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Volumn 77, Issue 1, 2008, Pages

Electric-field-induced displacement of a charged spherical colloid embedded in an elastic Brinkman medium

Author keywords

[No Author keywords available]

Indexed keywords

ELASTIC DEFORMATION; ELECTRIC FIELD EFFECTS; POLYELECTROLYTES; SATURATION (MATERIALS COMPOSITION);

EID: 38749096636     PISSN: 15393755     EISSN: 15502376     Source Type: Journal    
DOI: 10.1103/PhysRevE.77.011404     Document Type: Article
Times cited : (16)

References (33)
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    • Here, the elastic restoring force is the value when a rigid sphere with radius a is embedded in an elastic continuum with Young's modulus E and Poisson's ratio ν=0.5.
    • Here, the elastic restoring force is the value when a rigid sphere with radius a is embedded in an elastic continuum with Young's modulus E and Poisson's ratio ν=0.5.
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    • ASRAA9 0365-7132 10.1063/1.1312272
    • H. C. Brinkman, Appl. Sci. Res., Sect. A ASRAA9 0365-7132 10.1063/1.1312272 1, 27 (1949).
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    • Assuming a constant shear modulus E/ [2 (1+ν)].
    • Assuming a constant shear modulus E/ [2 (1+ν)].
  • 27
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    • With a slipping boundary condition (i.e., zero radial displacement and zero tangential stress at r=a), the force is -12πEaZ (1-ν) / [(7-8ν) (1+ν)].
    • With a slipping boundary condition (i.e., zero radial displacement and zero tangential stress at r=a), the force is -12πEaZ (1-ν) / [(7-8ν) (1+ν)].
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    • A finite-difference scheme based on the methodology of Hill, Saville, and Russel is adopted. This features an adaptive, nonuniform grid to handle the disparate length scales.
    • A finite-difference scheme based on the methodology of Hill, Saville, and Russel is adopted. This features an adaptive, nonuniform grid to handle the disparate length scales.
  • 30
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    • The electrophoretic mobilities reported here were calculated using software (called MPEK, available from the corresponding author) based on the methodology of Hill, Saville, and Russel for the electrophoretic mobility and other single-particle properties of spherical polymer-coated colloids. Here, the influence of a polymer coating is removed by specifying an infinite (large) Darcy permeability for the coating. The mobilities in Figs. 5 6 are in excellent agreement with the O'Brien and White calculations; small differences can be attributed to the opposite sign of the ζ potential.
    • The electrophoretic mobilities reported here were calculated using software (called MPEK, available from the corresponding author) based on the methodology of Hill, Saville, and Russel for the electrophoretic mobility and other single-particle properties of spherical polymer-coated colloids. Here, the influence of a polymer coating is removed by specifying an infinite (large) Darcy permeability for the coating. The mobilities in Figs. 5 6 are in excellent agreement with the O'Brien and White calculations; small differences can be attributed to the opposite sign of the ζ potential.
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    • Squires and Brady present a compelling case to associate Sutherland with this famous relationship.
    • Squires and Brady present a compelling case to associate Sutherland with this famous relationship.


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