Micro-acting Force in Boundary Layer in Low-Permeability Porous Media

  • Received Date: October 07, 2010
  • Published Date: January 31, 2011
  • There are lots of reasons to restrict a low-permeability oil layer to enhance the recovery factor. Based on the research results of non-Darcy flow, microflow of water drive and micro-acting force in low permeability porous media are studied by establishing the expression of fluid viscosity factor. Numerical calculation shows that under the condition of L/S interaction, the radial velocity distribution near the solid wall changes obviously, and the curve form changes from convex to concave. The tinier the capillary radius is, the stronger the L/S interaction is. The larger the n value is, more obviously the flowing velocity decreases. The results will help people to deal with improving recovery factor of low permeability reservoir, and understanding the fluid flow behavior in blood capillary.
  • Article Text

  • [1] Bear J 1972 Dynamics of Fluid in Porous Media (New York: Dover)
    [2] Barry R 2010 SPE Western Regional Meeting (Anaheim, California, USA 27–29 May 2010)
    [3] Ho Ch M and Tai Y Ch 1998 Micro-electro Mechanical Systems (MEMS) and Fluid Flows Annual Review of Fluid Mechanics 30 579
    [4] Kong L J, Li H B, Chen R H and Liu M R 1999 Acta Phys. Sin. 48 1080 (in Chinese)
    [5] Bird G A 1998 Computers and Mathematics with Applications 35 1
    [6] Ji Q F, Liu Ch and Zheng B M 2000 Chin. J. Comput. Mech. 17 390 (in Chinese)
    [7] Heyes D M 1998 The Liquid State: Applications of Molecular Simulation (NewYork: John Wiley & Sons)
    [8] Shibahara M and Kotake S 1998 J. Heat Transfer 41 839
    [9] Zhang R L, Di Q F, Wang X L and Gu Ch Y 2010 J. Hydrodyn. 3 366 (in Chinese)
    [10] Ling Zh Y, Ding J N and Yang J Ch 2002 J. Jiangsu University (Natural Science) 23 1 (in Chinese)
    [11] Wen Sh M 2002 Theory and Application of Micro-boundary (Beijing: Metallurgical Industry Press) (in Chinese)
  • Related Articles

    [1]LIU Yuan, JIA Ya-Fei, LI Wei-Dong. Fermi-Decay Law of Bose–Einstein Condensate Trapped in an Anharmonic Potential [J]. Chin. Phys. Lett., 2012, 29(4): 040304. doi: 10.1088/0256-307X/29/4/040304
    [2]HAO Ya-Jiang. Ground State Density Distribution of Bose-Fermi Mixture in a One-Dimensional Harmonic Trap [J]. Chin. Phys. Lett., 2011, 28(1): 010302. doi: 10.1088/0256-307X/28/1/010302
    [3]YOU Yi-Zhuang. Ground State Energy of One-Dimensional δ-Function Interacting Bose and Fermi Gas [J]. Chin. Phys. Lett., 2010, 27(8): 080305. doi: 10.1088/0256-307X/27/8/080305
    [4]XIONG De-Zhi, CHEN Hai-Xia, WANG Peng-Jun, YU Xu-Dong, GAO Feng, ZHANG Jing. Quantum Degenerate Fermi--Bose Mixtures of 40K and 87Rb Atoms in a Quadrupole-Ioffe Configuration Trap [J]. Chin. Phys. Lett., 2008, 25(3): 843-846.
    [5]ZHANG Peng-Fei, ZHANG Hai-Chao, XU Xin-Ping, WANG Yu-Zhu. Monte Carlo Simulation of Cooling Induced by Parametric Resonance [J]. Chin. Phys. Lett., 2008, 25(1): 89-92.
    [6]WANG Jin-Feng, LIU Yang, XU You-Sheng, WU Feng-Min. Lattice Boltzmann Simulation for the Optimized Surface Pattern in a Micro-Channel [J]. Chin. Phys. Lett., 2007, 24(10): 2898-2901.
    [7]MA Yong-Li. Phase Diagram and Phase Separation of a Trapped Interacting Bose--Fermi Gas Mixture [J]. Chin. Phys. Lett., 2004, 21(12): 2355-2358.
    [8]LIU Rang-Su, DONG Ke-Jun, LI Ji-Yon, YU Ai-Bing, ZOU Rui-Ping. Molecular Dynamics Simulation of Microstructure Transitions in a Large-Scale Liquid Metal Al System During Rapid Cooling Processes [J]. Chin. Phys. Lett., 2002, 19(8): 1144-1147.
    [9]LIU Chang-Song, ZHU Zhen-Gang, XIA Jun-Chao, SUN De-Yan. Different Cooling Rate Dependences of Different Microstructure Units in Aluminium Glass by Molecular Dynamics Simulation [J]. Chin. Phys. Lett., 2000, 17(1): 34-36.
    [10]CHEN Yixin, NI Guangjiong. DIRAC-BERGMANN FORMALISM OF THE FERMI-BOSE TRANSMUTATION IN (2+1)-DIMENSIONS [J]. Chin. Phys. Lett., 1990, 7(10): 433-436.

Catalog

    Article views (0) PDF downloads (444) Cited by()

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return