DOI: 10.31274/etd-180810-212
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Development of unsteady algorithms for pressure-based unstructured solver for two-dimensional incompressible flows

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Cited by 4 publications
(4 citation statements)
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“…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.…”
Section: Introductionmentioning
confidence: 99%
“…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.…”
Section: Introductionmentioning
confidence: 99%
“…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.…”
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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.…”
mentioning
confidence: 99%
“…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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confidence: 99%