2.II.36E

Fluid Dynamics II
Part II, 2005

A volume VV of very viscous fluid of density ρ\rho and dynamic viscosity μ\mu is released at the origin on a rigid horizontal boundary at time t=0t=0. Using lubrication theory, determine the velocity profile in the gravity current once it has spread sufficiently that the axisymmetric thickness h(r,t)h(r, t) of the current is much less than the radius R(t)R(t) of the front.

Derive the differential equation

ht=βrr(rh3hr)\frac{\partial h}{\partial t}=\frac{\beta}{r} \frac{\partial}{\partial r}\left(r h^{3} \frac{\partial h}{\partial r}\right)

where β\beta is to be determined.

Write down the other equations that are needed to determine the appropriate similarity solution for this problem.

Determine the similarity solution and calculate R(t)R(t).