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Response Experiments for Reaction-Diffusion Systems

In chemical kinetics a marked species can be a molecule containing a radioactive isotope and we neglect the kinetic isotope effect. In fluid mechanics a marked species can be a colored fluid for which the hydrodynamic properties (density, viscosity, diffusion coefficients) are the same as the ones of the main fluid. In population genetics a marked species can be an individual carrying a neutral mutation, and for which the main functions describing the vital statistics (natality and mortality functions, diffusion coefficients) are the same as in the case of a nonmutant individual. In the following we denote by (r, t) and p (r,t), u = 1,2. the concentrations of the not marked and marked species, respectively, and by p (r, r) = Pj r,t)+p r,t),u = 1,2. the total concentrations of the species. [Pg.198]

At the beginning of the experiment the system contains only not marked species. The system need not be but may be in a stationary state. The experiment consists in [Pg.198]

We assume the existence of generalized neutrality conditions [8,11], in the form of scaling laws, which connect the kinetic and transport laws for the whole system to the corresponding laws for the marked and not marked species, respectively  [Pg.198]

Equations (12.132) express the fact that the marked and not marked species contribute equally to the transport process. We assume that the output fluxes, J [p (r, t)], are expressed by kinetic laws, and thus they also obey a scaling condition similar to eq. (12.132)  [Pg.198]

It is possible to show that the susceptibility function has a physical interpretation, similar to the one existing for homogeneous systems. It is related to the probability density [Pg.199]


See other pages where Response Experiments for Reaction-Diffusion Systems is mentioned: [Pg.197]   


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