introduction to microfluidics: basics and...
TRANSCRIPT
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© 2002 IBM Corporation
Micro & Nanobioengineering Lab Biomedical Engineering Department McGill University
| McGill, Nov 2005
Introduction to Microfluidics: Basics and Applications
Kate Turner
Hands-on Workshop in Micro and Nanobiotechnology
4th March 2013
wikisites.mcgill.ca/djgroup
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§ What is microfluidics?
§ Why microfluidics?
§ Basics of fluid mechanics
§ Special phenomena associated with the micro-scale § Laminar flow § Diffusion and mixing § Capillary phenomena § Surface energy
§ Microfluidics and lab-on-a-chip devices
Outline
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§ What is microfluidics?
§ Why microfluidics?
§ Basics of fluid mechanics
§ Special phenomena associated with the micro-scale § Laminar flow § Diffusion and mixing § Capillary phenomena § Surface energy
§ Microfluidics and lab-on-a-chip devices
Outline
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Microfluidics
§ Fluidics: handling of liquids and/or gases
§ Micro: has at least one of the following features: § Small volumes § Small size § Low energy consumption § Use of special phenomena
(we’ll talk more about this later) .
A microfluidic channel is about the same width as a human hair, 70 µm
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§ What is microfluidics?
§ Why microfluidics?
§ Basics of fluid mechanics
§ Special phenomena associated with the micro-scale § Laminar flow § Diffusion and mixing § Capillary phenomena § Surface energy
§ Microfluidics and lab-on-a-chip devices
Outline
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Advantages of Microfluidics § Low sample and reagent consumption; fluid volumes (µl; nl; pl; fl) § Small physical and economic footprint § Parallelization and high throughput experimentation § Unique physical phenomena: use of effects in the micro-domain:
§ Laminar flow
§ Capillary forces
§ Diffusion .
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P.J. Lee et al. (2007). Biotech. Bioeng. 97: 1340-6.
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Right: Quake lab group, Stanford, http://thebigone.stanford.edu/ Left: Juncker lab group, McGill, http://wikisites.mcgill.ca/djgroup/
Advantages of Microfluidics
§ Low sample and reagent consumption; fluid volumes (µl; nl; pl; fl) § Small physical and economic footprint
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Advantages of Microfluidics: Lab on a Chip § Parallelization and high throughput experimentation
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§ What is microfluidics?
§ Why microfluidics?
§ Basics of fluid mechanics
§ Special phenomena associated with the micro-scale § Laminar flow § Diffusion and mixing § Capillary phenomena § Surface energy
§ Microfluidics and lab-on-a-chip devices
Outline
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Fluid Mechanics
§ Law: Conservation of mass
§ Law: Conservation of momentum
§ Assumption: Incompressibility
§ Assumption: No-slip boundary condition, i.e. velocity of the fluid flow at a surface is zero
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No-slip Boundary Condition
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Basic Properties § Types of fluids:
§ Newtonian fluids § Non-Newtonian fluids
§ Types of fluid flow:
§ Laminar § Turbulent
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Shea
ring
stre
ss, τ
Rate of shearing strain, dv/dy
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Newtonian Fluids § Linear relationship between stress and strain, i.e. viscosity is
independent of stress and velocity
v + dv v
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Substance Viscosity (mPa·s) Air 0.017
Acetone 0.3 Water 0.9
Mercury 1.5 Olive oil 80 Honey 2,000 – 10,000
Viscosity
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§ Viscosity is a measure of internal friction (resistance) to flow
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Non-Newtonian Fluids
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§ Non-linear relationship between shear stress and shear strain
§ Examples: paint, blood, ketchup, cornstarch solution
Rate of shearing strain, dv/dy
Shea
ring
stre
ss, τ
Newtonian Non-Newtonian shear thickening
Non-Newtonian shear thinning
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Laminar and Turbulent Flow § Laminar flow:
§ Fluid particles move along smooth paths in layers § Most of energy losses are due to viscous effects § Viscous forces are the key players and inertial forces are negligible
§ Turbulent flow: § An unsteady flow where fluid particles move along irregular paths § Inertial forces are the key players and viscous forces are negligible
§ Reynolds number: § Measure of flow turbulence § Re < 2000 for laminar § Due to small dimensions Re < 1 in microfluidic systems
where
ρ: fluid density A: cross-sectional v: fluid velocity area of channel L: characteristic length P: wetted perimeter µ: viscosity
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Laminar and Turbulent Flow
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Couette Flow (Laminar)
§ Couette flow: § One of the plates moves parallel to the other § Steady flow between plates § No-slip condition applies
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Poiseuille Flow (Laminar)
§ Poiseuille flow: § Pressure-driven flow § No-slip condition applies
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§ What is microfluidics?
§ Why microfluidics?
§ Basics of fluid mechanics
§ Special phenomena associated with the micro-scale § Laminar flow § Diffusion and mixing § Capillary phenomena § Surface energy
§ Microfluidics and lab-on-a-chip devices
Outline
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§ What is microfluidics?
§ Why microfluidics?
§ Basics of fluid mechanics
§ Special phenomena associated with the micro-scale § Laminar flow § Diffusion and mixing § Capillary phenomena § Surface energy
§ Microfluidics and lab-on-a-chip devices
Outline
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Laminar Flow
Right: P. Yager et al. (2006). Nature 442: 412-18.
Left: P.J.A. Kenis et al. (1999). Science 285: 83-5.
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Diffusion Diffusion is the transport of particles from a region of higher concentration to one of lower concentration by random motion.
X: diffusion length D: diffusion constant t: time
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For an antibody, D ≈ 40 µm2 s-1
For urea, D ≈ 1400 µm2 s-1
For X = 100 µm, the time becomes: Antibody: 125 s; Urea: 3.6 s
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Diffusion and Mixing
University of Hertfordshire, STRI, http://www.herts.ac.uk/research/stri.html
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Direction of Flow
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Generating Biochemical Gradients
N.L. Jeon et al. (2000). Langmuir 16: 8311–16.
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Generating Biochemical Gradients
N. L. Jeon et al., Langmuir, 2000, 16, 8311–16.
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§ What is microfluidics?
§ Why microfluidics?
§ Basics of fluid mechanics
§ Special phenomena associated with the micro-scale § Laminar flow § Diffusion and mixing § Capillary phenomena § Surface energy
§ Microfluidics and lab-on-a-chip devices
Outline
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Capillary Phenomenon and Liquid Transport
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Capillary Phenomenon and Liquid Transport
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Capillary Phenomenon
r
h
θ
Pressure of the liquid column:
Capillary pressure:
Height of liquid column:
ghP ρ=Δ
rP γ2
−=Δ
grh
ρθγ cos2
=
: Surface tension γ
: Contact angle θ
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Surface Tension
Floating razor blades § Surface tension is a property of cohesion (the attraction of molecules
to like molecules)
§ When an interface is created, the distribution of cohesive forces is asymmetric
§ Molecules at the surface may be pulled on more strongly by bulk molecules
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Wettability § Adhesion vs. cohesion
§ Contact angles are a way to measure liquid-surface interactions
Hydrophobic Hydrophilic
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Capillary Systems
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Capillary Systems
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§ What is microfluidics?
§ Why microfluidics?
§ Basics of fluid mechanics
§ Special phenomena associated with the micro-scale § Laminar flow § Diffusion and mixing § Capillary phenomena § Surface energy
§ Microfluidics and lab-on-a-chip devices
Outline
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Microfluidic and Lab-on-a-Chip Devices
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Microfluidic Devices
Closed chips
Continuous flow Droplet-based
Digital microfluidics
Open Chips
Microfluidic probes (MFP) Micro-arrays
External pressure
Capillary effect
Electrokinetic mechanisms
Electrowetting-on-dielectirc
Surface acoustic waves
Optoelectrowetting
Ink-jet printing
Pin-printing technology
Microcontact printing
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Immunoassay § A biochemical test that measures the concentration of a
substance in a biological liquid § Enzyme-Linked ImmunoSorbent Assay (ELISA)
§ Sandwich assays
Immobilized capture antibody
Captured antigen from the sample
Fluorescently labelled detection antibody
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Capture 1
Capture 2
Fluorescently-labelled Detection Antibodies
Detection
Immobilization Recognition
Reading Signal
Sample Loading
Micromosaic Immunoassay
Immobilization
M. Pla-Roca, D. Juncker. (2011). Biological Microarrays, Humana Press, USA.
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Capture 1
Capture 2
Fluorescently-labelled Detection Antibodies
Detection
Immobilization Recognition
Reading Signal
Sample Loading
Micromosaic Immunoassay
Immobilization
M. Pla-Roca, D. Juncker. (2011). Biological Microarrays, Humana Press, USA.
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Capture 1
Capture 2
Fluorescently-labelled Detection Antibodies
Detection
Immobilization Recognition
Reading Signal
Sample Loading
Micromosaic Immunoassay
Immobilization
M. Pla-Roca, D. Juncker. (2011). Biological Microarrays, Humana Press, USA.
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Droplet-Based Microfluidics
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A.S. Utada et al. (2005). Science 22: 537-41.
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Isolation/Detection of Rare Cells
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S. Nagrath et al. (2007). Nature 450: 1235-39.
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Recapitulating Organ Function on a Chip
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D. Huh et al. (2010). Science 25: 1662-68.
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Microfluidic Probe for Perfusion of Brain Slices
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a b
c d
Technology developed in our laboratory
A. Queval et al. (2010). Lab Chip 10: 326-34.
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Thank You!
QUESTIONS?
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Microfluidics advantages § Parallelization and high throughout experimentation
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Source: The National Institute of Standards and Technology (NIST)
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Incompressible vs compressible:
Source: The Nucleus Learning website
Gas particles are very spread out, so can be compressed
Liquid particles are not spread out, so hard to be compressed
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Surface energy of various liquids
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Surface energy of various solids
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Autonomous control with hydrogels
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D. J. Beebe, Nature 404, 588-590 (2000).
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• Superhydrophobic Surfaces: Hydrophobic surface having
nano-‐scale roughness.
water
superhydrophobic • Hydrophobic Surfaces: “Water-‐fearing surface” Water tries to minimize contact with surface.
water
hydrophobic • Hydrophilic Surfaces: “Water-‐loving surface” Water tries to maximize contact with surface.
water hydrophilic
Surface energy
CONTACT ANGLE
0° 5° 40° 35° 100° 160° 115°
Plasma Cleaned Glass
Glass
Polyethylene Glycol SAM
Polystyrene PTFE (Teflon
)
Superhydrophobic IsotacWc
Polypropylene
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