Existence and approximation of a (regularized) Oldroyd-B model
John W. Barrett, Sebastien Boyaval

TL;DR
This paper develops finite element schemes for the Oldroyd-B model of dilute polymeric fluids, proving existence of global weak solutions and extending previous results by removing constraints on time steps and positivity conditions.
Contribution
It introduces new finite element approximations that satisfy energy bounds without time step restrictions and proves the existence of global weak solutions for regularized Oldroyd-B models.
Findings
Finite element schemes satisfy free energy bounds.
Existence of global-in-time weak solutions is established.
Extensions remove previous constraints on time step and positivity.
Abstract
Two finite element approximations of the Oldroyd-B model for dilute polymeric fluids are considered, in bounded 2- and 3-dimensional domains, under no flow boundary conditions. The pressure and the symmetric conformation tensor are aproximated by either (a) piecewise constants or (b) continuous piecewise linears, the velocity by (a) continuous piecewise quadratics or a reduced version with linear tangential component on each edge, and (b) by continuous piecewise quadratics or the mini-element. Both schemes (a) and (b) satisfy a free energy bound, which involves the logarithm of the conformation tensor, without any constraint on the time step for the backward Euler type time discretization. This extends the results of [Boyaval et al. M2AN 43 (2009) 523--561], where a piecewise constant approximation of the conformation tensor was necessary to treat the advection term in the stress…
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