Numerical Simulation of an Offset Jet in Bounded Pool with Deflection Wall

The k-ε turbulent model and VOF methods were used to simulate the three-dimensional turbulence jet. Numerical simulations were carried out for three different kinds of jets in a bounded pool with the deflection wall with angles of 0°, 3°, 6°, and 9°. The numerical simulation agrees well with the exp...

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Main Authors: Xin Li, Yurong Wang, Jianmin Zhang
Format: Article
Language:English
Published: Hindawi Limited 2017-01-01
Series:Mathematical Problems in Engineering
Online Access:http://dx.doi.org/10.1155/2017/5943143
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spelling doaj-a63007764d944b3e9a88c1a76644b2f62020-11-24T22:34:20ZengHindawi LimitedMathematical Problems in Engineering1024-123X1563-51472017-01-01201710.1155/2017/59431435943143Numerical Simulation of an Offset Jet in Bounded Pool with Deflection WallXin Li0Yurong Wang1Jianmin Zhang2State Key Laboratory of Hydraulics and Mountain River Engineering, Sichuan University, Chengdu 610065, ChinaState Key Laboratory of Hydraulics and Mountain River Engineering, Sichuan University, Chengdu 610065, ChinaState Key Laboratory of Hydraulics and Mountain River Engineering, Sichuan University, Chengdu 610065, ChinaThe k-ε turbulent model and VOF methods were used to simulate the three-dimensional turbulence jet. Numerical simulations were carried out for three different kinds of jets in a bounded pool with the deflection wall with angles of 0°, 3°, 6°, and 9°. The numerical simulation agrees well with the experimental data. The studies show that the length of the potential core zone increases with the increase of the deflection angle. The velocity distribution is consistent with the Gaussian distribution and almost not affected by the deflection angle in potential core zone. The decay rates of flow velocity in the transition zone are 1.195, 1.281, 1.439, and 1.532 corresponding to the unilateral deflection angles, 0°, 3°, 6°, and 9°, respectively. The decay rates of velocity in the transition zone are 1.928 and 2.835 corresponding to the bilateral deflection angles 3° and 6°. It is also found that the spread of velocity is stronger in the vertical direction as the deflection angles become smaller. The spread rates of velocity with unilateral deflection wall are higher than those with bilateral deflection walls in the horizontal plane in the pool.http://dx.doi.org/10.1155/2017/5943143
collection DOAJ
language English
format Article
sources DOAJ
author Xin Li
Yurong Wang
Jianmin Zhang
spellingShingle Xin Li
Yurong Wang
Jianmin Zhang
Numerical Simulation of an Offset Jet in Bounded Pool with Deflection Wall
Mathematical Problems in Engineering
author_facet Xin Li
Yurong Wang
Jianmin Zhang
author_sort Xin Li
title Numerical Simulation of an Offset Jet in Bounded Pool with Deflection Wall
title_short Numerical Simulation of an Offset Jet in Bounded Pool with Deflection Wall
title_full Numerical Simulation of an Offset Jet in Bounded Pool with Deflection Wall
title_fullStr Numerical Simulation of an Offset Jet in Bounded Pool with Deflection Wall
title_full_unstemmed Numerical Simulation of an Offset Jet in Bounded Pool with Deflection Wall
title_sort numerical simulation of an offset jet in bounded pool with deflection wall
publisher Hindawi Limited
series Mathematical Problems in Engineering
issn 1024-123X
1563-5147
publishDate 2017-01-01
description The k-ε turbulent model and VOF methods were used to simulate the three-dimensional turbulence jet. Numerical simulations were carried out for three different kinds of jets in a bounded pool with the deflection wall with angles of 0°, 3°, 6°, and 9°. The numerical simulation agrees well with the experimental data. The studies show that the length of the potential core zone increases with the increase of the deflection angle. The velocity distribution is consistent with the Gaussian distribution and almost not affected by the deflection angle in potential core zone. The decay rates of flow velocity in the transition zone are 1.195, 1.281, 1.439, and 1.532 corresponding to the unilateral deflection angles, 0°, 3°, 6°, and 9°, respectively. The decay rates of velocity in the transition zone are 1.928 and 2.835 corresponding to the bilateral deflection angles 3° and 6°. It is also found that the spread of velocity is stronger in the vertical direction as the deflection angles become smaller. The spread rates of velocity with unilateral deflection wall are higher than those with bilateral deflection walls in the horizontal plane in the pool.
url http://dx.doi.org/10.1155/2017/5943143
work_keys_str_mv AT xinli numericalsimulationofanoffsetjetinboundedpoolwithdeflectionwall
AT yurongwang numericalsimulationofanoffsetjetinboundedpoolwithdeflectionwall
AT jianminzhang numericalsimulationofanoffsetjetinboundedpoolwithdeflectionwall
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