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Unit 18: Theory of Space Curves




          We have, however, the following lemma:                                                Notes

          Lemma 2. There exists a continuous function  (s)    such that  (s)     (s) mod 2.
          Proof. We suppose  C  to  be a  closed curve  of  total length  L.  The continuous  mapping  g  is
          uniformly continuous. There exists therefore a number  > 0 such that for |s  – s | < , T(s ) and
                                                                          2
                                                                                  1
                                                                       1
          T(s ) lie in the same open half-plane. Let s (= O) < s  < · · · < s (= L) satisfy |s  – s | <  for i = 1,
             2
                                                                          i–1
                                           0
                                                   1
                                                                       i
                                                           i
          . . ., m. We put  (s )   0   = (s ). For s   s  s , we define  (s)    to be  (s )   0  plus the angle of rotation
                                           1
                               0
                                     0
          from g(s ) to  g(s) remaining in the same half-plane. Carrying out this process in successive
                 0
          intervals, we  define a  continuous function  (s)     satisfying the  condition in the lemma. The
                    
          difference  (L)    (O)  is an integral multiple of 2. Thus,  (L)    (O)  = 2. We assert that the
                                                          
          integer  is independent of the choice of the function  .   In fact let  '(s)    be a function satisfying
          the same conditions. Then we have  '(s)    –  (s)    = n(s)2p where n(s) is an integer. Since n(s) is
          continuous in s, it must be constant. It follows that  '(L)– (O)        t(L)    (O),  which proves the
          independence of  from the choice of  .   We call  the rotation index of C. In performing integration
          over C we should replace t(s) by     in (8). Then we have
                                     1         1       .
                                                   
                                     2     k ds   2    d                ...(10)
          We consider the mapping h which sends an ordered pair of points x(s ), x(s ), O  s   s   L, of C
                                                                      2
                                                                 1
                                                                               2
                                                                            1
          into the end-point of the unit vector through O parallel to the secant joining x(s ) to x(s ). These
                                                                                2
                                                                          1
          ordered pairs of points can be represented as a triangle  in the (s , s )-plane defined by O  s 1
                                                                  2
                                                               1
           s   L. The mapping h of  into  is continuous. Moreover, its restriction to the side s  = s  is the
            2
                                                                              1
                                                                                 2
          tangential mapping g in (9).
          To a point p   let (p) be the angle of inclination of  Oh(p)  to the x -axis, satisfying O  (p) <
                                                                 1
          2. Again this function need not be continuous. We shall, however, prove that there exists a
                                   ,
                                                          
                            
          continuous function  (p),p  such that  (p)     (p) mod 2 .  In fact, let m be an interior point
          of . We cover  by the radii through m. By the argument used in the proof of the above lemma
                                      ,
          we can define a function  (p),p  such that  (p)   (p)  mod 2, and such that it is continuous
                                                
                               
          on every radius through m. It remains to prove that it is continuous in .
          For this purpose let p   4. Since h is continuous, it follows from the compactness of the segment
                           0
          mp  that there exists a number  = (p ) > 0, such that for  q  mp  and for any point q   for
                                                          0
                                                               0
             0
                                          0
          which the distance d(q, q ) <  the points h(q) and h(q0) are never antipodal. The latter condition
                              0
          can be analytically expressed by
                                                     
                                       (q)    (q )  mod .                    ...(11)
                                             0
                             
          Now let R / > 0, R / <    be given. We choose a neighborhood U of p  such that U is contained
                             2                                    0
          in the -neighborhood of p  and such that, for p  U, the angle between  Oh(p ) and Oh(p)  is
                                                                          0
                                0
          < R. This is possible, because the mapping h is continuous. The last condition can be expressed in
          the form
                                     (p) – t(p ) = R' + 2k(p) ,                ...(12)
                                         
                                           0
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