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1 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, 1 st ed., Vol. 2., Elsevier, Amsterdam (2004). Also called the Stern layer
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Page 1: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

1

Introduction to BioMEMS & Medical Microdevices

Microfluidic Principles Part 2Companion 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)

WikipediaLi, D. Electrokinetics in Microfluidics, 1st ed., Vol. 2., Elsevier, Amsterdam (2004).

Also called the Stern layer

Page 2: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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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

Electro-Osmotic Flow (EOF)

Wikipedia

+ Anode- CathodeBattery

Page 3: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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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…

Steven S. Saliterman

Electrophoresis

Charge distribution around an electrophoretic particle:

Nguyen, NT and ST Wereley, Fundamentals and Applications of Microfluidics, Artech House, Boston, MA (2002).

Page 4: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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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

Where

v

E

Ev

-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)).

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

E

Li, D. Electrokinetics in Microfluidics, 1st ed., Vol. 2., Elsevier, Amsterdam (2004).

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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 increasingor 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 lesspolarizedSpatially

nonuniform electric field

Increasing field intensity

Decreasing field intensity

Page 6: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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Steven S. Saliterman

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 ,

facial tension, and

(theta) is the contact angle.

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.

Steven S. Saliterman

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

V

V

V Vt

-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

Page 7: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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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

Page 8: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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Steven S. Saliterman

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

A

d

d

V

dVF Ad d d

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.i

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

F

M

V

B

z

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.

Page 9: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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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…

Page 10: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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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

o

where

γ , 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 ,

r

h

p

r h p r h pr

nce across the gas-liquid interface.

Nguyen, NT and ST Wereley, Fundamentals and Applications of Microfluidics, Artech House, Boston, MA (2002).

Page 11: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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Steven S. Saliterman

Specified in more familiar terms of surface tension and specific weight the height is determined as follows:

LG

3

o

where

(sigma) is the surface tension (N/m) (same as ), and

(gamma) is specific weight of the fluid (N/m ).

2 cos ,hr

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).

Page 12: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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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 streamline2

Vp p z

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 g

z

p V zg

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 w

Dividing by g puts the relationship in terms of energy per unit weight or head:

2 2out out in in

out in2 2 s L

p V p Vz z h h

g g

Young, DF, et al, A Brief Introduction to Fluid Mechanics, 2nd ed., Wiley, New York (2001).

Page 13: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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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

W

m

w W Wh

g mg Q

&

&

& &

&

ss flowrate = ,

is the component of fluid velocity normal to the area , and

is the volume flow rate.

AV Q

V A

Q

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 Ww

w m

&

&

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.

Page 14: Introduction to BioMEMS & Medical Microdevices · PDF file1 Introduction to BioMEMS & Medical Microdevices Microfluidic Principles Part 2 Companion lecture to the textbook: Fundamentals

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Steven S. Saliterman

Electrowetting Microvalves – passive and active Micromixers Micropumps