2022
DOI: 10.3390/en15166051
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Refined 1D–3D Coupling for High-Frequency Forced Vibration Analysis in Hydraulic Systems

Abstract: High-Frequency Pressure Fluctuation (HFPF) is an extensively observed hydraulic phenomenon in pumped-storage power stations and water conveyance projects. The investigation of the propagation characteristics of the pressure perturbation is of great significance for the safe operation of hydraulic facilities. In this study, a one-dimensional (1D)–three-dimensional (3D) coupling model is established based on the combination of the Method of Characteristics (MOC) and Computational Fluid Dynamics (CFD) and implant… Show more

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Cited by 3 publications
(5 citation statements)
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“…Here, we compare the test data and the simulation results of the one-dimensional method of characteristics (1D-MOC) for this phenomenon. The MOC simplifies the pressure pipeline as a one-dimensional system, simplifies the continuity equation and momentum equation according to pipeline assumptions, and, finally, solves a set of quasi-hyperbolic partial differential equations using the method of characteristics to predict water hammer waves in complex pipeline systems [30]. Figure 24 shows a comparison of the test data and the MOC simulation results for the pressure at the volute inlet and the volute tongue.…”
Section: Pressure Change and Key Momentsmentioning
confidence: 99%
“…Here, we compare the test data and the simulation results of the one-dimensional method of characteristics (1D-MOC) for this phenomenon. The MOC simplifies the pressure pipeline as a one-dimensional system, simplifies the continuity equation and momentum equation according to pipeline assumptions, and, finally, solves a set of quasi-hyperbolic partial differential equations using the method of characteristics to predict water hammer waves in complex pipeline systems [30]. Figure 24 shows a comparison of the test data and the MOC simulation results for the pressure at the volute inlet and the volute tongue.…”
Section: Pressure Change and Key Momentsmentioning
confidence: 99%
“…ρt+][ρtrueUU6pt→g=0 $\frac{\partial \rho }{\partial t}+\nabla \cdot \left[\rho \left(\overrightarrow{U}-{\overrightarrow{U}}_{g}\right)\right]=0$ ρtrueUt++3pxρU6pt→true(trueUU6pt→gtrue)μtrueU=p $\frac{\partial \rho \overrightarrow{U}}{\partial t}+\nabla \cdot <mpadded xmlns="http://www.w3.org/1998/Math/MathML" lspace="+3px">\left[\rho \overrightarrow{U}(\overrightarrow{U}-{\overrightarrow{U}}_{g})\right]</mpadded>-\nabla \cdot \mu \nabla \overrightarrow{U}=-\nabla p$where U6pt→g ${\overrightarrow{U}}_{g}$ is the velocity of the moving mesh. The solution procedure follows the sonicLiquidFoam in OpenFOAM‐v2012 and has been reported in our previous work 20 …”
Section: Governing Equationsmentioning
confidence: 99%
“…The mechanism of pressure disturbance induced by the pipe walls vibration is analogous to that induced by the RPTs, where the water hammer phenomenon is caused by compressing the fluid inner the pipe. Zhou et al 20 employed the coupling of 1D and 3D methods to establish the numerical model. The vibration sources are modeled in the 3D region, and the propagation of the water hammer in long conduct is simulated by the 1D method.…”
Section: Introductionmentioning
confidence: 99%
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