The terminal velocity of a solid spherical particle falling through a
stationary fluid mass in the Stoke's law range is proportional to the
(A) Inverse of fluid viscosity
(B) Square of particle size
(C) Difference in the densities of the particle & fluid
(D) All (A), (B) and (C)
stationary fluid mass in the Stoke's law range is proportional to the
(A) Inverse of fluid viscosity
(B) Square of particle size
(C) Difference in the densities of the particle & fluid
(D) All (A), (B) and (C)