Numerical analysis of the Oseen-type Peterlin viscoelastic model by the stabilized Lagrange-Galerkin method, Part II: A linear scheme
arXiv:1603.01074 · doi:10.1051/m2an/2017032
Abstract
This is the second part of our error analysis of the stabilized Lagrange-Galerkin scheme applied to the Oseen-type Peterlin viscoelastic model. Our scheme is a combination of the method of characteristics and Brezzi-Pitkäranta's stabilization method for the conforming linear elements, which leads to an efficient computation with a small number of degrees of freedom especially in three space dimensions. In this paper, Part II, we apply a semi-implicit time discretization which yields the linear scheme. We concentrate on the diffusive viscoelastic model, i.e. in the constitutive equation for time evolution of the conformation tensor a diffusive effect is included. Under mild stability conditions we obtain error estimates with the optimal convergence order for the velocity, pressure and conformation tensor in two and three space dimensions. The theoretical convergence orders are confirmed by numerical experiments.
arXiv commentSee arXiv:1603.01339 for Part I: a nonlinear scheme
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- Kinetic models for polymers with inertial effects
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Cited by in corpus (7)
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- Existence, regularity and weak-strong uniqueness for the three-dimensional Peterlin viscoelastic model
- Global existence of weak solutions to viscoelastic phase separation: Part I Regular Case
- Global existence of weak solutions to viscoelastic phase separation: Part II Degenerate Case
- A two-step Lagrange-Galerkin scheme for the shallow water equations with a transmission boundary condition and its application to the Bay of Bengal region. Part I: Flat bottom topography
- Second-order finite difference approximations of the upper-convected time derivative
- A pressure-stabilized projection Lagrange--Galerkin scheme for the transient Oseen problem