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Reaction quotient

About: Reaction quotient is a research topic. Over the lifetime, 154 publications have been published within this topic receiving 3557 citations.


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TL;DR: The theory of absolute reaction rates for condensed phases was developed in this article, where the rate of a reaction of any order in any phase where the slow process is the passage over an energy barrier consists of the product of a transmission coefficient κ, a frequency kT/h, an equilibrium constant between an activated complex and the reactants and an activity coefficient factor.
Abstract: The theory of absolute reaction rates is developed for condensed phases. The equation for the rate of a reaction of any order in any phase where the slow process is the passage over an energy barrier consists of the product of a transmission coefficient κ, a frequency kT/h, an equilibrium constant between an activated complex and the reactants and an activity coefficient factor. Previous theories of reaction rates such as Bronsted's, the collision theory of Mc C. Lewis, etc., are seen to be special cases of the general theory. A variety of examples are considered.

385 citations

Journal ArticleDOI
TL;DR: In this paper, the authors present a method for the correlation of the experimentalb determined equilibrium constants, which can be used in adjusting the equilibrium data to permit their application to another gas-condensate system of similar composition.
Abstract: Planning of the efficient operation of a gas-condensate re;;ervoir requires a knowledge not only of the gross phase behavior of the system but also of the equilibrium distribution of the various components between the ga5 and condensate phases. This equilibrium distribution can be calculated with appropriate equilibrium constants. In this paper are presente::l equilibrium constants determined experimentally for the oil and gas phases initially present in the same reservoir and for the gas and condensate phases of the gas cap material at a series of pressures below the original reservoir pressure. Also presented is a method for the correlation of the experimentalb determined equilibrium constants. The utility of the correlation is demonstrated further by an example of its use in adjusting the equilibrium data to permit their application to another gas-condensate system of similar composition.

193 citations

Journal ArticleDOI
TL;DR: In this paper, the authors apply simple probabilistic rules of particle interaction and combination to simulate chemical reactions without regard to local concentrations, and the results show that when low mixing limits the reaction probabilities, the reaction rates drop significantly, including the rate of approach to global equilibrium.
Abstract: [1] Chemical reactions may be simulated without regard to local concentrations by applying simple probabilistic rules of particle interaction and combination. The forward reaction A + B→ C is coded by calculating the probability that any A and B particles will occupy the same volume over some time interval. This becomes a convolution of the location densities of the two particles. The backward reaction is a simple exponential decay of C particles into A and B particles. When the mixing of reactants is not a limiting process, the classical thermodynamic reaction rates are reproduced. When low mixing (as by diffusion) limits the reaction probabilities, the reaction rates drop significantly, including the rate of approach to global equilibrium. At long enough times, the law of mass action is reproduced exactly in the mean, with some irreducible deviation in the local equilibrium saturations (the equilibrium constant divided by the mass action expression) away from unity. The saturation variability is not sensitive to numerical parameters but depends strongly on how far from equilibrium the system is initiated. This is simply due to a relative paucity of particles of some species as the reaction moves far to one side or the other.

128 citations


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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
20212
20191
20183
20172
20163
20155