Contents lists available at ScienceDirect International Journal of Heat and Fluid Flow journal homepage: www.elsevier.com/locate/ijhff Flow characteristics in a volute-type centrifugal pump using large eddy simulation Beomjun Kye a , Keuntae Park a , Haecheon Choi a, , Myungsung Lee b , Joo-Han Kim b a Department of Mechanical and Aerospace Engineering, Seoul National University, 1, Gwanak-ro, Gwanak-gu, Seoul 08826, Republic of Korea b Intelligent Mechatronics Research Center, Korea Electronics Technology Institute, 388, Songnae-daero, Bucheon 14502, Republic of Korea ARTICLE INFO Keywords: Large eddy simulation Centrifugal pump Flow separation Leakage Impeller-volute interaction ABSTRACT The ow characteristics in a volute-type centrifugal pump operating at design (Q d = 35 m 3 /h) and o-design (Q o = 20 m 3 /h) conditions are investigated using large eddy simulation. Numerical results indicate that se- paration bubbles are generated on both the pressure and suction sides of impeller blades. At the o-design condition, the blade pressure side contains a larger recirculation zone with highly unsteady characteristics due to impeller-volute interactions. The vortices shed from a blade trailing edge due to its rotation strongly interact with those from the following blade and leakage through radial gaps at the o-design condition, generating stronger vortices in a wider region inside the volute, whereas this mutual interaction is weak at the design condition. Flow separation also occurs around the volute tongue at both operating conditions. At the o-design condition, a part of high-pressure uid discharged from the volute does not follow the main stream to the outlet duct but re-enters into the volute area near the volute tongue. This pressurized uid forms a high adverse pressure gradient on the blade pressure side, resulting in strong unsteady separation there. Also, a high pressure gradient in the axial direction at the radial gaps is formed especially near the volute tongue, creating the leakage into the cavities. Inside the volute, azimuthal vortices exist and grow along the volute passage. A secondary motion induced by these vortices also signicantly aects the leakage to the cavities. All of these ow losses contain unsteady features that are strongly inuenced by impeller-volute interactions, especially at the o- design condition. 1. Introduction A centrifugal pump, which is one of the most commonly used tur- bomachines, is widely utilized in residential buildings as well as in industries. In centrifugal pumps, complex three-dimensional ow phe- nomena involving turbulence, secondary ows and unsteadiness occur (Brennen, 1994). To meet various ranges of pressure rise and ow rates required, many centrifugal pumps are operated at o-design conditions as well as at the design condition. At o-design conditions, the ow characteristics inside centrifugal pumps become more complex than those at the design condition. Commonly used steady Reynolds-aver- aged Navier-Stokes (RANS) turbulence models often inaccurately pre- dict the ow inside centrifugal pumps at o-design conditions (Byskov et al., 2003). For this reason, a large eddy simulation (LES) technique is a promising alternative to predict such complex ow phenomena inside centrifugal pumps. Kato et al. (2003) conducted LES to predict the ow in a mixed-ow pump at o-design conditions, where the standard Smagorinsky model together with the van Driest damping function near the wall was used as a subgrid-scale model. The results from LES were compared with those measured by a laser Doppler velocimetry (LDV) and good agreements were obtained. Byskov et al. (2003) studied the ow in a shrouded six-bladed centrifugal pump impeller at design and o-design conditions using the localized dynamic Smagorinsky model (Piomelli and Liu, 1995). They showed that, at an o-design condition, LES predicts complex ow phenomena, such as steady nonrotating stalls and ow asymmetry between impeller passages, better than RANS. Although most of previous LESs of ows in centrifugal pumps used the standard Smagorinsky model or simulated ow only in ro- tating parts, LESs using more advanced subgrid-scale models such as a ltered structured function model (Posa et al., 2011) or a wall-adapting local eddy-viscosity model (Posa et al., 2015, 2016) were also per- formed to study the ow structures in a mixed-ow pump including all rotating and stationary parts. They showed that LES accurately predicts unsteady ow features, such as separated ow near the blade surfaces, backward ow near the shroud surface and rotor-stator interaction, at design and o-design conditions. A detached eddy simulation (DES) was also conducted to study the ow in a radial diuser pump at low https://doi.org/10.1016/j.ijheatuidow.2018.04.016 Received 5 December 2017; Received in revised form 30 March 2018; Accepted 30 April 2018 Corresponding author at: Institute of Advanced Machines and Design, Seoul National University, Republic of Korea. E-mail address: choi@snu.ac.kr (H. Choi). International Journal of Heat and Fluid Flow 72 (2018) 52–60 0142-727X/ © 2018 Elsevier Inc. All rights reserved. T