2016
DOI: 10.1063/1.4944629
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Constant-energetics physical-space forcing methods for improved convergence to homogeneous-isotropic turbulence with application to particle-laden flows

Abstract: Articles you may be interested in Single-particle Lagrangian and structure statistics in kinematically simulated particle-laden turbulent flows

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Cited by 55 publications
(26 citation statements)
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“…The continuity and linearly forced momentum equations are numerically integrated for the carrier phase, where Π is a hydrodynamic pressure computed from the integration of a Poisson equation obtained by taking the divergence of the momentum equation and making use of the divergence-free constraint for the velocity field 35 . The forcing coefficient A is such that statistically steady homogeneous-isotropic turbulence at constant kinetic energy is maintained 36 . The resulting Taylor–Reynolds number of the simulations is , where λ is the Taylor microscale.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…The continuity and linearly forced momentum equations are numerically integrated for the carrier phase, where Π is a hydrodynamic pressure computed from the integration of a Poisson equation obtained by taking the divergence of the momentum equation and making use of the divergence-free constraint for the velocity field 35 . The forcing coefficient A is such that statistically steady homogeneous-isotropic turbulence at constant kinetic energy is maintained 36 . The resulting Taylor–Reynolds number of the simulations is , where λ is the Taylor microscale.…”
Section: Methodsmentioning
confidence: 99%
“…The initial conditions used for integrating (Eq. ( 19 )) involve a synthetic, solenoidal-isotropic velocity field with a prescribed Passot–Pouquet kinetic-energy model spectrum 36 , 37 .…”
Section: Methodsmentioning
confidence: 99%
“…The initial fluctuating velocity field of the gas carrier phase is generated on the basis of the classical Rogallo's procedure [41] according to a Passot-Pouquet spectrum [42]. A constant-energetics physical-space forced homogeneous isotropic turbulence (HIT) is maintained by resorting to the procedure described in reference [43]. The present computations have been conducted with a Courant and Fourier number values set to 0.1.…”
Section: Computational Setupsmentioning
confidence: 99%
“…In order to keep the statistics of the initial fields at the desired values during this simulation, the control-based linear forcing approach of Bassenne et al [28] was used to achieve statistically steady target values of kinetic energy and energy dissipation rate after several large-eddy turn over times. The method suggested in [28] consists of introducing a source term to the momentum equation, in the form of Au. The forcing coefficient A reads…”
Section: Typical Configurationmentioning
confidence: 99%
“…with ( ) and ( ) being the turbulent kinetic energy and the energy dissipation rate, 0 and 0 denote their steady mean values respectively and 0 is the integral time based on 0 and 0 as (2 0 )/(3 0 ). G 1 and G 2 refer to the the controller's time constants set to be less than the Kolmogorov timescale to prevent interference with turbulence energy-containing time scales [28]. The terms B and E are expressed in function of the velocity gradient ∇ u, the Hessians of the velocity vector components H( ) and the molecular viscosity as…”
Section: Typical Configurationmentioning
confidence: 99%