Abstract

ABSTRACTThis paper presents a new macroscopic mesh-free particle method in which Darcy’s and Forchheimer’s terms are introduced into the governing equation to ensure the capacity of the particle method in simulating laminar and turbulent porous medium flows. A developed interfacial condition and inflow boundary condition are implemented in the macroscopic particle method to improve the stability of the Particle-based model. The comparisons of channel flow over and within porous bed among the present method, previous mesh-based method, and experimental data show that the macroscopic particle method is capable of simulating flows in both the clear flow region and porous flow region. Finally, two cases of flow over a rigid box and a cylinder lying on porous bed are simulated, and the numerical results are in good agreement with the measured data. The analysis and comparisons indicate that the newly developed particle-based method is reliable and has been successfully extended to macroscopic porous medium simulation.

Highlights

  • Most researchers have paid attention to channel flow over impermeable bed

  • The turbulence is not considered in Eq (2), similar approaches have been executed by Shao (2010), as indicated by Fu and Jin (2013) that in MPS simulation of steady state open channel flow, turbulence model will not significantly affect the simulation results; for the turbulent flow cases simulated in this study, the turbulent shear stress is calculated by a simple turbulence model (Fu & Jin, 2013; Nazari, Jin, & Shakibaeinia, 2012)

  • The interfacial condition used in numerical methods of channel flow over porous bed represents the effects from the porous flow region; some of the previous numerical studies introduced a slip velocity as the interfacial condition for simplicity, another widely used interfacial boundary condition is jump stress condition, which has been successfully utilized in mesh-based methods (Deresiewicz & Skalak, 1963; Ochoa-Tapia & Whitaker, 1995; Pedras & de Lemos, 2001; Vollmera, Ramos, Daebel, & Kuhn, 2002)

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Summary

Introduction

Most researchers have paid attention to channel flow over impermeable bed Coefficients such as Manning’s roughness coefficient n or roughness height ks (Yen, 1991; Zarrati, Tamai, & Jin, 2005) are required to represent the channel bed roughness in numerical studies (Delft3D WL & delft hydraulics, 2001; Fluent Inc, 1998). Tracking the free surface becomes troublesome, and the porous medium formula has to be adopted into the mesh-based form in these methods (Beavers & Joseph, 1967; Chan et al, 2007; Prinos et al, 2003; Silva & de Lemos, 2003). The developed particle-based macroscopic model will first be verified and applied to various kinds of channel flow over and within porous bed cases

Governing equations
Moving particle semi-implicit discretization
Effective parameters
Solid boundary condition
Inflow and outflow boundary condition
Interfacial condition
Testing case: laminar channel flow over porous bed
Testing case: turbulent channel flow over porous bed
Comparison of MPS and DNS of channel flow over porous media
Channel flow over a rigid box
Open channel flow over a cylinder
Conclusion
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