Journal of Computational Physics
Simulation of viscoelastic fluids: Couette-Taylor flow
Journal of Computational Physics
A Cartesian grid embedded boundary method for Poisson's equation on irregular domains
Journal of Computational Physics
An unsplit, cell-centered Godunov method for ideal MHD
Journal of Computational Physics
Multiscale simulations for suspensions of rod-like molecules
Journal of Computational Physics
Two-phase viscoelastic jetting
Journal of Computational Physics
A modified higher order Godunov's scheme for stiff source conservative hydrodynamics
Journal of Computational Physics
Journal of Computational Physics
An Improved Sharp Interface Method for Viscoelastic and Viscous Two-Phase Flows
Journal of Scientific Computing
Computation of viscoelastic fluid flows using continuation methods
Journal of Computational and Applied Mathematics
A hybrid Godunov method for radiation hydrodynamics
Journal of Computational Physics
Hi-index | 31.47 |
We present a new algorithm to simulate unsteady viscoelastic flows in abrupt contraction channels. In our approach we split the viscoelastic terms of the Oldroyd-B constitutive equation using Duhamel's formula and discretize the resulting PDEs using a semi-implicit finite difference method based on a Lax-Wendroff method for hyperbolic terms. In particular, we leave a small residual elastic term in the viscous limit by design to make the hyperbolic piece well-posed. A projection method is used to impose the incompressibility constraint. We are able to compute the full range of unsteady elastic flows in an abrupt contraction channel - from the viscous limit to the elastic limit - in a stable and convergent manner. We demonstrate the range of our method for unsteady flow of a Maxwell fluid with and without viscosity in planar contraction channels. We also demonstrate stable and convergent results for benchmark high Weissenberg number problems at We=1 and We=10.