Processing math: 100%
EI、Scopus 收录
中文核心期刊
Hu Yang, Peng Wei, Li Decai. The effective viscosity of a suspension of porous particles based on the darcy-stokes coupling model. Chinese Journal of Theoretical and Applied Mechanics, 2021, 53(7): 1922-1929. DOI: 10.6052/0459-1879-21-144
Citation: Hu Yang, Peng Wei, Li Decai. The effective viscosity of a suspension of porous particles based on the darcy-stokes coupling model. Chinese Journal of Theoretical and Applied Mechanics, 2021, 53(7): 1922-1929. DOI: 10.6052/0459-1879-21-144

THE EFFECTIVE VISCOSITY OF A SUSPENSION OF POROUS PARTICLES BASED ON THE DARCY-STOKES COUPLING MODEL

  • Received Date: April 07, 2021
  • Accepted Date: May 23, 2021
  • Available Online: May 23, 2021
  • Particle suspensions exist widely in nature and engineering applications, and their viscous characteristics have an important influence on their flow behavior. Based on the Darcy-Stokes coupling model, the analytical formulas of effective viscosity of dilute suspensions containing porous particles are derived in this paper. Firstly, an auxiliary problem is solved, that is, the disturbance caused by porous media spheres in the flow field with linear distribution under the condition of low Reynolds number. The fluid flows in the free-flow domain and porous medium are governed by the Stokes equation and Darcy’ law, respectively. The mass conservation law, the balance of normal forces, and the Beavers-Joseph (-Saffman) interface condition are used at the fluid–porous interface. An analytical solution for the present coupled free-flow and porous-medium system is derived by using the undetermined coefficient method. Then the additional heat dissipation rate caused by the porous media particle is calculated. Intrinsic viscosity of the porous media suspension under the condition of low concentration is determined as a function of the Darcy number and the Beavers-Joseph coefficient, which is based on the additional heat dissipation rate under the condition of low concentration. It is found that the intrinsic viscosity increases with increasing the Beavers-Joseph coefficient, and the larger the Beavers-Joseph coefficient is, the slower the increase of the intrinsic viscosity. When Darcy number is in the range of 106 to 104, the intrinsic viscosity is close to 2.5, which was consistent with the classical Einstein viscosity formula. When Darcy number is in the range of 104 to 101, the intrinsic viscosity decreases rapidly, so the effective viscosity coefficient of porous media suspension is closer to the viscosity of the based fluid. At last, the present effective viscosity formula is compared with that obtained by the Darcy-Brinkman equation coupling with the shear stress jump condition. It can be found that the effective viscosities obtained two different models agree well with each other in the low Darcy number regime when the sum of the Beavers-Joseph coefficient and the shear stress jump coefficient is unity.
  • [1]
    Mewis J, Wagner NJ. Theory and Applications of Colloidal Suspension Rheology. Cambridge: Cambridge University Press, 2021
    [2]
    Hasegawa H, Horikawa Y, Shikata T. Cellulose nanocrystals as a model substance for rigid rod particle suspension rheology. Macromolecules, 2020, 53(7): 2677-2685 doi: 10.1021/acs.macromol.9b02641
    [3]
    Stickel JJ, Powell RL. Fluid mechanics and rheology of dense suspensions. Annual Review of Fluid Mechanics, 2005, 37: 129-149 doi: 10.1146/annurev.fluid.36.050802.122132
    [4]
    Fabian DM, Hu S, Singh N, et al. Particle suspension reactors and materials for solar-driven water splitting. Energy & Environmental Science, 2015, 8(10): 2825-2850
    [5]
    爱因斯坦, 爱因斯坦文集. 第2卷. 北京: 商务印书馆, 2010

    (Einstein A. The Collected Papers of Albert Einstein, Volume 2. Beijing: Commercial Press, 2010 (in Chinese))
    [6]
    Batchelor GK, Green JT. The determination of the bulk stress in a suspension of spherical particles to order c2. Journal of Fluid Mechanics, 1972, 56(3): 401-427 doi: 10.1017/S0022112072002435
    [7]
    Batchelor GK. The effect of Brownian motion on the bulk stress in a suspension of spherical particles. Journal of Fluid Mechanics, 1977, 83(1): 97-117 doi: 10.1017/S0022112077001062
    [8]
    Zhu Z, Wang H, Peng D. Dependence of sediment suspension viscosity on solid concentration: a simple general equation. Water, 2017, 9(7): 474 doi: 10.3390/w9070474
    [9]
    Lin CJ, Peery JH, Schowalter WR. Simple shear flow round a rigid sphere: inertial effects and suspension rheology. Journal of Fluid Mechanics, 1970, 44(1): 1-17 doi: 10.1017/S0022112070001659
    [10]
    Kulkarni PM, Morris JF. Suspension properties at finite Reynolds number from simulated shear flow. Physics of Fluids, 2008, 20(4): 040602 doi: 10.1063/1.2911017
    [11]
    Yeo K, Maxey MR. Dynamics of concentrated suspensions of non-colloidal particles in Couette flow. Journal of Fluid Mechanics, 2010, 649: 205 doi: 10.1017/S0022112009993454
    [12]
    Yeo K, Maxey MR. Dynamics and rheology of concentrated, finite-Reynolds-number suspensions in a homogeneous shear flow. Physics of Fluids, 2013, 25(5): 053303 doi: 10.1063/1.4802844
    [13]
    Jeffery GB. The motion of ellipsoidal particles immersed in a viscous fluid. Proceedings of the Royal Society of London. Series A, 1922, 102(715): 161-179 doi: 10.1098/rspa.1922.0078
    [14]
    Yamamoto S, Matsuoka T. Viscosity of dilute suspensions of rodlike particles: A numerical simulation method. The Journal of Chemical Physics, 1994, 100(4): 3317-3324 doi: 10.1063/1.466423
    [15]
    Huang H, Wu YF, Lu X. Shear viscosity of dilute suspensions of ellipsoidal particles with a lattice Boltzmann method. Physical Review E, 2012, 86(4): 046305 doi: 10.1103/PhysRevE.86.046305
    [16]
    Mahmoudi Y, Hooman K, Vafai K, Convective Heat Transfer in Porous Media. Boca Raton: CRC Press, 2019
    [17]
    Thomas A. Much ado about nothing–a decade of porous materials research. Nature Communications, 2020, 11(1): 1-3 doi: 10.1038/s41467-019-13993-7
    [18]
    Natraj V, Chen SB. Primary electroviscous effect in a suspension of charged porous spheres. Journal of Colloid and Interface Science, 2002, 251(1): 200-207 doi: 10.1006/jcis.2002.8434
    [19]
    Ohshima H. Primary electroviscous effect in a dilute suspension of soft particles. Langmuir, 2008, 24(13): 6453-6461 doi: 10.1021/la800027m
    [20]
    Ohshima H. Effective viscosity of a concentrated suspension of uncharged porous spheres. Colloids and Surfaces A: Physicochemical and Engineering Aspects, 2009, 347(1-3): 33-37
    [21]
    Ohshima H. Effective viscosity of a concentrated suspension of uncharged spherical soft particles. Langmuir, 2010, 26(9): 6287-6294 doi: 10.1021/la904121p
    [22]
    Ohshima H. Primary electroviscous effect in a dilute suspension of charged spherical colloidal particles with a slip surface. Colloid and Polymer Science, 2020, 298(11): 1551-1557 doi: 10.1007/s00396-020-04741-1
    [23]
    Neale G, Nader W. Practical significance of Brinkman’s extension of Darcy’s law: coupled parallel flows within a channel and a bounding porous medium. The Canadian Journal of Chemical Engineering, 1974, 52(4): 475-478 doi: 10.1002/cjce.5450520407
    [24]
    Vafai K, Thiyagaraja R. Analysis of flow and heat transfer at the interface region of a porous medium. International Journal of Heat and Mass Transfer, 1987, 30(7): 1391-1405 doi: 10.1016/0017-9310(87)90171-2
    [25]
    李琪, 赵一远, 胡鹏飞. 多孔介质——自由流界面应力跳跃条件下流动特性解析解. 力学学报, 2018, 50(2): 415-426 (Li Qi, Zhao Yiyuan, Hu Pengfei. Analytical solution for porous-fluid flow characteristics with stress jump interfacial condition. Chinese Journal of Theoretical and Applied Mechanics, 2018, 50(2): 415-426 (in Chinese) doi: 10.6052/0459-1879-17-357
    [26]
    Prakash J, Sekhar GPR. Effective viscosity of a concentrated suspension of composite porous spherical particles. Meccanica, 2019, 54(6): 799-813 doi: 10.1007/s11012-019-01008-0
    [27]
    Xu A, Shi L, Zhao TS. Lattice Boltzmann simulation of shear viscosity of suspensions containing porous particles. International Journal of Heat and Mass Transfer, 2018, 116: 969-976 doi: 10.1016/j.ijheatmasstransfer.2017.09.060
    [28]
    Liu X, Huang H, Lu XY. Lattice Boltzmann study of effective viscosities of porous particle suspensions. Computers & Fluids, 2019, 181: 135-142
    [29]
    Liu J, Li C, Ye M, et al. On the shear viscosity of dilute suspension containing elliptical porous particles at low Reynolds number. Powder Technology, 2019, 354: 108-114 doi: 10.1016/j.powtec.2019.05.068
    [30]
    Wang L, Wang LP, Guo Z, et al. Volume-averaged macroscopic equation for fluid flow in moving porous media. International Journal of Heat and Mass Transfer, 2015, 82: 357-368 doi: 10.1016/j.ijheatmasstransfer.2014.11.056
    [31]
    Zhang M, Zhao Q, Huang Z, et al. Numerical simulation of the drag and heat-transfer characteristics around and through a porous particle based on the lattice Boltzmann method. Particuology, 2021, 58: 99-107 doi: 10.1016/j.partic.2021.01.013
    [32]
    Nield DA. The Beavers–Joseph boundary condition and related matters: a historical and critical note. Transport in Porous Media, 2009, 78(3): 537-540 doi: 10.1007/s11242-009-9344-y
    [33]
    Beavers GS, Joseph DD. Boundary conditions at a naturally permeable wall. Journal of Fluid Mechanics, 1967, 30(1): 197-207 doi: 10.1017/S0022112067001375
    [34]
    Saffman PG. On the boundary condition at the surface of a porous medium. Studies in Applied Mathematics, 1971, 50(2): 93-101 doi: 10.1002/sapm197150293
    [35]
    Yang G, Coltman E, Weishaupt K, et al. On the Beavers–Joseph interface condition for non-parallel coupled channel flow over a porous structure at high Reynolds numbers. Transport in Porous Media, 2019, 128(2): 431-457 doi: 10.1007/s11242-019-01255-5
    [36]
    Qiu C, He X, Li J, et al. A domain decomposition method for the time-dependent Navier-Stokes-Darcy model with Beavers-Joseph interface condition and defective boundary condition. Journal of Computational Physics, 2020, 411: 109400 doi: 10.1016/j.jcp.2020.109400
    [37]
    Cao L, He Y, Li J, et al. Decoupled modified characteristic FEMs for fully evolutionary Navier–Stokes–Darcy model with the Beavers–Joseph interface condition. Journal of Computational and Applied Mathematics, 2021, 383: 113128 doi: 10.1016/j.cam.2020.113128
    [38]
    Yu J, Sun Y, Shi F, et al. Nitsche’s type stabilized finite element method for the fully mixed Stokes–Darcy problem with Beavers–Joseph conditions. Applied Mathematics Letters, 2020, 110: 106588 doi: 10.1016/j.aml.2020.106588
    [39]
    张冉. 自由流和多孔介质流耦合问题的数学和数值分析[博士论文]. 济南: 山东大学, 2011

    (Zhang R, Mathematical and numerical analysis of the coupling problem of free flow and porous media flow [PhD Thesis]. Jinan: Shandong University, 2011 (in Chinese))
    [40]
    Batchelor CK, Batchelor GK. An Introduction to Fluid Dynamics. Cambridge: Cambridge University Press, 2000
  • Related Articles

    [1]Zhao Yong, Ge Yixuan, Chen Xinmeng, Chen Zhenyu, Wang Lei. MULTI-DISTRIBUTION REGULARIZED LATTICE BOLTZMANN METHOD FOR CONVECTION-DIFFUSION-SYSTEM-BASED INCOMPRESSIBLE NAVIER-STOKES EQUATION[J]. Chinese Journal of Theoretical and Applied Mechanics, 2025, 57(7): 1597-1610. DOI: 10.6052/0459-1879-25-096
    [2]Zhang Lei, Zhong Deyu, Wu Baosheng, Liu Lei. THE CONVECTION-DISPERSION EQUATION AND THE MECHANISM OF SUSPENSION IN TURBULENT OPEN-CHANNELS[J]. Chinese Journal of Theoretical and Applied Mechanics, 2013, 45(1): 83-93. DOI: 10.6052/0459-1879-12-146
    [3]Bing Chen, Xu Xu, Guobiao Cai. A space-marching algorithm for solving the parabolized Navier-Stokes equations[J]. Chinese Journal of Theoretical and Applied Mechanics, 2008, 40(2): 162-170. DOI: 10.6052/0459-1879-2008-2-2007-440
    [4]Xiongping Luo. The characteristic of precursor film in Navier-Stokes equations frame[J]. Chinese Journal of Theoretical and Applied Mechanics, 2007, 39(4): 455-459. DOI: 10.6052/0459-1879-2007-4-2006-437
    [5]T. Hayat, F. Shahzad, M. Ayub. Stokes' first problem for the fourth order fluid in a porous half[J]. Chinese Journal of Theoretical and Applied Mechanics, 2007, 39(1): 17-21. DOI: 10.6052/0459-1879-2007-1-2006-138
    [6]Chong Xie, Jing Fan. Assessment of second-order velocity-slip boundary conditions of the navier-stokes equations[J]. Chinese Journal of Theoretical and Applied Mechanics, 2007, 39(1): 1-6. DOI: 10.6052/0459-1879-2007-1-2005-577
    [7]A method of symplectic enginsolutions in Stokes flow[J]. Chinese Journal of Theoretical and Applied Mechanics, 2006, 38(5): 682-687. DOI: 10.6052/0459-1879-2006-5-2005-576
    [8]THE COMPLETE BOUNDARY INTEGRAL FORMULATION FOR GENERALIZED STOKES EQUATION AND ITS APPLICATION TO THE SOLUTION OF NAVIER-STOKES EQUATION[J]. Chinese Journal of Theoretical and Applied Mechanics, 1992, 24(6): 645-652. DOI: 10.6052/0459-1879-1992-6-1995-787
    [9]THE BASIC EQUATIONS FOR SUSPENSION FLOWS DERIVED THROUGH A NEW METHOD[J]. Chinese Journal of Theoretical and Applied Mechanics, 1992, 24(1): 122-128. DOI: 10.6052/0459-1879-1992-1-1995-719
    [10]SYMMETRIC BIFURCATION OF STOKES WATER WAVES[J]. Chinese Journal of Theoretical and Applied Mechanics, 1992, 24(1): 32-39. DOI: 10.6052/0459-1879-1992-1-1995-708
  • Cited by

    Periodical cited type(0)

    Other cited types(1)

Catalog

    Article Metrics

    Article views (805) PDF downloads (88) Cited by(1)
    Related

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return