Pulse pressure loading and erosion pattern of cavitating jet
Various erosion patterns generated through the cavitating water jet impacts under ambient pressure conditions were investigated in experiments and numerical simulations. A series of normalized stand-off distances $l_s/d_o $ ∈ [2.5 13.5] were studied during the erosion acceleration period. Two ring-l...
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Online Access: | http://dx.doi.org/10.1080/19942060.2019.1695675 |
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doaj-091d42e74d154600af4670482287804c2020-12-07T17:17:44ZengTaylor & Francis GroupEngineering Applications of Computational Fluid Mechanics1994-20601997-003X2020-01-0114113615010.1080/19942060.2019.16956751695675Pulse pressure loading and erosion pattern of cavitating jetB. Liu0Y. Pan1F. Ma2School of Mechanical Engineering, University of Science and Technology BeijingSchool of Mechanical Engineering, University of Science and Technology BeijingSchool of Mechanical Engineering, University of Science and Technology BeijingVarious erosion patterns generated through the cavitating water jet impacts under ambient pressure conditions were investigated in experiments and numerical simulations. A series of normalized stand-off distances $l_s/d_o $ ∈ [2.5 13.5] were studied during the erosion acceleration period. Two ring-like erosion areas were observed for comparatively low $l_s/d_o $ ∈ [2.5 6.5]. To gain insight into the pulse pressure loading on the erosion area, numerical calculations were performed using the volume of fluid (VOF) interface capturing methodology combined with the large-eddy simulation turbulence model. The erosion patterns are clarified based on the mass loss and distribution features of the eroded regions. The first ring, generated by the cavitation clouds impingement outside the central stagnation area, mainly contributes to the mass loss. The second ring moves inward, merges into the inner ring and eventually vanishes with increasing $l_s/d_o $. High pressure pulsation is found around the locations of the maximum erosion and the approximate intermediate radius of the second ring. The pressure pulsation in the first ring area are dominated by the frequency of the vortices shedding from the jet nozzle. Several higher frequencies are found as the spectral features of the eroded regions in each pattern.http://dx.doi.org/10.1080/19942060.2019.1695675cavitating jetpulse pressurelarge eddy simulationerosion pattern |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
B. Liu Y. Pan F. Ma |
spellingShingle |
B. Liu Y. Pan F. Ma Pulse pressure loading and erosion pattern of cavitating jet Engineering Applications of Computational Fluid Mechanics cavitating jet pulse pressure large eddy simulation erosion pattern |
author_facet |
B. Liu Y. Pan F. Ma |
author_sort |
B. Liu |
title |
Pulse pressure loading and erosion pattern of cavitating jet |
title_short |
Pulse pressure loading and erosion pattern of cavitating jet |
title_full |
Pulse pressure loading and erosion pattern of cavitating jet |
title_fullStr |
Pulse pressure loading and erosion pattern of cavitating jet |
title_full_unstemmed |
Pulse pressure loading and erosion pattern of cavitating jet |
title_sort |
pulse pressure loading and erosion pattern of cavitating jet |
publisher |
Taylor & Francis Group |
series |
Engineering Applications of Computational Fluid Mechanics |
issn |
1994-2060 1997-003X |
publishDate |
2020-01-01 |
description |
Various erosion patterns generated through the cavitating water jet impacts under ambient pressure conditions were investigated in experiments and numerical simulations. A series of normalized stand-off distances $l_s/d_o $ ∈ [2.5 13.5] were studied during the erosion acceleration period. Two ring-like erosion areas were observed for comparatively low $l_s/d_o $ ∈ [2.5 6.5]. To gain insight into the pulse pressure loading on the erosion area, numerical calculations were performed using the volume of fluid (VOF) interface capturing methodology combined with the large-eddy simulation turbulence model. The erosion patterns are clarified based on the mass loss and distribution features of the eroded regions. The first ring, generated by the cavitation clouds impingement outside the central stagnation area, mainly contributes to the mass loss. The second ring moves inward, merges into the inner ring and eventually vanishes with increasing $l_s/d_o $. High pressure pulsation is found around the locations of the maximum erosion and the approximate intermediate radius of the second ring. The pressure pulsation in the first ring area are dominated by the frequency of the vortices shedding from the jet nozzle. Several higher frequencies are found as the spectral features of the eroded regions in each pattern. |
topic |
cavitating jet pulse pressure large eddy simulation erosion pattern |
url |
http://dx.doi.org/10.1080/19942060.2019.1695675 |
work_keys_str_mv |
AT bliu pulsepressureloadinganderosionpatternofcavitatingjet AT ypan pulsepressureloadinganderosionpatternofcavitatingjet AT fma pulsepressureloadinganderosionpatternofcavitatingjet |
_version_ |
1724397451439243264 |