TY - JOUR
T1 - The formation process of annular starting jets
AU - Zhu, Jianwei
AU - Zhang, Guoqing
AU - Gao, Lei
AU - Yu, S. C.M.
N1 - Publisher Copyright:
©
PY - 2022/10/25
Y1 - 2022/10/25
N2 - The formation and evolution process of the outer vortex ring (denoted as OV0) in annular starting jets has been studied numerically at stroke ratio, and Reynolds number, where is the outer diameter of orifice, is the length of the fluid column, and are the ratio and difference between inner and outer radii of the annular orifice, respectively. The initial formation process of OV0 is found to be similar to that of the leading vortex ring in a circular starting jet, but the circulation strength is relatively lower and decreases gradually with increasing. The pinch-off process will also appear after OV0 grows to a certain size but is different from that of the circular starting jet. On one hand, OV0 is stretched and deformed by the strain field generated by the trailing jet's instability, and vorticity would be shed. On the other hand, OV0 accelerates the irrotational fluids around it under viscous action so as to form the induced velocity field, which would consume energy causing it to shed vorticity further under the limit of the Kelvin-Benjamin variational principle. Furthermore, OV0 would eventually become a stable vortex ring whose non-dimensional circulation ) is found to be between 0.59-0.62 and it would not change with different at, which is much less than the 2-2.5 of circular starting jets.
AB - The formation and evolution process of the outer vortex ring (denoted as OV0) in annular starting jets has been studied numerically at stroke ratio, and Reynolds number, where is the outer diameter of orifice, is the length of the fluid column, and are the ratio and difference between inner and outer radii of the annular orifice, respectively. The initial formation process of OV0 is found to be similar to that of the leading vortex ring in a circular starting jet, but the circulation strength is relatively lower and decreases gradually with increasing. The pinch-off process will also appear after OV0 grows to a certain size but is different from that of the circular starting jet. On one hand, OV0 is stretched and deformed by the strain field generated by the trailing jet's instability, and vorticity would be shed. On the other hand, OV0 accelerates the irrotational fluids around it under viscous action so as to form the induced velocity field, which would consume energy causing it to shed vorticity further under the limit of the Kelvin-Benjamin variational principle. Furthermore, OV0 would eventually become a stable vortex ring whose non-dimensional circulation ) is found to be between 0.59-0.62 and it would not change with different at, which is much less than the 2-2.5 of circular starting jets.
KW - jets
KW - vortex interactions
UR - http://www.scopus.com/inward/record.url?scp=85140356096&partnerID=8YFLogxK
U2 - 10.1017/jfm.2022.795
DO - 10.1017/jfm.2022.795
M3 - Article
AN - SCOPUS:85140356096
SN - 0022-1120
VL - 949
JO - Journal of Fluid Mechanics
JF - Journal of Fluid Mechanics
M1 - A47
ER -