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Exact Formula for Front Velocity

The optimal trajectory is that of a free particle, i.e., the straight line connecting the points X and y e S2q, where is the support of the initial condition  [Pg.168]

Let /(x, denote the minimal distance between the point x and the set Qq. Then, in terms of the phenomenological parameters tq, D, and r, the action functional G(x, t) can be rewritten as [Pg.168]

The effect of diffusion with finite velocity, x r 0, is to decrease the propagation rate corresponding to the RD equation. The last restriction x r 1 arises from the fact that the speed of light c = yjDjx is the maximal velocity of propagation. In other words, front motion with a velocity greater than the speed of light c is impossible. [Pg.168]

In the limiting case, where the relaxation time tq is small compared with the chemical time r i.e., x r -C 1, we can neglect the effect that the velocity of the transport mechanism is finite. [Pg.168]


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