Hopf bifurcation of the unsteady regularized driven cavity flow
Journal of Computational Physics
Vorticity boundary condition and related issues for finite difference schemes
Journal of Computational Physics
Essentially compact schemes for unsteady viscous incompressible flows
Journal of Computational Physics
A Compact Fourth-Order Finite Difference Scheme for Unsteady Viscous Incompressible Flows
Journal of Scientific Computing
Journal of Computational Physics
A Central-Difference Scheme for a Pure Stream Function Formulation of Incompressible Viscous Flow
SIAM Journal on Scientific Computing
A compact scheme for the streamfunction formulation of Navier-Stokes equations
ICCSA'03 Proceedings of the 2003 international conference on Computational science and its applications: PartI
Journal of Computational Physics
An efficient transient Navier-Stokes solver on compact nonuniform space grids
Journal of Computational and Applied Mathematics
Journal of Scientific Computing
A High Order Compact Scheme for the Pure-Streamfunction Formulation of the Navier-Stokes Equations
Journal of Scientific Computing
Recent Developments in the Pure Streamfunction Formulation of the Navier-Stokes System
Journal of Scientific Computing
Journal of Computational Physics
A new family of (5,5)CC-4OC schemes applicable for unsteady Navier-Stokes equations
Journal of Computational Physics
Computers & Mathematics with Applications
Hi-index | 31.47 |
A pure-streamfunction formulation is introduced for the numerical simulation of the two-dimensional incompressible Navier-Stokes equations. The idea is to replace the vorticity in the vorticity-streamfunction evolution equation by the Laplacian of the streamfunction. The resulting formulation includes the streamfunction only, thus no inter-function relations need to be invoked. A compact numerical scheme, which interpolates streamfunction values as well as its first order derivatives, is presented and analyzed. A number of numerical experiments are presented, including driven and double driven cavities, where the Reynolds numbers are sufficiently large, leading to symmetry breaking of asymptotic solutions.