“…The condition preceding that, which applies to a rigid porous sphere or to a high-viscosity liquid droplet, excludes tangential motion at the droplet surface; it is selected largely for the simplicity of avoiding the necessity of introducing additional parameters, such as the liquid viscosity, under the realization that much of the earlier work [5][6][7][8] has addressed various influences involving surface motion and that the other parameter-free approximation, (∂u/∂r) = 0, the opposite limit, is less realistic. In the first condition given in Eq.…”