Table 1:

Parameters for the modified Turek-Hron benchmark (Sec. 4.2).

Case	$\stackrel{\mathit{‾}}{\mathit{u}}\left[\frac{\mathrm{m}}{\mathrm{s}}\right]$	${\mathit{\mu }}^{\mathrm{f}}\left[\frac{\mathrm{kg}}{\mathrm{m}\cdot \mathrm{s}}\right]$	${\mathit{\rho }}^{\mathrm{f}}\left[{10}^3\times \frac{\mathrm{kg}}{{\mathrm{m}}^3}\right]$	${\rho }_0^{\mathrm{s}}\left[{10}^3\times \frac{\mathrm{kg}}{{\mathrm{m}}^3}\right]$	${\mathit{G}}^{\mathrm{s}}\left[{10}^6\times \frac{\mathrm{kg}}{\mathrm{m}\cdot {\mathrm{s}}^2}\right]$	$\mathit{\nu }$
1 (FSI2 of Turek & Hron [62])	1.0	1.0	1.0	10.0	0.5	0.499
2 (FSI3 of Turek & Hron [62])	2.0	1.0	1.0	1.0	2.0	0.499