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Expression theory

Expression is the separation of a liquid from a two-phase solid-liquid system by compression, due to movanent of the retaining wall rather than the pumping of the solid-liquid system into a fixed chamber as in filtration. In filtration, the original mixture is sufficiently fluid to be pumpable in expression, the material may appear either entirely sani-solid or slurry. Based on an expression theory [6,7], the time for expression is also proportional to the square of cake thickness. [Pg.1185]

Shirato M., Murase T. and Iwata M., 1986. Deliquoring by expression - theory and practice, in Progress in Filtration and Separation 4 , Ed. R.J. Wakeman, Elsevier, Amsterdam. [Pg.396]

The classic theory due to van der Waals provides an important phenomenological link between the structure of an interface and its interfacial tension [50-52]. The expression... [Pg.61]

The acconunodation coefficient for Kr on a carbon filament is determined experimentally as follows. The electrically heated filament at temperature 72 is stretched down the center of a cylindrical cell containing Kr gas at 7. Gas molecules hitting the filament cool it, and to maintain its temperature a resistance heating of Q cal sec cm is needed. Derive from simple gas kinetic theory the expression... [Pg.672]

The miderstanding of the quantum mechanics of atoms was pioneered by Bohr, in his theory of the hydrogen atom. This combined the classical ideas on planetary motion—applicable to the atom because of the fomial similarity of tlie gravitational potential to tlie Coulomb potential between an electron and nucleus—with the quantum ideas that had recently been introduced by Planck and Einstein. This led eventually to the fomial theory of quaiitum mechanics, first discovered by Heisenberg, and most conveniently expressed by Schrodinger in the wave equation that bears his name. [Pg.54]

If the long-range mteraction between a pair of molecules is treated by quantum mechanical perturbation theory, then the electrostatic interactions considered in section Al.5.2.3 arise in first order, whereas induction and dispersion effects appear in second order. The multipole expansion of the induction energy in its fill generality [7, 28] is quite complex. Here we consider only explicit expressions for individual temis in the... [Pg.190]

The situation for electrolyte solutions is more complex theory confimis the limiting expressions (originally from Debye-Htickel theory), but, because of the long-range interactions, the resulting equations are non-analytic rather than simple power series.) It is evident that electrolyte solutions are ideally dilute only at extremely low concentrations. Further details about these activity coefficients will be found in other articles. [Pg.361]

This is Kirkwood s expression for the chemical potential. To use it, one needs the pair correlation fimction as a fimction of the coupling parameter A as well as its spatial dependence. For instance, if A is the charge on a selected ion in an electrolyte, the excess chemical potential follows from a theory that provides the dependence of g(i 2, A) on the charge and the distance r 2- This method of calculating the chemical potential is known as the Gimtelburg charging process, after Guntelburg who applied it to electrolytes. [Pg.474]

McMillan-Mayer theory of solutions [1,2], which essentially seeks to partition the interaction potential into tln-ee parts that due to the interaction between the solvent molecules themselves, that due to die interaction between the solvent and the solute and that due to the interaction between the solute molecules dispersed within the solvent. The main difference from the dilute fluid results presented above is that the potential energy u(r.p is replaced by the potential of mean force W(rp for two particles and, for particles of solute in the solvent, by the expression... [Pg.564]

At concentrations greater than 0.001 mol kg equation A2.4.61 becomes progressively less and less accurate, particularly for imsynnnetrical electrolytes. It is also clear, from table A2.4.3. that even the properties of electrolytes of tire same charge type are no longer independent of the chemical identity of tlie electrolyte itself, and our neglect of the factor in the derivation of A2.4.61 is also not valid. As indicated above, a partial improvement in the DH theory may be made by including the effect of finite size of the central ion alone. This leads to the expression... [Pg.580]

Exponents derived from the analytie theories are frequently ealled elassieaT as distinet from modem or nonelassieaT although this has nothing to do with elassieaT versus quantum meehanies or elassieaT versus statistieaT thennodynamies. The important themiodynamie exponents are defined here, and their elassieal values noted the values of the more general nonelassieal exponents, detemiined from experiment and theory, will appear in later seetions. The equations are expressed in redueed units in order to eompare the amplitude eoeflfieients in subsequent seetions. [Pg.638]

Linear response theory is an example of a microscopic approach to the foundations of non-equilibrium thennodynamics. It requires knowledge of tire Hamiltonian for the underlying microscopic description. In principle, it produces explicit fomuilae for the relaxation parameters that make up the Onsager coefficients. In reality, these expressions are extremely difficult to evaluate and approximation methods are necessary. Nevertheless, they provide a deeper insight into the physics. [Pg.708]

If Other fall-off broadening factors arising m unimolecular rate theory can be neglected, the overall dependence of the rate coefficient on pressure or, equivalently, solvent density may be represented by the expression [1, 2]... [Pg.848]

This ensures the correct connection between the one-dimensional Kramers model in the regime of large friction and multidimensional imimolecular rate theory in that of low friction, where Kramers model is known to be incorrect as it is restricted to the energy diflfiision limit. For low damping, equation (A3.6.29) reduces to the Lindemann-Flinshelwood expression, while in the case of very large damping, it attains the Smoluchowski limit... [Pg.849]

As a result of several complementary theoretical efforts, primarily the path integral centroid perspective [33, 34 and 35], the periodic orbit [36] or instanton [37] approach and the above crossover quantum activated rate theory [38], one possible candidate for a unifying perspective on QTST has emerged [39] from the ideas from [39, 40, 4T and 42]. In this theory, the QTST expression for the forward rate constant is expressed as [39]... [Pg.891]

See, for example, Poliak E 1986 Theory of activated rate processes a new derivation of Kramers expression J. Chem. Phys. 85 865... [Pg.897]

Voth G A 1990 Analytic expression for the transmission coefficient in quantum mechanical transition state theory Chem. Phys. Lett. 170 289... [Pg.897]

A completely difierent approach to scattering involves writing down an expression that can be used to obtain S directly from the wavefunction, and which is stationary with respect to small errors in die waveftmction. In this case one can obtain the scattering matrix element by variational theory. A recent review of this topic has been given by Miller [32]. There are many different expressions that give S as a ftmctional of the wavefunction and, therefore, there are many different variational theories. This section describes the Kohn variational theory, which has proven particularly useftil in many applications in chemical reaction dynamics. To keep the derivation as simple as possible, we restrict our consideration to potentials of die type plotted in figure A3.11.1(c) where the waveftmcfton vanishes in the limit of v -oo, and where the Smatrix is a scalar property so we can drop the matrix notation. [Pg.968]

An important development in the quantum theory of scattering in the last 20 years has been the development of exact expressions which directly detennine either thennal rate constant lc(T) from the... [Pg.993]

The above describes the fundamental assumption of RRKM theory regarding the intramolecular dynamics of A. The RRKM expression for k E) is now derived. [Pg.1011]

In polymer solutions or blends, one of the most important thennodynamic parameters that can be calculated from the (neutron) scattering data is the enthalpic interaction parameter x between the components. Based on the Flory-Huggins theory [4T, 42], the scattering intensity from a polymer in a solution can be expressed as... [Pg.1416]


See other pages where Expression theory is mentioned: [Pg.144]    [Pg.1185]    [Pg.1218]    [Pg.144]    [Pg.1185]    [Pg.1218]    [Pg.31]    [Pg.208]    [Pg.136]    [Pg.465]    [Pg.113]    [Pg.172]    [Pg.706]    [Pg.714]    [Pg.32]    [Pg.66]    [Pg.469]    [Pg.475]    [Pg.571]    [Pg.595]    [Pg.664]    [Pg.666]    [Pg.687]    [Pg.754]    [Pg.755]    [Pg.781]    [Pg.783]    [Pg.885]    [Pg.891]    [Pg.999]    [Pg.1460]    [Pg.1502]   


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