Answer: A, B
Expanding gives PVm3−(Pb+RT)Vm2+aVm−ab=0, a cubic in Vm (A true). Below Tc the isotherm has a loop and the cubic has three real roots for pressures between the vapour pressure limits (B true). As Vm→b the term a/Vm2 remains finite and non-zero, so a still matters (C false). Vm−b must stay positive for finite P, so Vm cannot fall below b (D false).