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8 **Adamatzky et al**
Basing on these findings we generalize glider likehood matrices to a set **of abstract, quasi-chemical, reactions as follows:**

A + B1. −→ 2A A + 2B

$$\begin{array}{c}{{A+2B\stackrel{{0.4}}{{\longrightarrow}}2A+B}}\\ {{2A+2B\stackrel{{0.01}}{{\longrightarrow}}3A+B}}\\ {{A+B\stackrel{{1.}}{{\longrightarrow}}2B}}\\ {{2A+B\stackrel{{0.05}}{{\longrightarrow}}A+2B}}\\ {{A\stackrel{{0.054}}{{\longrightarrow}}S}}\end{array}\qquad\qquad\qquad(1)$$

2A + B

0.1

−→ 3A 2A + 2B

3A + B

0.01

−→ 4A A + B1. −→ 2B

A + 2B

0.1

−→ 3B 2A + B

B + S

0.01. −→ 2B A 0.054

B

0.**0015**

−→ S

A typical scenario of how the system (1) behaves in a well-stirred reactor is shown in Fig. 5. We have confirmed in the computational experiments that the reaction scheme developed represents an oscillatory chemical system, where concentration of substrate is significantly higher than concentrations of reactants A and B**. This**
indeed conforms with the nature of spreading localizations and pulsating behavior