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SISTEMA INTEGRAL DE INFORMACIÓN ACADÉMICA - PÚBLICO
Título del libro: Asme 2015 13th International Conference On Nanochannels, Microchannels, And Minichannels, Icnmm 2015, Collocated With The Asme 2015 International Technical Conference And Exhibition On Packaging And Integration Of Electronic And Photonic Microsystems Título del capítulo: EFFECT OF HYDRODYNAMIC SLIPPAGE ON OSCILLATING ELECTROOSMOTIC FLOWS IN INFINITELY EXTENDED MICROCAPILLARY
In this work we conduct a numerical analysis of the time periodic
electroosmotic flow in a cylindrical microcapillary, whose wall is
considered hydrophobic. The fluid motion is driven by the sudden
imposition of a time-dependent electric field. The electrical potential
is obtained by solving the nonlinear Poisson Boltzmann equation for high
zeta potential, under the assumption that the electrokinetic potential
is not affected by the oscillatory external field. In addition, we
neglect the channel entry and exit effects, in such manner that the flow
is fully developed. The governing equations are nondimensionalized, and
the solution is obtained as a function of three dimensionless
parameters: the ratio of the Navier slip length to the radius of the
microcapillary delta; R-w, which is the dimensionless frequency for the
flow or Strouhal number and measures the competition between the
diffusion time to the time scale associated to the frequency of the
oscillatory electric field; and (kappa) over bar, which represents the
ratio of the radius of the microcapillary to the Debye length. The
principal results show that using slippage, the bulk velocity increases
for increasing values of delta. For the values of the dimensionless
parameters used in this analysis, by using hydrophobic walls, the bulk
velocity can be increased in about 20% in comparison with the case of
no-slip boundary condition. On the other hand, the dimensionless
frequency for the flow or Strouhal number plays a fundamental role in
determining the motion of the fluid. For R-w << 1, the dissipation is
found in resonance with the frequency of the oscillatory electric field.
For R-w >> 1, the dissipation is not in phase with the frequency and,
therefore, the velocity in the center of the microcapillary, in some
cases, is almost null, and the maximum value of the velocity is near to
the microcapillary wall.
Entidades citadas de la UNAM:
Fuente:
ISBN: 9780791856871 Editorial: American Society of Mechanical Engineers