Abstract
A unified approach for assessing and characterizing both the non-equilibrium and
equilibrium states of planar homogeneous flows is analysed within the framework
of single-point turbulence closure equations. The underlying methodology is based
on the replacement of the modelled evolution equation for the Reynolds stress
anisotropy tensor by an equivalent set of three equations for characteristic scalar
invariants or state variables. For stress anisotropy evolution equations which use
modelled pressure–strain rate correlations that are quasi-linear, this equivalence then
leads to an analytic solution for the time evolution of the Reynolds stress anisotropy.
With this analysis, the transient system characteristics can be studied, including the
dependence on initial states, the occurrence of limit-cycle behaviour, and the system
global stability. In the fixed-point asymptotic limit, these results are consistent with
and unify previous equilibrium studies, and provide additional information allowing
the resolution of some questions that could not be answered in the framework of
previous developments. A new result on constraints applicable to the development of
realizable pressure–strain rate models is obtained from a re-examination of the stress
anisotropy invariant map. With the analytic solution for the transient behaviour, some
recent non-equilibrium models, which incorporate relaxation effects, are evaluated in
a variety of homogeneous flows in inertial and non-inertial frames.
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
23 articles.
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