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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 85 (1981), S. 4039-4040 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 86 (1982), S. 2197-2205 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 93 (1989), S. 6996-7003 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 94 (1990), S. 9-20 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 94 (1990), S. 1874-1876 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 7338-7345 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A unified treatment of polarization relaxation, dielectric dispersion and solvation dynamics in a dense, dipolar liquid is presented. It is shown that the information of solvent polarization relaxation that is obtained by macroscopic dielectric dispersion experiments is not sufficient to understand dynamics of solvation of a newly created ion or dipole. In solvation, a significant contribution comes from intermediate wave vector processes which depend critically on the short range (nearest-neighbor) spatial and orientational order that are present in a dense, dipolar liquid. An analytic expression is obtained for the time dependent solvation energy that depends, in addition to the translational and rotational diffusion coefficients of the liquid, on the ratio of solute–solvent molecular sizes and on the microscopic structure of the polar liquid. Mean spherical approximation (MSA) theory is used to obtain numerical results for polarization relaxation, for wave vector and frequency dependent dielectric function and for time dependent solvation energy. We find that in the absence of translational contribution, the solvation of an ion is, in general, nonexponential. In this case, the short time decay is dominated by the longitudinal relaxation time but the long time decay is dominated by much slower large wave vector processes involving nearest-neighbor molecules. The presence of a significant translational contribution drastically alters the decay behavior. Now, the long-time behavior is given by the longitudinal relaxation time constant and the short time dynamics is controlled by the large wave vector processes. Thus, although the continuum model itself is conceptually wrong, a continuum model like result is recovered in the presence of a sizeable translational contribution. The continuum model result is also recovered in the limit of large solute to solvent size ratio. In the opposite limit of small solute size, the decay is markedly nonexponential (if the translational contribution is not very large) and a complete breakdown of the continuum model takes place. The significance of these results is discussed.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 95 (1991), S. 467-478 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A theoretical study of the dielectric friction on an ion moving through a dipolar liquid is presented. A microscopic expression for the dielectric friction is derived from linear response theory for a Brownian ion. This expression supports the picture of a "dynamic solventberg'' model in the sense that much of the contribution to dielectric friction (ζDF) comes from the nearest-neighbor molecules. The translational modes of the solvent are found to have a very strong influence on the dielectric friction, in agreement with the observation of Colonomos and Wolynes [J. Chem. Phys. 71, 2644 (1979)]. In fact, except in the limit of small ion size, the microscopic ζDF is significantly larger than the continuum ζDF in the absence of the translational motion of the solvent molecules, but the reverse is obtained in the presence of a substantial translational contribution. It is found that the recovery of the continuum limit results from the molecular expression requires serious assumptions, some of which are hard to justify. It is also found that the point dipole approximation for the dipolar solvent molecule leads to improper results for ζDF because this approximation gives a wrong wave vector (k) dependence of the wave vector dependent dielectric function (ε(k)) of the liquid at large k (kσ(very-much-greater-than)2π, where σ is the solvent molecular diameter). We show that within a linear equilibrium theory for dipolar liquids, the cross correlations between the short ranged hard force and the long ranged dipolar force is zero so the calculations of Colonomos and Wolynes are internally consistent. However, this cross correlation can be quite important if the soft force also contains a spherically symmetric part. The similarity between the solvent role in ζDF and in the time-dependent fluorescence Stokes shift is discussed. The limitations of the present theory are also pointed out.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 8991-9001 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The orientational relaxation of molecules in a supercooled liquid is known to exhibit interesting dynamical behavior. As the temperature of the liquid is lowered towards its glass transition temperature, there is a bifurcation of the relaxation dynamics into primary (α) and secondary (β) processes; the former is associated with the collective motion responsible for the glass transition, while the latter is associated with single particle motion. In this paper we present a theory of orientational relaxation in a supercooled liquid. This theory provides both qualitative and quantitative descriptions of the (αβ) bifurcation phenomenon at a molecular level. The theory exploits the properties of a time dependent free energy functional which explicitly includes the effects of the collective motions in the liquid on the orientational motion of a solute (or a tagged) molecule. In the overdamped limit, this analysis leads to two coupled Smoluchowski equations for the orientation distribution function. These equations, when solved, reveal the essential features of the (αβ) bifurcation phenomenon. Explicit calculations are presented for orientational relaxation in a liquid of dipolar hard spheres, a liquid of nonpolar ellipsoids, and an orientationally disordered solid. Our calculations demonstrate the ubiquity of the (αβ) bifurcation phenomenon and they reveal many of its aspects. The relevance of the present work to current theories of glass transition is discussed briefly.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 2258-2261 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A microscopic expression for the free energy functional for polarization fluctuations in a dipolar liquid in the presence of an external field is derived from the first principles by using the density functional theory. The microscopic expression is shown to reduce to the well known free energy expressions of Marcus and Felderhof in the appropriate limits. The microscopic free energy functional can be especially useful to describe those dynamical processes when intermolecular correlations are important.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 689-695 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Binary liquids are known to be better glass formers than one component liquids. To understand this, we carried out a theoretical study of relaxation of density fluctuations in a dense liquid of binary hard spheres. This study is based on a coupled, modified, Smoluchowski equations where effects of interparticle interactions are included through two particle direct correlation functions of the binary mixture. Such a modified Smoluchowski equation description is reliable at intermediated values of wave vector k, but not at small k, so we have limited our study only to intermediate k. We find that the eigenvalues of the coupled equations show rich structure that depends on the composition of the binary liquid and also on the size ratio of the two constituents. At high density, the larger of the two eigenvalues becomes positive at intermediate wave vectors, indicating an instability of density fluctuation at that wave vector. As the density is further increased, the range of k over which the eigenvalue is positive, also increases. Although nonlinearities in density fluctuations and coupling with other hydrodynamic modes (neglected in this calculation) must be considered to gain an understanding of glass transition, the present results do indicate that the relaxation of density fluctuations in a binary liquid mixture is considerably different from that in a one component liquid.
    Type of Medium: Electronic Resource
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