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Reactive collision dynamics energy partitioning

Here va and va are the stoichiometric coefficients for the reaction. The formulation is easily extended to treat a set of coupled chemical reactions. Reactive MPC dynamics again consists of free streaming and collisions, which take place at discrete times x. We partition the system into cells in order to carry out the reactive multiparticle collisions. The partition of the multicomponent system into collision cells is shown schematically in Fig. 7. In each cell, independently of the other cells, reactive and nonreactive collisions occur at times x. The nonreactive collisions can be carried out as described earlier for multi-component systems. The reactive collisions occur by birth-death stochastic rules. Such rules can be constructed to conserve mass, momentum, and energy. This is especially useful for coupling reactions to fluid flow. The reactive collision model can also be applied to far-from-equilibrium situations, where certain species are held fixed by constraints. In this case conservation laws... [Pg.109]

When a reaction is studied in the bulk gas phase, the nascent products soon collide with other molecules, energy is transferred upon collision (thus becoming effectively partitioned among all molecules), and the overall reaction exoergicity is finally liberated in its most degraded form, i.e., heat. In macroscopic terms, the reaction is exothermic, i.e., A/f < 0. The microscopic approach of molecular dynamics, however, is concerned with the outcome of the individual reactive collisions. The experimental challenge, as discussed in Section 1.2.5, is to arrest the collisional relaxation of the nascent reaction products and to probe them as they exit from the reactive collision. In this sense, it is customary to speak about the nascent or newborn reaction products. [Pg.6]


See other pages where Reactive collision dynamics energy partitioning is mentioned: [Pg.83]    [Pg.178]    [Pg.96]    [Pg.90]    [Pg.203]    [Pg.103]    [Pg.144]   
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