Abstract
To further understand the wall-roughness effect, the present study has performed numerical simulations, by employing the Poisson–Nernst–Planck model, on the two-dimensional electroosmotic flow in a plane channel with dielectric walls of rectangle-waved surface roughness where the two electric double layers (EDLs) are overlapped. Results show that the steady electroosmotic flow and ionic-species transport depend significantly on the shape of the surface roughness such as the amplitude and periodic length of wall wave, but their characteristics are basically different from those in the case where the EDLs are not overlapped at all (Kang and Suh in Microfluid Nanofluid, doi:10.1007/s10404-008-0321-5, 2008). It is found that the fluid flows over the waved wall (or wall roughness) with involving a separation or recirculation of flow in the cavity, which resembles much the traditional pressure-driven flow. In addition, the flow characteristics are determined chiefly by the level of the electric-charge density in the bulk region above the waved wall. As a result, with increasing wall-wave amplitude (0.01 ≤ h/H ≤ 0.2), the flow rate increases due to the enhanced amount of electric charges released from the enlarged wet surface at low amplitudes and then decreases due to the reduced flow-passage area at high amplitudes above a certain critical value. With increasing periodic length (0.2 ≤ L/H ≤ 1.2), on the other hand, the flow rate decreases in a hyperbolic fashion due to the reduced amount of electric charges.
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Abbreviations
- C p , C m :
-
nondimensional concentrations
- C 0 :
-
molar ionic concentration in the bulk region (mol/m3)
- D p , D m , D :
-
ionic diffusion coefficients (m2/s)
- E i :
-
nondimensional total electric field
- E 0 :
-
mean external streamwise electric field (V/m)
- F :
-
Faraday constant (=96,485.338,3 C/mol)
- F e,i :
-
nondimensional total electric force
- F e,ϕ,i :
-
nondimensional force due to the external electric field
- F e,ψ,i :
-
nondimensional force due to the induced electric field
- H :
-
channel half-width (m)
- h :
-
nondimensional amplitude of wall wave
- L :
-
nondimensional periodic length of wall wave
- P :
-
nondimensional mean pressure
- Pe :
-
Peclet number (=U eo H/D)
- p :
-
nondimensional pressure
- Q :
-
nondimensional flow rate
- Q * :
-
real flow rate (m3/s)
- R :
-
gas constant (=8.314 J/Kmol)
- Sc :
-
Schmidt number (=ν/D)
- T :
-
absolute temperature (K)
- t :
-
nondimensional time
- U eo :
-
electroosmotic velocity [=ɛζ0 E 0/ρν, m/s]
- u i :
-
nondimensional velocity
- x i :
-
nondimensional Cartesian coordinates
- z p , z m , z :
-
ionic valences
- β:
-
nondimensional parameter (=PeΩ)
- ɛ:
-
fluid permittivity (C/Vm)
- ζ0 :
-
reference zeta potential (V)
- ζ *0 :
-
nondimensional reference zeta potential (=−zFζ0/RT)
- κ:
-
nondimensional EDL thickness (=λ/H)
- Λ:
-
aspect ratio of the cavity (=4h/L)
- λ:
-
EDL thickness [=(ɛRT/2F 2 z 2 C 0)1/2, m]
- ν:
-
fluid kinematic viscosity (m2/s)
- ρ:
-
fluid density (kg/m3)
- ρ e :
-
nondimensional volumetric electric-charge density
- σ0 :
-
surface electric-charge density (C/m2)
- Φ:
-
nondimensional total electric potential
- ϕ:
-
nondimensional external electric potential
- ψ:
-
nondimensional induced electric potential
- Ω:
-
nondimensional parameter (=ζ0/E 0 H)
- cr:
-
critical
- i, j :
-
coordinate indices (1, 2)
- m :
-
anions
- n :
-
wall-normal direction
- p :
-
cations
- t :
-
wall-tangential direction
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Acknowledgments
This work has been supported by the Korea Science and Engineering Foundation (KOSEF) through the National Research Laboratory Program funded by the Ministry of Education, Science and Technology (No. 2005-1091).
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Kang, S., Suh, Y.K. Electroosmotic flows in an electric double layer overlapped channel with rectangle-waved surface roughness. Microfluid Nanofluid 7, 337–352 (2009). https://doi.org/10.1007/s10404-008-0384-3
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DOI: https://doi.org/10.1007/s10404-008-0384-3