. 2015 Feb 18;11(2):e1004037. doi: 10.1371/journal.pcbi.1004037

Table 3. Steady states of the different models.

notations	steadystate
AC	A(s) = A ₀ e ^−βs/γ
A ^a C	$A (s) = A_{0} (1 - \frac{s}{L} \frac{1}{1 + \frac{γ}{ν L}} (1 - e^{- (ν L + γ) t}))$
A _R C	$A (s) = (A_{0} - A_{R}) e^{- (β + ν) s / γ} + A_{R}$
$A_{R}^{a} C$	$A (s) = (A_{0} - A_{R}) (e^{- B s / L} - e^{- B} \frac{1 - e^{- B s / L}}{M + (1 - e^{- B})}) + A_{R}$

The steady state, $\frac{\partial C}{\partial t} = 0$ , of the different models.