In 1851, George Gabriel Stokes derived an expression for the drag force on spherical objects with very small Reynold's numbers (e.g., very small particles) by solving the generally unsolvable Navier-Stokes equations. Stokes' law for drag force is expressed as: ![]() By equating Newton's resistance law and Stokes' law, the drag coefficient can be solved for (applicable when Re<1): ![]() |