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Diffusion dynamics coupling

The simple pore structure shown in Figure 2.69 allows the use of some simplified models for mass transfer in the porous medium coupled with chemical reaction kinetics. An overview of corresponding modeling approaches is given in [194]. The reaction-diffusion dynamics inside a pore can be approximated by a one-dimensional equation... [Pg.247]

We have described our most recent efforts to calculate vibrational line shapes for liquid water and its isotopic variants under ambient conditions, as well as to calculate ultrafast observables capable of shedding light on spectral diffusion dynamics, and we have endeavored to interpret line shapes and spectral diffusion in terms of hydrogen bonding in the liquid. Our approach uses conventional classical effective two-body simulation potentials, coupled with more sophisticated quantum chemistry-based techniques for obtaining transition frequencies, transition dipoles and polarizabilities, and intramolecular and intermolecular couplings. In addition, we have used the recently developed time-averaging approximation to calculate Raman and IR line shapes for H20 (which involves... [Pg.95]

As an attempt to connect the first discussion, which was concerned with diffusion-reaction coupling, with Dr. Williams presentation of enzymes as dynamic systems, I wanted to direct attention to a number of specific systems. These are the energy-transducing proteins that couple scalar chemical reactions to vectorial flow processes. For example, I am thinking of active transport (Na-K ATPase), muscular contraction (actomyosin ATPase), and the light-driven proton pump of the well-known purple... [Pg.102]

As a new subject we have considered the effect of the frequency-dependence of the elastic moduli on dynamic light scattering. The resultant nonexponential decay of the time-correlation function seems to be observable ubiquitously if gels are sufficiently compliant. Furthermore, even if the frequency-dependent parts of the moduli are very small, the effect can be important near the spinodal point. The origin of the complex decay is ascribed to the dynamic coupling between the diffusion and the network stress relaxation [76], Further scattering experiments based on the general formula (6.34) should be very informative. [Pg.118]

Deterministic analysis Coupled biochemical systems Reaction kinetics are represented by sets of ordinary differential equations (ODEs). Rates of activation and deactivation of signaling components are dependent on activity of upstream signaling components. Spatially specified systems Reaction kinetics and movement of signaling components are represented by partial differential equations (PDEs). Useful for studies of reaction-diffusion dynamics of signaling components in two or three dimensions. (64-70)... [Pg.2217]

In summary, the major feature of the dynamic model just described is the approximation that solute-solvent and solvent-solvent collisions can be described by hard-sphere interactions. This greatly simplifies the calculations the formal calculations are not difficult to carry out in the more general case, but the algebra is tedious. We want to describe the effects of solute and solvent dynamics on the reactive process as simply as possible, and the model is ideal for this purpose. Specific reactive events among the solute molecules are governed by the interaction potentials that operate among these species. The particular reactive model described here allows us to examine certain features of the coupling between reaction and diffusion dynamics without recourse to heavy calculations. More realistic treatments must of course be handled via the introduction of species operators for the system under consideration. [Pg.101]

Biot and Darcy theory shortcomings have been largely overcome by development of a coupled diffusion-dynamic formalism (de la Cruz et al. 1993, Spanos 2001, Spanos et al. 2(X)3). Porosity is treated as an explicit thermodynamic variable, so that dnumerical model development. Nevertheless, if they are solved subject to the assumption of the incompressibility of a liquid saturant, the existence of a slow wave is predicted. It is called the porosity dilation (PD) wave it is not a strain wav, it is a coupled liquid-solid displacement wave, and it has some interesting properties. [Pg.58]

Abstract We here treat a diffusion problem coupled with water flow in bentonite. The remarkable behavior originates from molecular characteristics of its constituent clay mineral, namely montmorillonite, and we show the behavior based on a unified simulation procedure starting with the molecular dynamic (MD) method and extending the obtained local characteristics to a macroscale behavior by the multiscale homogenization analysis (HA Sanchez-Palencia. 1980). Not only the macroscale effective diffusion property but also the adsorption behavior is well defined based on this method. [Pg.457]

The existence of important coupled diffusion-dynamic processes in porous media is well-documented empirically. The Russian literature contains many descriptions of earthquake-induced altered (generally enhanced) production from reservoirs of modest porosity (i.e. elastic conditions with no potential for compaction). Anecdotal evidence for increased well levels, release of fine-grained material into wells, and enhanced stream flow after earthquakes (Manga et al. 2003) has been reported. Triggering of sympathetic secondary earthquakes at a distance is well-known, and it is also known that the time of propagation for the triggering energy is far slower than the velocity of compressional, shear, or other common waves that are sufficiently conservative to travel hundreds of kilometres. [Pg.513]

Diffusive dynamics described by theTDGL, CDS, and DDFT methods can be used if the kinetic pathway toward eqiulibrium is important. It is assumed that the inertia term is negligible compared to the other forces. The physical reason for this is that the viscous environment of the chain hinders fast accelerations of the maaomolecules. However, the results should be analyzed with caution since diffusive dynamics does not induce a resistance associated with fluid viscosity in the presence of an external driving force, does not take into account drain entanglements, and finally, does not indude hydrodynamic and dastic stress couplings, which are often important. As a result, polymer-spedfic kinetic processes, such as viscodastic phase separation and shear enhancement of concentration fluctuations, cannot be studied. Note also that... [Pg.445]

In contrast to polymer theories, multi-component theories explicitly consider the dynamics of polyions, gegenions and coions and provide a detailed understanding of dynamic coupling phenomena. The theoretical formulation of the multi-component, coupled diffusion problem is quite complex and the mathematical treatment requires gross simplification. Current calculations treat all components as point particles exhibiting different mobilities and charges which obviously represent a rather poor approximation for the polyion structure. [Pg.94]

Spin dynamics studies in poly pyrrole-perchlorate (PPy-CIO4) have been performed by Devreux and Lecavellier [8]. At first, observation of the Overhauser effect proved the existence of a direct dynamic coupling between electronic and nuclear spins [104]. The frequency dependence of the proton relaxation rate is shown in Fig. 5.19. The data can be fitted with Ti" a for temperatures r < 150 K. For T > 150 K, the data deviate from 1-D diffusion behavior. They also cannot be fitted with the law of a pseudo-one-dimensional diffusion [Eq. (10)] with the introduction of a cutoff frequency o>c. Instead, they can be accounted for by taking the spectral density... [Pg.159]

The local dynamics of tire systems considered tluis far has been eitlier steady or oscillatory. However, we may consider reaction-diffusion media where tire local reaction rates give rise to chaotic temporal behaviour of tire sort discussed earlier. Diffusional coupling of such local chaotic elements can lead to new types of spatio-temporal periodic and chaotic states. It is possible to find phase-synchronized states in such systems where tire amplitude varies chaotically from site to site in tire medium whilst a suitably defined phase is synclironized tliroughout tire medium 51. Such phase synclironization may play a role in layered neural networks and perceptive processes in mammals. Somewhat suriDrisingly, even when tire local dynamics is chaotic, tire system may support spiral waves... [Pg.3067]


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See also in sourсe #XX -- [ Pg.57 , Pg.58 , Pg.59 , Pg.60 ]




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Diffusion coupled

Diffusion dynamics

Diffusive coupling

Dynamic coupling

Dynamical coupling

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