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  • Electronic Resource  (4)
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  • Electronic Resource  (4)
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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 6633-6639 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We present a new equation of state for hard chain fluids. This equation of state is developed by applying an extension of Wertheim's theory for associating fluids to a nonspherical reference fluid. Since the equation of state is developed in a similar manner to the statistical associating fluid theory (SAFT) we call this improved equation of state SAFT-Dimer (SAFT-D). The equation of state requires only the contact values of the hard sphere and hard disphere site–site correlation functions as input. We compare the compressibility factor from SAFT and SAFT-D with molecular simulation data for flexible hard chains with chain lengths of 16, 51, and 201 segments. The second virial coefficient and compressibility factor from SAFT-D are in better agreement with molecular simulation results than the generalized Flory dimer, TPT2, and Percus–Yevick compressibility equations of state.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 101 (1994), S. 6880-6887 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Due to the flexibility of associating polymer and protein molecules, intramolecular association can have a significant affect on the thermodynamic properties and structure of associating polymer and protein solutions. The equilibrium state is determined by the minimization of the appropriate free energy with respect to intermolecular association between like and unlike species and intramolecular association. As a first step to understanding this competition between intramolecular and intermolecular hydrogen bonding, we have conducted a molecular simulation study of flexible hard chain molecules that intramolecularly associate in the absence of intermolecular association. To explain the simulation results, we have developed a new simple and accurate theory of intramolecular association. By considering the limit of total bonding, we have also developed an accurate equation of state for hard rings. The theory is in good agreement with new molecular simulation results for intramolecularly associating hard chains, rigid hard rings, and bent triatomics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 102 (1995), S. 2585-2592 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A new theory to explain the competition between inter- and intramolecular association in flexible hard chain molecules is presented. The theory has been tested through comparisons with Metropolis Monte Carlo simulation results. For intermolecular association we use Wertheim's theory which has been shown to be accurate for intermolecular association in flexible associating hard chain molecules. For intramolecular association we use a theory we developed for intramolecular association in the absence of intermolecular association. These two theories are combined to develop a theory for the competition between inter- and intramolecular association. The new theory is in good agreement with simulation results and is able to predict some salient features of associating chain molecules. The theory predicts that intermolecular association becomes more important at high densities and that intramolecular association dominates at low density and low temperatures. In addition, theory and simulation show a minimum in the compressibility factor when plotted against the association energy at low density. This minimum is due to the presence of intramolecular association and is not observed for intermolecularly associating fluids. © 1995 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 8058-8067 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We present a class of closures specifically designed to satisfy the zero-separation theorems for the correlation functions y(r) (the cavity function), γ(r)=h(r)−C(r) (the indirect correlation), and B(r) (the bridge function) at coincidence r=0 for soft-sphere pair potentials. The rationale is to ensure the correct behavior of these correlation functions inside the core r〈σ. Since the coincidence theorems implicate the thermodynamic properties of the bulk fluid: the isothermal compressibility, the internal energy and the chemical potentials, we can hopefully enforce consistency between the structure and thermodynamic properties. We solve the Ornstein–Zernike equation for the Lennard-Jones molecules where plentiful Monte Carlo data are available for testing. It turns out that not only consistency is achieved, we also obtain accurate structures: the pair correlation function g(r), the cavity function, and the bridge function for wide ranges of fluid states (0.72〈T*〈1.5, ρ*〈0.9). Comparison with MC data attests to the accuracy. The closure of the zero-separation type (ZSEP), is sufficiently robust and flexible to ensure not only fulfillment of the zero-separation theorems but also pressure consistency. Success with the Lennard-Jones potential implies its applicability to other similar soft-sphere potentials. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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