end up back at the same point P without ever having crossed an edge. If you have constructed a M ö bius strip, try drawing a pencil line down the middle.

40. P4013.7 MOBIUS STRIP  Therefore, a M ö bius strip really has only one side. You can graph the M ö bius strip using the parametric equations in Exercise 28 in Section 13.6.

41. P4113.7 ORIENTED SURFACES  From now on, we consider only orientable (two- sided) surfaces.

42. P4213.7 ORIENTED SURFACES  We start with a surface S that has a tangent plane at every point (x, y, z) on S (except at any boundary point). There are two unit normal vectors n 1 and n 2 = – n 1 at (x, y, z). See Figure 6.

43. P4313.7 ORIENTED SURFACE & ORIENTATION  If it is possible to choose a unit normal vector n at every such point (x, y, z) so that n varies continuously over S, then S is called an oriented surface. The given choice of n provides S with an orientation.

44. P4413.7 POSSIBLE ORIENTATIONS  There are two possible orientations for any orientable surface.

45. P4513.7 UPWARD ORIENTATION  For a surface z = g(x, y) given as the graph of g, we use Equation 3 to associate with the surface a natural orientation given by the unit normal vector As the k-component is positive, this gives the upward orientation of the surface.

46. P4613.7 ORIENTATION  If S is a smooth orientable surface given in parametric form by a vector function r(u, v), then it is automatically supplied with the orientation of the unit normal vector The opposite orientation is given by – n.

47. P4713.7 ORIENTATION  For instance, in Example 4 in Section 13.6, we found the parametric representation r( ,  ) = a sin  cos  i + a sin  sin  j + a cos  k for the sphere x 2 + y 2 + z 2 = a 2

48. P4813.7 ORIENTATION  Then, in Example 9 in Section 13.6, we found that: r  × r  = a 2 sin 2  cos  i + a 2 sin 2  sin  j + a 2 sin  cos  k and |r  × r  | = a 2 sin 

49. P4913.7 ORIENTATION  So, the orientation induced by r( ,  ) is defined by the unit normal vector

50. P5013.7 POSITIVE ORIENTATION  Observe that n points in the same direction as the position vector — that is, outward from the sphere.  See Figure 8. Fig. 17.7.8, p. 1122

51. P5113.7 NEGATIVE ORIENTATION  The opposite (inward) orientation would have been obtained (see Figure 9) if we had reversed the order of the parameters because r  × r  = – r  × r 

52. P5213.7 CLOSED SURFACES  For a closed surface — a surface that is the boundary of a solid region E — the convention is that: The positive orientation is the one for which the normal vectors point outward from E. Inward-pointing normals give the negative orientation.

53. P5313.7 SURFACE INTEGRALS OF VECTOR FIELDS  Suppose that S is an oriented surface with unit normal vector n.  Then, imagine a fluid with density  (x, y, z) and velocity field v(x, y, z) flowing through S. Think of S as an imaginary surface that doesn ’ t impede the fluid flow — like a fishing net across a stream.

54. P5413.7 SURFACE INTEGRALS OF VECTOR FIELDS  Then, the rate of flow (mass per unit time) per unit area is  v.  If we divide S into small patches S ij, as in Figure 10 (compare with Figure 1), then S ij is nearly planar.

55. P5513.7 SURFACE INTEGRALS OF VECTOR FIELDS  So, we can approximate the mass of fluid crossing S ij in the direction of the normal n per unit time by the quantity (  v · n)A(S ij )  where , v, and n are evaluated at some point on S ij. Recall that the component of the vector  v in the direction of the unit vector n is  v · n.

56. P5613.7 VECTOR FIELDS  Summing these quantities and taking the limit, we get, according to Definition 1, the surface integral of the function  v · n over S: This is interpreted physically as the rate of flow through S.

57. P5713.7 VECTOR FIELDS  If we write F =  v, then F is also a vector field on.  Then, the integral in Equation 7 becomes:

58. P5813.7 FLUX INTEGRAL  A surface integral of this form occurs frequently in physics — even when F is not  v.  It is called the surface integral (or flux integral) of F over S.

59. P5913.7 Definition 8 If F is a continuous vector field defined on an oriented surface S with unit normal vector n, then the surface integral of F over S is This integral is also called the flux of F across S.

60. P6013.7 FLUX INTEGRAL  In words, Definition 8 says that: The surface integral of a vector field over S is equal to the surface integral of its normal component over S (as previously defined).

61. P6113.7 FLUX INTEGRAL  If S is given by a vector function r(u, v), then n is given by Equation 6. Then, from Definition 8 and Equation 2, we have: where D is the parameter domain.

62. P6213.7 FLUX INTEGRAL  Thus, we have:

63. P6313.7 Example 4  Find the flux of the vector field F(x, y, z) = z i + y j + x k across the unit sphere x 2 + y 2 + z 2 = 1

64. P6413.7 Example 4 SOLUTION  Using the parametric representation r( ,  ) = sin  cos  i + sin  sin  j + cos  k 0 ≤  ≤  0 ≤  ≤ 2  we have: F(r( ,  )) = cos  i + sin  sin  j + sin  cos  k

65. P6513.7 Example 4 SOLUTION  From Example 9 in Section 13.6, r  × r  = sin 2  cos  i + sin 2  sin  j + sin  cos  k  Therefore, F(r( ,  )) · (r  × r  ) = cos  sin 2  cos  + sin 3  sin 2  + sin 2  cos  cos 

66. P6613.7 Example 4 SOLUTION  Then, by Formula 9, the flux is:

67. P6713.7 Example 4 SOLUTION This is by the same calculation as in Example 1.

68. P6813.7 FLUX INTEGRALS  Figure 11 shows the vector field F in Example 4 at points on the unit sphere.

69. P6913.7 VECTOR FIELDS  If, for instance, the vector field in Example 4 is a velocity field describing the flow of a fluid with density 1, then the answer, 4  /3, represents: The rate of flow through the unit sphere in units of mass per unit time.

70. P7013.7 VECTOR FIELDS  In the case of a surface S given by a graph z = g(x, y), we can think of x and y as parameters and use Equation 3 to write:

71. P7113.7 VECTOR FIELDS  Thus, Formula 9 becomes: This formula assumes the upward orientation of S. For a downward orientation, we multiply by – 1.  Similar formulas can be worked out if S is given by y = h(x, z) or x = k(y, z). See Exercises 31 and 32.

72. P7213.7 Example 5  Evaluate where: F(x, y, z) = y i + x j + z k S is the boundary of the solid region E enclosed by the paraboloid z = 1 – x 2 – y 2 and the plane z = 0.

73. P7313.7 Example 5 SOLUTION  S consists of: A parabolic top surface S 1. A circular bottom surface S 2. See Figure 12.

74. P7413.7 Example 5 SOLUTION  Since S is a closed surface, we use the convention of positive (outward) orientation. This means that S 1 is oriented upward. So, we can use Equation 10 with D being the projection of S 1 on the xy-plane, namely, the disk x 2 + y 2 ≤ 1.

75. P7513.7 Example 5 SOLUTION  On S 1, P(x, y, z) = y Q(x, y, z) = x R(x, y, z) = z = 1 – x 2 – y 2  Also,

76. P7613.7 Example 5 SOLUTION  So, we have:

77. P7713.7 Example 5 SOLUTION

78. P7813.7 Example 5 SOLUTION  The disk S 2 is oriented downward.  So, its unit normal vector is n = – k and we have: since z = 0 on S 2.

79. P7913.7 Example 5 SOLUTION  Finally, we compute, by definition, as the sum of the surface integrals of F over the pieces S 1 and S 2 :

80. P8013.7 APPLICATIONS  Although we motivated the surface integral of a vector field using the example of fluid flow, this concept also arises in other physical situations.

81. P8113.7 ELECTRIC FLUX  For instance, if E is an electric field (Example 5 in Section 13.1), the surface integral is called the electric flux of E through the surface S.

82. P8213.7 GAUSS ’ S LAW  One of the important laws of electrostatics is Gauss ’ s Law, which says that the net charge enclosed by a closed surface S is: where  0 is a constant (called the permittivity of free space) that depends on the units used. In the SI system,  0 ≈ 8.8542 × 10 – 12 C 2 /N · m 2

83. P8313.7 GAUSS ’ S LAW  Thus, if the vector field F in Example 4 represents an electric field, we can conclude that the charge enclosed by S is: Q = 4  0 /3

84. P8413.7 HEAT FLOW  Another application occurs in the study of heat flow. Suppose the temperature at a point (x, y, z) in a body is u(x, y, z).  Then, the heat flow is defined as the vector field F = – K ∇ u where K is an experimentally determined constant called the conductivity of the substance.

85. P8513.7 HEAT FLOW  Then, the rate of heat flow across the surface S in the body is given by the surface integral

86. P8613.7 Example 6  The temperature u in a metal ball is proportional to the square of the distance from the center of the ball. Find the rate of heat flow across a sphere S of radius a with center at the center of the ball.

87. P8713.7 Example 6 SOLUTION  Taking the center of the ball to be at the origin, we have: u(x, y, z) = C(x 2 + y 2 + z 2 ) where C is the proportionality constant.  Then, the heat flow is F(x, y, z) = – K ∇ u = – KC(2x i + 2y j + 2z k) where K is the conductivity of the metal.

88. P8813.7 Example 6 SOLUTION  Instead of using the usual parametrization of the sphere as in Example 4, we observe that the outward unit normal to the spherex 2 + y 2 + z 2 = a 2 at the point (x, y, z) is: n = 1/a (x i + y j + z k)  Thus,

89. P8913.7 Example 6 SOLUTION  However, on S, we have: x 2 + y 2 + z 2 = a 2 Thus, F · n = – 2aKC

90. P9013.7 Example 6 SOLUTION  Thus, the rate of heat flow across S is: