Table 3:

Physical parameters for the horizontal flexible plate inside a flow phantom benchmark (Sec. 4.4). We use a nearly incompressible material unlike the original work that uses $\nu =0.3151$.

Case	${\mathit{u}}^{\max }\left[\frac{\mathrm{cm}}{\mathrm{s}}\right]$	${\mathit{u}}_{\max }^{\mathrm{bottom}}\left[\frac{\mathrm{cm}}{\mathrm{s}}\right]$	${\mathit{f}}_{\mathrm{r}}\left[\frac{1}{\mathrm{s}}\right]$	${\mathit{\mu }}^{\mathrm{f}}\left[\frac{\mathrm{g}}{{\mathrm{cm}}^{\mathrm{s}}}\right]$	${\mathit{\rho }}^{\mathrm{f}}\left[\frac{\mathrm{g}}{{\mathrm{cm}}^3}\right]$	${\mathit{\rho }}_0^{\mathrm{s}}\left[\frac{\mathrm{g}}{{\mathrm{cm}}^3}\right]$	${\mathit{G}}^{\mathrm{s}}\left[\frac{\mathrm{d}\mathrm{y}\mathrm{n}}{{\mathrm{cm}}^2}\right]$	$\mathit{\nu }$
Hydrostatic	(0, 0, 0)	(0, 0, 0)	-	0.1250	1.1633	1.0583	$6.1\times {10}^5$	0.499
Phase I	(0, 0, 61.5)	(0, 0, 63.0)	-	0.1250	1.1633	1.0583	$6.1\times {10}^5$	0.499
Phase II	See Fig. 22(a)	See Fig. 22(a)	1/6	0.1337	1.1640	1.0583	$6.1\times {10}^5$	0.499