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Barrier crossings starting equations

Kramers solution of the barrier crossing problem [45] is discussed at length in chapter A3.8 dealing with condensed-phase reaction dynamics. As the starting point to derive its simplest version one may use the Langevin equation, a stochastic differential equation for the time evolution of a slow variable, the reaction coordinate r, subject to a rapidly statistically fluctuating force F caused by microscopic solute-solvent interactions under the influence of an external force field generated by the PES F for the reaction... [Pg.848]

The starting point of a non-Markovian theory of barrier crossing is the generalized Langevin equation (cf. Eqs (8.61) and (8.62))... [Pg.516]

To solve the time-dependent Schrodinger equation with the boundary condition for (jc, r = 0) in the form of a wave packet. The wave packet may be directed into the entrance channel toward the reaction barrier (from various starting conditions). In the barrier range, the wave packet splits into a wave packet crossing the barrier and a wave packet reflected from the barrier (cf., p. 180). [Pg.892]

Starting with the molecular movement, the rate of a molecular process crossing an activation energy barrier can be related to temperature through the Arrhenius equation. [Pg.51]


See other pages where Barrier crossings starting equations is mentioned: [Pg.199]    [Pg.214]    [Pg.1126]    [Pg.1126]    [Pg.1126]    [Pg.476]    [Pg.451]   
See also in sourсe #XX -- [ Pg.474 , Pg.475 ]

See also in sourсe #XX -- [ Pg.474 , Pg.475 ]




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Barrier crossings

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