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Equilibrium and Nonequilibrium

In summary, the requirements of selectivity show that the relative velocity difference V/V must remain substantial, but Eq. 9.17 tells us that the velocity increments must occur over a short distance d. As the distance d between velocity extremes decreases, the shear rate and the pressure gradient needed to generate high shear increases. Thus a trend to increasing pressure drops in F(+) systems is a natural outgrowth of these basic considerations. Again the most direct confirmation of theory is HPLC, where pressures of several hundred atmospheres are common. [Pg.197]

In some cases the speed of separation becomes crucial, so we change our focus, as in Section 8.9, to that of maximizing the number of plates per unit time Nit. From Eq. 9.17, N = XIH is [Pg.197]

Since XIV is the time t expended in reaching point X, we have [Pg.197]

Quantity Nit is increased in much the same way as H is decreased by finding ways to reduce d and to increase D. However H is proportional to zone velocity V (which we are therefore advised to reduce) whereas Nit is independent of V. (If we add in the effects of ordinary longitudinal diffusion, we find Nit largest at high velocities.) [Pg.197]

While the random walk model employed here is widely applicable to F(+) methods, it fails if the molecules do not transfer rapidly between velocity states, equivalent to many random steps. Such a limitation applies to electrodecantation (noted below), where the distances are too great for rapid diffusional exchange. The random walk model is most meaningful for zonal separation methods such as chromatography and field-flow fractionation. [Pg.197]


A method is outlined by which it is possible to calculate exactly the behavior of several hundred interacting classical particles. The study of this many-body problem is carried out by an electronic computer which solves numerically the simultaneous equations of motion. The limitations of this numerical scheme are enumerated and the important steps in making the program efficient on the computer are indicated. The applicability of this method to the solution of many problems in both equilibrium and nonequilibrium statistical mechanics is discussed. [Pg.65]

Mazur, P. (1990). Equilibrium quasi-equilibrium, and nonequilibrium freezing of mammalian embryos. Cell Biophy. 17, 53-92. [Pg.383]

Experimental studies in electrochemistry deal with the bulk properties of electrolytes (conductivity, etc.) equilibrium and nonequilibrium electrode potentials the structure, properties, and condition of interfaces between different phases (electrolytes and electronic conductors, other electrolytes, or insulators) and the namre, kinetics, and mechanism of electrochemical reactions. [Pg.191]

When monomers with dependent groups are involved in a polycondensation, the sequence distribution in the macromolecules can differ under equilibrium and nonequilibrium regimes of the process performance. This important peculiarity, due to the violation in these nonideal systems of the Flory principle, is absent in polymers which are synthesized under the conditions of the ideal polycondensation model. Just this circumstance deems it necessary for a separate theoretical consideration of equilibrium and nonequilibrium polycondensation. [Pg.189]

A brief review is given of the important qualitative features of thermoplastic elastomers. Particular emphasis is given to the molecular structure, bulk morphology and interfacial character of these materials. Both equilibrium and nonequilibrium structures are discussed... [Pg.484]

Solvation Thermodynamics and the Treatment of Equilibrium and Nonequilibrium Solvation Effects by Models Based on Collective Solvent Coordinates... [Pg.63]

Nonequilibrium solvent effects can indeed by significant at the kcal level-maybe even at a greater level, but so far there is no evidence for that when the reaction coordinate involves protonic or heavier motions. Our goal in this section has been to emphasize just how powerful and general the equilibrium model is. In addition, in both the previous section and the present section, we have emphasized the use of models based on collective solvent coordinates for calculating both equilibrium and nonequilibrium solvation properties. [Pg.89]

The theory is capable of describing both the regimes of equilibrium and nonequilibrium solvation for the latter we have developed a framework of natural solvent coordinates which greatly helps the analysis of the reaction system along the ESP, and displays the ability to reduce considerably the burden of the calculation of the free energy surface in the nonequilibrium solvation regime. While much remains to be done in practical implementations for various reactions, the theory should prove to be a very useful and practical description of reactions in solution. [Pg.278]

Kim, H. J. and Hynes, J. T. Equilibrium and nonequilibrium solvation and solute electronic structure, IntJ.Quantum Chem., 24 (1990), 821-833... [Pg.356]

Den Otter, W. K. and Briels, W. J. (2003). The bending rigidity of an amphiphilic bilayer from equilibrium and nonequilibrium molecular dynamics, J. Chem. Phys., 118, 4712-4720. [Pg.108]

Munk P (1996) Equilibrium and nonequilibrium polymer micelles. In Webber SE, Munk P, Tuzar Z (eds) NATO ASI series, series E Applied sciences, vol 327. Kluwer, Dordrecht... [Pg.140]

Particle Dynamics A Useful Thermostat for Equilibrium and Nonequilibrium Molecular Dynamics Simulations. [Pg.122]

Johnson TM, Bullen TD (2004) Mass-dependent fractionation of selenium and chromim isotopes in low-temperature environments. Rev Mineral Geochem 55 289-317 Kim S-T, O Neil JR (1997) Equilibrium and nonequilibrium oxygen isotope effects in synthetic carbonates. Geochim Cosmochim Acta 61 3461-3475... [Pg.23]

M. Le Bellac, R Mortessagne, and G. Batrouni. Equilibrium and nonequilibrium statistical thermodynamics. Gambridge, England Cambridge University Press, 2004. [Pg.431]

MSN. 102. I. Prigogine, Entropy, time and kinetic description, in Order and Fluctuations in Equilibrium and Nonequilibrium Statistical Mechanics, 17th International Solvay Conference on Physics, G. Nicolis, G. Dewel, and J. W. Turner, eds., Wiley, 1980, pp. 35-75. [Pg.58]

R. Balescu, Equilibrium and Nonequilibrium Statistical Mechanics, John Wiley Sons, New York, 1975. [Pg.131]

We can now distinguish three general cases, depending on whether the first decaying species has a longer, a much longer, or a shorter half-hfe than that of the daughter nuclide. These three cases are transient equilibrium, secular equilibrium, and nonequilibrium. [Pg.724]

In this chapter, we review the current status of doping of SiC by ion implantation. Section 4.2 examines as-implanted depth profiles with respect to the influence of channeling, ion mass, ion energy, implantation temperature, fluence, flux, and SiC-polytype. Experiments and simulations are compared and the validity of different simulation codes is discussed. Section 4.3 deals with postimplant annealing and reviews different annealing concepts. The influence of diffusion (equilibrium and nonequilibrium) on dopant profiles is discussed, as well as a comprehensive review of defect evolution and electrical activation. Section 4.4 offers conclusions and discusses technology barriers and suggestions for future work. [Pg.114]

G. Brown, P. A. Rikvold, S. J. Mitchell, Monte Carlo methods for equilibrium and nonequilibrium problems in interfacial electrochemistry in Interfacial Electrochemistry. Theory, Experiment and Applications (Ed. A. Wi ckowski), Marcel Dekker, New York-Basel, 1999, p. 47. [Pg.908]

Figure 6.6 shows the relationship among 750, ysv, and ire. It is apparent that the value of 6 might be quite different between equilibrium and nonequilibrium situations, depending on the value of ire. There are several concepts that will assist us in anticipating the range of ire values ... [Pg.267]

From the point of view of statistical mechanics there are many problems, such as strongly anharmonic lattices, to which the theory can be applied.14 It appears as a natural generalization of Landau s theory of quasi-particles in the case when dissipation can no longer be neglected. The most interesting feature is that equilibrium and nonequilibrium properties appear linked. The very definition of the strongly coupled anharmonic phonons depends on their lifetime. [Pg.34]

A.I. Khinchin, Mathematical Foundations of Statistical Mechanics (G. Gamow transl., Dover Publications, New York 1949) R. Balescu, Equilibrium and Nonequilibrium Statistical Mechanics (Wiley-Interscience, New York 1975) Appendix. [Pg.108]

Isotopic fractionation resulting from evaporation from standing water bodies can be described in terms of equilibrium and nonequilibrium fractionation effects. Equilibrium fractionation occurs when the isotopic composition of the evaporated water or lake evaporate is in thermodynamic equilibrium with the lake water (23). Equilibrium fractionation, however, can occur only when the water vapor in the air mass above the lake is 100% saturated. The process of equilibrium isotopic fractionation is described by Raleigh fractionation. The isotopic composition of water vapor in equilibrium with liquid water at any time is given by... [Pg.79]

In 1977. Professor Ilya Prigogine of the Free University of Brussels. Belgium, was awarded Ihe Nobel Prize in chemistry for his central role in the advances made in irreversible thermodynamics over the last ihrec decades. Prigogine and his associates investigated Ihe properties of systems far from equilibrium where a variety of phenomena exist that are not possible near or al equilibrium. These include chemical systems with multiple stationary states, chemical hysteresis, nucleation processes which give rise to transitions between multiple stationary states, oscillatory systems, the formation of stable and oscillatory macroscopic spatial structures, chemical waves, and Lhe critical behavior of fluctuations. As pointed out by I. Procaccia and J. Ross (Science. 198, 716—717, 1977). the central question concerns Ihe conditions of instability of the thermodynamic branch. The theory of stability of ordinary differential equations is well established. The problem that confronted Prigogine and his collaborators was to develop a thermodynamic theory of stability that spans the whole range of equilibrium and nonequilibrium phenomena. [Pg.349]

The last Solvay Conference that I have rather arbitrarily put in this class is the 17th on Order and Fluctuations in Equilibrium and Nonequilibrium Statistical Mechanics held in October 1978.92... [Pg.26]

Order arising through nucleation occurs both in equilibrium and nonequilibrium systems. In such a process the order that appears is not always the most stable one there are often competing processes that will lead to different structures, and the structure that appears is the one that nucleates first. For instance, in the analysis of the different possible structures in diffusion-reaction systems17-20 one can show, by analyzing the bifurcation equations, that there are several possible structures and some of them require a finite amplitude to become stable if this finite amplitude is realized through fluctuation, this structure will appear. In the formation of crystals (hydrates) the situation is similar the structure that is formed depends, according to the Ostwald rule, on the kinetics of nucleation and not on the relative stability. [Pg.60]

Several kinetic models have appeared to describe phosphorus reactions in soils. Enfield (1978) classified models for estimating phosphorus concentrations in percolate waters derived from soil that had been treated with wastewater into three categories (1) empirical models that are not based on known theory (2) two-phase kinetic models that assume a solution phase and some adsorbed phase and (3) multiphase models, which include solution, adsorbed, or precipitated phases. Mansell and Selim (1981) classified models as shown in Table 9.2. The reader is urged to consult this reference for a complete discussion of the phosphorus kinetic models. For the purpose of this discussion, attention will be given to models that assume reversible phosphorus removal from solution, which can occur simultaneously by equilibrium and nonequilibrium reactions, and mechanistic multiphase models for reactions and transport of phosphorus applied to soils. [Pg.177]

Mathematical models that assume reversible phosphorus removal from solution to occur simultaneously by equilibrium and nonequilibrium reactions Transport models that assume two types of phosphorus sorption sites... [Pg.178]

Equilibrium and nonequilibrium thermodynamics can be combined to give a complete thermodynamic description of a process or process step. Equilibrium thermodynamics allows us to calculate the changes in thermodynamic properties with the change in process conditions. Nonequilibrium thermodynamics allows us to calculate unambiguously the work that is lost associated with the process taking place. It relates this loss to the process s flows and forces driving these flows and identifies the various friction factors as a function of the relationship between flows and forces. [Pg.46]

Miroslav Grmela, Multiscale Equilibrium and Nonequilibrium Thermodynamics in Chemical Engineering... [Pg.237]

The MD technique permits thin films to be investigated under both equilibrium and nonequilibrium conditions. Therefore, in addition to equilibrium properties, such as structure, density, etc., MD predicts the nonequilibrium behavior of thin films, for example, energy relaxation for an ion interacting... [Pg.479]


See other pages where Equilibrium and Nonequilibrium is mentioned: [Pg.733]    [Pg.8]    [Pg.249]    [Pg.434]    [Pg.62]    [Pg.67]    [Pg.29]    [Pg.138]    [Pg.590]    [Pg.681]    [Pg.573]    [Pg.28]    [Pg.88]    [Pg.254]    [Pg.91]   


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