Page 71 - Carbon Nanotubes
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60                                    R. SETTON
















                                                                                         b
                                                          Fig. 3.  The two possible orientations of the hexagons in non-
                                                          helical  sheets,  relative  to the  cylinder  axis  (broken  line);
                                                                   (a) case I; (b) case I1 (see text).


               Fig.  1. Approximate  cross  section  of  a tubule  with  scroll
               helicity. The distance d between successive rolls of the spiral   dius ri of the cylinder can conveniently be described
               is assumed to be constant, and no is the initial radius of the
                              innermost fold.             in  terms  of  two  orthogonal vectors[4],  Pi and  Qi
                                                          (Fig. 4), respectively integral multiples of the unit vec-
                                                          tors x and 7 with  moduli  I XI  = (3/2)G  and  I y I =
                                                          (&/2)G.  For the ith layer, we can write:
               drical sheets which, for simplicity, will be assumed to
               have a common axis and a circular cross-section. The
               hexagons of the unrolled cylinders all have one of their
               three sets of parallel opposite sides respectively per-   or, for the scalars Ri, Pi, Qi,
               pendicular (case I) or parallel (case 11) to the common
               axis of the cylinders (Fig. 3).
                 The orientation of the hexagons with respect to the
               tube axis of the unrolled ith cylinder as well as the ra-
                                                          where Pi, Qi are integers of  identical parity,  and

                                                                         Ri = 27rri.             (4)
                                                            The pitch angle ai characteristic of this orientation
                                                          of the hexagons is:
                                                                     ai = arctan(Qi/fiPi),       (5)

                                                          but one can also distinguish an apparent angle of pitch
                                                          pi between the helical rows  of  unbroken  hexagons
                                                          and the plane perpendicular to the cylinder axis, with



                                                            Although the limits of  LY  are:




                                                          this angle can be limited to 30", since every (Pi, Qi)
                                                          doublet  is associated  with a corresponding  doublet
                                                          (Pi,-Qi),  symmetric of  (Pi,Qi) with respect to a =
                                                          O",  yielding the same value of the radius (Fig. 5) and
                                                          characterizing the stereoisomer of the chiral ith cylin-
               Fig. 2.  A portion of an unrolled cylinder with screw helicity.   drical sheet, The doublet (Pi,Qi) is also equivalent to
               The broken line is parallel to the cylinder axis, and the cylin-   the doublet (Pi, Qj), with Pi = (P, + Q,)/2 and Qi  =
               drical sheet has been cut along a generatrix (full line paral-
               lel to the cylinder axis). a and b are the unit vectors of the   (3P, - 2Qi)/2, with the pitch  angle ai = 60" - ai.
                  two-dimensional  carbon layer in sp2 hybridization.   which also yields the same value of ri.
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