TY - JOUR
T1 - Numerical study of coupled flow in blocking pulsed jet impinging on a rotating wall
AU - Zhang, Li
AU - Wang, Chuan
AU - Zhang, Yingchong
AU - Xiang, Wei
AU - He, Zhaoming
AU - Shi, Weidong
N1 - Funding Information:
This work was supported by the National Natural Science Foundation of China (No. 51979240 and 51609105).
Funding Information:
This research was funded by the National Natural Science Foundation of China (No. 51979240 and 51609105).
Publisher Copyright:
© 2021, The Brazilian Society of Mechanical Sciences and Engineering.
PY - 2021/11
Y1 - 2021/11
N2 - In order to study the complex unsteady flow characteristics of pulsed jet impinging on a rotating wall, the Wray–Agarwal turbulence model was adopted. The following conditions were used to simulate the internal flow mechanism, namely: jet with Re = 10,000; rotational speed n = 500 rpm; impinging height H/D = 5; pulse period T = 0.5 s + 0.5 s. The results show that: (1) The flow field structure of pulsed jet impinging the rotating wall is symmetrical about the jet axis. With the development of time, a pair of entrainment vortices and rotating vortices are formed on both sides of the jet and on the rotating wall, respectively. (2) In the vicinity of the jet outlet, the radial distribution of the velocity V gradually becomes non-uniform as time progresses and eventually coincides with the velocity at steady state. (3) During 0 s ≤ t < 0.5 s, the velocity at nozzle-exit increases with time, and the V/Vj along the axis coincides with the steady state. During 0.5 s ≤ t < 1 s, the nozzle-exit velocity V/Vj decreases to 0, along the axis direction, the V/Vj increase first and then decrease. (4) The impact pressure of pulsed jet on the impact wall is greater than that of continuous jet on the impact wall in a certain period when water hammer effect occurs.
AB - In order to study the complex unsteady flow characteristics of pulsed jet impinging on a rotating wall, the Wray–Agarwal turbulence model was adopted. The following conditions were used to simulate the internal flow mechanism, namely: jet with Re = 10,000; rotational speed n = 500 rpm; impinging height H/D = 5; pulse period T = 0.5 s + 0.5 s. The results show that: (1) The flow field structure of pulsed jet impinging the rotating wall is symmetrical about the jet axis. With the development of time, a pair of entrainment vortices and rotating vortices are formed on both sides of the jet and on the rotating wall, respectively. (2) In the vicinity of the jet outlet, the radial distribution of the velocity V gradually becomes non-uniform as time progresses and eventually coincides with the velocity at steady state. (3) During 0 s ≤ t < 0.5 s, the velocity at nozzle-exit increases with time, and the V/Vj along the axis coincides with the steady state. During 0.5 s ≤ t < 1 s, the nozzle-exit velocity V/Vj decreases to 0, along the axis direction, the V/Vj increase first and then decrease. (4) The impact pressure of pulsed jet on the impact wall is greater than that of continuous jet on the impact wall in a certain period when water hammer effect occurs.
KW - Blocking pulsed jet
KW - Flow mechanism
KW - Numerical simulation
KW - Rotating wall
UR - http://www.scopus.com/inward/record.url?scp=85117693262&partnerID=8YFLogxK
U2 - 10.1007/s40430-021-03212-0
DO - 10.1007/s40430-021-03212-0
M3 - Article
AN - SCOPUS:85117693262
SN - 1678-5878
VL - 43
JO - Journal of the Brazilian Society of Mechanical Sciences and Engineering
JF - Journal of the Brazilian Society of Mechanical Sciences and Engineering
IS - 11
M1 - 508
ER -