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Associated equilibrium states

In what sense might a thermodynamic variable be considered as a vector, or the associated equilibrium state as a geometrical space of vectors ... [Pg.331]

Even when a sample is not in equilibrium (and hence some process of adjustment toward equilibrium is running, such as diffusion of material from one point to another) for each component at a point, an associated equilibrium state can be identified. Then one can say that the component s behavior will be very much as if it had the chemical potential it would have if it were in the associated equilibrium state. For example, material will tend to migrate from a site where the associated equilibrium potential is high to a site where the associated equilibrium potential is lower this is a reliable... [Pg.6]

Summary. For any small portion of the graded bar, we can imagine a portion of the same size and overall R-content, in which R is homogeneous instead of being graded. The imagined sample is in equilibrium its state is the associated equilibrium state that is associated with the disequilibrium portion we decided to consider. [Pg.32]

Does every small portion of a nonequilibrium system have an associated equilibrium state And if so, how do we discover it According to de Groot s prescription (1951, p. 11) we imagine the nonequilibrium portion to be suddenly isolated from its surroundings in all respects and allowed to grind to a halt—all gradients flattened and all rates of processes gone to zero the state so reached is the associated equilibrium state for the portion of nonequilibrium system considered. [Pg.33]

The idea of an associated equilibrium state is thus quite general it is a very powerful concept that can be used more accurately and more confidently than the concept of local equilibrium. Confidence comes fi om two sources first we can see that the real nonequilibrium state and the imagined equilibrium state are closely similar, and second, we can bring the exact differences to light—even, in some circumstances, express them quantitatively and demonstrate their smallness. It is the second aspect that brings confidence, and allows us to use associated equilibrium states to define potentials and predict material responses, even in situations where the exact magnitude of the small differences cannot actually be worked out in numbers. [Pg.33]

Comparison of the two situations. The sequence of compressive stress magnitudes normal to the slot that affect a wafer as it slides sideways is exactly the same in the two situations—the specifications were devised to make this so. Then if the process of assigning an associated equilibrium state to a plane is valid, we have to assign the same sequence of associated equilibrium states to successive points, regardless of which path we are following. Then further, if the gradient down a sequence of associated... [Pg.87]

The populations, /Q, appear on the diagonal as expected, but note that there are no off-diagonal elements—no coherences this is reasonable since we expect the equilibrium state to be time-independent, and we have associated the coherences with time. [Pg.233]

The solution to this fourth-order partial differential equation and associated homogeneous boundary conditions is just as simple as the analogous deflection problem in Section 5.3.1. The boundary conditions are satisfied by the variation in lateral displacement (for plates, 5w actually is the physical buckle displacement because w = 0 in the membrane prebuckling state however, 5u and 8v are variations from a nontrivial equilibrium state. Hence, we retain the more rigorous variational notation consistently) ... [Pg.304]

Because membranes components participate in nearly every cell activity their structures are also dynamic and far from the equilibrium states that are most readily understood in biophysical terms. Newly synthesized bilayer lipids are initially associated with endoplasmic reticulum (Ch.3) whereas phospholipids initially insert into the cytoplasmic leaflet while cholesterol and sphingolipids insert into the luminal endoplasmic reticulum (ER) leaflet. Glycosylation of ceramides occurs as they transit the Golgi compartments, forming cerebrosides and gangliosides in the luminal leaflet. Thus, unlike model systems, the leaflets of ER membranes are asymmetric by virtue of their mode of biosynthesis. [Pg.26]

We consider the reactive solute system with coordinate x and its associated mass p, in the neighborhood of the barrier top, located at x=xi=0, and in the presence of the solvent. We characterize the latter by the single coordinate. v, with an associated mass ps. If the solvent were equilibrated to x in the barrier passage, so that there is equilibrium solvation and s = seq(x), the potential for x is just -1/2 pcc X2, where (, , is the equilibrium barrier frequency [cf. (2.2)]. To this potential we add a locally harmonic restoring potential for the solvent coordinate to account for deviations from this equilibrium state of affairs ... [Pg.238]

A pressure perturbation results in the shifting of the equilibrium the return of the system to the original equilibrium state (i.e., the relaxation) is related to the rates of all elementary reaction steps. The relaxation time constant associated with the relaxation can be used to evaluate the mechanism of the reaction. During the shift in equilibrium (due to pressure-jump and relaxation) the composition of the solution changes and this change can be monitored, for example by conductivity. A description of the pressure-jump apparatus with conductivity detection and the method of data evaluation is given by Hayes and Leckie (1986). [Pg.127]

Intuitively we might associate the low shear limit with the order-disorder transition at literature data for the packing fraction in this limit is more widely scattered. We must remember that the approach to equilibrium in these systems can take a while to progress. So it is feasible that some systems have been measured away from the equilibrium state when the samples have been transferred and placed in the measuring geometry on an instrument. We could... [Pg.230]

Undoubtedly one of the most used LFER in transition metal chemistry involves electron transfer rate constants and associated equilibrium constants in outer sphere redox reactions. These are an unusual class of reactions in chemistry since bonds are only stretched or contracted in the formation of the activated complex. They therefore lend themselves well to theoretical treatment. We shall have more to say about these reactions in Chap. 5. It is sufficient here to state the simple form of the LFER with an example (Fig. 2.8). For the reaction... [Pg.97]

In order to better understand the detailed dynamics of this system, an investigation of the unimolecular dissociation of the proton-bound methoxide dimer was undertaken. The data are readily obtained from high-pressure mass spectrometric determinations of the temperature dependence of the association equilibrium constant, coupled with measurements of the temperature dependence of the bimolecular rate constant for formation of the association adduct. These latter measurements have been shown previously to be an excellent method for elucidating the details of potential energy surfaces that have intermediate barriers near the energy of separated reactants. The interpretation of the bimolecular rate data in terms of reaction scheme (3) is most revealing. Application of the steady-state approximation to the chemically activated intermediate, [(CH30)2lT"], shows that. [Pg.48]


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See also in sourсe #XX -- [ Pg.6 , Pg.30 , Pg.31 , Pg.32 , Pg.33 , Pg.34 , Pg.66 , Pg.67 , Pg.68 , Pg.75 , Pg.87 ]




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