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Online since: May 2016
Authors: Zong Wei Zhang, Wei Jia Qian, Jing Min Hu
Through numerical simulation with CFX at a single blowing ratio of 0.5 and Reynold number of 11000, we analyze and compare the performance and behavior of five kinds of cratered holes with the conventional cylindrical hole.
The simulation employs k-ε turbulent model and wall function.
Their large eddy simulation shows that the contoured crater can improve cooling performance significantly because it can generate a pair of vortices which diminish the main kidney-pair vortex caused by the coolant jet.
Using ICEM CFD, an unstructured fine mesh was generated.
The simulation was run with CFX.
The simulation employs k-ε turbulent model and wall function.
Their large eddy simulation shows that the contoured crater can improve cooling performance significantly because it can generate a pair of vortices which diminish the main kidney-pair vortex caused by the coolant jet.
Using ICEM CFD, an unstructured fine mesh was generated.
The simulation was run with CFX.
Online since: September 2011
Authors: Wei Zhong, Jian Peng Yang, Bao An Pei, Jian Jun Niu
Large Eddy Simulation model (LES) was used to assess the effect of mechanical smoke exhausting under the different ventilation modes.
The character of smoke flow in different smoke extraction strategies are studies in this paper by Large Eddy Simulation model, and the suitable strategy is put forward based on the simulation. 2.
Numerical simulation method and Fire scenario design This paper selects the numerical simulation tool FDS5.0 (Fire Dynamics Simulator) developed by NIST, which is a Computational Fluid Dynamics (CFD) simulation model of fire-driven flow[5].
Stair exhaust pipe Escalator Ceiling Screen Fig.1 The sketch map of platform The platform is divided into two calculation areas named platform area and fire area, grid in both areas are cube, the platform area size is 1/8m, and the fire area size is 1/16m. the simulation cases is listed in table 1.
The simulation results shows that the smoke layer’s height maintains over 2m at 400s, the smoke control effect is better than other smoke extraction strategies.
The character of smoke flow in different smoke extraction strategies are studies in this paper by Large Eddy Simulation model, and the suitable strategy is put forward based on the simulation. 2.
Numerical simulation method and Fire scenario design This paper selects the numerical simulation tool FDS5.0 (Fire Dynamics Simulator) developed by NIST, which is a Computational Fluid Dynamics (CFD) simulation model of fire-driven flow[5].
Stair exhaust pipe Escalator Ceiling Screen Fig.1 The sketch map of platform The platform is divided into two calculation areas named platform area and fire area, grid in both areas are cube, the platform area size is 1/8m, and the fire area size is 1/16m. the simulation cases is listed in table 1.
The simulation results shows that the smoke layer’s height maintains over 2m at 400s, the smoke control effect is better than other smoke extraction strategies.
Online since: May 2020
Authors: Antonio Gilson Barbosa de Lima, João de Mélo Vieira Neto, Carlos Antonio de Araújo Mota, Juliana Andreza Figueirôa, Michelly Dayane Araújo de Almeida, Loredanna Melyssa Costa de Souza, T.R. Nascimento Porto
In Ansys CFX®, the aspect ratio is one of the most important simulation criteria, influencing numerical convergence.
The numerical mesh generated for the simulation was directly influenced by the relationship between the mold thickness and the ribbon thickness, where the pre-established quality criterion, aspect ratio, was a determining factor for the convergence of the simulation.
Wang, Simulation and analysis of shape memory alloy fiber reinforced composite based on cohesive zone model, Mater.
Giordano, Finite element simulation of low velocity impact on shape memory alloy composite plates, Compos.
Oliveira, Applying CFD in manufacturing of polymer composite reinforced with shape memory alloy via Resin Transfer Molding, Inter.
The numerical mesh generated for the simulation was directly influenced by the relationship between the mold thickness and the ribbon thickness, where the pre-established quality criterion, aspect ratio, was a determining factor for the convergence of the simulation.
Wang, Simulation and analysis of shape memory alloy fiber reinforced composite based on cohesive zone model, Mater.
Giordano, Finite element simulation of low velocity impact on shape memory alloy composite plates, Compos.
Oliveira, Applying CFD in manufacturing of polymer composite reinforced with shape memory alloy via Resin Transfer Molding, Inter.
Online since: March 2011
Authors: Jin Chun Song, Song Li, Ming Li Han, Yu Jie Ren
The Finite Volume Method of Fluent has been used to the simulation of fluid three-dimensional velocity field and pressure field.
The simulation result of the pressure distribution shows that the flow pressure was not changing in linear gradient all around the gap under moving condition.
Wang, Computational Fluid Dynamics analysis – CFD Software Principle and Application, Tsinghua University Press, Beijing, (2004)
[6] Xiaodong Yu, Yanqin Zhang and Junpeng Shao etc.: Simulation Research on Gap Flow of Circular Cavity Multi-pad Hydrostatic Thrust Bearing, IHMSC (2009), p.41-44
The simulation result of the pressure distribution shows that the flow pressure was not changing in linear gradient all around the gap under moving condition.
Wang, Computational Fluid Dynamics analysis – CFD Software Principle and Application, Tsinghua University Press, Beijing, (2004)
[6] Xiaodong Yu, Yanqin Zhang and Junpeng Shao etc.: Simulation Research on Gap Flow of Circular Cavity Multi-pad Hydrostatic Thrust Bearing, IHMSC (2009), p.41-44
Online since: August 2015
Authors: Piotr Kula, Konrad Dybowski, Sebastian Lipa, Emilia Wołowiec Korecka, Jacek Sawicki
The proposed flowchart did not include the flow effect, which greatly reduced the computation time by eliminating tedious CFD calculations.
All this served the purpose of developing a tool for simulation of inductive quenching.
A carburized layer was proposed in the simulations, defined by 10 sub-layers with the depth of 0.2 mm.
In conclusion, it can be said that the simulations and experiments have shown that the computational algorithm used in the study provides results of simulation similar to the experimental findings.
Arimoto et al., Development of heat treatment simulation system DEFORMTM-HT, in: R.A.
All this served the purpose of developing a tool for simulation of inductive quenching.
A carburized layer was proposed in the simulations, defined by 10 sub-layers with the depth of 0.2 mm.
In conclusion, it can be said that the simulations and experiments have shown that the computational algorithm used in the study provides results of simulation similar to the experimental findings.
Arimoto et al., Development of heat treatment simulation system DEFORMTM-HT, in: R.A.
Online since: August 2013
Authors: Ling Zhao, Zhong An Jiang
Numerical Simulation on Effect of Obstructing Airflow by Different Outlet Parameters of Mine Air Curtain
Ling Zhao1,2,a ,Zhongan Jiang1
1 Civil and Environmental Engineering School, University of Science and Technology Beijing, Beijing, China
2 Resource and Environmental Engineering School, Jiangxi University of Science and Technology, Ganzhou, Jiangxi, China
a jxlgdxzl@163.com
Keywords: mine air curtain; outlet parameters; numerical simulation; the amount of air leakage; obstructing airflow capability
Abstract.
According to characteristics of air curtain obstructing airflow in mine tunnel, utilized turbulent flow dynamic viscosity method, and three-dimensional steady-state incompressible Navier-Stokes equations of computational fluid mechanics, the simulation of flow field in mine tunnel was made by changing outlet parameters of air curtain.
When the parameters are the same, the obstructing airflow capability of acyclic air curtain is better than that of circular air curtain.The result of simulation analysis of mine air curtain can be used as the basis for optimized design.
In the simulation, the outlet air volume was 12.87 m3/s, the outlet angle was 30°, the relation curves about the amount of air leakage and outlet width were gained and were shown in Fig.4.
Flexible damper numerical simulation and application[J].Journal of China Coal Society, 2010,35(Sup):123-127 [2] Qianli Zhao Qian,Gao, Chuangzhou Gao.Cutting Airflow Theory Model and Applied Study of Air curtain Used in Mine[J].Nonferous Metals(mine section) ,2007,59(5):39-42 [3] Haining Wang, Zhongyu Niu, Yanjun Wu.Study of controlling circulated air flow by air curtain in underground mine[J].Mining Research and Development, 2010,30(1):84-87 [4] Haining Wang, Hongying Zhang, Test and application of air curtain in mine[J].Journal of China Coal Society,2006,31(5):615-617 [5] Bao-yu Han, Ying Xiong, Shuangqiao Chen.Numerical simulation of cavitation around 2-dimentional hydrofoil[J].Chinese Journal of Hydrodynamics, 2009,24(6):740-746 [6] Zhiyi Sun, Xiaorong Wu.Discussion and application of CFD numerical simulation technology[J].Water Conservancy Science and Technology and Economy, 2008,14(2):126-128 [7] A.M.Foster, M.J.Swain, R.Barrett, etc.Three-dimensional effects of an air curtain
According to characteristics of air curtain obstructing airflow in mine tunnel, utilized turbulent flow dynamic viscosity method, and three-dimensional steady-state incompressible Navier-Stokes equations of computational fluid mechanics, the simulation of flow field in mine tunnel was made by changing outlet parameters of air curtain.
When the parameters are the same, the obstructing airflow capability of acyclic air curtain is better than that of circular air curtain.The result of simulation analysis of mine air curtain can be used as the basis for optimized design.
In the simulation, the outlet air volume was 12.87 m3/s, the outlet angle was 30°, the relation curves about the amount of air leakage and outlet width were gained and were shown in Fig.4.
Flexible damper numerical simulation and application[J].Journal of China Coal Society, 2010,35(Sup):123-127 [2] Qianli Zhao Qian,Gao, Chuangzhou Gao.Cutting Airflow Theory Model and Applied Study of Air curtain Used in Mine[J].Nonferous Metals(mine section) ,2007,59(5):39-42 [3] Haining Wang, Zhongyu Niu, Yanjun Wu.Study of controlling circulated air flow by air curtain in underground mine[J].Mining Research and Development, 2010,30(1):84-87 [4] Haining Wang, Hongying Zhang, Test and application of air curtain in mine[J].Journal of China Coal Society,2006,31(5):615-617 [5] Bao-yu Han, Ying Xiong, Shuangqiao Chen.Numerical simulation of cavitation around 2-dimentional hydrofoil[J].Chinese Journal of Hydrodynamics, 2009,24(6):740-746 [6] Zhiyi Sun, Xiaorong Wu.Discussion and application of CFD numerical simulation technology[J].Water Conservancy Science and Technology and Economy, 2008,14(2):126-128 [7] A.M.Foster, M.J.Swain, R.Barrett, etc.Three-dimensional effects of an air curtain
Online since: May 2014
Authors: Bin Chen, Bo Ao Xu, Qiang Chen, Long Dou
The commercial CFD code FLUENT is used to model the plasma and the solid anode part.
Hsu first used MHD and hydrodynamic equations successfully numerical simulation of free-burning argon arc,and verified the accuracy of the simulation results through experiment [1].
For numerical simulation and industrial application there are still very important indicators.
Numerical simulation of heat transfer and flow of the free burning arc[J].
Plasma Process. 19153-70 [12] Zhao G Y, Dassanayabe M and Etemadi K 1990 Numerical simulation of a free-burning argon arc with copper evaporation from the anode plasma chem.
Hsu first used MHD and hydrodynamic equations successfully numerical simulation of free-burning argon arc,and verified the accuracy of the simulation results through experiment [1].
For numerical simulation and industrial application there are still very important indicators.
Numerical simulation of heat transfer and flow of the free burning arc[J].
Plasma Process. 19153-70 [12] Zhao G Y, Dassanayabe M and Etemadi K 1990 Numerical simulation of a free-burning argon arc with copper evaporation from the anode plasma chem.
Online since: June 2009
Authors: Jong Hee Kim, Ji Hoon Kim, Youn Suk Choi, Jong Heun Lee, Young Joon Yoon, Jae Kyung Choi, Jong Woo Lim, Hyo Tae Kim
It was confirmed that the degree of mixing in ceramic-based microfluidic
passive mixers was well matched with the numerical simulation data.
After manufacturing the various kinds of mixers, the microfluidic test was progressed and their performance was evaluated comparing with simulation result.
In addition, a numerical simulation using a commercial tool (CFD-ACE+; ESI, Huntsville, AL) was progressed to obtain the mixing efficiency of T-type mixers and chaotic mixer.
Comparing with simulation data, it could be deduced that ceramic-based T-type mixers shown here were well operated under the diffusion driven liquid mixing.
Comparison of mixing efficiency at the point of microchannel outlet between numerical simulation data and experiment result Channel width Mixing efficiency (η) Simulation Experiment T-type mixer 1 mm 26% 12.1% 200 µm 90% 80.6% Chaotic mixer 200 µm 47% 45.0% Conclusion Here, we showed a novel process to fabricated ceramic-based microfluidic passive mixer using LTCC and photolithography.
After manufacturing the various kinds of mixers, the microfluidic test was progressed and their performance was evaluated comparing with simulation result.
In addition, a numerical simulation using a commercial tool (CFD-ACE+; ESI, Huntsville, AL) was progressed to obtain the mixing efficiency of T-type mixers and chaotic mixer.
Comparing with simulation data, it could be deduced that ceramic-based T-type mixers shown here were well operated under the diffusion driven liquid mixing.
Comparison of mixing efficiency at the point of microchannel outlet between numerical simulation data and experiment result Channel width Mixing efficiency (η) Simulation Experiment T-type mixer 1 mm 26% 12.1% 200 µm 90% 80.6% Chaotic mixer 200 µm 47% 45.0% Conclusion Here, we showed a novel process to fabricated ceramic-based microfluidic passive mixer using LTCC and photolithography.
Online since: February 2012
Authors: Qing Ming Chang, Xia Chen, Yin Kai Yang, Min Zhang, Jing Yuan
A simulation parameter with dimension is multiplied by to give the physical quantities.
The plot shows that a linear relationship between the pressure difference and the mean curvature is consistent with the assumption that the assumed equations of state would lead to a fluid with properties compatible with those used in standard CFD simulations.
obtained through along the center line of a bubble. , through simulation
The points from the simulations fit the theory.
A consistent relationship between the simulation parameter and interfacial tension is determined.
The plot shows that a linear relationship between the pressure difference and the mean curvature is consistent with the assumption that the assumed equations of state would lead to a fluid with properties compatible with those used in standard CFD simulations.
obtained through along the center line of a bubble. , through simulation
The points from the simulations fit the theory.
A consistent relationship between the simulation parameter and interfacial tension is determined.
Online since: May 2007
Authors: Ying Zhou, Ming Hui Huang, Da Heng Mao, Tao Liang
Accounting of both the nozzle and
front-box fields will yield more accurate simulation results.
Simulation conditions for Finite Element Analysis Mesh Type.
Results of fluid flow simulations Post-processing by ANSYS.
[5] Huey-Jiuan Lin: Modelling and Simulation in Materials Science and Engineering, vol. 12 (2004), p. 255-72
[7] Nastac, L., Li, B.Q.: Multiphase Phenomena and CFD Modeling and Simulation in Materials Processes Symposium[C] (2004). p. 325-34
Simulation conditions for Finite Element Analysis Mesh Type.
Results of fluid flow simulations Post-processing by ANSYS.
[5] Huey-Jiuan Lin: Modelling and Simulation in Materials Science and Engineering, vol. 12 (2004), p. 255-72
[7] Nastac, L., Li, B.Q.: Multiphase Phenomena and CFD Modeling and Simulation in Materials Processes Symposium[C] (2004). p. 325-34