A sphere or radius $a$ moves with uniform speed $v$ through a fluid of viscosity $\eta$. The frictional retarding force $f$ acting on the sphere must then be some function of $a, v$, and $\eta$. (It cannot depend on the density of the fluid since the inertial properties of the fluid are of no consequence in the absence of accelerstion.) Use arguments of dimensional analyeis to find (except for a constant of proportionality) the dependence of the frictional force $f$ on these parametars. Show that the result agrees with Stokes's law in (15-6-2).