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              Macromolecules, Structure                                                                   877

                                                                                      2
              initiated polymer (b) is almost exclusively a pair of dou-     [mm] = P ,
                                                                                     m
              blets;  quantitative  assessment  shows  that  this  polymer
              is  95%  isotactic.  The  methylene  spectrum  of  the  free    [mr] = 2P m (1 − P m ),
              radical  polymer  (a)  is  more  complex,  but  the  principal               2
                                                                               [rr] = (1 − P m ) .
              resonance—at 1.9 ppm—is a singlet, showing that this
              polymer is predominantly syndiotactic but more irregular
              than (b). This is generally the case for free radically initi-  The heterotactic sequence must be given double weight-
              ated vinyl polymers. (The other resonances are discussed  ing because both directions, mr and rm—observationally
              later in this section.)                           indistinguishable—must be counted. A plot of these re-
                We see that proton NMR can provide absolute stereo-  lationships  is  shown  in  Fig.  20.  Note  that  the  propor-
              chemical information concerning polymer chains without  tion of mr (heterotactic) units rises to a maximum when
              recourse to X-ray or other methods. Somewhat more de-  P m  is 0.5, corresponding to a strictly random or atactic
              tailed,butnotabsolute,informationcanbegainedfromthe  configuration  for  which  [mm]:[mr]:[rr]  will  be  1:2:1.
              methyl proton resonances near 1.2 ppm. [The ester methyl  For any polymer, if Bernoullian, the [mm], [mr], and [rr]
              resonance at ∼3.6 ppm (not shown) is less sensitive to  sequence intensities will lie on a single vertical line in
              stereochemistry.] In both spectra we note three peaks—  Fig.  20,  corresponding  to  a  single  value  of  P m .  Spec-
              or, more correctly, groups of peaks—appearing in similar  trum  (a)  in  Fig.  19  corresponds  to  these  simple  statis-
              positions but with greatly different intensities. These cor-  tics, P m being 0.25 ± 0.01; the polymer corresponding to
              respond to the α-methyl groups in the center monomer  spectrum (b) does not. The propagation statistics in this
              unit of the three possible triad sequences:isotactic, syn-  case can be interpreted to indicate that the probability of
              diotactic, and heterotactic. These may be more simply and  isotactic placement is dependent on the stereochemical
              appropriately designated by the m and r terminology, as  configuration of the growing chain and cannot properly
              indicated. Measurement of the relative intensities of the  be expressed by a single parameter such as P m . Free-
              mm, mr, and rr α-methyl peaks, which appear from left  radical and cationic propagations always give predomi-
              to right in both spectra in this order, gives a valid statistical  nantly syndiotactic chains. Anionic initiators may also do
              representation of the structure of each polymer.

              O   OCH 3 O  OCH 3  O  OCH 3  O  OCH 3  O  OCH 3
                C  H   C  H   C         C  H   CH  H  C

                   H      H                H   C  H
                CH 3   CH 3   CH 3      CH 3          CH 3
                     ISOTACTIC, mm           O   OCH 3
                                          SYNDIOTACTIC, rr
                         O   OCH 3 O  OCH 3
                           C   H  C   H  CH 3
                               H      H
                           CH 3   CH 3   C
                                        O  OCH 3
                            HETEROTACTIC, mr [or rm]

                From the triad data we may gain considerable insight
              into  the  mechanism  of  propagation.  This  is  one  of  the
              principal uses of such information. Let us designate by P m
              the probability that the polymer chain will add a monomer
              unit to give the same configuration as that of the last unit
              at its growing end (i.e., that an m dyad will be generated).
              We assume that P m  is independent of the stereochemical
                                                                FIGURE 20 The probabilities of isotactic [mm], heterotactic [mr],
              configuration of the growing chain. The generation of the  and syndiotactic [rr] triads as a function of P m , the probability
              chain is a Bernoulli trial process; it is like reaching into  of m placement. The points on the left-hand side are for methyl
              a large jar of balls marked m  and r  and withdrawing a  methacrylate polymers prepared with free-radical initiators and
              ball at random. The proportion of m balls in the jar is P m .  those on the right-hand side are for polymers prepared with an-
                                                                ionic initiators. For polymer (a) the points for [rr] have been arbi-
              Since two monomer additions are required to form a triad
                                                                trarily placed on the [rr] curve and the others fall where they may
              sequence, it is readily evident that the probabilities of their  and for polymer (b) the [mm] points have been placed on the [mm]
              formation are                                     curve.
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