Numerical Analysis of the High Speed Driven Cavity Flow in 2-D Curved Channel

Numerical experiments were carried out on the high speed driven cavity flows in 2D curved channels to investigate mainly the pressure field. A density-based algorithm in ANSYS Fluent 13.0 was used in the present URANS simulations. The SST k- ω model was used for modeling the turbulence within an...

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Main Authors: M. M. Ashraful Alam, Toshiaki Setoguchi, Manabu Takao, Heuy Dong Kim
Format: Article
Language:English
Published: Isfahan University of Technology 2016-01-01
Series:Journal of Applied Fluid Mechanics
Subjects:
Online Access:http://jafmonline.net/JournalArchive/download?file_ID=39358&issue_ID=225
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spelling doaj-78a5b5a34eff41a0b744ffcf1e3bfa852020-11-25T01:16:17ZengIsfahan University of Technology Journal of Applied Fluid Mechanics1735-35722016-01-0192529536.Numerical Analysis of the High Speed Driven Cavity Flow in 2-D Curved ChannelM. M. Ashraful Alam0Toshiaki Setoguchi1Manabu Takao2Heuy Dong Kim3National Institute of Technology, Matsue College, JapanSaga University, JapanMatsue National College of Technology, JapanAndong National University, KoreaNumerical experiments were carried out on the high speed driven cavity flows in 2D curved channels to investigate mainly the pressure field. A density-based algorithm in ANSYS Fluent 13.0 was used in the present URANS simulations. The SST k- ω model was used for modeling the turbulence within an unstructured mesh solver. Validation of the numerical code was accomplished, and the results showed a good agreement between the numerical simulation and experimental data. Three channels (straight, concave and convex) with a nominal height of H = 4 × 10 −3 m under the transonic flow conditions were considered in the study. The cavity studied is L = 12 × 10 −3 m long with the depth ranging from D = 12 × 10 −3 m to 48 × 10 −3 m to obtain the length-to-depth ratios of L /D=1 to 1 /4. The study comprised the analysis of the cavity surface pressures and the associated flow structures. The channel configuration influenced the cavity flowfield, and that influence finally resulted in a change in the surface pressure fluctuations in the cavity. The deep cavity attenuated the flowfield oscillation inside the cavity.http://jafmonline.net/JournalArchive/download?file_ID=39358&issue_ID=225Compression wave; Compressible flow; Oscillation; Pressure fluctuation; URANS (unsteady Reynolds-averaged Navier-Stokes)
collection DOAJ
language English
format Article
sources DOAJ
author M. M. Ashraful Alam
Toshiaki Setoguchi
Manabu Takao
Heuy Dong Kim
spellingShingle M. M. Ashraful Alam
Toshiaki Setoguchi
Manabu Takao
Heuy Dong Kim
Numerical Analysis of the High Speed Driven Cavity Flow in 2-D Curved Channel
Journal of Applied Fluid Mechanics
Compression wave; Compressible flow; Oscillation; Pressure fluctuation; URANS (unsteady Reynolds-averaged Navier-Stokes)
author_facet M. M. Ashraful Alam
Toshiaki Setoguchi
Manabu Takao
Heuy Dong Kim
author_sort M. M. Ashraful Alam
title Numerical Analysis of the High Speed Driven Cavity Flow in 2-D Curved Channel
title_short Numerical Analysis of the High Speed Driven Cavity Flow in 2-D Curved Channel
title_full Numerical Analysis of the High Speed Driven Cavity Flow in 2-D Curved Channel
title_fullStr Numerical Analysis of the High Speed Driven Cavity Flow in 2-D Curved Channel
title_full_unstemmed Numerical Analysis of the High Speed Driven Cavity Flow in 2-D Curved Channel
title_sort numerical analysis of the high speed driven cavity flow in 2-d curved channel
publisher Isfahan University of Technology
series Journal of Applied Fluid Mechanics
issn 1735-3572
publishDate 2016-01-01
description Numerical experiments were carried out on the high speed driven cavity flows in 2D curved channels to investigate mainly the pressure field. A density-based algorithm in ANSYS Fluent 13.0 was used in the present URANS simulations. The SST k- ω model was used for modeling the turbulence within an unstructured mesh solver. Validation of the numerical code was accomplished, and the results showed a good agreement between the numerical simulation and experimental data. Three channels (straight, concave and convex) with a nominal height of H = 4 × 10 −3 m under the transonic flow conditions were considered in the study. The cavity studied is L = 12 × 10 −3 m long with the depth ranging from D = 12 × 10 −3 m to 48 × 10 −3 m to obtain the length-to-depth ratios of L /D=1 to 1 /4. The study comprised the analysis of the cavity surface pressures and the associated flow structures. The channel configuration influenced the cavity flowfield, and that influence finally resulted in a change in the surface pressure fluctuations in the cavity. The deep cavity attenuated the flowfield oscillation inside the cavity.
topic Compression wave; Compressible flow; Oscillation; Pressure fluctuation; URANS (unsteady Reynolds-averaged Navier-Stokes)
url http://jafmonline.net/JournalArchive/download?file_ID=39358&issue_ID=225
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