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(a) Assume stationary and purely rotary motion, u = u(r)ˆeθ, and show that u(r

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University of Warsaw Advanced Hydrodynamics

Faculty of Physics Selected Topics in Fluid Mechanics

Summer Semester 2019/20

Exercise Sheet 1

Exact solutions of simplified Navier-Stokes equations

1. A semi-infinite body of fluid with constant density ρ and viscosity µ is bounded by a flat plate. The plate is in the xy plane. The system is initially at rest. At time t = 0, the plate is suddenly set in motion in the x-direction with a constant velocity U .

(a) Assume the flow has the form u = [u(z, t), 0, 0] with u = U f (η), η = z

√4νt, where ν = µ/ρ.

(b) Evaluate the vorticity ω = ∇ × u and show that it is exponentially small beyond a distance of order√

νt from the boundary (flat plate).

2. A viscous fluid of viscosity µ occupies the gap between two circular cylinders, the inner having radius R1 and angular velocity Ω1, the other one having radius R2 and angular velocity Ω2.

(a) Assume stationary and purely rotary motion, u = u(r)ˆeθ, and show that u(r) = Ar + B

r, where

A = Ω2R22− Ω1R21

R22− R22 , B = (Ω1− Ω2)R21R22 R22− R21 .

(b) Determine the moment M1 of the frictional forces acting on the inner cylinder cylinder:

M1 = −4πµ(Ω1− Ω2)R21R22 R22− R21 .

How can this flow be used to determine the viscosity of the fluid?

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