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Equilibrium Thermodynamic Properties

The fluctuations in different ensembles are related to thermodynamic derivatives, such as the specific heat or the isothermal compressibility. The transformation and relation between different ensembles has been discussed in detail by Allen and Tildesley (1987). To obtain the equilibrium thermodynamic properties of a structure, the time average of a variable, A, (Equation 1.20) yields the thermodynamic value for the selected variable  [Pg.12]

This dynamic variable can be any function of the coordinates and momentum of the particles in the structure. Through time averaging, the first-order properties of a system such as internal energy, kinetic energy, pressure, and virial can be computed. The microscopic expressions in the form of fluctuations of these first-order properties can be used to calculate thermodynamic properties such as specific heat, thermal expansion, and bulk modulus. In the thermodynamic Umit, the first-order properties obtained in one ensemble are equivalent to those obtained in other ensanbles. However, second-order properties differ among ensembles. Therefore, it is important to use the appropriate ensemble to obtain the desired properties. [Pg.12]


D. Blankschtein, G. Thurston, G. Benedek. Phenomenological theory of equilibrium thermodynamic properties and phase separation of micellar solutions. J Chem Phys 25 7268-7288, 1986. [Pg.550]

The mechanism of radiative transfer in flares was found to depend on compn, flare diameter and pressure (Ref 69). The flare efficiency calcn is complicated by the drop-off in intensity at increasing altitudes and at very large diameters owing to the lower reaction temps (Ref 11, p 13) and the narrowing of the spectral emittance band (Ref 35). The prediction of the light output in terms of compn and pressure (ie, altitude) is now possible using a computer program which computes the equilibrium thermodynamic properties and the luminance (Ref 104) Flare Formulations... [Pg.983]

The Boltzmann constant is represented by kB. It is more difficult to use Monte Carlo methods to investigate dynamic events as there is no intrinsic concept of time but an ensemble average over the generated states of the system should give the same equilibrium thermodynamic properties as the MD methods. A good review of both MD and the Monte Carlo methods can be found in the book by Frenkel and Smit [40]. [Pg.693]

Film balance techniques 49 Equilibrium thermodynamic properties 51 n/A curves and phase transitions 54 Dynamic methods 57... [Pg.45]

The mixture we have just described, even with a chemical reaction, must obey thermodynamic relationships (except perhaps requirements of chemical equilibrium). Thermodynamic properties such as temperature (T), pressure (p) and density apply at each point in the system, even with gradients. Also, even at a point in the mixture we do not lose the macroscopic identity of a continuum so that the point retains the character of the mixture. However, at a point or infinitesimal mixture volume, each species has the same temperature according to thermal equilibrium. [Pg.25]

In the bottom-up approach, a large variety of ordered nano-, micro-and macrostructures may be obtained by changing the balance of all the attractive and repulsive forces between the structure-forming molecules or particles. This can be achieved by altering the environmental conditions (temperature, pH, ionic strength, presence of specific substances or ions) and the concentration of molecules/particles in the system (Min et al., 2008). As this takes place, the interrelated processes of formation and stabilization are both important considerations in the production of nanoparticles. In addition, as particles grow in size a number of intrinsic properties change, some qualitatively, others quantitatively some affect the equilibrium (thermodynamic) properties, and others affect the nonequilibrium (dynamic) properties such as relaxation times. [Pg.7]

Oxides. Experimental work concerning the equilibrium thermodynamic properties of Ti20, Ti30, and TieO has been reviewed.28 Cubic (NaCl type) TiO has been prepared by shock compression of an equimolar mixture of Ti and Ti02.29 The temperature of the mixture was estimated to reach 3000 K at a pressure of 850 kbar. The TiO prepared by this method had a = 4.179 + 0.002 A for a single compression and 4.177 A for two successive compressions, and d45 = 4.860 + 0.005 gem-3. Variations in the composition of the initial mixture led to the formation of non-stoicheiometric oxides TiOx, e.g. [Pg.4]

Although the prediction of polymer-polymer miscibility based on chemical structure and/or equilibrium thermodynamic properties has been a goal of polymer chemists for decades (1,2), the complexity of... [Pg.425]

The energy landscape approach can elucidate such general properties of molecular recognition as the nature of the thermodynamic phases and barriers on the ligand-protein association pathway [127,128]. This method evaluates equilibrium thermodynamic properties of the system from Monte Carlo simulations of the system at a broad temperature range with the aid of the optimized data analysis and the weighted histogram analysis technique [148-153],... [Pg.309]

Of central interest to the study of clusters is information on both dynamic and equilibrium properties of the systems. Dynamic properties such as diffusion coefficients can be used to investigate solidlike to liquidlike phase transitions as the cluster temperatures are varied. Equilibrium thermodynamic properties are of great utility in identifying cluster stability. Further-... [Pg.139]

Fully thermalised excited states may be treated as distinct chemical species with their own equilibrium thermodynamic properties, including redox potentials. We may therefore define standard redox potentials U°.. and f/%. for reactions of the excited states D and A ... [Pg.220]

As the fundamental concepts of chemical kinetics developed, there was a strong interest in studying chemical reactions in the gas phase. At low pressures the reacting molecules in a gaseous solution are far from one another, and the theoretical description of equilibrium thermodynamic properties was well developed. Thus, the kinetic theory of gases and collision processes was applied first to construct a model for chemical reaction kinetics. This was followed by transition state theory and a more detailed understanding of elementary reactions on the basis of quantum mechanics. Eventually, these concepts were applied to reactions in liquid solutions with consideration of the role of the non-reacting medium, that is, the solvent. [Pg.305]

Using Flory-Huggins theory it is possible to account for the equilibrium thermodynamic properties of polymer solutions, particularly the fact that polymer solutions show major deviations from ideal solution behavior, as for example, the vapor pressure of solvent above a polymer solution invariably is very much lower than predicted from Raoult s law. The theory also accounts for the phase separation and fractionation behavior of polymer solutions, melting point depressions in crystalline polymers, and swelling of polymer networks. However, the theory is only able to predict general trends and fails to achieve precise agreement with experimental data. [Pg.156]

Finally and fairly obviously it should be mentioned that equilibrium thermodynamic properties of the reaction system may be afforded if the kinetics of the reaction can be monitored in both the forward and reverse directions. This leads to the value of the equilibrium constant as a function of pressure and the reaction volume, the difference in volume between the partial molar volumes of products and reactants. This information can also be established if the equilibrium constant can be obtained directly as a function of... [Pg.112]

Figure 1.11. Equilibrium thermodynamic properties of LJ38 in the canonical ensemble, (a) The heat capacity, Cv (b) The probability of the cluster being in the fee, icosahedral and liquid-like regions of bound configuration space. These results were obtained using an anharmonic form of the superposition method (Section III.C). Figure 1.11. Equilibrium thermodynamic properties of LJ38 in the canonical ensemble, (a) The heat capacity, Cv (b) The probability of the cluster being in the fee, icosahedral and liquid-like regions of bound configuration space. These results were obtained using an anharmonic form of the superposition method (Section III.C).
VIII. EQUILIBRIUM THERMODYNAMIC PROPERTIES A. Specific Heat... [Pg.498]

Now we specify the fluid equilibrium thermodynamic properties. The internal energy is... [Pg.515]

Equilibrium thermodynamic properties, such as internal energy, are calcn-lated from the time-dependent expectation value of the total system energy as follows ... [Pg.758]

ThermKin (Thermodynamic Estimation of Radical and Molecular Kinetics) evolved (see Sheng s thesis [74]) from a previously developed computer code, i.e. THERMRXN (included in THERM) [82] which calculates equilibrium thermodynamic properties for any given reaction. Additionally, ThermKin determines the forward rate constants, k(T), based on the canonical transition state theory (CTST). [Pg.26]

The direction of a chemical reaction or a phase transformation can be determined from the equilibrium thermodynamic properties of the phases involved. Note, though, that the speed of any transformation is not accessible from thermodynamics. Thermodynamics clearly states that diamond will transform into graphite at room temperature, but the rate of the reaction is insignificant. This chapter is concerned mainly with the kinetics of reactions, the speed at which they occur. Marrying this aspect with thermodynamics lies outside the scope of this chapter, but some introductory notes are given in Section S3.2. [Pg.225]

The direction (but not the rate) of a phase transformation can be determined from the equilibrium thermodynamic properties of the phases involved. For this purpose, the most important thermodynamic parameter is the Gibbs energy (or Gibbs free energy) of the phases. The Gibbs energy, G (units J moP ), of a pure material is dehned by the equation ... [Pg.534]

Polymers are involved in many practical adhesion problems. A polymer liquid can be present in the gap between the two media that adhere to one another in order to create strong attractive forces that strengthen the adhesion. In this context it is important to understand how polymer solutions interact with surfaces and how they create strong interactions between them [1]. The aim of this short review is to present rather qualitatively our understanding of the equilibrium thermodynamic properties of polymer solutions close to surfaces. This is clearly one of the important factors in understanding the adhesion between two surfaces mediated by polymers, but one must keep in mind that adhesion is a nonequilibrium process where energy dissipation plays a major role. This aspect will not be considered in this chapter. [Pg.151]

Because the potential-pH diagrams characterize equilibrium thermodynamic properties only, the Pourbaix diagrams cannot be used to predict the rates of reactions. They can be used to evaluate the conditions for the formation of barrier oxide films but not... [Pg.152]


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