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 Encyclopedia of Physical Science and Technology  EN008C-602  July 25, 2001  20:31






               892                                                                              Macromolecules, Structure


               TABLE  V  Characteristic  Ratios  C ∞  for  Selected  Polymer  TABLE VI Calculated and Experimental Values of the Char-
                                                                                    2
                                                                                        2
               Chains                                            acteristic Ratio C ∞ =  r   /nl (300 K) and Its Temperature
                                                                                     0
                                                                 Coefficient for the Polymethylene Chain
                                                        2
                   Polymer          Conditions    C ∞ =  r   /nl  2
                                                         0
                                                                                                     Temperature
               Polymethylene    Decanol-1, 138 C       6.7                             Characteristic  coefficient
                                          ◦
               Polyoxymethylene                      ∼10.0               Model           ratio C ∞  dC ∞ /dT × 10 3
               Polyoxyethylene  Aqueous K 2 SO 4 , 35 C  4.0
                                             ◦
                                                                 Experimental              6.7        −1.1 ± 0.1
               Polytetramethylene                     ∼2.0                                            (390–420 K)
                 oxide
                                                                 (a) Freely rotating       2.1           0
               Polypropylene    Diphenyl ether
                                                                 (b) 3-State RIS, E g = 500 cal  3.4
                                    ◦
                 Isotactic        145 C                4.7
                                                                    E g + g − = 0 (independent
                 Atactic          153 C                (5.3)        rotations)
                                    ◦
               Polystyrene      Diphenyl ether                   (c) 3-State RIS, E g = 500 cal  6.7    −1.0
                 Atactic          Cyclohexane, 35 C   10.2          E g + g − = 2200 cal
                                            ◦
               Poly(methyl                                       (d) 3-State RIS, E g = 800 cal  8.3    −1.5
                 methacrylate)                                      E g + g − = 2200 cal
                 Atactic          Various solvents     6.9       (e) 3-State RIS, E g = 500 cal  7.1    −0.7
                 Isotactic        Acetonitrile, 28 C   9.3          E g + g − = 3500 cal
                                            ◦
               Polydimethylsiloxane  Butanone          6.2
                                                                 formed. With respect to synthetic polymers, there is some
               The length, l, is usually 0.15 nm and M can be obtained  UV evidence that isotactic polystyrene partially retains
               from  any  of  the  usual  molecular  weight  measurements  a helical conformation in solution. This is confirmed by
               (see Section II.B). Thus, the characteristic ratio can be  infrared measurements.
               determineddirectlyfromintrinsicviscositymeasurements  Infrared spectroscopy (IR) (Section III.A) is used pri-
               under θ conditions. Table V lists characteristic ratios for  marily for characterizing polymer conformations in bulk
               selected polymers.                                samples and will be discussed in this regard in the fol-
                 The RIS model can be used to calculate characteristic  lowing section. However, it can also be used to study
               ratios, and these calculations can be compared with ex-  solution state conformations, since the skeletal vibra-
               perimentally derived values. Such comparisons are useful  tion frequencies are conformationally sensitive. Bands
               for testing various assumptions used in RIS calculations.  can be identified that are signatures for the tt, tg, and
               Table VI shows such a comparison for a polymethylene  longer sequences. Using these conformationally sensitive
               chain. The experimental value for C ∞  is 6.7. Table VI  IR bands, researchers have observed helical sequences in
               lists C ∞  calculated for (a) a freely rotating chain; (b) a  isotactic polystyrene and have also shown the absence
               chain with a reasonable gauche energy of 500 cal but with  of cooperative helix-coil transitions in this material. IR
               independent rotational states for the neighboring bonds;  spectroscopy is also very useful for studying hydrogen
               and (c), (d), and (e) neighbor-dependent three-state model  bonding interactions bond in biopolymers and in synthetic
               with different values for the energy of the gauche and of  polymers.
                               −                                   Raman spectroscopy (Section III.A) provides informa-
               the gauche –gauche conformations. Table VI shows that
                        +
               entry (c) comes closest to matching the experimental val-  tion that is complementary to that obtained from IR mea-
               ues. [The energies used in (c) were deduced from studies  surements. We have already seen that to be IR active, a
               on small paraffins.]                               vibrational mode must undergo a change in dipole mo-
                                                                 ment. Thus, OH, NH, and CH bonds are examples
                                                                 of IR-active groups. In fact, the OH infrared bands are
                 2.  Spectroscopic Determination of
                    Chain Conformation in Solution               so strong that they often make difficult the use of wa-
                                                                 ter as a solvent for some IR studies. In contrast, a sym-
               Many spectroscopic techniques are useful for observing  metrical bond, for example a carbon–carbon bond C C,
               polymer  chain  conformations.  Ultraviolet  spectroscopy  has an IR-inactive stretching vibration. However, the C C
               (UV) is used almost exclusively for biopolymers to es-  stretching vibration gives a strong Raman band. Further-
               tablish the degree of helicity and to study other aspects  more, aqueous solvents can be used in Raman studies,
               of protein and nucleic acid tertiary structure. For ex-  making Raman spectroscopy an ideal method for studying
               ample, the UV spectra of nucleic acids and nucleotides  the conformations of biological macromolecules. Raman
               show hypochromic effects when helical conformations are  spectroscopy provides much new information concerning
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