Asymptotic analysis of the steady-state and time-dependent Berman problem

Authors
Citation
Jr. King et Sm. Cox, Asymptotic analysis of the steady-state and time-dependent Berman problem, J ENG MATH, 39(1-4), 2001, pp. 87-130
Citations number
40
Categorie Soggetti
Engineering Mathematics
Journal title
JOURNAL OF ENGINEERING MATHEMATICS
ISSN journal
00220833 → ACNP
Volume
39
Issue
1-4
Year of publication
2001
Pages
87 - 130
Database
ISI
SICI code
0022-0833(200103)39:1-4<87:AAOTSA>2.0.ZU;2-L
Abstract
The Berman problem for two-dimensional flow of a viscous fluid through an i nfinite channel is studied. Fluid motion is driven by uniform suction (or i njection) of fluid through the upper channel wall, and is characterised by a Reynolds number R; the lower wall is impermeable. A similarity solution i n which the streamfunction takes the form psi = -xF(y, t) is examined, wher e x and y are coordinates parallel to and normal to the channel walls, resp ectively. The function F satisfies the Riabouchinsky-Proudman-Johnson equat ion, a partial differential equation in y and t; steady flows satisfy an or dinary differential equation in y. The steady states are computed numerical ly and the asymptotics of these solutions described in the limits of small wall suction or injection, large wall injection and large wall suction, the last of these being given more concisely and more accurately than in previ ous treatments. In the time-dependent problem, the solution appears to be a ttracted to a limit cycle when R >> 1 (large wall suction). This solution h as been computed numerically for epsilon = 1/R down to 0.011, but the struc ture of the solution makes further numerical progress currently infeasible. The limit cycle consists of several phases, some with slow and others with very rapid evolution. During one of the rapid phases, the solution achieve s a large amplitude, and this feature of the solution lies behind the pract ical difficulties encountered in numerical simulations. The profile of the solution is plotted during the various phases and corresponding asymptotic descriptions are given. An exact solution to the Riabouchinsky-Proudman-Joh nson equation covers most of the phases, although separate discussion is re quired of the boundary layers near the two walls and an interior layer near a zero of F. Particular consideration is required when this zero approache s the upper channel wall.