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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 91 (1989), S. 7900-7911 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The translational diffusion coefficient D of long enough polymer chains without excluded volume is studied on the basis of the discrete helical worm-like (HW) chain with partially fluctuating (orientation-dependent) hydrodynamic interaction (HI). In order to evaluate D(∞) in the long time limit, which corresponds to diffusion experiments usually done on the long time scales, the time-dependent part of D is explicitly treated by an application of the projection operator method. The result may be written as D(∞)=D(Z)(1−δ0−δ1), where D(Z) is the Zimm value with preaveraged HI, δ0 is the relative decrease at time t=0 due to constraints, and δ1 is the additional relative decrease at t=∞ due to coupling between the translational motion and the Rouse vector (dielectric) modes for the HW chain, especially the long wavelength ones. It is found that D(∞) is decreased as the local conformation of the chain becomes rather compact, and that D(∞)=D(Z) (i.e., δ0=δ1=0) in the stiff-chain limit. Thus the ratio ρ of the root-mean-square radius of gyration to the hydrodynamic radius defined from D is not a universal constant but depends on the chain conformation and stiffness. A comparison of theory with experiment is made with respect to ρ, and it is found that the theory may well explain experimental results. For comparison, also for the Gaussian chain (spring–bead model), which is an unconstrained chain, D(∞) is evaluated, and it is found that δ0=0 but δ1≠0.
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 5167-5178 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Oscillatory flow birefringence of flexible chain polymers in dilute solution is studied on the basis of the discrete helical worm-like chain such that a local polarizability tensor is attached rigidly to each of the subbodies composing the chain. The mechano-optic coefficient S is formulated by the time-correlation function formalism, and is expressed in terms of the (1,1)- and (1,2)-body time-correlation functions of "total angular momentum quantum number'' L=2. The (1,2)-body time-correlation functions are evaluated following a procedure analogous to the one developed previously in the higher-order subspace approximations. It is then shown that the three branches (one global and two local) of the viscoelastic eigenvalue spectrum and the five local branches of the magnetic one make contributions to S. With these results, examination is made of the frequency behavior of the phase angle θs of S and also of its dependence on the local polarizability tensor. It is found that the high-frequency behavior of observed θs, which deviates from the prediction for the Zimm spring–bead model, may well be explained by the contributions from the local chain motions with proper local polarizability tensors. A comparison of theory with experiment is made for atactic polystyrene with respect to the frequency dependence of θs, and the good agreement is found with the model parameters determined from an analysis of experimental data for equilibrium properties.
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 4207-4213 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The expansion factor αμ for the mean-square electric dipole moment is studied on the basis of the helical wormlike chain with the excluded-volume effect incorporated in the Yamakawa–Stockmayer–Shimada scheme. A general expression is formulated for the first-order perturbation coefficient Kμ(L) for the chain of total contour length L. The asymptotic solution for Kμ(L) in the limit of L→∞ is evaluated analytically in the Daniels approximation by an application of the operational method. In contradiction to the common notion, it is found that, in the case of κ0τ0≠0 with κ0 and τ0 being the constant curvature and torsion, respectively, of the characteristic helix, Kμ(∞) does not vanish even for the chain having a local electric dipole moment vector perpendicular to the chain contour, indicating that αμ diverges with increasing molecular weight.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 9145-9155 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Dynamic depolarized light scattering from dilute solutions of flexible chain polymers is studied on the basis of the discrete helical wormlike (HW) chain. A preliminary consideration leads to the conclusion that the spring-bead model with the Kuhn–Grün expression for the spring polarizability tensor is, in principle, inappropriate for the description of the depolarized scattering, so that the Ono–Okano theory is invalid for real chains. In the approximations that the orientational fluctuations of the subbodies composing the HW chain may be decoupled from their density fluctuation at very small magnitude of the scattering vector and that the former relax much faster than the latter, which are good enough under the condition of usual measurements, it is shown that the spectrum JΓ of the excess depolarized component of the scattered light may be written in terms of the same class of basic time-correlation functions with the "total angular momentum quantum number'' L=2 and the number of "excited'' subbodies n=1, as in the case of nuclear magnetic relaxation and fluorescence depolarization. Numerical evaluation of JΓ is carried out, taking atactic polystyrene (a-PS) and atactic poly(methyl methacrylate) as typical examples of flexible polymers. It is then found that for both polymers JΓ may be represented in terms of a small number of those eigenvalues λj2,k of the diffusion operator for the HW model with very small wave numbers k which belong to two branches specified by the superscript j, one corresponding to the low frequency modes and the other to the high frequency modes. For a-PS, this result is consistent with the experimental result obtained by Bauer, Brauman, and Pecora [Macromolecules 8, 443 (1975)] except that the present low frequency modes do not correspond to the Rouse–Zimm modes of the spring-bead model.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 105 (1996), S. 5618-5625 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: In order to examine the effect of fluctuating (nonpreaveraged) hydrodynamic interaction on the hydrodynamic-radius expansion factor αH and also the viscosity-radius one αη, a Monte Carlo simulation study is made on the basis of the polymethylenelike rotational isomeric state chain in the Zimm rigid-body ensemble approximation. All the results obtained are consistent with the recent finding (by Yamakawa's group) that the experimental values of αH are appreciably smaller than the values predicted by any available theory and rather agree with the theoretical and experimental values of αη, indicating that the effect is significant on αH but is negligibly small on αη if any. The present results along with the recent experimental ones also confirm the validity of the quasi-two-parameter scheme for αH and αη as well as for the gyration-radius expansion factor αS; i.e., these expansion factors are functions only of the scaled excluded-volume parameter z˜ defined in the Yamakawa–Stockmayer–Shimada theory of the excluded-volume effect in the Kratky–Porod wormlike chain and the helical wormlike chain. © 1996 American Institute of Physics.
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  • 6
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Macromolecules 10 (1977), S. 359-361 
    ISSN: 1520-5835
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
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  • 7
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Macromolecules 13 (1980), S. 1518-1525 
    ISSN: 1520-5835
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 105 (1996), S. 11268-11275 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The eigenvalue problem for the matrix representation of the diffusion operator appearing in the diffusion equation previously derived for the coarse-grained helical wormlike (HW) chain model is considered. Following the procedure already established in the study of the original diffusion equation for the discrete HW chain, the problem is solved in the subspace and block-diagonal approximations in the subspace L(1), where L is the "total angular momentum quantum number'' and (1) indicates the one-body excitation basis set. The 1(1) eigenvalues λ1,kj thus obtained form three branches of the eigenvalue spectrum specified by the index j as before, and it is shown that λ1,k0 in the j=0 (lowest) branch at small wave number k is approximately proportional to the corresponding Rouse–Zimm eigenvalue in the Hearst version. The behavior of the eigenvalue spectra is also numerically examined taking atactic polystyrene with the fraction of racemic diads fr=0.59 and atactic poly(methyl methacrylate) with fr=0.79 as typical examples of flexible polymers. It is found that the ratio λ1,k0/λ1,10 at small k depends somewhat (appreciably for large k) on chain stiffness and local chain conformation. © 1996 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 1313-1325 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The dynamic intrinsic viscosity of flexible chain polymers in dilute solution is studied on the basis of the discrete helical worm-like chain. The correlation function formalism of the complex intrinsic viscosity [η] is given, taking account of the effect of the finite hydrodynamic volumes of subbodies of the chain. A new basis set, which is a hybrid of the one- and two-body excitation basis functions, is introduced. Then the eigenvalue problem for the representation of the diffusion operator may be reduced to N six-dimensional eigenvalue problems with N the number of subbodies. Among the six branches of the eigenvalue spectrum, one global and two local branches make contribution to the dynamic intrinsic viscosity. The theory predicts the existence of the high-frequency plateau which is distinguished from the infinitely high-frequency viscosity. The plateau arises from the interaction between the global and local chain motions (caused by the helical nature of the local chain contour), the constraints, and the finite hydrodynamic volumes of the subbodies. The interaction above vanishes for the Kratky–Porod worm-like chain possessing no helical nature. A comparison of theory with experiment is made with respect to the plateau value, and it is found that its dependence on the chemical structure of the chain may well be explained.
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 1120-1129 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: An alternative representation of the diffusion equation is derived for the discrete helical wormlike (HW) chain model by treating the constraints in a manner different from that previously adopted. In contrast to the previous diffusion equation for the same HW model, which can describe local motions but not global to quasi-global motions of flexible polymers in dilute solution because of the defect arising from the preaveraging of the constraining matrix, the present equation may be considered to be suitable for the description of the latter since it can give explicitly the Rouse–Zimm eigenvalues in the ground (global) state. It is shown that the present and previous equations are exactly the same before the constraining matrix common to them is preaveraged, as is natural, and that the above difference between their characteristics arises from the difference in the effect of the preaveraging approximation. A comparison is also made of the present model (or diffusion equation) with other models for polymer chain dynamics. In particular, the present theory is shown to be rather similar to the Fixman–Kovac theory for the conventional bond chain in the physical meaning as well as the formulation. © 1996 American Institute of Physics.
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