2016
DOI: 10.1155/2016/7010645
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Analysis of a Decoupled Time-Stepping Scheme for Evolutionary Micropolar Fluid Flows

Abstract: Micropolar fluid model consists of Navier-Stokes equations and microrotational velocity equations describing the dynamics of flows in which microstructure of fluid is important. In this paper, we propose and analyze a decoupled time-stepping algorithm for the evolutionary micropolar flow. The proposed method requires solving only one uncoupled Navier-Stokes and one microrotation subphysics problem per time step. We derive optimal order error estimates in suitable norms without assuming any stability condition … Show more

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Cited by 5 publications
(7 citation statements)
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“…in [10], [25], [12] and [11]. For the special subcase of micropolar fluids with p = 2 optimal convergence rates for strong solutions are proved in [41], [43]. The convergence of a fully discrete approximation towards a mollified problem for electrorheological fluids with variable exponents is proved in [15].…”
Section: Ad (Iii)mentioning
confidence: 94%
“…in [10], [25], [12] and [11]. For the special subcase of micropolar fluids with p = 2 optimal convergence rates for strong solutions are proved in [41], [43]. The convergence of a fully discrete approximation towards a mollified problem for electrorheological fluids with variable exponents is proved in [15].…”
Section: Ad (Iii)mentioning
confidence: 94%
“…To decouple the velocity components and get a symmetric stiffness matrix for the velocity subproblems, we will treat convection explicitly, extrapolating false(normal∇bold-italicufalse)bold-italicu$$ \left(\nabla \boldsymbol{u}\right)\boldsymbol{u} $$. Moreover, to separate bold-italicσ$$ \boldsymbol{\sigma} $$ and bold-italicu$$ \boldsymbol{u} $$ and even decouple all stress components, we discretize the constitutive equation (6) in time as done by Ravindran, 11 see Section 4.2.…”
Section: Weak Form and Time Discretizationmentioning
confidence: 99%
“…4,5 Therefore, it is of scientific interest to design methods that segregate the calculation of the unknowns. [6][7][8] Such decoupling schemes have lately become more common [9][10][11][12] and are currently the most effective way to enable large-scale viscoelastic flow simulations.…”
Section: Introductionmentioning
confidence: 99%
“…X is the vector consisting of the nodal values of the velocity and pressure. A second-order backward differentiation formula (BDF2) [29,30] is applied for the temporal discretization of Eq. (2.12), as shown in Eq.…”
Section: Discrtizationmentioning
confidence: 99%