A New Method of Identifying the Aerodynamic Dipole Sound Source in the Near Wall Flow

Consider that the sound dipole source in the flow field is composed of multiple micro-spherical oscillating sources. An aerodynamic sound source identification method is established by the relationship among the oscillating source, the radiated sound pressure, and the pressure gradient of flow in th...

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Bibliographic Details
Main Authors: Wang, Y. (Author), Zhang, H. (Author)
Format: Article
Language:English
Published: MDPI 2023
Subjects:
Online Access:View Fulltext in Publisher
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LEADER 02237nam a2200229Ia 4500
001 10.3390-math11092070
008 230529s2023 CNT 000 0 und d
020 |a 22277390 (ISSN) 
245 1 0 |a A New Method of Identifying the Aerodynamic Dipole Sound Source in the Near Wall Flow 
260 0 |b MDPI  |c 2023 
856 |z View Fulltext in Publisher  |u https://doi.org/10.3390/math11092070 
856 |z View in Scopus  |u https://www.scopus.com/inward/record.uri?eid=2-s2.0-85159170223&doi=10.3390%2fmath11092070&partnerID=40&md5=8a3cd1b4c0d4fd74633370b4bed9b66e 
520 3 |a Consider that the sound dipole source in the flow field is composed of multiple micro-spherical oscillating sources. An aerodynamic sound source identification method is established by the relationship among the oscillating source, the radiated sound pressure, and the pressure gradient of flow in the near-wall flow field, and the formula for calculating the sound power of the sound dipole source in unsteady flow is derived. It shows that the power of sound dipole sources is proportional to the square of the oscillating force or pressure gradient. The combination of the formula and CFD method is further applied to the flow around the cylinder, which clearly presents the sound power and location characteristics of sound dipole sources. Further, the relationship between the sound source and the flow separation, or flow vortex shedding, is analyzed. The corresponding correlation analysis is also carried out, which indicates that the sound dipole source exists in a finite area of the attached wall. The front end of the area is at the separation point along the circumferential direction of the wall, and the end is at the location where the separation vortex completely falls off and a trailing vortex begins to form. In addition, the thickness of the area exists along the radial direction and gradually increases backward. © 2023 by the authors. 
650 0 4 |a aerodynamic sound dipole source 
650 0 4 |a Computational Fluid Dynamics (CFD) 
650 0 4 |a flow around circular cylinder 
650 0 4 |a sound power 
650 0 4 |a turbulence field 
700 1 0 |a Wang, Y.  |e author 
700 1 0 |a Wang, Y.  |e author 
700 1 0 |a Zhang, H.  |e author 
773 |t Mathematics