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ELECTRO OSMOTIC PUMPS

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Title: ELECTRO OSMOTIC PUMPS


1
ELECTRO OSMOTIC PUMPS
  • ME-595 TERM PROJECT
  • M. EMRE BASARAN

2
Outlines
  • Electro osmotic pumps
  • Application areas
  • Governing equations
  • Electro-osmotic pump types
  • Concluding remarks

3
Features of electro-osmotic pumps
  • Involves no moving parts
  • Moves fluid by the application of an electric
    field through electro-osmosis mechanism
  • Only field induced flow design that can move low
    conductivity fluids
  • Pressure Flow rate range are typically greater
    than that of other designs

4
Comparison with other micro pumps
5
Physical Aspects
  • Dimensions Geometry
  • Typical widths of the channels are 5-100 mm
  • Rectangular, circular or irregular cross
    sections
  • Fluid Properties
  • Low and high conductivity fluids can be used.
  • Newtonian and non-Newtonian fluids (blood)
  • Different viscosity and densities used
  • Usually requires a electrolyte buffer solution

6
Physical Aspects
  • Applied voltages
  • For portable systems DC, otherwise AC power
    used. (up to 10 kV range)
  • Ohmic heating
  • Occurs at high currencies.
  • Generates bubbles, destroy biological samples
  • Its an upper limit for the systems.
  • .

7
Application Areas
  • Generally used in micro total analysis systems
    (mMTAS)
  • Drug Delivery,
  • Sample analysis, Separation and mixing
    processes.
  • Also used in micro-processor cooling systems

8
EOF Mechanism Governing Equations
  • Surface Reactions
  • Electric Double Layer (EDL)
  • Momentum Equation
  • Velocity profiles
  • Max. flow rate (Qmax)
  • Max. Pressure (Pmax)

9
Surface Reactions
  • Surfaces charge when contact with liquid
  • SiOH OH-? SiO- H2O
  • SiOH H ? SiOH2
  • PH value determines the surface charge
  • In EOF most common reaction is deprotonation of
    the surface
  • Surface becomes negatively charged

10
Electric Double Layer
  • Positive ions adsorbed by inner layer. Theyre
    immobile.
  • Diffuse layer consists of mostly positive ions
  • Diffuse layer is mobile and positive ions have
    neutral H2O molecules around them.

11
Electric Double Layer
  • Zeta potential is the value of the wall potential
    at the shear plane. This is the effective
    potential for the diffuse layer.
  • Net charge density given as

12
Momentum Equation
  • A steady, laminar, constant density flow in a
    channel is given as

  • (1)
  • In EOF the body force (f) is the applied electric
    field force (E) and the density is the net charge
    density (rE)

  • (2)

13
Momentum Equations
  • Momentum equation becomes

  • (3)
  • Assumptions
  • Channel is long and straight
  • Electro double layer has a finite width
  • Cross section of the channel is constant along
    the flow direction
  • The applied electric field is uniform and along
    the x axis of the channel
  • The potential at the wall is constant and uniform
  • Debye-length much smaller than the capillary
    radius

14
Helmutz-Smoluchowski velocity (uEO)

  • (3)
  • where Electro-osmotic mobility

15
EOF velocity with back-pressure

(4)
16
Max flow-rate and pressure
  • Maximum flow rate is achieved when there is no
    back pressure
  • (5)
  • Maximum pressure is achieved when there is no
    flow in the channel
  • ? (6)

17
Effects of the channel dimensions
18
Types of the electro-osmotic pumps
  • Cascade pumps
  • Planar (shallow) pumps
  • Porous electro-osmotic pumps

19
Low voltage cascade pump
  • Low voltage consumption (10 V )
  • Suitable for on chip applications
  • Single stage
  • Pmax281 (Pa)
  • 15 stage
  • Pmax-154200 (Pa)
  • Qmax34.6 (nl/min)

20
Low voltage cascade pump
  • Narrow channels work as high pressure pump
  • Wide channel works in opposite direction as a low
    pressure pump
  • Disadvantages
  • Low flow rate
  • Electrode span life

21
Planar Electro-osmotic pumps
  • Large flow area for high flow rates and shallow
    depth for high back pressure capacity
  • Pressure Range0.1-5 (atm)
  • Flow rate range 10-20 mm/min

22
Planar Electro-osmotic pumps
  • Disadvantages
  • Requires high voltages(1-5 kV), therefore they
    are not portable and suitable for on chip
    applications
  • Wide and shallow channels requires high
    structural stability

23
Porous type electro-osmotic pumps
  • Whole frit surface becomes charged
  • Fluid flows through the tiny irregular channels
    of the frit
  • High flow rates (0.8-1 ml/min)
  • High backpressure range (1-5 atm)

24
Porous type electro-osmotic pumps
  • Pump dimensions are not suitable for on chip
    applications
  • High voltage consumption, not portable
  • Suitable for microchip cooling applications

25
CONCLUDING REMARKS
  • Among the given pump types, cascade pumps are
    the most promising because of their low voltage
    consumption.
  • Most of the Micro systems require on chip
    applications. So more research should be done on
    low voltage portable systems.
  • Structural stability is one of the key factors in
    planar type pumps, so new manufacturing
    techniques should be observed.
  • Porous type pumps are good for microchip cooling
    systems, yet theyre not portable.

26
THANKS
27
References
  • Alarie, J.P., et al. (2001), Electroosmotically
    Induced Hydraulic Pumping on Microchips, Oak
    Ridge National Laboratory, Oak Ridge.
  • Brask, A., (2003), Principles of Electroosmotic
    Pumps, Tecnical University of Denmark
    Mikroelektronik Centret, Master Thesis c961052.
  • Brask, A., Goranovic Bruus, H., (2003),
    Theoretical analysis of the low-voltage cascade
    electro-osmotic pump, Sensors and Actuators B
    Chemical, Volume 92, Issues 1-2 (July) 127-132
  • Chen, C.H. Santiago, J.G., (2002) A Planar
    Electroosmotic Micropump, Journal of
    Microelectromechanical Systems, Vol. 11, No. 6,
    (December), 672-683.
  • Goranovic, G., (2003), Electrohydrodynamic
    aspects of two-fluid microfluidic systemstheory
    and simulation, Tecnical University of Denmark
    Mikroelektronik Centret, Ph.D. Thesis PhD no.
    000699.
  • Selvaganapathy, P.,et al., Buble Free
    Electrokinetic actuation, submitted to Journal of
    MicroElectroMechanical Systems (in press)
  • Sharp, K.V., et al. (2001), Liquid Flows in
    Microchanells, in The MEMS Handbook, M.
    Gad-el-Hak, Ed., CRC Press, London etc..
  • Takamura, Y., et al. in Brask, A., (2001),
    Principles of Electroosmotic Pumps, Tecnical
    University of Denmark Mikroelektronik Centret,
    Master Thesis c961052(2003).
  • Thopasridharan, M., Parnham, C., Yeary, L.,
    Electroosmotic Pump, 16 October 2004,
    lthttp//www.cep.tntech.edu/mems/Electroosmotic20P
    ump.pdfgt
  • Yao, S., Huber, D., Mikkelsen, J.C. Santiago,
    J.G., (2001), A Large Flowrate Electroosmotic
    Pump with Micron Pores, 2001 ASME International
    Mechanical Engineering Congress and Exposition,
    November 11-16, 2001 New York, NY.
  • Zeng,S., et al. (2002), Electroosmotic flow pumps
    with polymer frits, Sensors and Actuators B
    Chemical, Volume 82, Issues 2-3, (February),
    209-212.
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