Abstract
Effective characteristics, such as the effective particle diameter and hydraulic radius, are usually used to determine the pressure loss associated with single-phase flow through an isotropic, dense non-spherical granular packing. These quantities can be considered as those of an equivalent spherical particle system. This paper reviews different methods to select effective particle diameters taking into account the effect of particle shape. A new method is proposed to determine an equivalent spherical particle system with both the hydraulic radius and the pressure loss equivalent to those in the actual non-spherical particle packing. This equivalent system can be used to determine the characteristics of flow in the actual system. The analyses provide theoretical justification for adoption of proper effective particle diameters and porosity as well as the dependency of Ergun–Kozeny constant on the shape factor of particles. It is also shown theoretically that the critical Reynolds number for Darcian flow depends on the porosity and the shape factor of particles.
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Abbreviations
- a :
-
Empirical constant
- b :
-
Empirical constant
- c :
-
Circularity of the projected surface, defined as the ratio of the perimeter of a sphere with equal projected surface area to the perimeter of the projected surface of the actual particle
- A :
-
Ergun–Kozeny constant for viscous flow
- \( A_{\text{eq}} \) :
-
Ergun–Kozeny constant for viscous flow in the equivalent system of spherical particles
- \( \bar{A}_{\text{eq}} \) :
-
Surface area of an equivalent spherical particle with diameter \( \bar{D}_{\text{eq}} = \bar{D}_{32} = \psi_{\text{s}} \bar{D}_{\text{v}} \), m2
- \( \bar{A}_{\text{eV}} \) :
-
Surface area of a sphere having the same volume as an irregular particle, m2
- \( A_{\text{P}} \) :
-
Surface area of a particle, m2
- B :
-
Ergun–Kozeny constant for Newtonian flow
- \( C_{D} \) :
-
Drag coefficient
- \( C_{\text{Deq}} \) :
-
Drag coefficient of an equivalent spherical particle or the equivalent spherical particle system
- \( C_{\text{Dv}}^{{}} \) :
-
Drag coefficient in viscous flow regime
- \( C_{\text{Dn}}^{{}} \) :
-
Drag coefficient in Newtonian flow regime
- \( d_{50} \) :
-
The mean grain size, m
- \( d_{\text{eq}} \) :
-
Equivalent diameter, m
- \( d_{p} \) :
-
Particle diameter or the diameter of an equivalent-volume sphere, m
- \( d_{x} \) :
-
Particle size corresponding to x% passing on the particle size distribution curves, m
- \( \bar{D}_{21} \) :
-
Length average particle size, m
- \( \bar{D}_{31}^{{}} \) :
-
The volume-to-length mean diameter, m
- \( \bar{D}_{32}^{{}} \) :
-
Volume-to-surface-area mean diameter, m
- \( \bar{D}_{A} \) :
-
Projected surface equivalent sphere diameter, \( \bar{D}_{A} = \sqrt {4 \times {\text{Projected Area/}}\pi } \), m
- \( \bar{D}_{eff} \) :
-
Effective diameter, m
- \( \bar{D}_{\text{eq}} \) :
-
Equivalent diameter \( \bar{D}_{\text{eq}} = \psi_{\text{s}} \bar{D}_{\text{v}} \), m
- \( D_{h} \) :
-
Mean pore diameter or average hydraulic diameter, m
- \( \bar{D}_{p} \) :
-
Characteristic particle diameter, m
- \( \bar{D}_{pore} \) :
-
Characteristic pore size, m
- \( \bar{D}_{\text{v}} \) :
-
Diameter of an equivalent-volume sphere, \( \bar{D}_{\text{v}} = (6V_{\text{P}} /\pi )^{1/3} \), m
- F D :
-
Drag force on a single particle in unhindered flow, N
- F DS :
-
Drag force on a particle in a cluster of particles, N
- g :
-
Acceleration of gravity, m/s2
- Ga:
-
Fluid-particle Galileo number
- J :
-
Hydraulic gradient defined as \( J = \nabla p/(\rho_{f} g) \)
- \( k_{KC} \) :
-
Kozeny constant
- \( l_{p} \) :
-
Microscopic characteristic length, m
- N :
-
Number of particles in a granular assembly or RVE
- \( N_{\text{P}} \) :
-
Number of particles in a unit volume of the granular bed
- \( q_{i} \) :
-
Particle size distribution parameters
- \( R_{\text{CDeq}} \) :
-
Ratio between the drag coefficients of a granular particle system and its equivalent spherical particle system \( R_{\text{CDeq}} = C_{\text{D}} /C_{\text{Deq}} \)
- \( R_{\text{CDeqV}} \) :
-
Ratio between the drag coefficients of an irregular particle and an equivalent-volume spherical particle \( R_{\text{CDeqV}} = C_{\text{D}} /C_{\text{DeqV}} \)
- \( \text{Re} \) :
-
Reynolds number
- \( \text{Re}_{\text{a}} \) :
-
Reynolds number for angular particles
- \( \text{Re}_{h} \) :
-
Pore Reynolds number, \( \text{Re}_{h} = \rho_{f} UR_{h} /\mu = \text{Re}_{\text{S}} /6 \)
- \( \text{Re}_{\text{int}} \) :
-
Interstitial Reynolds number, \( \text{Re}_{\text{int}} = \frac{{\rho_{f} Ud_{\text{p}} }}{\mu } = \frac{{\rho_{f} v_{\text{s}} d_{\text{p}} }}{\mu \varepsilon } \)
- \( \text{Re}_{p} \) :
-
Particle Reynolds number \( \text{Re}_{\text{p}} = \rho v_{s} d_{\text{p}} /\mu \)
- \( {\text{Re}}_{\text{r}} \) :
-
Reynolds number for rounded particles
- \( \text{Re}_{\text{S}} \) :
-
Blake/Ergun Reynolds number
- \( \text{Re}_{\kappa } \) :
-
Reynolds number with the characteristic length being a function of permeability \( \kappa \)
- \( \text{Re}_{\tau } \) :
-
Reynolds number defined as \( \text{Re}_{\tau } = \rho v_{s} /(\mu \bar{\tau }) \) with the characteristic length \( \bar{\tau }^{ - 1} = 2d_{50} \)
- \( R_{\text{hv}} \) :
-
Hydraulic radius of the pore space in a spherical particle system defined as \( R_{\text{hv}} = \varepsilon d_{p} /[6(1 - \varepsilon )] \). For an equivalent spherical particle system, \( \bar{D}_{\text{eq}} = \bar{D}_{32} = \psi_{\text{s}} \bar{D}_{\text{v}} \), is used as the particle diameter, m
- \( S_{pore}^{{}} \) :
-
Specific surface area based on the volume of pores, \( S_{\text{pore}} = A_{\text{p}} /V_{\text{pore}} \), m2
- \( S_{V}^{{}} \) :
-
Specific surface area of a particle, \( S_{\text{v}} = A_{\text{p}} /V_{\text{p}} = \bar{D}_{32} /6 \), m2
- U :
-
Magnitude of interstitial velocity defined as \( {\mathbf{U}} = {\mathbf{v}}_{s} /\varepsilon \), m/s
- \( v_{s} \) :
-
Magnitude of superficial velocity \( {\mathbf{v}}_{s} \), m/s
- \( V_{\text{eq}} \) :
-
Volume of an equivalent spherical particle with diameter \( \bar{D}_{\text{eq}} = \bar{D}_{32} = \psi_{\text{s}} \bar{D}_{\text{v}} \), m3
- \( V_{\text{P}} \) :
-
Volume of a particle, m3
- \( \beta \) :
-
Non-Darcian coefficient that is usually referred to as the “inertial parameter”
- \( \delta \) :
-
Shape-dependent factor to determine the specific surface area of a particle
- \( \varepsilon \) :
-
Bulk porosity
- \( \varepsilon_{\text{eq}} \) :
-
Porosity of an equivalent particle system
- \( \kappa \) :
-
Velocity-dependent permeability, m2
- \( \kappa_{0} \) :
-
Permeability in the viscous flow regime, m2
- \( \mu \) :
-
The dynamic viscosity of the fluid (\( \mu = 1.002 \times 10^{ - 3} Pa \cdot s \) for water at 20 °C),
- \( \rho_{f} \) :
-
Density of fluid, kg/m3
- \( \tau \) :
-
Tortuosity factor
- \( \tau_{\text{eq}}^{{}} \) :
-
Tortuosity of an equivalent particle system
- \( \tau_{np} \) :
-
Shear stress on the surface of a spherical particle induced by flowing fluid, kPa
- \( \psi_{\text{s}} \) :
-
Shape factor or Wadell’s sphericity, which is defined as the ratio of the surface area of an equivalent-volume sphere to that of the particle
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Guo, P., Stolle, D. & Guo, S.X. An Equivalent Spherical Particle System to Describe Characteristics of Flow in a Dense Packing of Non-spherical Particles. Transp Porous Med 129, 253–280 (2019). https://doi.org/10.1007/s11242-019-01286-y
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DOI: https://doi.org/10.1007/s11242-019-01286-y