Table 5.

Summary of the validation cases under constant shear rates $\left(I_0{U}_3{r}_1{\chi }_1\right.$ and $\left.I_0{U}_4{r}_3{\chi }_1\right)$, and stepwise oscillatory flows ($I_s{\psi }_1{r}_1{\chi }_2$, $I_s{\psi }_2{r}_1{\chi }_2$, $I_s{\psi }_3{r}_1{\chi }_2$ and $I_s{\psi }_4{r}_1{\chi }_3$, $I_s{\psi }_5{r}_1{\chi }_3$, $I_s{\psi }_6{r}_1{\chi }_3$). The stepwise oscillatory flows with the forward $\left({\psi }_f\right)$, backward $\left({\psi }_b\right)$ velocities and the forward Capillary number are defined in section 2.8.2. The maximum shear rate $({\stackrel{-}{\dot{\gamma }}}_f)$ and the maximum Reynolds number $\left(R{e}_f\right)$ are defined in section 2.8.1. The definition of the RBC’s radial shift $r$ is shown in Figure 2b.

Case	Inflow	${\psi }_f(mm/s)$	${\psi }_b(mm/s)$	${\stackrel{-}{\dot{\gamma }}}_f\left(s^{-1}\right)$	$r(\mu m)$	$R{e}_f$	$C{a}^f$
$I_0{U}_3{r}_1{\chi }_1$	$I_0$	2	-	200	0	1.34 × 10−2	0.49
$I_0{U}_4{r}_3{\chi }_1$	$I_0$	6	-	600	0.7	4 × 10−2	1.47
$I_s{\psi }_1{r}_1{\chi }_2$	$I_s$	1.05	−0.27	66	0	7 × 10−3	0.1
$I_s{\psi }_1{r}_1{\chi }_2$	$I_s$	1.58	−0.39	98	0	1.05 × 10−2	0.15
$I_s{\psi }_2{r}_1{\chi }_2$	$I_s$	2.1	−0.53	132	0	1.4 × 10−2	0.2
$I_s{\psi }_4{r}_1{\chi }_3$	$I_s$	1.9	−0.48	119	0	1.27 × 10−2	0.1
$I_s{\psi }_5{r}_1{\chi }_3$	$I_s$	2.8	−0.7	175	0	1.87 × 10−2	0.15
$I_s{\psi }_6{r}_1{\chi }_3$	$I_s$	3.7	−0.93	232	0	2.47 × 10−2	0.2