Aerodynamics of two-dimensional bristled wings in low-Reynolds-number flow

The smallest flying insects commonly possess bristled wings and use drag to provide flight forces. A bristled wing, with a wing area about 10% of that of a flat-plate wing, operating at the relevant Reynolds number of 5–15, produces a drag close to the plate wing. How this is done is not well unders...

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Main Authors: Yu Kai Wu, Yan Peng Liu, Mao Sun
Format: Article
Language:English
Published: AIP Publishing LLC 2021-04-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/5.0050236
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spelling doaj-4487686efa9a4318842e401c6df2f5982021-05-04T14:07:18ZengAIP Publishing LLCAIP Advances2158-32262021-04-01114045322045322-1010.1063/5.0050236Aerodynamics of two-dimensional bristled wings in low-Reynolds-number flowYu Kai Wu0Yan Peng Liu1Mao Sun2Institute of Fluid Mechanics, Beihang University, Beijing 100191, ChinaInstitute of Fluid Mechanics, Beihang University, Beijing 100191, ChinaInstitute of Fluid Mechanics, Beihang University, Beijing 100191, ChinaThe smallest flying insects commonly possess bristled wings and use drag to provide flight forces. A bristled wing, with a wing area about 10% of that of a flat-plate wing, operating at the relevant Reynolds number of 5–15, produces a drag close to the plate wing. How this is done is not well understood. Here, detailed flows around each of the bristles are investigated numerically using simple model wings, and the following results are shown. (1) The drag production mechanism of the bristled wing is different from that of the plate wing: For the plate wing, the flow is blocked by the wing, giving a small positive pressure on the windward surface, and there exists a pair of weak vortices on the wing back, giving a small negative pressure on the leeward surface; the drag is due to the pressure forces (the frictional stress has almost no contribution). For the bristled wing, each bristle operates in a creeping flow and produces thick and strong shear layers. Strong viscous force generates a very large pressure difference between the windward and leeward surfaces of each bristle and very large frictional stress on the bristle surface, resulting in a large drag on each bristle, and the drag is equally contributed by the pressure and frictional forces. (2) Due to the flow-interference effect, when the bristle number reaches a certain value, a further increase in bristles has little effect on force production but has the disadvantage of increasing wing mass; this means that for a bristled wing of miniature insects, the distribution density of the bristles will not be too large, which agrees with observations.http://dx.doi.org/10.1063/5.0050236
collection DOAJ
language English
format Article
sources DOAJ
author Yu Kai Wu
Yan Peng Liu
Mao Sun
spellingShingle Yu Kai Wu
Yan Peng Liu
Mao Sun
Aerodynamics of two-dimensional bristled wings in low-Reynolds-number flow
AIP Advances
author_facet Yu Kai Wu
Yan Peng Liu
Mao Sun
author_sort Yu Kai Wu
title Aerodynamics of two-dimensional bristled wings in low-Reynolds-number flow
title_short Aerodynamics of two-dimensional bristled wings in low-Reynolds-number flow
title_full Aerodynamics of two-dimensional bristled wings in low-Reynolds-number flow
title_fullStr Aerodynamics of two-dimensional bristled wings in low-Reynolds-number flow
title_full_unstemmed Aerodynamics of two-dimensional bristled wings in low-Reynolds-number flow
title_sort aerodynamics of two-dimensional bristled wings in low-reynolds-number flow
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2021-04-01
description The smallest flying insects commonly possess bristled wings and use drag to provide flight forces. A bristled wing, with a wing area about 10% of that of a flat-plate wing, operating at the relevant Reynolds number of 5–15, produces a drag close to the plate wing. How this is done is not well understood. Here, detailed flows around each of the bristles are investigated numerically using simple model wings, and the following results are shown. (1) The drag production mechanism of the bristled wing is different from that of the plate wing: For the plate wing, the flow is blocked by the wing, giving a small positive pressure on the windward surface, and there exists a pair of weak vortices on the wing back, giving a small negative pressure on the leeward surface; the drag is due to the pressure forces (the frictional stress has almost no contribution). For the bristled wing, each bristle operates in a creeping flow and produces thick and strong shear layers. Strong viscous force generates a very large pressure difference between the windward and leeward surfaces of each bristle and very large frictional stress on the bristle surface, resulting in a large drag on each bristle, and the drag is equally contributed by the pressure and frictional forces. (2) Due to the flow-interference effect, when the bristle number reaches a certain value, a further increase in bristles has little effect on force production but has the disadvantage of increasing wing mass; this means that for a bristled wing of miniature insects, the distribution density of the bristles will not be too large, which agrees with observations.
url http://dx.doi.org/10.1063/5.0050236
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AT yanpengliu aerodynamicsoftwodimensionalbristledwingsinlowreynoldsnumberflow
AT maosun aerodynamicsoftwodimensionalbristledwingsinlowreynoldsnumberflow
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