Page 400 - Advanced engineering mathematics
P. 400

380    CHAPTER 12  Vector Integral Calculus


                        SECTION 12.3        PROBLEMS



                     In each of Problems 1 through 5, evaluate  F · dR over  −y             x
                                                     C              3. F =       + x  2  i +    − 2y j
                     anysimpleclosedpathinthe x, y-plane that does not     x + y  2       x + y  2
                                                                                           2
                                                                            2
                     pass through the origin. This may require cases, as in     −y          x
                     Example 12.10.                                 4. F =       + 3x i +       − y j
                                                                           x + y  2       x + y  2
                                                                                           2
                                                                            2
                             x        y
                      1. F =     i +     j                                    x                y
                                     2
                           x + y  2  x + y  2                                                      − 3y 2  j
                            2
                                                                    5. F =        + 2x i +
                                                                                              2
                                                                              2
                                    3/2                                      x + y 2         x + y 2

                               1
                      2. F =         (xi + yj)
                             x + y  2
                             2
                     12.4        Independence of Path and Potential Theory
                                   A vector field F is conservative if it is derivable from a potential function. This means that
                                   for some scalar field ϕ,
                                                                   ∂ϕ    ∂ϕ    ∂ϕ
                                                           F =∇ϕ =    i +   j +  k.
                                                                    ∂x   ∂y    ∂z
                                   We call ϕ a potential function,or potential,for F. Of course, if ϕ is a potential, so is ϕ + c
                                   for any constant c.


                                     One consequence of F being conservative is that the value of  F · dR depends only on
                                                                                        C
                                 the endpoints of C.If C has differentiable coordinate functions x = x(t), y = y(t), z = z(t) for
                                 a ≤ t ≤ b, then

                                                              ∂ϕ     ∂ϕ     ∂ϕ
                                                    F · dR =    dx +   dy +    dy
                                                   C        C ∂x     ∂y     ∂z
                                                             b

                                                                ∂ϕ dx  ∂ϕ dy   ∂ϕ dz
                                                         =           +       +        dt
                                                                ∂x dt   ∂y dt  ∂z dt
                                                            a
                                                               d
                                                              b
                                                         =      ϕ(x(t), y(t), z(t))dt
                                                            a dt
                                                         = ϕ(x(b), y(b), z(b)) − ϕ(x(a), y(a), z(a))
                                 which requires only that we evaluate the potential function for F at the endpoints of C.Thisis
                                 the line integral version of the fundamental theorem of calculus, and applies to line integrals of
                                 conservative vector fields.


                           THEOREM 12.2

                                 Let F be conservative in a region D (of the plane or of 3-space). Let C be a path from P 0 to P 1 in
                                 D. Then

                                                              F · dR = ϕ(P 1 ) − ϕ(P 0 ).               (12.4)
                                                             C



                      Copyright 2010 Cengage Learning. All Rights Reserved. May not be copied, scanned, or duplicated, in whole or in part. Due to electronic rights, some third party content may be suppressed from the eBook and/or eChapter(s).
                      Editorial review has deemed that any suppressed content does not materially affect the overall learning experience. Cengage Learning reserves the right to remove additional content at any time if subsequent rights restrictions require it.

                                   October 14, 2010  14:53  THM/NEIL   Page-380        27410_12_ch12_p367-424
   395   396   397   398   399   400   401   402   403   404   405