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Online since: September 2016
Authors: Mohannad Naeem Houshi
Jha, S & Jain, VK2006, ‘Modeling and simulation of surface roughness in magnetorheological abrasive flow finishing (MRAFF) process’, Wear, vol.261,no.7-8, pp. 856–866
Jayswal, SC, Jain, VK & Dixit, PM2005, ‘ Modeling and simulation of magnetic abrasive finishing process’, International Journal of Advanced Manufacturing Technology, vol. 26, no.5-6, pp. 477–490
Jayswal , SC, Jain , VC & Dixit, PM 2005, ‘ Modeling and simulation of magnetic abrasive finishing process’, International Journal of Advanced Manufacturing Technology, vol.26, no.5-6, pp.477-490
Jain, VC, Jayswal, SC, & Dixit, PM 2007, ‘Modeling and simulation of surface roughness in magnetic abrasive finishing using non-uniform surface profiles’, Materials and Manufacturing Processes, vol.22, no.2, pp.256-270
Wan, S, Ang, YJ , Sato, T & Lim, GC 2014,’ Process modeling and CFD simulation of two-way abrasive flow machining’, International Journal of Advanced Manufacturing Technology, vol.71, no.5-8, pp.1077–1086
Jayswal, SC, Jain, VK & Dixit, PM2005, ‘ Modeling and simulation of magnetic abrasive finishing process’, International Journal of Advanced Manufacturing Technology, vol. 26, no.5-6, pp. 477–490
Jayswal , SC, Jain , VC & Dixit, PM 2005, ‘ Modeling and simulation of magnetic abrasive finishing process’, International Journal of Advanced Manufacturing Technology, vol.26, no.5-6, pp.477-490
Jain, VC, Jayswal, SC, & Dixit, PM 2007, ‘Modeling and simulation of surface roughness in magnetic abrasive finishing using non-uniform surface profiles’, Materials and Manufacturing Processes, vol.22, no.2, pp.256-270
Wan, S, Ang, YJ , Sato, T & Lim, GC 2014,’ Process modeling and CFD simulation of two-way abrasive flow machining’, International Journal of Advanced Manufacturing Technology, vol.71, no.5-8, pp.1077–1086
Flow in a Three-Sided Lid-Driven Cavity: Genesis of Vortices under Asymmetric Parallel Upward Motion
Online since: February 2026
Authors: Samir Houat, El Amin Azzouz
Careful calibration of both the pseudo-CFL and URFs ensures efficient, stable, and physically consistent convergence throughout the simulation.
Results and Discussion The results from the numerical simulations of the 2D flow in a three-sided lid-driven cavity with parallel upward motion are presented in this section.
A future extension of this work will consider three-dimensional simulations to further examine these complex flow phenomena.
Lin, "Multi relaxation time lattice Boltzmann simulations of transition in deep 2D lid driven cavity using GPU," Computers and Fluids, 80 (2013) 381–387.
Hanna, "Numerical simulation of three-sided lid-driven square cavity," Engineering Reports, 2 (2020) e12151. https://doi.org/10.1002/eng2.12151
Results and Discussion The results from the numerical simulations of the 2D flow in a three-sided lid-driven cavity with parallel upward motion are presented in this section.
A future extension of this work will consider three-dimensional simulations to further examine these complex flow phenomena.
Lin, "Multi relaxation time lattice Boltzmann simulations of transition in deep 2D lid driven cavity using GPU," Computers and Fluids, 80 (2013) 381–387.
Hanna, "Numerical simulation of three-sided lid-driven square cavity," Engineering Reports, 2 (2020) e12151. https://doi.org/10.1002/eng2.12151
Online since: November 2024
Authors: Andrii Cheilytko, David Brust
The temperature distribution for both types of backfill was found by computer simulation.
Utilizing computer simulation, it has been determined that the heating temperature of a catalyst featuring a staggered arrangement of backfill fractions surpasses that of a catalyst with a corridor arrangement of equal thickness.
Avila-Marin, CFD parametric analysis of wire meshes open volumetric receivers with axial-varied porosity and comparison with small-scale solar receiver tests, Renewable Energy 193 (2022) 1094–1105. https://doi.org/10.1016/j.renene.2022.05.060
Utilizing computer simulation, it has been determined that the heating temperature of a catalyst featuring a staggered arrangement of backfill fractions surpasses that of a catalyst with a corridor arrangement of equal thickness.
Avila-Marin, CFD parametric analysis of wire meshes open volumetric receivers with axial-varied porosity and comparison with small-scale solar receiver tests, Renewable Energy 193 (2022) 1094–1105. https://doi.org/10.1016/j.renene.2022.05.060
Online since: July 2025
Authors: Sebastian Breitfelder, Timo Strobl, Torsten E.M. Staab, Dominik Boras
After this correction the peak position of the simulation and our experimental data are identical (see appendix).
When the DRS4 evalu- ation board receives the external trigger from the two Constant Fraction Discriminators (CFDs), the capacitor arrays are successively charged by the pules employing a sampling rate of 5.12 GHz with a sweep of 200 ns.
DDRS4PALS: A software for the acquisition and simulation of lifetime spectra using the DRS4 evaluation board.
When the DRS4 evalu- ation board receives the external trigger from the two Constant Fraction Discriminators (CFDs), the capacitor arrays are successively charged by the pules employing a sampling rate of 5.12 GHz with a sweep of 200 ns.
DDRS4PALS: A software for the acquisition and simulation of lifetime spectra using the DRS4 evaluation board.
Online since: February 2024
Authors: Balaji Bakthavatchalam, Raghvendran Pala Raviramachandran, Middela Mohith Venkatesh, Nagoor Basha Shaik, Omar A. Hussein, Namdev Ashok Patil
.,[56]
Mxene/ water
single-phase model
Numerical CFD simulation shows that thermal and electrical efficiency of the system increased with MXene nanofluid mass fraction and flow rate.
Nguyen, Simulation and optimization of Tesla valves. 2003
Nguyen, Simulation and optimization of Tesla valves. 2003
Online since: January 2017
Authors: Mario Rosso, Ildiko Peter, Christian Castella
Being the two forming processes substantially different, appropriate CAD models for the corresponding simulations were developed in SolidworksTM, and successively imported in the numerical simulation tool.
Isotropic Norton-Hoff law is used for viscoelastic behaviour and the constitutive laws for both simulations are expressed in terms of a viscoplastic potential [65].
Yang et al.; Numerical simulation of semi-solid Magnesium alloy in continuous roll-casting process; International Conference on Semi-Solid Processing of Alloys and Composites, Trans Tech Publications, Switzerland, Solid State Phenomena 116-117 (2006) pp.583–586
Charette; Effect of Different Fraction Solids on the Fluidity of Rheocast 356 Al–Si Alloy; Multi Phase Phenomena and CFD Modeling and Solidification in Materials Processes, TMS Publication, North Carolina, March (2004) pp. 119–128
Koeune; Study of the Liquid Fraction and Thermophysical Properties of Semi-Solid Steels and Application to the Simulation of Inductive Heating for Thixoforming; Chapter Advanced Methods in Material Forming pp.321-347
Isotropic Norton-Hoff law is used for viscoelastic behaviour and the constitutive laws for both simulations are expressed in terms of a viscoplastic potential [65].
Yang et al.; Numerical simulation of semi-solid Magnesium alloy in continuous roll-casting process; International Conference on Semi-Solid Processing of Alloys and Composites, Trans Tech Publications, Switzerland, Solid State Phenomena 116-117 (2006) pp.583–586
Charette; Effect of Different Fraction Solids on the Fluidity of Rheocast 356 Al–Si Alloy; Multi Phase Phenomena and CFD Modeling and Solidification in Materials Processes, TMS Publication, North Carolina, March (2004) pp. 119–128
Koeune; Study of the Liquid Fraction and Thermophysical Properties of Semi-Solid Steels and Application to the Simulation of Inductive Heating for Thixoforming; Chapter Advanced Methods in Material Forming pp.321-347
Online since: January 2024
Authors: Fayçal Bouzit, Mohamed Bouzit, Djamila Derbal, Abderrahim Mokhefi
In this simulation, multiple numbers of mesh elements have been considered.
After performing a numerical simulation, the following principal points have been concluded: · The heat transfer inside the expanded curved duct proves to be significant as the Reynolds number increases.
Arivazhagan, , P.Sivashanmugam, Experimental and CFD Heat Transfer Studies of Al2O3-Water Nanofluid in a Coiled Agitated Vessel Equipped with Propeller, Chinese Journal of Chemical Engineering 21(11) (2013) 1232-243
Zhang, Numerical simulation of laminar forced convection heat transfer of Al2O3–water nanofluid in a pipe with return bend, International Journal of Thermal Sciences 55(2012) 90-102
Bouzit, 3D Simulation of incompressible poiseuille flow through 180 curved duct of square cross-section under effect of thermal buoyancy, Periodica Polytechnica Mechanical Engineering 63(4) (2019) 257–269
After performing a numerical simulation, the following principal points have been concluded: · The heat transfer inside the expanded curved duct proves to be significant as the Reynolds number increases.
Arivazhagan, , P.Sivashanmugam, Experimental and CFD Heat Transfer Studies of Al2O3-Water Nanofluid in a Coiled Agitated Vessel Equipped with Propeller, Chinese Journal of Chemical Engineering 21(11) (2013) 1232-243
Zhang, Numerical simulation of laminar forced convection heat transfer of Al2O3–water nanofluid in a pipe with return bend, International Journal of Thermal Sciences 55(2012) 90-102
Bouzit, 3D Simulation of incompressible poiseuille flow through 180 curved duct of square cross-section under effect of thermal buoyancy, Periodica Polytechnica Mechanical Engineering 63(4) (2019) 257–269
Online since: July 2021
Authors: Jumaa S. Chiad, Abbas H. Jeryo, Wajdi S. Abbod
ANSYS's holistic analysis includes three steps: geometry simulation and the output mesh, then configuration and solution aggregation of the limit conditions [69-74].
Such pressure touch values were employed in three regions with maximal system pressure monitoring for orthosis at the knee-foot level in the simulation software ANSYS 16.1.
The ANSYS program Numerical Simulation: Compared with usable composite content (4 Perlon 2 carbon fiber 4 Perlon), the total safeguard level of optimal content (10 Perlon and 0.75%Wt of MWCNTs) was improved from 2.298 to 4.06. 5.
Al-Waily, Optimization CFD Study of Erosion in 3D Elbow During Transportation of Crude Oil Contaminated with Sand Particles (International Journal of Engineering & Technology) vol 07 no 03 ,2018,pp 1420–1428
Mumtaz Rajab, Investigation Of Partially Pressurized Thick Cylindrical Shells (Modelling, simulation & control B AMSE Press) vol 25 no 03,1989. pp 47–64
Such pressure touch values were employed in three regions with maximal system pressure monitoring for orthosis at the knee-foot level in the simulation software ANSYS 16.1.
The ANSYS program Numerical Simulation: Compared with usable composite content (4 Perlon 2 carbon fiber 4 Perlon), the total safeguard level of optimal content (10 Perlon and 0.75%Wt of MWCNTs) was improved from 2.298 to 4.06. 5.
Al-Waily, Optimization CFD Study of Erosion in 3D Elbow During Transportation of Crude Oil Contaminated with Sand Particles (International Journal of Engineering & Technology) vol 07 no 03 ,2018,pp 1420–1428
Mumtaz Rajab, Investigation Of Partially Pressurized Thick Cylindrical Shells (Modelling, simulation & control B AMSE Press) vol 25 no 03,1989. pp 47–64
Online since: June 2010
Authors: Cecilia Surace, Manuela Battipede, Keith Worden, W.E. Becker
Furthermore, the
complicated nature of the material properties is an additional source of epistemic uncertainty
indeed, some work has been done to investigate
analysis of a typical heart valve FE model would provide useful insight into the robustness of the
simulation.
The simulation was performed over the initial opening movement of the valve: a total time of 0.1s, starting from the direction.
It was therefore considered enough to pick eight input parameters to examine, that were found to vary substantially from one simulation to the next in a comprehensive literature review on the topic.
As in the case of the heart-valve model, the FE software LS-Dyna was used; the solver being capable of handling highly nonlinear and transient simulations, and the coupling of Lagrangian and Arbitrary-Lagrangian-Eulerian (ALE) meshes required for FSI.
The possibility of structural deformation that would change the boundary conditions of a standard CFD model necessitates this approach.
The simulation was performed over the initial opening movement of the valve: a total time of 0.1s, starting from the direction.
It was therefore considered enough to pick eight input parameters to examine, that were found to vary substantially from one simulation to the next in a comprehensive literature review on the topic.
As in the case of the heart-valve model, the FE software LS-Dyna was used; the solver being capable of handling highly nonlinear and transient simulations, and the coupling of Lagrangian and Arbitrary-Lagrangian-Eulerian (ALE) meshes required for FSI.
The possibility of structural deformation that would change the boundary conditions of a standard CFD model necessitates this approach.