310 0 CHAPTER 16 VECTOR CALCULUS 51. The work done in moving the object is fc F · dr = fc F · T ds. We can approximate this integral by dividing C. into 7 segments of equal length t:.s = 2 and approximating F · T , that is, the tangential component of force, at a point (xi , yi) on each segment. Since C is compos<strong>ed</strong> of straight line segments, F · T is the scalar projection of each force vector onto C. If we choose (xi, yi) to be the point on the segment closest to the origin, then the work done is . 7 fc F · T d.s ~ E (F(xi, yi) · T(xi, yi)] t:.s = (2 + 2 + 2 + 2+ 1 + 1 + 1)(2) = 22. Thus, we estimate the work done to i=l . be approximately 22 J. 16.3 The Fundamental Theorem for Line Integrals 1. C appears to be a smooth curve, and since \J f is continuous, we know f is differentiable. Then Theorem 2 says that the value of fc \J f · dr is simply the difference of the values off at the terminal and initial points of C. From the graph, this is 50- 10 = 40. 3. 8(2x- 3y)j8y = - 3 = 8( -3x + 4y- 8)j8x and the domain ofF is IR 2 which is open and simply-connect<strong>ed</strong>, so by Theorem 6 F is conservative. Thus, there exists a function f such that \J f = F , that is, f:r:(x, y) = 2x - 3y and f 11 (x, y) = -3x + 4y - 8. But f,.(x, y) = 2x - 3y implies f(x, y) = x 2 - 3xy + g(y) and differentiating both sides of this equation with respect to y gives f 11 ( x, y) = - 3x + g' (y). Thus - 3x + 4y - 8 = -3:~.: + g' (y) so g' (y ) = 4y - 8 and g(y) = 2y 2 - By+ [(where I< is a constant. Hence f(x, y) = x 2 - 3xy + 2y 2 - 8y +I< is a potential function for F . 5. 8(e"' cosy)j8y := - e"' sin y, 8(e"' siny)f8x = e" sin y. Since these are not equal, F is not conservative. 7. o(ye"' + sin y)j8y =ex+ cosy= o(e"' + X cosy)f8x and the domain ofF is IR 2 • Hence F is conservative so there exists a function f such that \J f =F. Then fx (x, y) = ye" +sin y implies f(x, y) = ye" + x sin y + g(y) and fv(x, y) = e"' + xcos y + g'(y). But f 11 (x, y) = e"' + x cosy so g(y) = K and f(x, y) = ye" + xsin y + K is a potential function for F. 9. 8(lny + 2xy 3 )j8y = 1/y + 6xy 2 = 8(3x 2 y 2 + xfy)j8x and the domain ofF is {(x, y) I y> 0} which is open and simply connect<strong>ed</strong>. Hence F is conservative so there exists a function f such that \J f = F . Then f:z:(x, y) =In y + 2xy 3 implies f(x,y) = xlny + x 2 y 3 + g(y) and ! 11 (x,y) = xfy + 3x 2 y 2 + g'(y). But f 11 (x,y) = 3x 2 y 2 + xjy so g'(y) = 0 =} g(y) = [(and f(x, y) = xlny + x 2 y 3 + [(is a potential function for F . 11. (a) F has continuous first-order partial derivatives and 8 8 2xy = 2x = 8 8 (x 2 ) on JR 2 , which is open and simply-connect<strong>ed</strong>. y X . Thus, F is conservative by Theorem 6. Then we know that the line integral ofF is independent of path; in particular, the value of fc F · dr depends only on the endpoints of C. Sin.ce all three curves have the same initial and terminal points, J~ F · dr will have the same value for each curve. ® 2012 Cengagc Lc:uning. All Rights Reserv<strong>ed</strong>. Mny not be scann<strong>ed</strong>, copi<strong>ed</strong>. or duplicatcdt or post<strong>ed</strong> to a publicly occcssiblc ~vcbs i tc, jo whole or in pan.
SECTION 16.3 THE FUNDAMENTAL THEOREM FOR LINE INTEGRALS 0 311 (b) We first find a potential function f, so that \l f = F. We know ! :r:(x, y) = 2xy and jy(x, y) = x 2 • Integrating fx(x, y) with respect to x, we have f(x, y) = x 2 y + g(y). Differentiating both sides with respect toy gives · J 11 (x, y) = x 2 + g'(y), so we must have x 2 + g'(y) = x 2 =? g'(y) = 0 => g(y) = K, a constant. Thus f(x, y) = x 2 y + K. All three curves start at (1, 2) and end at (3, 2), so by Theorem 2, fe F · dr = !(3, 2) - !(1, 2) = 18 - 2 = 16 for each curve. 13. (a) f r(x, y) = xy 2 implies J(x, y) = ~x 2 y 2 + g(y) and fy (x, y) = x 2 y + g'(y). But /y(x, y) = x 2 y so g'(y) = 0 => g(y) = K, a constant. We can take K = 0, so f(x, y) = ~x 2 y 2 . (b) The initial point of C is r (O) = (0, 1) and the terminal point is r(1) = (2, _1), so fe F · dr = /(2, 1) - f(O, 1) = 2 - 0 = 2. 15. (a) f x(x, y, z ) = yz implies f(x, y, z) = xyz + g(y, z) and so jy(x, y , z) = xz + g 11 (y, z). But jy(x, y, z) = xz so gy(y, z ) = 0 => g(y, z) = h(z). Thus f(x, y, z) = xyz + h(z) and f:(x, y, z) = X'!f + h'(z). But f:(x, y, z) = xy + 2z, so h'(z) = 2z => h(z) = z 2 + K.. Hence f(x, y, z) = xyz + z 2 (taking J( = 0). (b) fe F · dr = !(4,6,3)-!(1, 0, - 2) = 81 - 4 = 77. 17. (a) f:r:(x, y, z) = yze"'= implies f(x, y, z) = ye"'= + g(y, z) and so fv(x, y, z) = e"'= + gy(y, z). But jy(x, y, z ) = e"'= so. gy{y,z) = 0 =? g(y,z) = h(z). Thus f(x,y,z)·= ye"'= + h(z) and fz(x, y,z) = xyex= + h'(z). But f:.:(x,y,z) = xyex=, so h'(z) = 0 =? h(z) = K. Hence f(x,y,z) = ye"'= (taking!(= 0). (b) r (O) = (1, -1, 0), r(2) = (5, 3, 0) so fe F · dr = /(5, 3, 0) - /(1, - 1, 0) = 3e 0 + e 0 = 4. 19. The functions 2xe-Y and 2y - x 2 e- v have continuous first-order derivatives on JR 2 and ~ (2xe-v) = -2xe- Y = ~ (2y- x 2 e:-v), so F(x, y) = 2xe-Y i + (2y- x 2 e-Y) j is a conservative vector field by Ulj vx . . Theor~m 6 and hence the line integral is independent of path. Thus a potential function f exists, and fx(x, y) = 2xe-v implies f(x, y) = x 2 e- 11 + g(y) and fv(x, y) = - x 2 e-Y + g'(y). But fv(x, y) = 2y- x 2 e-v so g'(y) = 2y =? g(y) = y 2 + K. We can take K = 0, so f(x,y) = x 2 e- 11 + y 2 • Then .fe 2xe-v dx + (2y - x 2 e- v) dy = /(2, 1) - f(l, 0) = 4e- 1 + 1 - 1 = 4/e. 21. IfF is conservative, then fe F · dr is independent of path. This means that the work done along all piecewise-smooth curves that have the describ<strong>ed</strong> initial and terminal points is the same. Your reply: It doesn't matter which curve is chosen. 23. F (x, y) = 2y 3 1 2 i + 3x Jyj, W = .fe F · dr. Since 8(2y 3 1 2 )/8y = 3 y'Y = 8(3x Jy )/ ax, there exists a function f suchthat\lf=F.Infact,fx(x, y)='2y 3 1 2 => f(x,y)=2xy 312 +g(y) => fv(x,y)=3xy 1 1 2 +g'(y). But /y (x, y) = 3x y'Y so g'(y) = 0 or g(y) = K. We can take I< = 0 =? f(x, y) = 2xy 3 1 2 • Thus W = fe F · dr = j(2, 4) :.... j(I,·l) = 2(2)(8)- 2(1) .= 30. © 2012 Ccngogc Leoming. All Rights Resen'Od. May nol b< scann<strong>ed</strong>, copi<strong>ed</strong>. orduplicalcd. or posl
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.. BROOKS/COLE ~ I ~~r CENGAGE Lear
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D ABBREVIATIONS AND SYMBOLS CD cu D
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viii o CONTENTS 12.4 The Cross Prod
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