Numerical simulation of unsteady cavitating flows around a transient pitching hydrofoil
The objective of this paper is to improve the understanding of the influence of multiphase flow on the turbulent closure model, the interplay between vorticity fields and cavity dynamics around a pitching hydrofoil. The effects of pitching rate on the sub- cavitating and cavitating response of the p...
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          | Published in | Science China. Technological sciences Vol. 57; no. 1; pp. 101 - 116 | 
|---|---|
| Main Authors | , , | 
| Format | Journal Article | 
| Language | English | 
| Published | 
        Berlin/Heidelberg
          Springer Berlin Heidelberg
    
        2014
     | 
| Subjects | |
| Online Access | Get full text | 
| ISSN | 1674-7321 1869-1900  | 
| DOI | 10.1007/s11431-013-5423-y | 
Cover
| Abstract | The objective of this paper is to improve the understanding of the influence of multiphase flow on the turbulent closure model, the interplay between vorticity fields and cavity dynamics around a pitching hydrofoil. The effects of pitching rate on the sub- cavitating and cavitating response of the pitching hydrofoil are also investigated. In particular, we focus on the interactions between cavity inception, growth, and shedding and the vortex flow structures, and their impacts on the hydrofoil performance. The calculations are 2-D and performed by solving the incompressible, multiphase Unsteady Reynolds Averaged Navier Stokes (URANS) equations via the commercial CFD code CFX. The k-co SST (Shear Stress Transport) turbulence model is used along with the transport equation-based cavitation models. The density correction function is considered to reduce the eddy viscosity according to the computed local fluid mixture density. The calculation results are validated with experiments conducted by Ducoin et al. (see Computational and experimental investigation of flow over a transient pitching hydrofoil, Eur J Mech/B Fluids, 2009, 28:728-743 and An experimental analysis of fluid structure interaction of a flexible hydrofoil in vari- ous flow regimes including cavitating flow, Eur J Mech B/fluids, 2012, 36: 63-74). Results are shown for a NACA66 hydro- foil subject to slow (quasi static, t2=6~/s, &* =0.18) and fast (dynamic, &=63~/s, dr" =1.89) pitching motions from a =0~ to a =15~. Both subcavitaing (or =8.0) and cavitating (cr=3.0) flows are considered. For subcavitating flow (or=8.0), low frequency fluctuations have been observed when the leading edge vortex shedding occurs during stall, and delay of stall is ob- served with increasing pitching velocity. For cavitating flow (tr=3.0), small leading edge cavities are observed with the slow pitching case, which significantly modified the vortex dynamics at high angles of attack, leading to high frequency fluctuations of the hydrodynamic coefficients and different stall behaviors compared to the subcavitating flow at the same pitching rate. On the other hand, for the fast pitching case at or=3.0, large-scale sheet/cloud cavitation is observed, the cavity behavior is un- steady and has a strong impact on the hydrodynamic response, which leads to high amplitude fluctuations of the hydrodynamic coefficients, as well as significant changes in the stall and post-stall behavior. The numerical results also show that the local density modification helps to reduce turbulent eddy viscosity in the cavitating region, which significantly modifies the cavity lengths and shedding frequencies, particularly for the fast pitching case. In general, compared with the experimental visualiza- tions, the numerical results with local density correction have been found to agree well with experimental measurements and observations for both slow and fast transient pitching cases. | 
    
|---|---|
| AbstractList | The objective of this paper is to improve the understanding of the influence of multiphase flow on the turbulent closure model, the interplay between vorticity fields and cavity dynamics around a pitching hydrofoil. The effects of pitching rate on the subcavitating and cavitating response of the pitching hydrofoil are also investigated. In particular, we focus on the interactions between cavity inception, growth, and shedding and the vortex flow structures, and their impacts on the hydrofoil performance. The calculations are 2-D and performed by solving the incompressible, multiphase Unsteady Reynolds Averaged Navier Stokes (URANS) equations via the commercial CFD code CFX. The
k
-
ω
SST (Shear Stress Transport) turbulence model is used along with the transport equation-based cavitation models. The density correction function is considered to reduce the eddy viscosity according to the computed local fluid mixture density. The calculation results are validated with experiments conducted by Ducoin et al. (see Computational and experimental investigation of flow over a transient pitching hydrofoil, Eur J Mech/B Fluids, 2009, 28: 728–743 and An experimental analysis of fluid structure interaction of a flexible hydrofoil in various flow regimes including cavitating flow, Eur J Mech B/fluids, 2012, 36: 63–74). Results are shown for a NACA66 hydrofoil subject to slow (quasi static,
,
) and fast (dynamic,
,
) pitching motions from
α
= 0° to
α
= 15°. Both subcavitaing (
σ
=8.0) and cavitating (
σ
=3.0) flows are considered. For subcavitating flow (
σ
=8.0), low frequency fluctuations have been observed when the leading edge vortex shedding occurs during stall, and delay of stall is observed with increasing pitching velocity. For cavitating flow (
σ
=3.0), small leading edge cavities are observed with the slow pitching case, which significantly modified the vortex dynamics at high angles of attack, leading to high frequency fluctuations of the hydrodynamic coefficients and different stall behaviors compared to the subcavitating flow at the same pitching rate. On the other hand, for the fast pitching case at
σ
=3.0, large-scale sheet/cloud cavitation is observed, the cavity behavior is unsteady and has a strong impact on the hydrodynamic response, which leads to high amplitude fluctuations of the hydrodynamic coefficients, as well as significant changes in the stall and post-stall behavior. The numerical results also show that the local density modification helps to reduce turbulent eddy viscosity in the cavitating region, which significantly modifies the cavity lengths and shedding frequencies, particularly for the fast pitching case. In general, compared with the experimental visualizations, the numerical results with local density correction have been found to agree well with experimental measurements and observations for both slow and fast transient pitching cases. The objective of this paper is to improve the understanding of the influence of multiphase flow on the turbulent closure model, the interplay between vorticity fields and cavity dynamics around a pitching hydrofoil. The effects of pitching rate on the sub-cavitating and cavitating response of the pitching hydrofoil are also investigated. In particular, we focus on the interactions between cavity inception, growth, and shedding and the vortex flow structures, and their impacts on the hydrofoil performance. The calculations are 2-D and performed by solving the incompressible, multiphase Unsteady Reynolds Averaged Navier Stokes (URANS) equations via the commercial CFD code CFX. The objective of this paper is to improve the understanding of the influence of multiphase flow on the turbulent closure model, the interplay between vorticity fields and cavity dynamics around a pitching hydrofoil. The effects of pitching rate on the sub- cavitating and cavitating response of the pitching hydrofoil are also investigated. In particular, we focus on the interactions between cavity inception, growth, and shedding and the vortex flow structures, and their impacts on the hydrofoil performance. The calculations are 2-D and performed by solving the incompressible, multiphase Unsteady Reynolds Averaged Navier Stokes (URANS) equations via the commercial CFD code CFX. The k-co SST (Shear Stress Transport) turbulence model is used along with the transport equation-based cavitation models. The density correction function is considered to reduce the eddy viscosity according to the computed local fluid mixture density. The calculation results are validated with experiments conducted by Ducoin et al. (see Computational and experimental investigation of flow over a transient pitching hydrofoil, Eur J Mech/B Fluids, 2009, 28:728-743 and An experimental analysis of fluid structure interaction of a flexible hydrofoil in vari- ous flow regimes including cavitating flow, Eur J Mech B/fluids, 2012, 36: 63-74). Results are shown for a NACA66 hydro- foil subject to slow (quasi static, t2=6~/s, &* =0.18) and fast (dynamic, &=63~/s, dr" =1.89) pitching motions from a =0~ to a =15~. Both subcavitaing (or =8.0) and cavitating (cr=3.0) flows are considered. For subcavitating flow (or=8.0), low frequency fluctuations have been observed when the leading edge vortex shedding occurs during stall, and delay of stall is ob- served with increasing pitching velocity. For cavitating flow (tr=3.0), small leading edge cavities are observed with the slow pitching case, which significantly modified the vortex dynamics at high angles of attack, leading to high frequency fluctuations of the hydrodynamic coefficients and different stall behaviors compared to the subcavitating flow at the same pitching rate. On the other hand, for the fast pitching case at or=3.0, large-scale sheet/cloud cavitation is observed, the cavity behavior is un- steady and has a strong impact on the hydrodynamic response, which leads to high amplitude fluctuations of the hydrodynamic coefficients, as well as significant changes in the stall and post-stall behavior. The numerical results also show that the local density modification helps to reduce turbulent eddy viscosity in the cavitating region, which significantly modifies the cavity lengths and shedding frequencies, particularly for the fast pitching case. In general, compared with the experimental visualiza- tions, the numerical results with local density correction have been found to agree well with experimental measurements and observations for both slow and fast transient pitching cases.  | 
    
| Author | HUANG Biao WU Qin WANG GuoYu | 
    
| AuthorAffiliation | School of Mechanical and Vehicular Engineering, Beijing Institute of Technology, Beijing 100081, China | 
    
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| CitedBy_id | crossref_primary_10_1016_j_oceaneng_2023_116547 crossref_primary_10_1063_5_0189068 crossref_primary_10_1016_j_oceaneng_2019_04_028 crossref_primary_10_1007_s10409_018_0782_z crossref_primary_10_1007_s11431_015_5957_2 crossref_primary_10_1007_s42241_019_0050_0 crossref_primary_10_1088_1755_1315_163_1_012017 crossref_primary_10_3390_jmse7110398 crossref_primary_10_1007_s11431_015_5827_y crossref_primary_10_1063_5_0124388 crossref_primary_10_1155_2014_808034 crossref_primary_10_1016_j_renene_2020_01_006 crossref_primary_10_1007_s10409_015_0484_8 crossref_primary_10_1016_j_renene_2020_07_080 crossref_primary_10_1007_s11431_015_5842_z  | 
    
| Cites_doi | 10.1017/S0022112090001483 10.1016/j.euromechflu.2009.06.001 10.1016/j.ijmultiphaseflow.2012.02.006 10.1016/S1001-6058(10)60084-4 10.1007/s00348-003-0622-0 10.1007/s11431-013-5315-1 10.1017/S0022112088002101 10.1016/j.euromechflu.2012.03.009 10.1017/S0022112004009851 10.1146/annurev.fl.14.010182.001441 10.1115/1.4023650 10.1115/1.4006416 10.1017/S0022112001005420 10.2514/3.45534 10.1115/1.3243624 10.1007/s11431-011-4369-1 10.1006/jfls.1993.1012 10.2514/3.9982 10.1115/1.1486223 10.1299/jsmeb.49.797 10.1016/j.ijheatmasstransfer.2012.06.065 10.1146/annurev.fl.13.010181.001421 10.1016/j.apm.2005.11.019 10.1016/S0045-7930(99)00039-0 10.1016/j.ijmultiphaseflow.2012.11.008 10.1115/1.1524584 10.2514/3.45507 10.2514/3.45621 10.1103/PhysRevE.51.R1649 10.1016/S1001-6058(11)60390-X 10.1016/j.jfluidstructs.2010.11.013 10.1006/jcph.2002.6992 10.2514/3.10246 10.1016/S0376-0421(01)00014-8 10.1002/fld.1047 10.1088/0256-307X/28/2/026401 10.1016/j.jfluidstructs.2011.08.004  | 
    
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| Copyright | Science China Press and Springer-Verlag Berlin Heidelberg 2013 | 
    
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| Keywords | pitching hydrofoil turbulence model unsteady cavitating flow  | 
    
| Language | English | 
    
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| Notes | The objective of this paper is to improve the understanding of the influence of multiphase flow on the turbulent closure model, the interplay between vorticity fields and cavity dynamics around a pitching hydrofoil. The effects of pitching rate on the sub- cavitating and cavitating response of the pitching hydrofoil are also investigated. In particular, we focus on the interactions between cavity inception, growth, and shedding and the vortex flow structures, and their impacts on the hydrofoil performance. The calculations are 2-D and performed by solving the incompressible, multiphase Unsteady Reynolds Averaged Navier Stokes (URANS) equations via the commercial CFD code CFX. The k-co SST (Shear Stress Transport) turbulence model is used along with the transport equation-based cavitation models. The density correction function is considered to reduce the eddy viscosity according to the computed local fluid mixture density. The calculation results are validated with experiments conducted by Ducoin et al. (see Computational and experimental investigation of flow over a transient pitching hydrofoil, Eur J Mech/B Fluids, 2009, 28:728-743 and An experimental analysis of fluid structure interaction of a flexible hydrofoil in vari- ous flow regimes including cavitating flow, Eur J Mech B/fluids, 2012, 36: 63-74). Results are shown for a NACA66 hydro- foil subject to slow (quasi static, t2=6~/s, &* =0.18) and fast (dynamic, &=63~/s, dr" =1.89) pitching motions from a =0~ to a =15~. Both subcavitaing (or =8.0) and cavitating (cr=3.0) flows are considered. For subcavitating flow (or=8.0), low frequency fluctuations have been observed when the leading edge vortex shedding occurs during stall, and delay of stall is ob- served with increasing pitching velocity. For cavitating flow (tr=3.0), small leading edge cavities are observed with the slow pitching case, which significantly modified the vortex dynamics at high angles of attack, leading to high frequency fluctuations of the hydrodynamic coefficients and different stall behaviors compared to the subcavitating flow at the same pitching rate. On the other hand, for the fast pitching case at or=3.0, large-scale sheet/cloud cavitation is observed, the cavity behavior is un- steady and has a strong impact on the hydrodynamic response, which leads to high amplitude fluctuations of the hydrodynamic coefficients, as well as significant changes in the stall and post-stall behavior. The numerical results also show that the local density modification helps to reduce turbulent eddy viscosity in the cavitating region, which significantly modifies the cavity lengths and shedding frequencies, particularly for the fast pitching case. In general, compared with the experimental visualiza- tions, the numerical results with local density correction have been found to agree well with experimental measurements and observations for both slow and fast transient pitching cases. unsteady cavitating flow, pitching hydrofoil, turbulence model 11-5845/TH ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23  | 
    
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2nd Int Symp on Flow Visualization, Bochum year: 1980 ident: 5423_CR9  | 
    
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| SubjectTerms | Cavitation Computational fluid dynamics Engineering Fluid flow Hydrofoils Mathematical models Navier-Stokes equations Turbulent flow Unsteady 实验分析 数值模拟 水动力系数 水翼船 流体结构相互作用 空泡流 计算结果 非定常  | 
    
| Title | Numerical simulation of unsteady cavitating flows around a transient pitching hydrofoil | 
    
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