Introduction to BioMEMS & Medical Microdevices
Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals of BioMEMS and Medical Microdevices, by Prof. Steven S. Saliterman, http://saliterman.umn.edu/
Steven S. Saliterman
Electrokinetic Phenomena
Electro-osmosis Fluid movement relative to a stationary charged or conducting
surface through application of an electric field. Electrophoresis
In the presence of an electric field the particle can be induced to move relative to a stationary (e.g. gel) or moving liquid.
Streaming potential Occurs when an aqueous ion containing solution is forced to
flow through a capillary or microchannel under an applied hydrostatic pressure in the absence of an applied electric field. An electroviscous effect occurs, or resistant to flow.
Dielectrophoresis Movement of dielectric particles in a spatially nonuniform
electric field. Electrowetting
Steven S. Saliterman
Electric Double Layer (EDL)
Wikipedia Li, D. Electrokinetics in Microfluidics, 1st ed., Vol. 2., Elsevier, Amsterdam (2004).
Also called the Stern layer
Steven S. Saliterman
EDL about a Spherical Particle…
Kopeliovich, D. Stabilization of colloids, SubsTech.com, 2013
Steven S. Saliterman
Origin of Surface Charge…
1. Most materials obtain a surface charge when they are brought into contact with an aqueous solution.
2. Both glass and polymer microfluidic devices tend to have negatively charged surfaces.
3. Ionization of acidic vs basic surface groups. 4. Different affinities for ions of different signs to two
phases: The distribution of anions and cations between two
immiscible phases such as oil and water, Preferential adsorption of certain ions from an electrolyte
solution onto a solid surface, or Preferential dissolution of ions from a crystal lattice.
5. Charged crystal surfaces. Li, D. Electrokinetics in Microfluidics, 1st ed., Vol. 2., Elsevier, Amsterdam (2004).
Steven S. Saliterman
Calculation Assumptions…
Uniform zeta potential. Electric double layer is thin compared to the
channel dimensions. Electrically insulated channel walls. Low Reynolds numbers. Parallel flow at inlets and outlets. Uniform fluid properties. Constant viscosity and electrical permittivity.
Gad-el-Hak, M. et al. , The MEMS Handbook, CRC Press, New York, NY (2002)
Steven S. Saliterman
The Poisson equation describes the electrical field potential in a dielectric medium.
The Boltzmann equation describes the distribution of ions near a charged surface.
The Poisson-Boltzmann equation is used to describe the ion and potential distributions in the diffuse layer.
The Debye-Huckel parameter is used to define the characteristic thickness of the diffuse layer.
The Helmholtz-Smoluchowski equation is used for both electro-osmotic flow velocity and electrophoretic velocity determination.
Governing Equations…
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Electrophoresis
Charge distribution around an electrophoretic particle:
Nguyen, NT and ST Wereley, Fundamentals and Applications of Microfluidics, Artech House, Boston, MA (2002).
Steven S. Saliterman Images courtesy of Topac
Horizontal Gel Electrophoresis Vertical Slab Gel Electrophoresis
Example: Gel Electrophoresis
Steven S. Saliterman
Electrophoretic Velocity…
A particle’s electrophoretic velocity may be calculated by the Helmholtz-Smoluchowski equation:
o
is the particle's electrophoretic velocity (m/s),
is the applied electrical field (V/m), (epsilon-relative) is the dielectric constant of th
,
ep
z
r
z r pep
Wherev
E
Ev
ε
ε ε ζµ= −
-12o
e medium,
(epsilon-nought) is the permittivity of a vacuum (8.85 x 10 F/m), (zeta) is the zeta potential at the shear plane (V), and (mu) is the dynamic viscosity (kg/(m s)).
εζµ ⋅
Li, D. Electrokinetics in Microfluidics, 1st ed., (2) Elsevier, Amsterdam, 2004.
Steven S. Saliterman
Electrophoretic Motility…
Electrophoretic motility is defined as the electrophoretic velocity per unit of applied electrical field strength, characterizing how fast a particle moves in an electrical field:
ep or pE
z
vv
Eε ε ζ
µ= =
Li, D. Electrokinetics in Microfluidics, 1st ed., Vol. 2., Elsevier, Amsterdam (2004).
Steven S. Saliterman
Streaming Potential
Illustration of the flow-induced electrokinetic field in a microchannel:
Li, D. Electrokinetics in Microfluidics, 1st ed., Vol. 2., Elsevier, Amsterdam (2004).
Fluid is forced through channel.
Steven S. Saliterman
Dielectrophoresis
Physical phenomenon whereby dielectric particles (uncharged particles), in response to a spatially nonuniform electric field, experience a net force directed toward locations with increasing or decreasing field intensity according to the physical properties of the particles and medium.
Steven S. Saliterman
Dielectrophoresis…
Dielectrophoresis is defined as the lateral motion imparted on uncharged particles as a result of polarization (relative to the surrounding medium) induced by non-uniform electric fields.
+
-
Medium Pin electrode
Particle more polarized
Particle less polarized Spatially
nonuniform electric field
Increasing field intensity
Decreasing field intensity
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Wetting
Young’s equation (after Thomas Young who first proposed it in 1805) describes the simple balance of force between the liquid-solid, liquid-vapor, and solid-vapor interfacial surface energies of a droplet on a solid surface:
LG
SL
SG
where (gamma liquid-gas) is the liguid-gas interfacial tension, (gamma solid-liquid) is the solid-liquid interfacial tension, (gamma solid-gas) is the solid-gas inter
LG SL SGcos ,
γγγ
γ θ γ γ+ =
facial tension, and (theta) is the contact angle.θ
Cho, SK, et al., “Creating, transporting, cutting and merging liquid droplets by electrowetting-based actuation for digital microfluidic circuits.” Journal of Microelectrochemcial Systems 12(1) pp. 70-80 (2003)
Thomas Young lived from 1773 to 1829 and was an English scientist and researcher. Discovered interference of light.
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Electrowetting…
Electrowetting Digital Microfluidic Circuit
Cho, SK, et al, “Creating, transporting, cutting and merging liquid droplets by electrowetting-based actuation for digital microfluidic circuits.” Journal of Microelectrochemcial Systems 12(1) pp. 70-80 (2003)
Steven S. Saliterman
The effect of a potential V on the contact angle is then determined by the following:
o
2o
LG
where (theta) is the contact angle, (theta-nought) is the equilibrium contact angle at 0, is the electric potential across the interface (V), (epsilon
cos ( ) cos ,2
r
ro
VV
V Vt
θθ
ε
ε εθ θ γ
=
− =
-12o
) the dielectric constant of the dielectric layer,
(epsilon) is the permittivity of a vacuum (8.85 × 10 F/m), (where F = farad per m) and is its thickness (m). t
ε
Steven S. Saliterman
Microvalves
Passive Valves Check Valves
Directional, like a diode. “Smart” polymers, external stimuli.
Stop Valves Surface modifications of
hydrophobicity/hydrophilicity for immobilization of fluid and materials.
Steven S. Saliterman
Passive Valve…
Hydrogel check valve: (a) Valve leaflets, (b) Anchors, (c) Expanding and closing the valve, and (d) Contacting and opening the valve.
Beebe, DJ, et al, “Physics and applications of microfluidics in biology.” Annual Review of Biomedical Engineering 4, pp. 261-286 (2002)
Steven S. Saliterman
Active Valve Types
Pneumatic Thermopneumatic Thermomechanical Piezoelectric Electrostatic Electromagnetic Electrochemical Capillary force
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Electrostatic Valves…
Electrostatic valves are based on the attractive force between two oppositely charged plates:
22
o
where is the overlapping plate area, is the distance between plates, is an insulator layer thickness, is the applied voltage, (epsilon-
1 ,2
i
r
ir
r i i
AddV
dVF A d d d
ε
εε ε ε ε
=+
o
relative) is the relative dielectric coefficient of the medium, (epsilon-insulator) is the relative dielectric coefficient of the insulator, and (epsilon-nought) is the permittivity of a vacuum.
iεε
Nguyen, NT and ST Wereley, Fundamentals and Applications of Microfluidics, Artech House, Boston, MA (2002).
Steven S. Saliterman
Electromagnetic Valves…
Electromagnetic valves offer the advantage of large deflection and disadvantage of size, low efficiency, and heat generation.
where is the vertical force of a magnetic field,
is the magnetization (A/m), the volume of the magnet, is the magnetic field (Tesla), and is the direction in which the forc
,
m
m
FMVBz
dBF M dVdz= ∫
e is acting.
Nguyen, NT and ST Wereley, Fundamentals and Applications of Microfluidics, Artech House, Boston, MA (2002).
Steven S. Saliterman
Capillary-Force Valves…
Capillary-force valves are based on active and passive control of surface tension and capillary forces. Electrocapillary
Electrowetting phenomena Application of a DC potential moves the fluid
towards the negative cathode.
Steven S. Saliterman
Thermocapillary valves – the Marangoni effect:
Nguyen, NT and ST Wereley, Fundamentals and Applications of Microfluidics, Artech House, Boston, MA (2002).
Faster moving molecules, smaller attractive force, lower viscosity and lower surface tension.
Slower moving molecules, higher attractive force, higher viscosity and higher surface tension.
Fluid
Liquid is pulled from area of low to high surface tension.
Steven S. Saliterman
Passive mixers have no moving parts, but instead rely on diffusion and geometry of the device.
Micromixers
Active mixing increases the interfacial area between fluids and can be accomplished by piezoelectric devices, electrokinetic mixers, chaotic convection.
Image courtesy of Micronit
Steven S. Saliterman
T-mixer and Y-mixer:
Nguyen, NT and ST Wereley, Fundamentals and Applications of Microfluidics, Artech House, Boston, MA (2002).
Passive Micromixer…
Steven S. Saliterman
Serpentine mixers:
Liu, RH, et al., “A passive micromixer: three-dimensional serpentine microchannel.” Proceedings of Transducer ‘99, pp. 730-733 (1999).
Passive Micromixer…
Steven S. Saliterman
Micropumps
Non-mechanical pumping: Electrokinetic methods, Surface tension and capillary effects.
Nguyen, NT and ST Wereley, Fundamentals and Applications of Microfluidics, Artech House, Boston, MA (2002).
Steven S. Saliterman
The energy balance in the liquid column and driving pressure are calculated as follows:
SG SL LG
o
2 LGo oSG SL
owhereγ , γ , and γ (gamma) are interfacial tensions (N/m),
is the capillary radius (m), is the height of the column (m), and
is the pressure differe
2 cos2 ( ) and ,
rh
p
r h p r h pr
γ θπ γ γ π
∆
− = ∆ ∆ =
nce across the gas-liquid interface.
Nguyen, NT and ST Wereley, Fundamentals and Applications of Microfluidics, Artech House, Boston, MA (2002).
Steven S. Saliterman
Specified in more familiar terms of surface tension and specific weight the height is determined as follows:
LG3
o
where (sigma) is the surface tension (N/m) (same as ), and
(gamma) is specific weight of the fluid (N/m ).
2 cos ,hr
σ γ
γ
σ θγ
=
Nguyen, NT and ST Wereley, Fundamentals and Applications of Microfluidics, Artech House, Boston, MA (2002).
Steven S. Saliterman
Mechanical Pumps
Classification: Displacement or dynamic, Check-valve pumps.
Types: Peristaltic pumps, Rotary pumps, Ultrasonic pumps, Magnetic pumping.
Steven S. Saliterman
Ultrasonic Pump…
Ultrasonic pumps work by causing acoustic streaming, which is induced by a mechanical traveling wave (FPW or SAW).
Tabib-Azar, M., Microactuators: Electrical, magnetic, Thermal, Optical, Mechanical, Chemical, and Smart Structures. Kluwer Academic., Boston (1997).
Steven S. Saliterman
Pump Parameters…
Maximum flow rate: Volume of liquid per unit of time delivered by the
pump at zero back pressure (Qmax). Maximum back pressure:
Maximum pressure the pump can work against, At this pressure the flow rate becomes zero.
Pump head: Bernoulli equation, Extended Bernoulli equation.
Efficiency
Young, DF, et al, A Brief Introduction to Fluid Mechanics, 2nd ed., Wiley, New York (2001).
Steven S. Saliterman
Bernoulli’s Equation…
Total pressure (static, hydrostatic, and dynamic) remains constant along a streamline (for a steady, inviscid, and incompressible flow):
2
Total constant along a streamline2Vp p zρ γ= + + =
2
2
where (gamma) is the specific weight of the liquid, / is the pressure head,
/ 2 is the velocity head, and is the
constant along a streamline2
p
V gz
p V zg
γγ
γ + + =
elevation head.
Head:
Young, DF, et al, A Brief Introduction to Fluid Mechanics, 2nd ed., Wiley, New York (2001).
Daniel Bernoulli lived from 1700 to 1782 and was a Dutch-born mathematician and lived in Switzerland much of his life.
Steven S. Saliterman
Extended Bernoulli Equation…
Energy equation for a 1D incompressible, steady flow between two sections, such as an inlet and outlet:
2 2out in in
out in actuator friction loss2 2
outp V p Vgz gz wρ ρ
+ + = + + + −
Dividing by g puts the relationship in terms of energy per unit weight or head:
2 2out out in in
out in2 2 s Lp V p Vz z h h
g gγ γ+ + = + + + −
Young, DF, et al, A Brief Introduction to Fluid Mechanics, 2nd ed., Wiley, New York (2001).
Steven S. Saliterman
where hs is defined as:
actuator
(or work per unit mass of the actuator)actuator actuator actuator
where is the power delivered to the actuator, is the ma
= = ,s
Wm
w W Wh g mg Qγ=
ss flowrate = , is the component of fluid velocity normal to the area , and is the volume flow rate.
AV QV AQ
ρ ρ=
For a pump in control volume, the pump head equals hs and the head loss is hL.
Young, DF, et al, A Brief Introduction to Fluid Mechanics, 2nd ed., Wiley, New York (2001).
Steven S. Saliterman
Efficiency…
The efficiency is the ratio of amount or work that produces a useful effect:
actuator actuatoractuator
actuator
loss and .w Www m
η−
= =
Young, DF, et al, A Brief Introduction to Fluid Mechanics, 2nd ed., Wiley, New York (2001).
Steven S. Saliterman
Summary
Electro-osmosis Fluid movement relative to a stationary charged or conducting
surface through application of an electric field. Electrophoresis
In the presence of an electric field the particle can be induced to move relative to the stationary or moving liquid.
Streaming potential Occurs when an aqueous ion containing solution is forced to
flow through a capillary or microchannel under an applied hydrostatic pressure in the absence of an applied electric field. An electroviscous effect occurs, or resistant to flow.
Dielectrophoresis Movement of dielectric particles in a spatially nonuniform
electric field.
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