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The wave stops as soon as the sphere contains only a and all of b has been
consumed. If we identify the concentration of a with [ a ]
u and nor-
malize the total concentration to 1 everywhere, mass action kinetics gives
the reaction term f ( u )
=
u ). Inserting this into Eq. (35) yields a
nonlinear PDE. Such systems can exhibit bifurcations (cf. Sec. 2), which
is the case in the present example as Fisher waves only exist for speeds
s
=
ku (1
s *, no moving front exists.
For the stochastic simulations, we denote by X p the total number
of molecules contained in particle p , and define an analog to
Avogadro's number, viz. M , the number of molecules per unit mass.
Gillespie introduced the product h c as the expected number of reac-
tions per unit time. For the binary reaction here, it is h =
s *
=
2
f
(0)
=
2
k. 136,137 For s
<
X p X p . The
rate constant k and the reaction parameter c are related as k
MVc . 61
We interpret c as the probability that two molecules of species a and b
react, provided they meet in space and time. This probability is inde-
pendent of the particle volume. c
Figure 10(a) shows the total mass, integrated over the surface of the
sphere, of a and b as they evolve in time. The front position is also shown,
defined as the location where [ a ]
=
0.5. As long as reactions occur,
[ a ] and [ b ] change and the wave travels at a more or less constant speed
s , given by the slope of the dashed curve in Fig. 10(a). If the dimension-
less front speed is plotted against the dimensionless reaction parameter,
the curves for different diffusion constants D collapse as shown in Fig. 10(b).
We also observe that the theoretical scaling 136,137 is well approximated,
particularly if the reaction is significantly faster than the diffusion.
=
[ b ]
=
9. Conclusions
Spatiotemporal models and numerical computer simulations are of rap-
idly growing importance in almost all areas of biology. Besides computa-
tional data analysis, including image processing, gene and protein sequence
analysis, clustering, and machine learning, modeling and simulation are
c The probability of an encounter to occur, on the other hand, does depend on the
particle volume. This is, however, already accounted for in h, as the number of mol-
ecules X p per particle is an extensive property.
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