Two immiscible, incompressible, viscous fluids having same densities but different viscosities are contained between two infinite horizontal parallel plates, 2 m apart as shown below. The bottom plate is fixed and the upper plate moves to the right with a constant velocity of 3 m/s. With the assumptions of Newtonian fluid, steady and fully developed laminar flow with zero pressure gradient in all directions, the momentum equations simplify to
d2udy2=0
If the dynamic viscosity of the lower fluid μ2, is twice that of the upper fluid μ1, then the velocity at the interface (round off to two decimal places) is
Velocity profile is laminar in both fluids
d2udy2=0
dudy=c1
u=c1y+c2
i.e. we can assume linear velocity profile. If velocity profile is linear shear stress will be constant in gap everywhere i.e. in fluid (1) and fluid (2)
Also at the interface shear stress will be constant.
τ1=τ2
μ2Vih2=μ1(V−Vi)h1
where Vi is velocity at the interface
2μ1Vi1=μ1(3−Vi)1
2Vi=3−Vi
3Vi=3
Vi=1 m/s