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Coefficient phenomenological

Here A, C and E are phenomenological coefficients in the Landau expansion in tenns of the smectic ordering ... [Pg.2559]

Irreversible thermodynamics has also been used sometimes to explain reverse osmosis [14,15]. If it can be assumed that the thermodynamic forces responsible for reverse osmosis are sufficiently small, then a linear relationship will exist between the forces and the fluxes in the system, with the coefficients of proportionality then referred to as the phenomenological coefficients. These coefficients are generally notoriously difficult to obtain, although some progress has been made recently using approaches such as cell models [15]. [Pg.780]

According to the Onsager assumption, the square matrix of the phenomenological coefficients... [Pg.91]

The corresponding phenomenological coefficient is then given by the relationship... [Pg.96]

Some of the elements of thermodynamics of irreversible processes were described in Sections 2.1 and 2.3. Consider the system represented by n fluxes of thermodynamic quantities and n driving forces it follows from Eqs (2.1.3) and (2.1.4) that n(n +1) independent experiments are needed for determination of all phenomenological coefficients (e.g. by gradual elimination of all the driving forces except one, by gradual elimination of all the fluxes except one, etc.). Suitable selection of the driving forces restricted by relationship (2.3.4) leads to considerable simplification in the determination of the phenomenological coefficients and thus to a complete description of the transport process. [Pg.431]

Of the remaining three cross phenomenological coefficients, Lwn can be found from the volume flux during dialysis (Ap =0, A = 0, because electrodes Wx and W2 are short-circuited) ... [Pg.433]

O Kedem, A Katchalsky. A physical interpretation of the phenomenological coefficients of membrane permeability. J Gen Physiol 45 143-179, 1961. [Pg.38]

The coupled processes described by Eqs. (8), (14), (17), and (22) can be added in (20) as parallel solute transport pathways across the membrane. The phenomenological coefficients (Ly) describe the membrane permeability by these pathways [potential-dependent, Eq. (8) via membrane lipid partition and diffusion, Eq. (14) carrier-mediated, Eq. (17) and convectively coupled, Eq. (22)]. These pathways define parallel resistances through the intestinal barrier in series with precellular resistances to solute transport. [Pg.191]

The transport of both solute and solvent can be described by an alternative approach that is based on the laws of irreversible thermodynamics. The fundamental concepts and equations for biological systems were described by Kedem and Katchalsky [6] and those for artificial membranes by Ginsburg and Katchal-sky [7], In this approach the transport process is defined in terms of three phenomenological coefficients, namely, the filtration coefficient LP, the reflection coefficient o, and the solute permeability coefficient to. [Pg.426]

Table 1 Phenomenological Coefficients and Partition Coefficients for Urea, Glucose, and Sucrose in Various Membranes... [Pg.428]

As a matter of fact, one may think of a multiscale approach coupling a macroscale simulation (preferably, a LES) of the whole vessel to meso or microscale simulations (DNS) of local processes. A rather simple, off-line way of doing this is to incorporate the effect of microscale phenomena into the full-scale simulation of the vessel by means of phenomenological coefficients derived from microscale simulations. Kandhai et al. (2003) demonstrated the power of this approach by deriving the functional dependence of the singleparticle drag force in a swarm of particles on volume fraction by means of DNS of the fluid flow through disordered arrays of spheres in a periodic box this functional dependence now can be used in full-scale simulations of any flow device. [Pg.157]

A parabolic rate law will also be obtained if part or even all, of the diffusion through the product layer is by grain boundary diffusion rather than diffusion through the volume of each grain. The volume diffusion coefficient is quite simply defined as the phenomenological coefficient in Fick s laws. The grain boundary diffusion must be described by a product, DbS, where S is the grain... [Pg.251]

R D - research and development AG, AH, AS, q, w - classical thermodynamic significance J, X, L - fluxes, forces and phenomenological coefficients of irreversible thermodynamics ... [Pg.294]

For inter diffusion between same-valence ions (ionic exchange) in an aqueous solution, or a melt, or a solid solution such as olivine (Fe +, Mg +)2Si04, an equation similar to Equation 3-135c has been derived from the Nemst-Planck equations first by Helfferich and Plesset (1958) and then with refinement by Barter et al. (1963) with the assumption that (i) the matrix (or solvent) concentration does not vary and (ii) cross-coefficient Lab (phenomenological coefficient in Equation 3-96a) is negligible, which is similar to the activity-based effective binary diffusion treatment. The equation takes the following form ... [Pg.306]

We shall not, however, assume that the phenomenological coefficients are independent of frequency. To provide some insight into this assertion, we must digress briefly. Consider, for example, the susceptibility. The polarization P is... [Pg.13]

Thus, the perhaps unfamiliar constitutive relations (2.23)-(2.25) yield familiar results when the fields are time harmonic moreover, because of (2.26) and (2.27), physical meaning can now be attached to the phenomenological coefficients even for arbitrarily time-dependent fields. [Pg.18]


See other pages where Coefficient phenomenological is mentioned: [Pg.30]    [Pg.251]    [Pg.811]    [Pg.196]    [Pg.275]    [Pg.91]    [Pg.97]    [Pg.98]    [Pg.431]    [Pg.433]    [Pg.436]    [Pg.485]    [Pg.351]    [Pg.187]    [Pg.233]    [Pg.30]    [Pg.8]    [Pg.348]    [Pg.201]    [Pg.255]    [Pg.256]    [Pg.562]    [Pg.563]    [Pg.13]    [Pg.15]    [Pg.15]    [Pg.15]    [Pg.17]    [Pg.18]    [Pg.21]    [Pg.185]   
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A comparison of the phenomenological diffusion coefficients

Frequency-Dependent Phenomenological Coefficients

Friction coefficient phenomenological

Linear phenomenological coefficients

Multicomponent phenomenological coefficients

Onsager phenomenological coefficients

Phenomenological

Phenomenological Coefficients and Kinetic Theory

Phenomenological coefficients activation energies

Phenomenological coefficients relations

Phenomenological diffusion coefficients

Phenomenological flow coefficients

Phenomenological stoichiometric coefficient

Phenomenological transport coefficients

Phenomenological transport coefficients reciprocal relations

Phenomenology/phenomenologic

Reduced phenomenological coefficients

Relationships between the conductance and resistance phenomenological coefficients

Thermodynamic phenomenological coefficient

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