Title: Chapter 01: Flows in micro-fluidic systems
1Chapter 01Flows in micro-fluidic systems
- Xiangyu Hu
- Technical University of Munich
2What is a micro-fluidic system?
Nano-tubes
Micro-channels
- A system manipulating fluids in channels having
cross section dimension on less than 100
micro-meters - Smallest micro-channel Nano-tube
3The objectives of micro-fluidic systems
- Micro-Total-Analysis-Systems (mTAS)
- One system to provide all of the possible
required analyses for a given type problem - All processing steps are performed on the chip
- No user interaction required except for
initialization - Portable bedside systems possible
- Lab-on-a-chip
- Micro-fluidics in nature
- Aveoli (Lung bubbles)
4Micro-fluidics is Interdisciplinary
- Micro-Fabrication
- Chemistry
- Biology
- Mechanics
- Control Systems
- Micro-Scale Physics and Thermal/Fluidic Transport
- Numerical Modeling
- Simulation of micro-flows
- Material Science
5The fluids in micro-fluidic system
Injection of a droplet into a micro-channel.
- Simple fluids
- liquids and gases
- Complex fluids
- immersed structures, surfactants, polymers, DNA
Cells in a micro-channel.
Polymer flow in a micro-channel
6Typical fluidic components
Channel-circuit
- Micro-channels and channel-circuit
- Functional structures
- Micro-pump and switches
- Mixing and separating devices
Electroosmotic Pumping
Typical functional structre
7Length scales in micro-fluidic systems
Typical size of a chip
1mm
100mm
Extended lenght of DNA
Micro-channel
10mm
Microstructure and micro-drops
Cellular scale
1mm
Radius of Gyration of DNA
100nm
Colloid and polymer molecular size
10nm
8Deviations from continuum hypothesis for
micro-fluidics I gas microflows
9Deviations from continuum hypothesis for
micro-fluidics II simple liquid micro-flows
- How small should a volume of fluid be so that we
can assign it mean properties? - Nano-meter scale
- At what scales will the statistical fluctuations
be significant? - Nano-meter scales
10Deviations from continuum hypothesis for
micro-fluidics II simple liquid micro-flows
- Slip at wall in nano-scale?
- High shear rate
- Hydrophobic surface
11Deviations from continuum hypothesis for
micro-fluidics III micro-flows with complex
fluids
DNA molecule stretched by flow
- Detailed modeling can not use continuum model
- Nano-Scale
Polymer molecules in a channel flow
Nanowires deformed under shearing
12Conclusion on continuum hypothesis for
micro-fluidics
- Dependent on length scales
- Nano-meter scales NO
- Micro-meter scales Yes, but NO for Gas
- Influence on numerical method
- Nano-meter scales non- continuum
- Micro- and meso-copic methods
- Micro-meter scales continuum
- Macroscopic methods
- Micro-meter scales for gas non- continuum
- Micro- and meso-copic methods
- Nano- to micro-meter scales
- Multi-scale modeling
13Other flow features for micro-fluidics
- Low Reynolds number flow
- Large viscous force
- Low Capillary number flow
- Large surface force
- High Peclet number flow
- Disperse and diffusion
- Slow diffusion effects
- Special transport mechanism
- Mixing chaotic mixing
- Separation particle, polymer and DNA
14Low Reynolds number flow (Stokes flow)
- Reynolds number (Re) is the ratio between
inertial force to viscous force - Scaling between intertial force and viscous force
in NS equation - Length scale L
- Velocity scale U
- Flow classification based on Re
http//www.youtube.com/watch?vgbDscDSUAg4feature
channel_page
http//www.youtube.com/watch?v2ghBUcQG1lQfeature
channel_page
15Low Reynolds number flow (Stokes flow)
- In micro-fluidics, Relt1
- Laminar flow
- the viscous force dominant the inertial force
- Inertial irrelevance
Purcell 1977
http//www.youtube.com/user/Swimmers1
16Low Capillary number flow
- Capillary number (Ca) is the ratio between
viscous force to surface force - What is surface tension?
- Stretch force along the material interface
17Low Capillary number flow
- Capillary number (Ca) is the ratio between
viscous force to surface force - Scaling between viscous force and surface force
in NS equation - Length scale L
- Velocity scale U
18Low Capillary number flow
- In micro-fluidics, Ca ltlt1
- Surface force dominant flow
- Wetting effects
Micro-fluidic pin-ball routing
19High Peclet number flow
- Peclet number (Pe) is the ratio advection rate of
a flow to its diffusion rate - Advection, diffusion and dispersion
- Advection transport that is due to flow
- Diffusion results from movement of particles
along concentration gradients - Dispersion transport that describes local
mixing, which results in locally varying fluid
flow velocity
http//ccl.northwestern.edu/netlogo/models/run.cgi
?SolidDiffusion.591.481
20High Peclet number flow
- In most of the liquid flow, also in
micro-fluidics, Pe gtgt1 - Strategy for faster mixing
- increase the length of mixing layer
- Long channel
- Long trajactory line Chaotic mixing (Use of
disperseion)
21Chaotic Mixing
- Stretching and folding the mixing layer by
localized flows - Different approaches
- Geometric structure
- Surface tension effects
- Electrohydrodynamically-driven
Micro-fluidics crystallization system.
Electrohydrodynamically-driven microfluidic
mixing
22Separation in micro-fluidics
- External force used to move the solute
- Separating particle on different mobility
- Large mass, small velocity
- Dielectric properties
23Separating long DNAs
- Long DNAs
- Same mobility
- Mechanism of separation
- Weissenberger number relaxation time to shear
rate or flow time scale - Longer chain, longer relaxation time
- Longer chain, less diffusion coefficient
24Separating long DNAs (1)
25Separating long DNAs (1)
26Numerical Modeling Challenges
- Multi Physical Phenomenon
- Thermal, Fluidic, Mechanical, Biological,
Chemical, Electrical - Multi-scale
- Continuum and atomistic modeling may coexist
- Multi-phase
- Gas, liquid
- Complex fluids
- Particle, nano-structures, polymer, DNA
- Complex geometry