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Molecular systems thermodynamic approach

While at a temperature below Tg, some degree of molecular motion does occur. With time the molecular system does approach the true equilibrium state, i.e., the equilibrium values of volume, enthalpy or other state function variables. Physical aging represents a thermodynamic drive towards the equilibrium glassy state, and the recovery process involves a decrease in free volume as the material ages. [Pg.630]

In this chapter, the diverse coupling constants and MEC components identified in the combined electronic-nuclear approach to equilibrium states in molecules and reactants are explored. The reactivity implications of these derivative descriptors of the interaction between the electronic and geometric aspects of the molecular structure will be commented upon within both the EP and EF perspectives. We begin this analysis with a brief survey of the basic concepts and relations of the generalized compliant description of molecular systems, which simultaneously involves the electronic and nuclear degrees-of-freedom. Illustrative numerical data of these derivative properties for selected polyatomic molecules, taken from the recent computational analysis (Nalewajski et al., 2008), will also be discussed from the point of view of their possible applications as reactivity criteria and interpreted as manifestations of the LeChatelier-Braun principle of thermodynamics (Callen, 1962). [Pg.456]

An analogy may be drawn between the phase behavior of weakly attractive monodisperse dispersions and that of conventional molecular systems provided coalescence and Ostwald ripening do not occur. The similarity arises from the common form of the pair potential, whose dominant feature in both cases is the presence of a shallow minimum. The equilibrium statistical mechanics of such systems have been extensively explored. As previously explained, the primary difficulty in predicting equilibrium phase behavior lies in the many-body interactions intrinsic to any condensed phase. Fortunately, the synthesis of several methods (integral equation approaches, perturbation theories, virial expansions, and computer simulations) now provides accurate predictions of thermodynamic properties and phase behavior of dense molecular fluids or colloidal fluids [1]. [Pg.118]

The past three decades have witnessed the development of three broad techniques—molecular dynamics (MD), Monte Carlo (MC), and cellular automata simulations—that approach the study of molecular systems by simulating submicroscopic chemical events at this intermediate level. All three methods focus attention on a modest number of molecules and portray chemical phenomena as being dependent on dynamic, and interactive events (a portrayal consistent with our scientific intuition and a characteristic not intrinsic to either thermodynamics or the traditional deterministic approach based on differential equations). These techniques lend themselves to a visual portrayal of the evolution of the configurations of the systems under study. Because each approach has its own particular advantages and shortcomings, one must take into consideration the pros and cons of each, especially in light of the nature of the problem to be solved. [Pg.207]

A predictive molecular thermodynamics approach is developed for microemulsions, to determine their structural and compositional characteristics [3.7]. The theory is built upon a molecular level model for the free energy change. For illustrative purposes, numerical calculations are performed for the system water, cyclohexane, sodium dodecyl sulfate as surfactant, pentanol as cosurfactant and NaCl as electrolyte. The droplet radius, the thickness of the surfactant layer at the interface, the number of molecules of various species in the droplets, and the distribution of the components between droplets and the continuous phase are calculated. The theory also predicts the transition from a mi-... [Pg.202]

Most food biopolymers have limited miscibility on a molecular level and form multicomponent, heterophase and nonequilibrium dispersed systems. A thermodynamic approach is applicable for studying structure-property relationships in formulated foods since their structures are based on nonspecific interactions between components and such thermodynamically based operations as mixing of components, changing temperature and/or pH, underlies processing conditions. [Pg.41]

Riccardo and coworkers [50, 51] reported the results of a statistical thermodynamic approach to study linear adsorbates on heterogeneous surfaces based on Eqns (3.33)—(3.35). In the first paper, they dealt with low dimensional systems (e.g., carbon nanotubes, pores of molecular dimensions, comers in steps found on flat surfaces). In the second paper, they presented an improved solution for multilayer adsorption they compared their results with the standard BET formalism and found that monolayer capacities could be up to 1.5 times larger than the one from the BET model. They argued that their model is simple and easy to apply in practice and leads to new values of surface area and adsorption heats. These advantages are a consequence of correctly assessing the configurational entropy of the adsorbed phase. Rzysko et al. [52] presented a theoretical description of adsorption in a templated porous material. Their method of solution uses expansions of size-dependent correlation functions into Fourier series. They tested... [Pg.65]

A schematic representation of the variation of G j, G p Ga, and Gj with surface-surface separation distance h is shown in Figure 8.4. G j increases very sharply with a decrease in h, when h<28 likewise, G i increases very sharply with a decrease in h, when h<8 and Gj versus h shows a minimum, G j , at separation distances comparable to 28. When h < 28, Gj shows a rapid increase with decrease in h. The depth of the minimum depends on the Hamaker constant A, the particle radius R, and the adsorbed layer thickness 8. G p increases with increases of A and R and, at a given A and R, also increases with a decrease in 8 (i.e., with decrease in the molecular weight, M, of the stabiliser). This is illustrated in Figure 8.5, which shows the energy-distance curves as a function of S/R. The larger the value of 5/R, the smaller the value of G j in this case, the system may approach thermodynamic stability, as occurs with nanodispersions. [Pg.119]

The present chapter is organized in three sections the first section is devoted to basic theoretical backgroimd concerning the spin-crossover phenomenon, viz ligand field theory, thermodynamics and cooperativity the second section reports on some examples that we feel are particularly relevant to illustrate the main directions in which research on synthetic aspects of cooperativity is being directed finally, the third section describes three approaches, up to now reported, concerning spin bistability in supramolecular and molecular systems and memory effect. [Pg.54]

It is well appreciated that thermodynamic and kinetic parameters are difficult to compute for organometallic molecular systems (see, e.g.. Refs 12-14 and Chap. 4 by Frenking in the present volume). In particular, such quantities cannot be predicted within an independent-particle, single-determinant Hartree-Fock type of approach electron correlation must be included in the computational methods applied to achieve reliable and accurate results. In this work, we examine the performance of three first-principles methods, generally acknowledged by the abbreviations BLYP, B3LYP, and MP2. The first two are methods based on density functional theory (DFT) (15) the latter is an ab initio, molecular orbital (MO)-based method (16). [Pg.324]

The different efficiencies of chemical lasers governed by different kinetic coupling schemes can be derived from a general statistical-thermodynamic approach to work processes in nonequilibrium molecular systems " . The two major components of this approach are the maximum entropy principle and the entropy deficiency function. The entropy deficiency is a generalized thermodynamic potential (free energy). That is, it decreases monotonically in time in spontaneous relaxation processes and provides an upper bound to the thermodynamic work performed by the system in a controlled process. For systems of weakly interacting molecules the entropy deficiency DS[X X ] is given by... [Pg.75]

The aim of the descriptions and analyses presented in the foregoing sections was to illuminate some aspects of chemical lasers as molecular systems far from equilibrium. Particular emphasis was drawn on the limits of weak and strong rotational coupling since they represent extremely different kinetic schemes and consequently different kinetic behaviors. Thermodynamic considerations were employed to complement the detailed kinetic description. The thermodynamic approach can yield additional physical insights, but (at least so far) not new quantitative data. These are... [Pg.80]

In this chapter, we introduce a novel system coefficient approach developed in our research center. The system coefficient approach uses a set of probe compoimds to measure the molecular interaction strengths of a skin/chemical mixture system. A linear free-energy relationship (LEER, a thermodynamic principle) is used to dissect the complicated molecular interactions in the absorption system into basic molecular interaction forces, which can be parameterized and used to predict a free-energy-related property of the system, such as partition coefficients or permeability. In the system coefficient approach, a chemical mixture is treated as a medium composed of the major components and other minor or trace components. A set of system coefficients represents the relative molecular interaction strengths of the chemical mixture, and a set of solute descriptors represents the molecular interaction strengths of a chemical. A free-energy-related specific property is interactively correlated to the system coefficients of the chemical mixture and the solute descriptors of the chemicals, which can be used to provide quantitative predictions... [Pg.72]


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Molecular approach

Molecular thermodynamics

Systemic approach

Thermodynamic approach

Thermodynamical system

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