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          184                      CAM DESIGN HANDBOOK


                                                2
                                           2
                                          r + 2 r¢ -  rr¢¢
                                       l¢
                                 k = sgn ()
                                                 2
                                           ( r +  r¢ ) 32
                                             2
          where the argument q has been dropped for compactness.
          7.3 GLOBAL PROPERTIES OF THE CAM PROFILE
          The global properties of a planar contour are its area, the position vector of its centroid,
          and its moments and products of inertia about a certain point, e.g., its centroid. Likewise,
          the global geometric properties of a closed region of the 3-D space are its volume, the
          position vector of its centroid, and its 3 ¥ 3 inertia matrix about a certain point such as its
          centroid. Below we recall the formal definitions of these items.


          7.3.1 Planar Contours
          Let  R denote  the  region  bounded  by  a  closed  contour  C in  the  x-y plane,  and  p the
          position vector of a point P of R in a frame F (O, x, y, z). Moreover, its area is denoted
          by A, its first moment by vector q, and its inertia matrix about the given origin O by I O.
          Thus,

                                   A =  dA                             (7.23a)
                                      Ú R
                                   q =  pdA
                                      Ú R                              (7.23b)
                                   I = (  p 1 pp )dA
                                           2
                                             -
                                                T
                                    0 Ú R                              (7.23c)
                                                 2
          where dA = dx dy, 1 is the 2 ¥ 2 identity matrix, ||p|| denotes the square of the magnitude
          of p, that is,
                                         2
                                       p = x 2  + y 2
                T
          and pp is the 2 ¥ 2 matrix external product recalled below:
                                      x È ˘     x È  2  xy ˘
                                   T
                                 pp =  Í ˙  x [  y] =  Í  ˙ .
                                                    2
                                      y Î ˚    Î xy  y ˚
             Moreover, from the mean-value theorem of integral calculus [1], a vector c exists such
          that
                                         q = Ac.
             Vector c thus defines the position of the centroid C of R. Henceforth, the two com-
                                                      T
          ponents of c in F are denoted by c 1 and c 2, i.e., c = [c 1, c 2] .
             The moment of inertia of R about C is then defined as
                              I ∫ [  pc 1 -( pc pc) ]  dA.
                                                     T
                                        2
                                                  -
                                             - )(
                                     -
                              C Ú
                                  R
             Moreover, I C reduces to
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