+ 13.5 Curl and Divergence Copyright © Cengage Learning. All rights reserved. : closed surface 13.5 Curl and Divergence Copyright © Cengage Learning. All rights reserved. Vector Forms of Green’s Theorem Its line integral is and, regarding F as a vector field on ¡ 3 with third component 0, we have F = P i + Q j + 0 k. 3 Vector Forms of Green’s Theorem Then, from equation 16.3 (3) we have F = P i + Q j + 0 k. N M 4 The Divergence Theorem We write Green’s Theorem in a vector version as where C is the positively oriented boundary curve of the plane region D. If we were seeking to extend this theorem to vector fields on we might make the guess that where S is the boundary surface of the solid region E. It turns out that Equation 1 is true, under appropriate hypotheses, and is called the Divergence Theorem. 5 13.9 The Divergence Theorem Copyright © Cengage Learning. All rights reserved. The Divergence Theorem The boundary of E is a closed surface, and we use the convention(?), that the positive orientation is outward; that is, the unit normal vector n is directed outward from E. Thus the Divergence Theorem states that, under the given conditions, the flux of F across the boundary surface of E is equal to the triple integral of the divergence of F over E. 8 Example 4 (in 13.7) Find the flux of the vector field F(x, y, z) = z i + y j + x k over the unit sphere x 2 + y 2 + z 2 =1. Solution: We use the parametric representation 9 Example 1(We use the Divergence Theorem) Find the flux of the vector field F(x, y, z) = z i + y j + x k over the unit sphere x 2 + y 2 + z 2 =1. Solution: First we compute the divergence of F: The unit sphere S is the boundary of the unit ball B given by 10 Example 2 Solution: 11 Example 2 Solution: 12 The Divergence Theorem Let’s consider the region E that lies between the closed surfaces S1 and S2, where S1 lies inside S2. Let n1 and n2 be outward normals of S1 and S2. Then the boundary surface of E is S = S1 ∪ S2 and its normal n is given by n = −n1 on S1 and n = n2 on S2. (See Figure 3.) Applying the Divergence Theorem to S, we get Figure 3 13 #2 with upward orientation. Solution: ( ) (-) with downward orientation. D 14 # 37 Solution: ? = 20 15 Final exam 18 Type I =y =y Solution: Type II Solution: The region R can be described as R = {(x, y) | x, y 0, 1 x 2 + y 2 4} It is the half-ring shown in Fig., and in polar coordinates it is given by 1 r 2, 0 /4. Type_1 위 아래 Figure 9 Type 1; 위/아래 #. Evaluate the integral by changing to spherical coordinates. #. 25. Solution: R #. Solution: Example 3 Solution: Using Equation 2, we have f (1,1,2) - f (0,0,0) = 8 36 Recall (Green’s Theorem) C:+ 37 Example 1 Solution: n = <0, 1, 1> / 2 curl F ≠ 0 :+ choice! r (x, y) = < x, y, g(x, y) > = < x, y, 2 - y > Figure 3 rx × ry = = < 0, 1, 1 > 38 Example 1 Solution: curl F ≠ 0 :+ choice! Figure 3 39 ① Example 2 (의도/의미?) Solution: 뿔룩한 곡면 : + : counterclockwise (+ orientation) ② Note that in Example 2 we computed a surface integral simply by knowing the values of F on the boundary curve C. This means that if we have another oriented surface with the same boundary 40 curve C, then we get exactly the same value for the surface integral! ② Example 2 (의도/의미?) Solution: : + : counterclockwise (+ orientation) n = < 0, 0, 1> 41 Example 3 : counterclockwise (+ orientation) Solution: n(=k)= < 0, 0, 1> -n :+ < 0, 0, -1> (-1) 42 Recall (Surface Integrals, Flux) ③ + 43 13.7. #31 44