Large eddy simulation of energy gradient field in a centrifugal pump impeller

Author(s):  
Xiaoping Chen ◽  
Zuchao Zhu ◽  
Hua-Shu Dou ◽  
Yi Li

Large eddy simulation of the fluid flow in a centrifugal pump impeller is conducted at design load and quarter load, and the energy gradient field is analyzed to reveal the behavior of internal flow. A universal equation for calculating the energy gradient function, which is defined as the ratio of energy increase (transversal gradient of the mechanical energy gradient) to energy loss (stream-wise gradient of the work done by shear stress), is adopted. Research results show that positive and negative 0.3 for the logarithm of energy gradient function are critical values that reflect dominant energy increase and dominant energy loss, respectively. The large eddy simulation results indicate that the magnitude and shape of energy gradient field are affected by turbulent fluctuation. The energy gradient field in the impeller at mid-height has more small-scale features than those in the impeller at zero and one heights. The regions of dominant energy increase and dominant energy loss are highly distinct at both design load and quarter load. In some large areas, neither dominant energy increase nor dominant energy loss is observed at quarter load in the impeller passage. These results, which are mainly attributed to a highly separated flow, are not evident at design load. The region of dominant energy increase at design load is larger than that at quarter load, particularly close to the volute. The magnitude of mean logarithm of energy gradient function at quarter load is evidently smaller than that at design load, but its value remains higher than 1.0.

Symmetry ◽  
2021 ◽  
Vol 13 (2) ◽  
pp. 311
Author(s):  
Renfei Kuang ◽  
Xiaoping Chen ◽  
Zhiming Zhang ◽  
Zuchao Zhu ◽  
Yu Li

This paper presents a large eddy simulation of a centrifugal pump impeller during a transient condition. The flow rate is sinusoidal and oscillates between 0.25Qd (Qd indicates design load) and 0.75Qd when the rotating speed is maintained. Research shows that in one period, the inlet flow rate will twice reach 0.5Qd, and among the impeller of one moment is a stall state, but the other is a non-stall state. In the process of flow development, the evolution of low-frequency pressure fluctuation shows an obviously sinusoidal form, whose frequency is insensitive to the monitoring position and equals to that of the flow rate. However, inside the impeller, the phase and amplitude in the stall passages lag behind more and are stronger than that in the non-stall passages. Meanwhile, the strongest region of the high-frequency pressure fluctuation appears in the stall passages at the transient rising stage. The second dominant frequency in stall passages is 2.5 times to that in non-stall passages. In addition, similar to the pressure fluctuation, the evolution of the low-frequency head shows a sinusoidal form, whose phase is lagging behind that by one-third of a period in the inlet flow rate.


2007 ◽  
Vol 23 (6) ◽  
pp. 635-643 ◽  
Author(s):  
Xuelin Tang ◽  
Fujun Wang ◽  
Yulin Wu

2003 ◽  
Vol 125 (1) ◽  
pp. 73-83 ◽  
Author(s):  
Rikke K. Byskov ◽  
Christian B. Jacobsen ◽  
Nicholas Pedersen

The flow field in a shrouded six-bladed centrifugal pump impeller has been investigated using large eddy simulation (LES). The effect of the subgrid scales has been modeled through a localized dynamic Smagorinsky model implemented in the commercial CFD code FINE/Turbo. A detailed analysis of the results of LES at design load, Q=Qd, and severe off-design conditions, at quarter-load Q=0.25Qd, is presented. At design load LES reveals a well-behaved flow field with no significant separation. At quarter-load significant differences between adjacent impeller passages are revealed. A steady nonrotating stall phenomenon is observed in the entrance of one passage and a relative eddy develops in the remaining part of the passage. The stall unblocks the adjacent passage which exhibits a flow dominated by rotational effects. Velocities predicted by LES and steady-state Reynolds averaged Navier-Stokes (RANS) simulations based on the Baldwin-Lomax and Chien k-ε turbulence models are compared with experimental data obtained from particle image velocimetry (PIV). The complex two-channel phenomena observed by LES is with satisfactory agreement confirmed by PIV. However, it is found that the two RANS models do not reproduce the stall phenomenon observed at quarterload and are incapable of detecting the differences between the two passages.


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