Virtual components for droplet control using Marangoni flows :size-selective filters, traps, channels, and pumps Advisor: Cheng-Hsien Liu Reporter: Y.

Slides:



Advertisements
Similar presentations
CM 4120 Julie King Original Presentation by Todd King and I edited it.
Advertisements

第 5章 太陽電池MATLAB模擬 Program 1: 太陽能電池之輸出電壓、電流、功率響應
Teacher : Cheng-Hsien Liu Student : Chien-Yu Chen(陳鍵瑜)
Soft-lithographic methods for the fabrication of dielectrophoretic devices using molds by proton beam writing 指導教授:許藝菊 報告者:陳亞維.
Introduction to Engineering Mechanics Dar-Yun Chiang.
Advanced Chemical Engineering Thermodynamics
Fluid Dynamics.
CHE/ME 109 Heat Transfer in Electronics LECTURE 17 – INTERNAL FORCED CONVECTION FUNDAMENTALS.
Section 2.2 Correlation 相關係數. 散佈圖 1 散佈圖 2 散佈圖的盲點 兩座標軸的刻度不同,散佈圖的外觀呈 現的相聯性強度,會有不同的感受。 散佈圖 2 相聯性看起來比散佈圖 1 來得強。 以統計數字相關係數做為客觀標準。
Young/Freeman University Physics 11e. Ch 18 Thermal Properties of Matter © 2005 Pearson Education.
彈性變形 點的位移 線的旋轉.
1 EnergyEnergy 能量. 2 哲音與吟詠 構成宇宙的元素? 構成宇宙的元素? 西方哲學家:亞理斯多德 西方哲學家:亞理斯多德 東方哲人:悉達多 東方哲人:悉達多 科學研究的範疇:(化學) 科學研究的範疇:(化學)
演講者:蕭錫源 A new BEM formulation for transient axisymmetric poroelasticity via particular integrals K.H. Park a, P.K. Banerjee b,*
An Electrohydrodynamic Micropump for On-Chip Fluid Pumping on a Flexible Parylene Substrate Reporter: sang-chung yang Advisor: Prof. C.H. Liu Chia-Ling.
Naomi Alandt, Paul Andrews, Jeremiah Zimmerman
第七章 連續機率分配.

Kinetic Model of Gases Section 1.9, Assumptions A gas consists of molecules in ceaseless random motion The size of the molecules is negligible in.
Illumination Normalization with Time-Dependent Intrinsic Images for Video Surveillance Yasuyuki Matsushita, Member, IEEE, Ko Nishino, Member, IEEE, Katsushi.
連續隨機變數 連續變數:時間、分數、重量、……
2015/7/131 Microsystems for UV-Visible and X-Ray Analysis of Protein Crystals Advisor : Cheng-Hsien Liu Report : Ming-Ju Lee Date : 2007/06/06 L.S.L. Cheung.
1 非 線 性 液 流 阻 尼 器 行 為 分 析非 線 性 液 流 阻 尼 器 行 為 分 析 侯建元 致遠管理學院營建管理學系 結構防振液流阻尼器之研發製造及應用研討會 ( )
2009/1/6 Sensing and Actuation in Miniaturized systems Final report Hello everyone !!!!! I am Wu Chih-Wei !!!!!
1 Chemical and Engineering Thermodynamics Chapter 1 Introduction Sandler.
Time-multiplexed droplet manipulation via vibrating ratcheted micro-channels IEEE MEMS(2007) Zhenwen Ding, Woo-Bin Song,Babak Ziaie Purdue University,
Professor: Cheng-Hsien, Liu Student: Hao-Ran, Shih ( ) Date: 2010/12/28 Philip N. Duncan, Transon V. Nguyen and Elliot E. Hui Department of Biomedical.
1 Karthik Visvanathan, Farah Shariff, Seow Yuen Yee and Amar S. Basu Department of Mechanical Engineering, University of Michigan, Ann Arbor, USA Department.
Introduction to Heat Transfer
Forces.
Adsorption Refrigeration System. INTRODUCTION  Adsorption refrigeration system uses adsorbent beds to adsorb and desorb a refrigerant to obtain cooling.
SURVIVAL MODE Quiz 3 –
Thermal Hydraulic Simulation of a SuperCritical-Water-Cooled Reactor Core Using Flownex F.A.Mngomezulu, P.G.Rousseau, V.Naicker School of Mechanical and.
指導老師:許藝菊 學生:邱建龍 介電電泳(DEP)基於微流體粒子分離器Dielectrophoresis (DEP) Based Microfluidic Particle Separator.
楊氏係數測量實驗. Stresses in Solids The level of stress required to obtain a given deformation ※ Tensile stress( 伸長應力 ) , Tensile strain ( 伸長應變 ) and Young’s.
Induction II. Law of Induction The magnitude of the induced emf in a circuit is equal to the rate at which the magnetic flux through the circuit is.
1 Surface Tension Surface tension is a measure of the elastic force (strength) in the surface of a liquid. Also, surface tension is defined as the amount.
Modern Control Systems 2-1 Lecture 02 Modeling (i) –Transfer function 2.1 Circuit Systems 2.2 Mechanical Systems 2.3 Transfer Function.
States of Matter 3 States of Matter: 1)solid- a substance with a definite shape and a definite volume. The particles of a solid vibrate, but do not move.
CHAPTER 6 REVIEW. Boiling Point  The temperature at which a liquid begins to enter the gaseous state.
今日課程內容 摩擦力 阻力與終端速度 等速率圓周運動. 6.2 Friction 摩擦力 Frictional forces are very common in our everyday lives. Examples: 1.If you send a book sliding down a horizontal.
Hydrostatic Transmission Reservoir Internal reservoir-defining body for permitting oil expansion within a hydrostatic transmission housing: –“In a hydrostatic.
Chapter 2: Fluid Statics Chapter 2 Fluid Statics Engineering Mechanics Fluid Mechanics (Week 4) Hsin-Yuan Miao, Ph. D. Assistant Professor Department of.
1. Wafer clean 2. Thermal oxidation 3. PR coating and patterning, Mask #1 4. Wet BOE etching SiO2 Dry RIE etching low stress nitride 5. Positive resist.
1 PicoFill-Systems Outlicensing Electrospray Deposition onto Small Targets Target Applications:  MicroArray Applications: spraying of enzymes, metabolites,
Convection in Flat Plate Boundary Layers P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi A Universal Similarity Law ……
Phases of Matter Vocabulary Heat of Fusion Amount of heat needed to change from a solid to a liquid.
Electromagnetic 1 Chapter 5 Steady electric currents Conduction currents : Drift motion of conduction electrons of holes in conductor or semicond. Electrolytic.
Current spreading of III-nitride light-emitting diodes using plasma treatment Hsin-Ying Lee Ke-Hao Pan Chih-Chien Lin Yun-Chorng Chang Fu-Jen Kao Ching-Ting.
35 Ton LAr Impurity Distribution Measurements and CFD simulation Erik Voirin – Fermilab – Thermal and Fluids Engineering Group / Engineering.
Kinetics Senior Chemistry. Particle Collisions For a reaction to proceed to products, the reactants must collide with one another. Rate of reaction The.
Liquids By:MaKenzie,Lei-Lani,Isis & Noah. Definition: Liquids: have a definite volume and takes the shape of a container. Fluid: a substance that can.
Separation Techniques Using Microfluidics
Valves.
Beijing Institute of Technology
Date of download: 10/16/2017 Copyright © ASME. All rights reserved.
THERMOACOUSTIC REFRIGERATION
Extended Surface Heat Transfer
Figure 35.1 Typical port fuel-injection system, indicating the location of various components. Notice that the fuel-pressure regulator is located on.
Vocabulary Chapter 4.
States of Matter d. Students know the states of matter (solid, liquid, gas) depend on molecular motion. e. Students know that in solids the atoms are closely.
CHAPTER 6 Viscous Flow in Pipes
INTERNAL FORCED CONVECTION
Fundamentals of Convection
Fluids derived from the compaction and
Chapter 10 Properties of Liquids
Solids, Liquids, Gases, and Plasmas
Y. Murakami1, T. Arakawa1, E. H. Jeong2, J. S. Go2 and S. Shoji1
Chapter 4 Lesson 1 States of matter
Fluid Mechanics (Week 4)
States of Matter Chapter 3 Section 1.
Presentation transcript:

Virtual components for droplet control using Marangoni flows :size-selective filters, traps, channels, and pumps Advisor: Cheng-Hsien Liu Reporter: Y. S. Lin Date: 2007/6/20 Amar S.Basu, Seow Yuen Yee, and Yogesh B. Gianchandani University of Michigan, Ann Arbor, USA MEMS2007

Outline Introduction Size-selective virtual channel Single droplet trap Guidewire pump Conclusion

Introduction In droplet-based microfluidic systems, droplet motion is generally guided by microfabricated patterned surfaces Disadvantages - Droplet contact with solid surfaces and sample adsorption to channel walls or other surfaces - Actuators contact the liquid that has contamination concerns

Introduction Several virtual microfluidic components, including channels, filters, traps, and pumps on unpatterned substrates, accomplish their function entirely by localized Marangoni flows by heat sources suspended just above the liquid surface

Introduction Marangoni flow on a liquid surface driven by surface tension gradients Temperature gradient causes surface tension gradients and flow directed from high to low temperature MicroTAS05

Size-selective channel Two heated wires parallel to the liquid surface Recirculating flows occurring as a result of the Marangoni effect are shown with arrows

Size-selective channel 500um diameters droplets entering the channel while a smaller one is rejected S=600um, the minimum diameter for entry into the channel is 250um S=970um, the minimum diameter is 350um Nearly 100% exclusion of off-sized droplet is shown

Single droplet trap The single droplet trap is implemented using a ring- shaped annular heat source Metal pin (s=600um) that a 700um diameter droplet is actively pulled into the trap

Guidewire pump A triangular heat flux projected on the fluid surface pulls droplets in and along its longitudinal axis The droplet achieves a maximum velocity of 196 um/sec

Conclusion Several components for droplet manipulation were presented, all of which operate without physical structures solely by localized Marangoni flows Advantages -It is a non-contact method of actuation -Droplets do not make contact with solid surfaces -It does not require patterned substrates These virtual components are building blocks toward a microsystem for droplet-based assays

Thanks for your listening !!

Droplet mixing The four droplets (φ= um) merge together, one by one, eventually forming a single, φ=600 um droplet in 9 seconds. MicroTAS05

Surface tension & Marangoni effect t=t 0 (1-bT) t0 、 b :隨液體而定之常數 T :溫度 t :表面張力 Ma=|dt/dT|α -1 μ -1 ΔTR 2 L -1 Ma : Marangoni number 熱對流強度 dt/dT :表面張力對溫度的變化率 α :熱擴散係數 ΔT :溫度差 μ : 黏滯性 L :流動區長度 R :流動區半徑

Size-selective channel