Paper 2, Section II, A

Fluid Dynamics II
Part II, 2010

What is lubrication theory? Explain the assumptions that go into the theory.

Viscous fluid with dynamic viscosity μ\mu and density ρ\rho is contained between two flat plates, which approach each other at uniform speed VV. The first is fixed at y=0,L<x<Ly=0,-L<x<L. The second has its ends at (L,h0ΔhVt),(L,h0+ΔhVt)\left(-L, h_{0}-\Delta h-V t\right),\left(L, h_{0}+\Delta h-V t\right), where Δhh0L\Delta h \sim h_{0} \ll L. There is no flow in the zz direction, and all variation in zz may be neglected. There is no applied pressure gradient in the xx direction.

Assuming that VV is so small that lubrication theory applies, derive an expression for the horizontal volume flux Q(x)Q(x) at t=0t=0, in terms of the pressure gradient. Show that mass conservation implies that dQ/dx=Vd Q / d x=V, so that Q(L)Q(L)=2VLQ(L)-Q(-L)=2 V L. Derive another relation between Q(L)Q(L) and Q(L)Q(-L) by setting the pressures at x=±Lx=\pm L to be equal, and hence show that

Q(±L)=VL(Δhh0±1)Q(\pm L)=V L\left(\frac{\Delta h}{h_{0}} \pm 1\right)

Show that lubrication theory applies if Vμ/h0ρV \ll \mu / h_{0} \rho.