TABLE II.

Schnakenberg system reactional flux stoichiometry projections.

Reaction	$J_k^1\left(x_1,x_2,t\right)=s_k^1{J}_k\left(x_1,x_2,t\right)$	$J_k^2\left(x_1,x_2,t\right)=s_k^2{J}_k\left(x_1,x_2,t\right)$
R1	r1ap(x1, x2, t)	0
R2	−r2(x1 + 1)p(x1 + 1, x2, t)	0
R3	0	r3bp(x1, x2, t)
R4	0	−r4(x2 + 1)p(x1, x2 + 1, t)
R5	$r_5\frac{x_1\left(x_1-1\right)x_2}{2}p\left(x_1,x_2,t\right)$	$-r_5\frac{x_1\left(x_1-1\right)x_2}{2}p\left(x_1,x_2,t\right)$
R6	$-r_6\frac{\left(x_1-1\right)x_1\left(x_1+1\right)\left(x_1-2\right)}{6}p\left(x_1+1,x_2-1,t\right)$	$r_6\frac{\left(x_1-1\right)x_1\left(x_1+1\right)\left(x_1-2\right)}{6}p\left(x_1+1,x_2-1,t\right)$