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Equilibria mechanical

Using the SFA teclmique, it could be demonstrated that there is an intimate relationship between adliesion hysteresis and friction [28, 29, 77]. Both processes dissipate energy tlnough non-equilibrium mechanisms... [Pg.1743]

Demonstrating that the value of parameter k (evaluated from the kinetics) agrees with K]P (evaluated from an independent method such as spectroscopy) does not constitute proof of the prior-equilibrium mechanism. The values will be the same, regardless. Even if the association complex is immaterial to the chemistry, the value of its formation constant will result from the workup of the kinetic data. To prove this requirement, consider that the system in question does form an appreciable quantity of the ion pair,... [Pg.147]

In the definition of b, Ro is the equilibrium mechanical-to-scalar time-scale ratio found with Sc = 1 and = 0.34 The parameters Cd, Cb, and Cd appear in the SR model for the scalar dissipation rate discussed below. Note that, by definition, xi + Yi + K3 + Kd = 1. ... [Pg.149]

The Rapid Equilibrium Mechanism The following scheme depicts this mechanism ... [Pg.526]

In this rapid equilibrium mechanism, with all binding steps expressed with dissociation constants, then under initial rate conditions (i.e., [P] = 0) the initial rate expres-... [Pg.526]

Rapid Equilibrium Mechanism. If the rate-determining step is the catalytic step and all binding steps can be described by dissociation constants (e.g., K = [E][A]/ [EA]), then, in the absense of products i.e., [P] and [Q] 0), the initial rate equation for the rapid equihbrium Uni Bi mechanism is identical to that of the Uni Uni... [Pg.604]

QUASI-EQUILIBRIUM ASSUMPTION RAPID EQUILIBRIUM MECHANISMS Rapid gel filtration of biomacromolecules, RAPID BUFFER EXCHANGE RAPID MIXING... [Pg.777]

Figure 8.1 Model energy diagrams for non-enzymic reactions (A), enzymic reaction following the rapid equilibrium mechanism (see Table 8.1) (B) and enzymic reaction following Briggs-Haldane kinetics (C). E represents the activation energy of transition and the positive and... Figure 8.1 Model energy diagrams for non-enzymic reactions (A), enzymic reaction following the rapid equilibrium mechanism (see Table 8.1) (B) and enzymic reaction following Briggs-Haldane kinetics (C). E represents the activation energy of transition and the positive and...
The swelling and equilibrium mechanical measurements were the basic methods used for determination of the appearance and magnitude of the phase transition. Swelling of the gels (prepared in the form of cylinders) was characterized by the swelling ratio [11]... [Pg.184]

Solvation—Desolvation Equilibrium. From the observation of migration of plasticizer from plasticized polymers it is dear that plasticizer molecules, or at least some of them, are not bound permanendy to the polymer as in an internally plasticized resin, but rather an exchange—equilibrium mechanism is present. This implies that there is no stoichiometric relationship between polymer and plasticizer levds, although some quasi-stoichiometric relationships appear to exist (3,4). This idea is extended later in the discussion of specific interactions. [Pg.124]

Raman scattering 192 Random mechanism 120 Rapid equilibrium mechanism 120 Rapid mixing techniques 133-136 Rapid quenching techniques 135-136... [Pg.326]

The kinetics and mechanism of the acid-catalysed hydration of dihydro-1,4-dioxin have been reinvestigated. The solvent isotope effect (A h+Ad+ = 2.2) indicates that the reaction proceeds by a rate-determining proton transfer from the catalyst to the substrate68 rather than by a pre-equilibrium mechanism. [Pg.1143]

A typical evolution of equilibrium mechanical properties during reaction is shown in Fig. 6.1. The initial reactive system has a steady shear viscosity that grows with reaction time as the mass-average molar mass, Mw, increases and it reaches to infinity at the gel point. Elastic properties, characterized by nonzero values of the equilibrium modulus, appear beyond the gel point. These quantities describe only either the liquid (pregel) or the solid (postgel) state of the material. Determination of the gel point requires extrapolation of viscosity to infinity or of the equilibrium modulus to zero. [Pg.198]

Replacement of Pext by P, however, does not require complete equilibrium mechanical equilibrium with the surroundings is sufficient. In many slow processes, the system pressure closely tracks the external pressure and can be substituted for it in Eq. (5). The most commonly encountered of these is the constant-pressure process. Because we define our constraints in the surroundings, a constant-pressure process has constant Pext. If the system has a moveable boundary and the system is initially in mechanical equilibrium with the surroundings (P, = Pcxtl), then P will remain equal to Pcxl for the following two processes ... [Pg.59]

A reversible adiabatic expansion of an ideal gas is infinitely slow, so the system maintains internal equilibrium (mechanical, thermal, and material) and equilibrium with its surroundings. Mechanical equilibrium with the surroundings requires that the external pressure be only infinitesimally less than the internal pressure. We can therefore set P = Pext. Thermal and material equilibria with the surroundings are not at issue, because the system is closed with adiabatic walls. A reversible adiabatic expansion is a highly idealized process Nevertheless, it will serve as a cornerstone in our discussions of thermodynamics. Applying the first law to such a process,... [Pg.75]

Weizsacker s theory shared with other theories of element formation the assumption of an equilibrium mechanism. It was the abandonment of this assumption in the 1940s that paved the way for the first successful big-bang model of the universe, proposed by George Gamow and his collaborators in 1948. That the equilibrium hypothesis might not be tenable had been suggested as early as 1931, when the two American chemists Harold Urey and Charles Bradley argued that the relative abundance of terrestrial elements could not be reconciled with the hypothesis, whatever the temperature of the equilibrium mixture. [45]... [Pg.168]

The cooperativity of amplification, switching, and memory in synthetic helical polymers might thus be shared with ideas of a scenario for the biomolec-ular homochirality, autocatalytic mechanism in chiral chemical synthesis, and bifurcation equilibrium mechanisms in crystallization of chiral crystals. Indeed, amplification phenomena in several optical activity and helicity of synthetic polymers in isotropic solution appears to be common and are now established as sergeants and soldiers experiment and majority rules in polymer stereochemistry [17,18]. Any minute chiral forces caused by intramolecular and intermolecular systems can be detectable, when a proper model polymer system is chosen to elucidate the cooperativity of amplification, switching, and memory. [Pg.122]

The relationship between the structure of the disordered heterogeneous material (e.g., composite and porous media) and the effective physical properties (e.g., elastic moduli, thermal expansion coefficient, and failure characteristics) can also be addressed by the concept of the reconstructed porous/multiphase media (Torquato, 2000). For example, it is of great practical interest to understand how spatial variability in the microstructure of composites affects the failure characteristics of heterogeneous materials. The determination of the deformation under the stress of the porous material is important in porous packing of beds, mechanical properties of membranes (where the pressure applied in membrane separations is often large), mechanical properties of foams and gels, etc. Let us restrict our discussion to equilibrium mechanical properties in static deformations, e.g., effective Young s modulus and Poisson s ratio. The calculation of the impact resistance and other dynamic mechanical properties can be addressed by discrete element models (Thornton et al., 1999, 2004). [Pg.157]

Equations (15) and (15a) allow, in theory, the assignment of any reasonable ry value for each step. Thus, for the overall pre-equilibrium mechanism above, the overall substituent effect can be represented as a single linear Y-T correlation with an apparent r value. It is of great importance that equation (14) is applicable also for the simultaneous contribution of more than two substituent effects on a single elementary reaction step. We have already discussed the additivity of the substituent effects on the solvolysis of bis-arylethyl tosylates [27(X = Y)]. [Pg.303]

For H2BP3 and H2BP4, similar dependency studies indicate that another equilibrium mechanism may come into play where one H2BP ligand is coordinated with the species being M(BP )(OH) or M(HBP )(0H)2. ... [Pg.320]


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Equilibrium mechanism

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