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Numerical simulation of axisymmetric unsteady incompressible flow by a vorticity‐velocity method
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AbstractA new numerical method for solving the axisymmetric unsteady incompressible Navier‐Stokes equations using vorticity‐velocity variables and a staggered grid is presented. The solution is advanced in time with an explicit two‐stage Runge‐Kutta method. At each stage a vector Poisson equation for velocity is solved. Some important aspects of staggering of the variable location, divergence‐free correction to the velocity field by means of a suitably chosen scalar potential and numerical treatment of the vorticity boundary condition are examined. The axisymmetric spherical Couette flow between two concentric differentially rotating spheres is computed as an initial value problem. Comparison of the computational results using a staggered grid with those using a non‐staggered grid shows that the staggered grid is superior to the non‐staggered grid. The computed scenario of the transition from zero‐vortex to two‐vortex flow at moderate Reynolds number agrees with that simulated using a pseudospectral method, thus validating the temporal accuracy of our method.
Title: Numerical simulation of axisymmetric unsteady incompressible flow by a vorticity‐velocity method
Description:
AbstractA new numerical method for solving the axisymmetric unsteady incompressible Navier‐Stokes equations using vorticity‐velocity variables and a staggered grid is presented.
The solution is advanced in time with an explicit two‐stage Runge‐Kutta method.
At each stage a vector Poisson equation for velocity is solved.
Some important aspects of staggering of the variable location, divergence‐free correction to the velocity field by means of a suitably chosen scalar potential and numerical treatment of the vorticity boundary condition are examined.
The axisymmetric spherical Couette flow between two concentric differentially rotating spheres is computed as an initial value problem.
Comparison of the computational results using a staggered grid with those using a non‐staggered grid shows that the staggered grid is superior to the non‐staggered grid.
The computed scenario of the transition from zero‐vortex to two‐vortex flow at moderate Reynolds number agrees with that simulated using a pseudospectral method, thus validating the temporal accuracy of our method.
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