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Summarized by Ji-Yeon Lee & Soo-Yong Shin

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1 Summarized by Ji-Yeon Lee & Soo-Yong Shin
Using three-dimensional microfluidic networks for solving computationally hard problems PNAS March 13, 2001 vol. 98 no ~2966 Daniel T. Chiu, Elena Pezzoli, Hongkai Wu, Abraham D. Stroock, and George M. Whitesies Harvard University Summarized by Ji-Yeon Lee & Soo-Yong Shin

2 (C) 2001, SNU Biointelligence Lab, http://bi.snu.ac.kr/
Abstract Solving Maximal clique problem 3-MCP, 6-MCP Algorithm parallel fabrication of the microfluidic system parallel searching of all potential solutions by using fluid flow parallel optical readout of all solutions (C) 2001, SNU Biointelligence Lab, 

3 (C) 2001, SNU Biointelligence Lab, http://bi.snu.ac.kr/
Algorithm Four steps 1) for every edge [i,j] of G, label (tag) every subgraph of G that contains vertices i and j 2) for every subgraph, count the number of tags 3) decide whether there are enough tags (edges) in each subgraph to be a clique 4) return the size and identity of the largest clique (C) 2001, SNU Biointelligence Lab, 

4 Implementation of algorithm
Fig A : schematic diagram of 3-vertex graph subgraph well edge reservoir 3D microfluidic system  to avoid the crossover  three vertices & four layers Quantitation of the connectivity  measure the flow from reservoir into well  use liquid containing a uniform suspension of fluorescent beads (filter membrane was used) connected by channel (C) 2001, SNU Biointelligence Lab, 

5 putting a calibrated number of beads into each reservoir
Step 1 putting a calibrated number of beads into each reservoir (parallel operation) spilts and flows simultaneously into both channels Step 2 exploit the optical systems to read out the relative amount of fluorescence in each well (parallel) Step 3 setting the appropriate optical detection threshold for each clique size Step 4 observing the position of the clique along the x and y axes in microfluidic device the size of a clique can be easily derived by knowing its relative displacement along the y axis (C) 2001, SNU Biointelligence Lab, 

6 Schematic of the microfluidic device
(C) 2001, SNU Biointelligence Lab, 

7 Quntitation with fluorescence
(C) 2001, SNU Biointelligence Lab,  [1,2][1,3][2,3] introduced [1,2][2,3] introduced

8 (C) 2001, SNU Biointelligence Lab, http://bi.snu.ac.kr/
Materials and Methods PDMS REM Small sizes of fluorescent beads (400nm or smaller) (C) 2001, SNU Biointelligence Lab, 

9 Results and Discussion
Needed layer (= edges layer + bottom layer) n(n-1)/2 for edges in six vertex problem, = 16 layer Subgraphs with k vertices must have k(k-1)/2 units of fluorescence to be clique  threshold criterion More relaxed criterion to account for errors set a threshold halfway between the intensities expected for a k clique and a k-1 clique must have [(k-1)(k-2)/2 + (k-1)/2] fluorescence intensities (C) 2001, SNU Biointelligence Lab, 

10 (C) 2001, SNU Biointelligence Lab, http://bi.snu.ac.kr/
Even splitting the pressure drop along the two branches is identical cross section and the total length of each channel pathway from reservoir to waste are the same!  flow rate in each channel are indistinguishable (C) 2001, SNU Biointelligence Lab, 

11 Experimental solution to a Three-Vertex Graph
exactly three times!! (C) 2001, SNU Biointelligence Lab, 

12 Experimental solution to a Six-Vertex Graph I
(C) 2001, SNU Biointelligence Lab, 

13 (C) 2001, SNU Biointelligence Lab, http://bi.snu.ac.kr/
Experimental solution to a Six-Vertex Graph II (C) 2001, SNU Biointelligence Lab, 

14 Discussion and Conclusions I
Analog computation device Parallel operation Microfluidic channel Multi-layer structure Fluorescent beads strength high parallelism vs space-time tradeoff weakness exponential increase in its physical size (C) 2001, SNU Biointelligence Lab, 

15 Discussion and Conclusions II
Potential sources of error 1) biased splitting of fluorescent beads at each channel branching 2) misalighment between layers that results in error in the integrated fluorescence intensities  main cause of misalignment between layers is differential shrinkage of PDMS in different layers during fabrication To overcome errors 1) implement error-correction step before integrating the intensities from each layer (reset to zero) 2) use exactly the same procedures (using the same amount of catalyst and curing at the same temperature) (C) 2001, SNU Biointelligence Lab, 

16 Discussion and Conclusions III
Limitation largest graph : 20 vertices or 40 vertices impractical Advantages to using microfluidic system using parallel optical system different color beads (fluorescent) no requirement in power Personal thinking scale-up : both device and fluorescence (C) 2001, SNU Biointelligence Lab, 

17 Using Microfluidic Systems as Analog Devices for Solving Computational Problems
D. R. Reyes, G. M. Whitesides, and A. Manz TAS 2001 Summarized by Soo-Yong Shin

18 (C) 2001, SNU Biointelligence Lab, http://bi.snu.ac.kr/
Abstract Solving shortest path problems using microfluidic chip. Maze searches (C) 2001, SNU Biointelligence Lab, 

19 (C) 2001, SNU Biointelligence Lab, http://bi.snu.ac.kr/
Algorithms Graphical representation of the problems were generated. The graphical representations were fabricated on glass chips Helium gas was used. (C) 2001, SNU Biointelligence Lab, 

20 (C) 2001, SNU Biointelligence Lab, http://bi.snu.ac.kr/
Results Small problems (C) 2001, SNU Biointelligence Lab, 

21 (C) 2001, SNU Biointelligence Lab, http://bi.snu.ac.kr/
Results A segment of a map of London From Traflagar Square to Victoria Station (C) 2001, SNU Biointelligence Lab, 

22 (C) 2001, SNU Biointelligence Lab, http://bi.snu.ac.kr/
Results Solutions of the problems were obtained in less than 250ms. (C) 2001, SNU Biointelligence Lab, 


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