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11.5 Divergence and Curl   365


                                        11.5.2  A Physical Interpretation of Curl
                                        The curl vector is interpreted as a measure of rotation or swirl about a point. In British literature,
                                        the curl is often called the rot (for rotation) of a vector field.
                                           To understand this interpretation, suppose an object rotates with uniform angular speed ω
                                        about a line L, as in Figure 11.11. The angular velocity vector   has magnitude ω and is directed
                                        along L as a right-handed screw would progress if given the same sense of rotation as the object.
                                        Put L through the origin and let R = xi + yj + zk for any point (x, y, z) on the rotating object.
                                        Let T(x, y, z) be the tangential linear velocity and R =  R  . Then

                                                                    T  = ωR sin(θ) =    × R  ,

                                        with θ the angle between R and  . Since T and   × R have the same direction and magnitude,
                                        we conclude that T =   × R. Now write   = ai + bj + ck to obtain

                                                         T =   × R = (bz − cy)i + (cx − az)j + (ay − bx)k.

                                        Then


                                                                         i       j       k

                                                              ∇× T =     ∂/∂z   ∂/∂y    ∂/∂z

                                                                        bz − cy  cx − az  ay − bx
                                                                    = 2ai + 2bj + 2ck = 2 .

                                        Therefore,

                                                                             1
                                                                           = ∇× T.
                                                                             2

                                        The angular momentum of a uniformly rotating body is a constant times the curl of the linear
                                        velocity.



                                                                          (x, y, z)
                                                                                    T
                                                                                         Ω



                                                                                        R sin(θ)
                                                                       R
                                                                        θ




                                                                   (0, 0, 0)
                                                              L
                                                              FIGURE 11.11 Interpretation of curl.





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                                   October 15, 2010  16:11  THM/NEIL   Page-365        27410_11_ch11_p343-366
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