Sort by:
Publication Type:
Open access:
Publication Date:
Periodicals:
Search results
Online since: September 2013
Authors: Li Li, Xiao Ling Lei, Ji Wan, Dong Kui He
Based on the mechanism of intermittent aeration, the model above can be improved and further simulations are obtained: different impacts of particle deposition and absorbing to the pore size decrease; different impacts of particle size distribution and flow turbulence to membrane pore blockage.
[5] Xiaoling Lei. (2010) Simulation and mechanisms of aeration impacts on the permeate flux in submerged membrane systems.
CFD (2002).Modelling of gas sparged ultrafiltration in tubular membranes.
[5] Xiaoling Lei. (2010) Simulation and mechanisms of aeration impacts on the permeate flux in submerged membrane systems.
CFD (2002).Modelling of gas sparged ultrafiltration in tubular membranes.
Online since: July 2014
Authors: P. Nagaraj, G.S. Jinu, J. Thanikachalam
An optimum MRB design with two rotating disks based on design optimization procedure using simulated annealing combined with FE simulations involving magneto static, fluid flow and heat transfer analysis was also carried out by them .The performance of the MRB in a vehicle was studied with the help of a quarter vehicle model.
The simulation result shows the potential of their proposed MRB system to provide fast anti-lock braking [3].
A CFD model can then be built to obtain the velocity of the MR fluid within the brake.
The simulation result shows the potential of their proposed MRB system to provide fast anti-lock braking [3].
A CFD model can then be built to obtain the velocity of the MR fluid within the brake.
Online since: June 2018
Authors: Abdellah Guenaim, Houssem Laidoudi, Mohamed Bouzit, Fayçal Bouzit, Bilal Blissag
The simulations showed that the Dean vortex depends on Bingham fluid and gap spacing.
Numerical Procedure The numerical investigations are realized by using the commercial CFD package called ANSYS-CFX.
Fig. 2: Typical grid used for simulation.
Summary This paper presents a numerical simulation of power-law fluids inside of a 180° curved duct under the effect of aiding thermal buoyancy.
Mompean, Numerical simulation of viscoelastic Dean Vortices in a curved duct, J.
Numerical Procedure The numerical investigations are realized by using the commercial CFD package called ANSYS-CFX.
Fig. 2: Typical grid used for simulation.
Summary This paper presents a numerical simulation of power-law fluids inside of a 180° curved duct under the effect of aiding thermal buoyancy.
Mompean, Numerical simulation of viscoelastic Dean Vortices in a curved duct, J.
Online since: July 2023
Authors: Elizaldo Domingues dos Santos, Liércio André Isoldi, Luiz Alberto Oliveira Rocha, Giovanni Antonio Vielma Vivas, Michel Kepes Rodrigues, Ruth da Silva Brum
However, a small increase in the values of the liquid
fraction at 48 h was observed, that is, at the end of the simulation, when compared to those reached
at 24 h.
The simulations carried out for this work represent a time interval of 2 years.
Here we used the same configuration in Fluent described in section 2.3, with the exception that the simulation time was 15 and a half days.
Santos, Thermal performance simulations of Earth-Air Heat Exchangers for different soils of a coastal city using in-situ data, Sustain.
Wilcox, Turbulence Modeling For CFD, third ed., DCW Industries, California, 2006
The simulations carried out for this work represent a time interval of 2 years.
Here we used the same configuration in Fluent described in section 2.3, with the exception that the simulation time was 15 and a half days.
Santos, Thermal performance simulations of Earth-Air Heat Exchangers for different soils of a coastal city using in-situ data, Sustain.
Wilcox, Turbulence Modeling For CFD, third ed., DCW Industries, California, 2006
Online since: February 2015
Authors: E.M.A. Pereira, J.V. Silva, T.H.F. Andrade, S.R. de Farias Neto, A.G. Barbosa de Lima
Table 1 - Physical and geometrical parameters used in the simulations of the rough rice grain drying.
The mesh representing the bean grain was generated by using the ICEM CFD software.
Figure 3 - (a) Numerical mesh of the bean and (b) details of the mesh used in the simulation.
Table 2 - Physical and geometrical parameters used in the simulations of the “mulatinho” bean grains drying.
Somchart, Simulation and grain quality for in-store drying of paddy, J.
The mesh representing the bean grain was generated by using the ICEM CFD software.
Figure 3 - (a) Numerical mesh of the bean and (b) details of the mesh used in the simulation.
Table 2 - Physical and geometrical parameters used in the simulations of the “mulatinho” bean grains drying.
Somchart, Simulation and grain quality for in-store drying of paddy, J.
Online since: September 2013
Authors: Rui Nie, Da Wei Li, Jin Hao Qiu, Hong Li Ji
The amplitude is ranged from 0.0005c to 0.003c in the simulation.
The pressure distribution is another parameter to verify the method of simulation.
Simulation of two dimension model 4.1.
The simulation method can be using to study the effect of active control
The CFD results predicted that the drag coefficient is increased when the vibrational amplitude A+ exceed 2.4.
The pressure distribution is another parameter to verify the method of simulation.
Simulation of two dimension model 4.1.
The simulation method can be using to study the effect of active control
The CFD results predicted that the drag coefficient is increased when the vibrational amplitude A+ exceed 2.4.
Online since: October 2013
Authors: Prasad K.D.V. Yarlagadda, Yuan Tong Gu, Beat Schmutz, Michael Schuetz, Javad Malekani
This paper discusses about the parameters affecting simulation of deforming a distal tibial orthopedic bone plate.
But inaccuracy of the results can be under %2 which is excellent for most of numerical simulations
Also less computational time is needed for 2D simulations.
[28] Ferziger, Joel H and Peric, Milovan, Further discussion of numerical errors in CFD.
[34] Bernstein, Joshua, Higher Returns on the Simulation Investment.
But inaccuracy of the results can be under %2 which is excellent for most of numerical simulations
Also less computational time is needed for 2D simulations.
[28] Ferziger, Joel H and Peric, Milovan, Further discussion of numerical errors in CFD.
[34] Bernstein, Joshua, Higher Returns on the Simulation Investment.
Online since: January 2019
Authors: E.A. Bonifaz
The current status of FSW research has been well summarized by Mishra and Ma [2], but despite of significant advances the basic knowledge is not sufficient to achieve reliable simulations.
Fourment, A 3D numerical simulation of different phases of friction stir welding, Modelling Simul.
Nelson, Friction model for friction stir welding process simulation: Calibrations from welding experiments, International Journal of Machine Tools & Manufacture 50 (2010) 143–155
Shercliff, 3-Dimensional CFD modeling of flow round a threaded friction stir welding tool profile, J.
Failla II, Friction Stir Welding and Microstructure Simulation of HSLA-65 and Austenitic Stainless Steels, Welding Engineering MS Thesis at the Ohio State University, 2009
Fourment, A 3D numerical simulation of different phases of friction stir welding, Modelling Simul.
Nelson, Friction model for friction stir welding process simulation: Calibrations from welding experiments, International Journal of Machine Tools & Manufacture 50 (2010) 143–155
Shercliff, 3-Dimensional CFD modeling of flow round a threaded friction stir welding tool profile, J.
Failla II, Friction Stir Welding and Microstructure Simulation of HSLA-65 and Austenitic Stainless Steels, Welding Engineering MS Thesis at the Ohio State University, 2009
Online since: October 2013
Authors: Xiao Rui Cheng, Ren Nian Li, Wei Li Guo, Nan Zhang, Yang Gao
The numerical simulation and experimental research of the transient flow in centrifugal pump start-up process [D].
CFD-Driving Pump Design Forward [J].World Pumps, 2002,18-22
The two-dimensional numerical simulation of internal transient flow in centrifugal pump start-up process[J].
The vane pump start-up characteristic simulation based on bond graph method [J].
Numerical simulation of centrifugal pump start-up process[J].
CFD-Driving Pump Design Forward [J].World Pumps, 2002,18-22
The two-dimensional numerical simulation of internal transient flow in centrifugal pump start-up process[J].
The vane pump start-up characteristic simulation based on bond graph method [J].
Numerical simulation of centrifugal pump start-up process[J].
Online since: August 2013
Authors: Mazlan A. Wahid, Hussein A. Mohammed, Nur Irmawati Om
For the radiation model, P1 method is used in the simulation and it is based on the expansion of the radiation intensity.
Hexagonal elements grid and non-uniform system are utilized in the simulations.
Simulations are performed for different Rayleigh numbers in the range of 2×106 ≤ Ra ≤ 2 × 107 and different Reynolds numbers in the range of 100 ≤ Re ≤ 1000.
Combined heat and mass transfer for laminar flow of moist air in a 3D rectangular duct: CFD simulation and validation with experimental data.
Direct numerical simulation of three-dimensional flow and augmented heat transfer in a grooved channel.
Hexagonal elements grid and non-uniform system are utilized in the simulations.
Simulations are performed for different Rayleigh numbers in the range of 2×106 ≤ Ra ≤ 2 × 107 and different Reynolds numbers in the range of 100 ≤ Re ≤ 1000.
Combined heat and mass transfer for laminar flow of moist air in a 3D rectangular duct: CFD simulation and validation with experimental data.
Direct numerical simulation of three-dimensional flow and augmented heat transfer in a grooved channel.