Numerical investigation of heat transfer performance of synthetic jet impingement onto dimpled/protrusioned surface
Dynamic mesh methods and user defined functions are adopted and the shear stress transport k-ω turbulent model has been used in the numerical investigation of heat transfer performance of synthetic jet impingement onto dimple/protrusioned surface. The results show that the local time-averag...
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VINCA Institute of Nuclear Sciences
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doaj-6e534cc90ad9419f9d9a65bc325170ec2021-01-02T07:15:06ZengVINCA Institute of Nuclear SciencesThermal Science0354-98362334-71632015-01-0119suppl. 122122910.2298/TSCI15S1S21Z0354-983615221ZNumerical investigation of heat transfer performance of synthetic jet impingement onto dimpled/protrusioned surfaceZhang Di0Yang Ke1Huan-Cheng Qu2Gao Ji3Xi’an Jiaotong University, School of Energy and Power Engineering, Xi’an, ChinaXi’an Jiaotong University, School of Energy and Power Engineering, Xi’an, ChinaXi’an Jiaotong University, School of Energy and Power Engineering, Xi’an, ChinaXi’an Jiaotong University, School of Energy and Power Engineering, Xi’an, ChinaDynamic mesh methods and user defined functions are adopted and the shear stress transport k-ω turbulent model has been used in the numerical investigation of heat transfer performance of synthetic jet impingement onto dimple/protrusioned surface. The results show that the local time-averaged Nusselt number of the dimpled/protrusioned target surface tends to be much closer with that of flat cases with increasing of frequency. The heat transfer performance gets better when frequency increases. The area-averaged time-averaged Nusselt number of protrusioned target surface is the most close to that of flat cases when f = 320 Hz while it is the smallest among the synthetic jet cases in dimpled target surface. The heat transfer enhancement performance of synthetic jet is 30 times better than that of natural convection. The time-averaged Nusselt number of stagnation point in the protrusioned target surface is higher than that of flat target surface while it is lower in the dimpled surface than that of flat surface no matter in the synthetic jet, steady jet or natural convection cases. Meanwhile, the timeaveraged Nusselt number of stagnation point in the synthetic jet cases increases with the increasing of frequency. It is worth pointing out that the time-averaged Nusselt number of stagnation point is lower than that of steady cases when the frequency is low. However, it shows a bit higher than that of steady cases when f = 320 Hz.http://www.doiserbia.nb.rs/img/doi/0354-9836/2015/0354-983615221Z .pdfsynthetic jetdimpled/protrusioned targetheat transfer enhancement |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Zhang Di Yang Ke Huan-Cheng Qu Gao Ji |
spellingShingle |
Zhang Di Yang Ke Huan-Cheng Qu Gao Ji Numerical investigation of heat transfer performance of synthetic jet impingement onto dimpled/protrusioned surface Thermal Science synthetic jet dimpled/protrusioned target heat transfer enhancement |
author_facet |
Zhang Di Yang Ke Huan-Cheng Qu Gao Ji |
author_sort |
Zhang Di |
title |
Numerical investigation of heat transfer performance of synthetic jet impingement onto dimpled/protrusioned surface |
title_short |
Numerical investigation of heat transfer performance of synthetic jet impingement onto dimpled/protrusioned surface |
title_full |
Numerical investigation of heat transfer performance of synthetic jet impingement onto dimpled/protrusioned surface |
title_fullStr |
Numerical investigation of heat transfer performance of synthetic jet impingement onto dimpled/protrusioned surface |
title_full_unstemmed |
Numerical investigation of heat transfer performance of synthetic jet impingement onto dimpled/protrusioned surface |
title_sort |
numerical investigation of heat transfer performance of synthetic jet impingement onto dimpled/protrusioned surface |
publisher |
VINCA Institute of Nuclear Sciences |
series |
Thermal Science |
issn |
0354-9836 2334-7163 |
publishDate |
2015-01-01 |
description |
Dynamic mesh methods and user defined functions are adopted and the shear
stress transport k-ω turbulent model has been used in the numerical
investigation of heat transfer performance of synthetic jet impingement onto
dimple/protrusioned surface. The results show that the local time-averaged
Nusselt number of the dimpled/protrusioned target surface tends to be much
closer with that of flat cases with increasing of frequency. The heat
transfer performance gets better when frequency increases. The area-averaged
time-averaged Nusselt number of protrusioned target surface is the most close
to that of flat cases when f = 320 Hz while it is the smallest among the
synthetic jet cases in dimpled target surface. The heat transfer enhancement
performance of synthetic jet is 30 times better than that of natural
convection. The time-averaged Nusselt number of stagnation point in the
protrusioned target surface is higher than that of flat target surface while
it is lower in the dimpled surface than that of flat surface no matter in the
synthetic jet, steady jet or natural convection cases. Meanwhile, the
timeaveraged Nusselt number of stagnation point in the synthetic jet cases
increases with the increasing of frequency. It is worth pointing out that the
time-averaged Nusselt number of stagnation point is lower than that of steady
cases when the frequency is low. However, it shows a bit higher than that of
steady cases when f = 320 Hz. |
topic |
synthetic jet dimpled/protrusioned target heat transfer enhancement |
url |
http://www.doiserbia.nb.rs/img/doi/0354-9836/2015/0354-983615221Z .pdf |
work_keys_str_mv |
AT zhangdi numericalinvestigationofheattransferperformanceofsyntheticjetimpingementontodimpledprotrusionedsurface AT yangke numericalinvestigationofheattransferperformanceofsyntheticjetimpingementontodimpledprotrusionedsurface AT huanchengqu numericalinvestigationofheattransferperformanceofsyntheticjetimpingementontodimpledprotrusionedsurface AT gaoji numericalinvestigationofheattransferperformanceofsyntheticjetimpingementontodimpledprotrusionedsurface |
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1724357588119715840 |