For a small sphere of radius rVolume V = (4/3)πr3density ρs falling through a fluid of density ρw and viscosity ηw weight of sphere = mg = ρsV gupthrust = weight of fluid displaced = ρwVgdrag force from Stokes' law = 6 π r η vAt terminal velocity there is no resultant force therefore:
weight of sphere = upthrust + drag forceρsVg = ρwVg + 6 π r ηw vtermRearranging gives:
| vterm | = | Vg (ρs - ρw ) 6 π r ηw |