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Rotational dyad state

From consideration of molecular models and the geometric requirements for excimer formation, we have concluded that the trans, trans meso rotational dyad is the predominant EPS in the aryl vinyl polymers. [5,22] The identification of the EPS trap with a particular rotational dyad state was a critical factor because it opened the way to utilize the powerful rotational isomeric state theory of Flory [23] to calculate the EPS population for the isolated PS chains. This trap population is relatively small in polystyrene. [Pg.23]

Flory, Marie, and Abe (194) carried out a statistical mechanics analysis of vinyl polymers on the basis of a three rotational state model. Energy maps have been calculated both for m and r dyads as a function of the rotation angles around the bonds astride the methylene groups (CHR—CH2—CHR). These maps differ from those examined for crystalline polymers where rotations around... [Pg.57]

The conformation of atactic polymers, with any value of the m/r ratio, must be treated as that of a copolymer, wherein the monomer unit statistics are compounded with those of the rotational states. In this case we may either refer to Monte-Carlo type procedures, as done by Floiy, Mark, and Abe (194), or to the pseudostereochemical equilibrium method used by Allegra (195) and Briick-ner (196). In the latter case the atactic polymer is formally considered as a homopolymer that may assume the conformations of either the m or r dyads, with suitable adjusted statistical weights. [Pg.58]

The conformational statistics of asymmetric vinyl chains such as P2VN are well-known 126). The rotational conformers of isotactic (meso) dyads are entirely different from those of syndiotactic (dl) dyads. Frank and Harrah132) have described each of the six distinct conformers for meso and dl dyads, using the t, g+ and g nomenclature of Flory 126). Excimer-forming sites (EFS) are found in the tt and g g+ meso states, and in the degenerate tg , g t dl state. Because the rotational conformers of compounds such as l,3-bis(2-naphthyl)propane do not match those of either the iso-or syndiotactic dyads of P2VN, the propane compounds make poor models of aryl vinyl polymers. However, the rate constants of fluorescence and decay of the intramolecular excimer in polymers can usually be determined from the propane compounds (but see the exceptional case of PVK and its models133)). [Pg.57]

Conformational energies of meso and racemic diads of PS are computed as functions of skeletal bond rotations. Confinement of rotations of the phenyl groups to a small range within which they are nearly perpendicular to the plane defined by the two adjoining skeletal bonds is confirmed. Steric interactions involving the relatively large planar phenyl group virtually preclude"g" conformations. A simple, two-state RIS scheme is applicable with states at 170° and 70° for both meso and racemic dyads. [Pg.174]

During last decades the domains C-2 symmetry (the dyad rotation symmetry) of low-B palindrome was established in many enzymes (chymotrypsin, trypsin, aspartyl proteinases, HIV-1 protease, carboxypeptidase A, phospholipase A-2 ribonuclease, etc.) (Lumry, 2002 and references therein). It is proposed that the pair domain closure causes constrain of pretransition state complex that activates cleavage or formation of chemical bonds. Thus control of strong bonds by the cooperation of many matrix or knots bonds takes place. As an example, in the active site of carboxypeptidase A the zinc ion is attached to one of the catalytic domains by histidine 69 and glutamine 72 and connected by hystidine 196 to the second domain. Similar structures were found in the chymotrypsin and pepsin active sites where protons are driven under compression of the domains closure. [Pg.71]

Electronic excitation of either the donor or acceptor of the dyad generates two sets of locally excited states. In principle, the population of the folded set of excited states may be increased but in practice, this likelihood becomes negligible for long chain lengths n > 6) since competing ET and decay processes occur more rapidly than the rate of production of a sandwich conformation from an extended one, which would require rotation about several C-C bonds to achieve. [Pg.1860]

The photophysics of the Pyr-B-An dyads 15( i) also displayed interesting solvent-dependent behavior. In the case of 15(1), photoinduced ET takes place readily in acetonitrile, to give the CS state, but it does not occur in nonpolar solvents— presumably because the driving force for formation of the CS is not very exergonic. Nevertheless, photoinduced ET is observed to take place for the three-atom chain dyad 15(3) in polar and nonpolar solvents. In acetonitrile, the extended CS state is formed, whereas the exciplex is formed in -hexane. In contrast to the shorter analogue 15(1), the ideal, face-to-face sandwich-like orientation between the chro-mophores is attainable in the exciplex formed from 15(3). Using the more viscous 2-propanol solvent allowed observation of the CS state, followed by slow formation of the exciplex. Apparently, the viscous solvent slows down the bond rotations that convert the CS state into the exciplex [51, 52]. [Pg.1861]

Here, we use the apostrophe mark / to indicate the state of the material body at a certain time t in the past. Let the material body be changed to the shape shown in the right of Fig. 5.4. Both the p and q points change their positions as a result of rotation and/or deformation of the material body. The vector dX between p and q is deformed to become dX. The change in dX with respect to dX is called the deformation gradient which is expressed by the dyad ( V X) (see Appendix 5.A), and is often represented... [Pg.83]

Here the probabilities in each matrix are normalised to make the highest probability unity in each. In the more general theory, the factor x is re-expressed in terms of the rotational constraints on individual bonds, and one typically needs five such variables for an acceptable description of an un-symmetrical vinyl polymer in which each bond has three rotational states. In the above case it may simply be defined as the relative probability of the gg state in the racemic dyad. [Pg.151]

The rotational states of the internal bond pair +1+1 > defined relative to their states when all backbone bonds are in the same plane. For the tt meso dyad, = 0 when there is... [Pg.565]

In a study of the conformational statistics of PS, Yoon, Sundararajan and Flory (YSF) included solvent effects in the analysis [47]. The influence of solvent on conformational energy is important because the distance between chemical groups separated by four bonds is large enough for solvent molecules to penetrate the space between them and provide additional interactions. These results are in complete agreement with the experimental studies of PS conformational structure. For example, YSF found the g rotational states to be insignificant due to severe steric interactions. In addition, the inclusion of solvent effects led to the conclusion that the tt conformation is not the ground state of the meso dyad. [Pg.567]


See other pages where Rotational dyad state is mentioned: [Pg.22]    [Pg.26]    [Pg.429]    [Pg.380]    [Pg.167]    [Pg.98]    [Pg.565]    [Pg.66]    [Pg.58]    [Pg.59]    [Pg.58]    [Pg.62]    [Pg.162]    [Pg.6]    [Pg.27]    [Pg.29]    [Pg.118]    [Pg.289]    [Pg.1953]    [Pg.1970]    [Pg.6]    [Pg.6]    [Pg.212]    [Pg.44]    [Pg.329]    [Pg.101]    [Pg.2106]    [Pg.221]    [Pg.565]    [Pg.565]    [Pg.567]    [Pg.22]   
See also in sourсe #XX -- [ Pg.23 ]




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