“…19 A non-iterative time advancement algorithm utilizing an explicit Runge-Kutta scheme for time advancement has been investigated by several researchers. [21][22][23] The method, called RK-SIMPLER, utilizes the pressure equation of the SIMPLER algorithm and is shown to provide significant runtime reduction over SIMPLER for unsteady problems at relatively high Reynolds numbers despite a small timestep requirement. The algorithm does not introduce relaxation or approximations into any of the equations and proves that if the pressure field is known, the momentum equations can be solved as a generic set of coupled ordinary differential equations using any suitable time advancement scheme.…”
A new solution procedure called Diagonal Split Corrected Linked Equations via Operator splitting (DS-CLEO) has been developed for solving the momentum equations in the pressure-based SIMPLER-type formulation of the incompressible Navier-Stokes equations. An explicit momentum predictor step based on a time splitting procedure is shown to possess unconditional stability while only the implicit pressure equation requires a computationally intensive iterative solver. No relaxation of any of the governing equations is necessary to ensure convergence for either steady or unsteady problems. It is demonstrated that pressure-velocity coupling and second order time accuracy is obtained through a set of inner iterations on the pressure and velocity fields using the exact discretized equations. The Diagonal Split procedure offered a 33.9 and 35.9x reduction in runtime compared to SIMPLER for two unsteady problems tested and a minor runtime reduction for steady lid-driven cavity flow.
“…19 A non-iterative time advancement algorithm utilizing an explicit Runge-Kutta scheme for time advancement has been investigated by several researchers. [21][22][23] The method, called RK-SIMPLER, utilizes the pressure equation of the SIMPLER algorithm and is shown to provide significant runtime reduction over SIMPLER for unsteady problems at relatively high Reynolds numbers despite a small timestep requirement. The algorithm does not introduce relaxation or approximations into any of the equations and proves that if the pressure field is known, the momentum equations can be solved as a generic set of coupled ordinary differential equations using any suitable time advancement scheme.…”
A new solution procedure called Diagonal Split Corrected Linked Equations via Operator splitting (DS-CLEO) has been developed for solving the momentum equations in the pressure-based SIMPLER-type formulation of the incompressible Navier-Stokes equations. An explicit momentum predictor step based on a time splitting procedure is shown to possess unconditional stability while only the implicit pressure equation requires a computationally intensive iterative solver. No relaxation of any of the governing equations is necessary to ensure convergence for either steady or unsteady problems. It is demonstrated that pressure-velocity coupling and second order time accuracy is obtained through a set of inner iterations on the pressure and velocity fields using the exact discretized equations. The Diagonal Split procedure offered a 33.9 and 35.9x reduction in runtime compared to SIMPLER for two unsteady problems tested and a minor runtime reduction for steady lid-driven cavity flow.
“…Recently, Lestari [35] used a CVFEM like method with median-dual control volumes [53] for solving the two-dimensional, unsteady Navier-Stokes equations. Triangular grid elements were used and various implicit and explicit time integration schemes were examined.…”
mentioning
confidence: 99%
“…35 Induced velocity profiles, Rotor -II In order to visualize discrete vortices for a rotor hovering in OGE, the 'θ' component of vorticity in different (r − z) planes is visualized for Rotor-II. The data is obtained by moving the plane of observation in positive 'θ' direction in increments of 7 0 while the rotor blades rotate in negative θ direction.…”
“…The local coordinate system, illustrated inFig. 2.4, of a typical tetrahedral control volume with nodes numbered(1,2,3,4). The global coordinate system (x, y, z) is transformed to the local coordinate system (X, Y, Z) using the following steps:…”
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