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Complex Analysis and Differential Geometry




                    Notes          Since the curves e(0, t) and e(t, L) are related via a rigid motion, i.e., e(t, L) = Re(0, t) where R is
                                   rotation by , it follows that  (t)   (t,L)  (0,L)  (0,t)  (0,0)   is a constant. Since clearly
                                                                            
                                   (0) 0,  we get (0, L) – (0, 0) = (L,L) – (0,L), and we conclude:
                                       

                                                   (L,L)   (0,0)    (t,L)    (0,L)   (0,t)     (0,0)    2 .
                                                                                              
                                                                                                n
                                   Definition 8. A piecewise smooth curve is a continuous function  :[a,b]     such that there is
                                   a partition of [a, b]:
                                                               a = a  < a  < · · · < b  = b
                                                                               n
                                                                      1
                                                                   0
                                   such that for each 1  j  n the curve segment       a   j 1  ,a   is smooth. The points  (a )  j   are
                                                                                   j 
                                                                          j
                                                                                
                                   called the corners of . The directed angle        from  '(a ) to '(a )  is called the exterior
                                                                                         
                                                                                             
                                                                                 
                                                                                     
                                                                                            j
                                                                                    j
                                                                         j
                                   angle at the j-th corner. Define  j  :[a j 1 ,a ]  as in Proposition 2, i.e., so that  '    cos ,sin j     j  .
                                                                  j
                                                                                                  j
                                                               
                                   The rotation number of  is given by:
                                                              1  n               1  n
                                                          n     2     (a )   (a   j 1 )    2    . j
                                                                    j
                                                                          j
                                                                      j
                                                                                     j 1
                                                                  j 1
                                   Again, n  is an integer, and we have:
                                         
                                                                               n
                                                               n      2 1   [a,b] k ds   2 1    . j
                                                                     
                                                                                j 1
                                   The Rotation Theorem can  be generalized to piecewise smooth curves  provided corners are
                                   taken into account.
                                                          2
                                   Theorem 6. Let  :[0,L]     be a piecewise smooth, regular, simple, closed curve, and assume
                                   that none of the exterior angles are equal to . Then  n   1.
                                                                              
                                   20.3.3 Convexity
                                                          2
                                   Definition 9. Let  :[0,L]     be a regular closed plane curve. We say that  is convex if for each
                                   t   [0, L] the curve lies on one side only of its tangent at t , i.e., if one of the following inequality
                                                                                0
                                   0
                                   holds:
                                                                     (t0)  e  2   0,

                                                                     (t0)  e  2   0,

                                                         2
                                   Theorem 7. Let  :[0,L]     be a regular simple closed plane curve, and let k be its curvature.
                                   Then  is convex if and only if either k  0 or k  0.
                                   We note that an orientation reversing reparametrization of  changes k  0 into k  0 and vice
                                   versa. Thus, ignoring orientation, those two conditions are equivalent. We also note that the
                                   theorem fails if  is not assumed simple.






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