Experimental and numerical investigation on the effect of tip leakage vortex induced cavitating flow on pressure fluctuation in an axial flow pump
Autor: | Xu Bin, Zhang Desheng, B.P.M. van Esch, Shen Xi, Shi Weidong |
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Přispěvatelé: | Group Kuerten, Power & Flow, EIRES Eng. for Sustainable Energy Systems |
Jazyk: | angličtina |
Rok vydání: | 2021 |
Předmět: |
Cavitation
Materials science 060102 archaeology Axial-flow pump Renewable Energy Sustainability and the Environment 020209 energy 06 humanities and the arts 02 engineering and technology Mechanics Pressure fluctuation Volumetric flow rate Vortex Impeller Amplitude Tip leakage vortex Frequency domain 0202 electrical engineering electronic engineering information engineering 0601 history and archaeology Detached eddy simulation SDG 7 - Affordable and Clean Energy Axial flow pump SSPCV SDG 7 – Betaalbare en schone energie |
Zdroj: | Renewable Energy, 163, 1195-1209. Elsevier |
ISSN: | 0960-1481 |
Popis: | In this paper, the cavitating flow and pressure fluctuation in the tip region were simulated based on Delayed Detached Eddy Simulation (DDES). The high-speed photography and transient pressure measurements were employed to capture the cavitation structures and pressure fluctuation. The numerical results show a reasonable agreement with the available experiments. The maximum errors of head and efficiency are 2.9% and 2.2%. The impeller rotation dominants the tip pressure field, with some obvious high-frequency components induced by the cavitating flow. Increasing the flow rate from 0.8Qopt to 1.2Qopt, the amplitudes of the frequency domain in P2 decrease from 0.13 to 0.08. There are more harmonic-frequency components at 0.8Qopt, including 5BPF, 6BPF, 7BPF. Suction-side-perpendicular cavitating vortices (SSPCVs) appeared in severe cavitation conditions, which leads to the collapse of the triangular cavitation cloud. The spatial-temporal evolution of SSPCV was divided into three stages: Generating stage, Shedding stage, and Dissipating stage. The pressure fluctuates significantly in the flow passage caused by SSPCV. The amplitudes of dominant frequency in P3 vary from 0.031 to 0.089, as the cavitation number decreased from 0.582 to 0.231. In particular, there is an obvious low-frequency N∗ = 0.5 shown in the frequency domains of P2 and P3. |
Databáze: | OpenAIRE |
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