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The inertial draining of a thin fluid layer between parallel plates with a constant normal force. Part 2. Boundary layer and exact numerical solutions

Published online by Cambridge University Press:  20 April 2006

C. J. Lawrence
Affiliation:
Department of Mechanical Engineering, The City College of The City University of New York, New York, New York 10031
Y. Kuang
Affiliation:
Department of Mechanical Engineering, The City College of The City University of New York, New York, New York 10031
S. Weinbaum
Affiliation:
Department of Mechanical Engineering, The City College of The City University of New York, New York, New York 10031

Abstract

The draining of a fluid layer between rigid plane parallel boundaries under a constant normal force is considered. In Part 1 the effect of fluid inertia was considered in the inviscid and low- but finite-Reynolds-number limits along with the inertia of the moving body; in Part 2, we consider the case of negligible inertia of the moving body. We develop an approximate large-Reynolds-number solution, valid until the boundary layers of the rigid surfaces begin to overlap, and present a new exact solution of the full Navier–Stokes equations for a time-dependent double-axisymmetric stagnation-point flow. These solutions exhibit interesting new features that illustrate the coupling of a time-dependent inviscid core flow with the growth of an unsteady boundary layer started from rest and the effect of Reynolds number on the merging of the boundary layers at large time.

Type
Research Article
Copyright
© 1985 Cambridge University Press

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References

Frössling, N. 1940 Lunds Univ. Arsskr. N. F. Afd. 2, 35, no. 4.
Weinbaum, S., Lawrence, C. J. & Kuang, Y. 1985 J. Fluid Mech. 156, 463.