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具雙重力學刺激之細胞移動研究微流道裝置

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國立臺灣大學電機資訊學院生醫電子與資訊學研究所 碩士論文

Graduate Institute of Biomedical Electronics and Bioinformatics College of Electrical Engineering and Computer Science

National Taiwan University Master Thesis

具雙重力學刺激之細胞移動研究微流道裝置

Microfluidic Device with Dual Mechanical Cues for Cell Migration Investigation

蔡錦雄

Chin-Hsiung Tsai

指導教授:郭柏齡 博士 林致廷 博士 Advisor: Po-Ling Kuo, Ph.D.

Chih-Ting Lin, Ph.D.

中華民國 101 年 7 月

July, 2012

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致謝

非常感謝郭柏齡老師和林致廷老師,在這兩年的共同指導,提供 許多寶貴的建議,奠基我在學術研究上的基礎。特別感謝郭老師給予 我參加學術會議的機會,得以與其他研究團隊交流互動,拓展視野。

雖然同時參加兩位老師的會議、報告以及實驗會較為忙碌,但學 術上的收穫卻遠大於付出;而與兩邊實驗室成員日常生活的互動、研 究上的討論砥礪,更是令人難忘。特別感謝智傑、毛毛、小田田、Pinky、

翊倫提供的協助與歡樂。

謝謝我的父母與姊姊,給予我各種協助,使我得以無後顧之憂,

盡力學習。最後要感謝的是與我交往八年的女友高秀華,接受我的優 點與缺點,陪伴我走過人生的痛苦與歡笑。

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摘要

細胞移動在許多生理現象及疾病扮演非常重要的角色,例如血管 新生、傷口癒合以及癌症轉移。因此研究細胞移動的基本機制,將對 疾病治療與再生醫學的發展至為關鍵。部分生物力學刺激對細胞移動 的影響,已被廣泛研究並深入探討;然而,在多重訊號同時刺激下,

細胞將如何受到調控,仍是目前了解甚少的領域。在本篇研究中,我 們將具有硬度梯度的水膠整合進入微流道系統中,此一整合型裝置將 能同時提供雙重力學刺激去調控細胞移動。藉由此一裝置,我們將能 在一個更接近人體生理狀況的環境中,深入探討硬度梯度與滲透壓梯 度對細胞移動的影響,此一裝置同時也具有應用在其它研究目的的潛 力。

關鍵字:細胞移動、微流道、水膠、硬度梯度、滲透壓梯度

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Abstract

Cell migration plays an important role in both physiology and disease, such as

angiogenesis, wound healing and cancer metastasis. Therefore, understanding the

fundamental mechanisms of cell migration is crucial to create strategies for disease

treatment and regenerative medicine. Some biomechanical cues have been well

studied about their effects on guiding cell migration, however, few discuss about

simultaneously generating dual or multiple cues to affect cell migration. Here, we

integrated a gradient-compliant polyacrylamide (PA) gel into the microfluidic system,

thus enabling the device to provide dual mechanical cues at the same time. By

adopting this advanced device, we can investigate the effects of stiffness and osmotic

gradients on guiding cell migration in a more in vivo-like environment, and this dual

cues system might also be useful for other applications.

Key words: cell migration, microfluidics, hydrogel, stiffness gradient, osmotic

gradient

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Content

致謝 ... i

摘要 ... ii

Abstract ... iii

Content ... iv

List of Figures ... v

List of Tables ... vi

Chapter 1. Introduction ... 1

Chapter 2. Materials and Methods ... 6

2.1 Device design and operation principle ... 6

2.2 Fabrication of microfluidic system ... 10

2.2.1 Photolithography ... 10

2.2.2 Soft lithography ... 12

2.3 Gradient-compliant polyacrylamide gel ... 13

2.3.1 Polymerization of the polyacrylamide gel ... 13

2.3.2 Functionalization of the polyacrylamide gel ... 14

2.3.3 Characterization of the polyacrylamide gel ... 15

2.4 Fabrication and characterization of the dual mechanical cues device ... 16

2.4.1 Fabrication of PDMS substrate... 16

2.4.2 Integration of the PA gel and the microfluidic channels ... 17

2.4.3 Quantification of the concentration gradient ... 20

2.5 Osmotic gradients simulation ... 20

2.6 Cell culture and cell migration analysis ... 22

Chapter 3. Results and Discussion ... 24

3.1 The integrated PA gel-microfluidic device ... 24

3.2 Concentration gradients generation and analysis ... 27

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3.2.1 Simulation of the sucrose concentration gradient ... 27

3.2.2 Trypan blue concentration gradient ... 30

3.3 Characterization of the gradient-compliant PA gel ... 31

3.3.1 Stiffness gradient ... 31

3.4 C2C12 cell culture and analysis ... 34

3.4.1 Cell culture in the integrated PA gel-microfluidic device ... 34

3.4.2 Cell culture in the high osmolarity cell culture medium ... 36

3.4.3 Cell migration on a gradient-compliant PA gel ... 39

3.5 Evaluation of 2D and 3D hydrogel-microfluidic integration systems ... 42

Chapter 4. Conclusion and Future works ... 44

Reference ... 46

List of Figures

Fig. 2.1: Schematic of the dual mechanical cues device ... 7

Fig. 2.2: Schematic of device operation, dual gradients and signals sensed by the cell ... 9

Fig. 2.3: Fabrication process of master mold ... 11

Fig. 2.4: Fabrication process of PDMS replica ... 12

Fig. 2.5: Polymerization of PA gel ... 14

Fig. 2.6: Protein conjugation with PA gel ... 15

Fig. 2.7: Planarization of PDMS substrate ... 17

Fig. 2.8: Fabrication process for integrating microfluidic system with PA gel ... 19

Fig. 3.1: A photograph of the assembled device and the mask design of the microfluidic channels ... 25

Fig. 3.2: Top-view phase contrast images of the cell culture chamber in the device ... 26

Fig. 3.3: Simulation of concentration gradient and data plots ... 29

Fig. 3.4: A photograph of the trypan blue concentration gradient generated by the device ... 31

Fig. 3.5: Stiffness measurement of the gradient-compliant PA gels ... 33

Fig. 3.6: Fibronectin densities of the PA gels ... 34

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Fig. 3.7: Cell culture after seeding for 24 hours in the devices ... 36 Fig. 3.8: Cell culture with or without high concentration sucrose ... 37 Fig. 3.9: Quantitative analysis of C2C12 cell morphology changes under

hypertonic stress... 38 Fig. 3.10: Windrose plot of cell migration path and positions of cell tracking

on a gradient-compliant PA gel. ... 40 Fig. 3.11: Quantitative analysis of C2C12 cell migration speed and TI. ... 40 Fig. 3.12: Distribution of cell numbers along a gradient-compliant PA gel.

... 41

List of Tables

Table 1: Quantitative description of C2C12 cell morphology under different hypertonic stress ... 38 Table 2: Quantitative description of C2C12 cell migration speed and TI ... 40 Table 3: A comparison table of 2D and 3D hydrogel-microfluidic integrated systems ... 43

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Chapter 1. Introduction

Cell migration plays an important role in physiology and disease (Gardel,

Schneider et al. 2010). Cells fail to migrate to the right position during embryogenesis

may cause severe development disorders. Cancer cells might change the extra cellular

matrix (ECM) and induce a series of events to help them migrate to other organs, the

metastasis. For tissue engineering, constructing an appropriate microenvironment and

guiding the cells to the right place are critical for cells to function as they did in the

original organs. Therefore, understanding the fundamental mechanisms of cell

migration is crucial to create strategies for disease treatment and regenerative

medicine.

Biochemical and biomechanical cues are two major stimulation types to guide

cell migration, and clarifying how these signals affect cell migration is an important

research field. Microfluidic systems are capable to generate stable linear or

logarithmic chemical gradients and therefore are widely used to study chemotaxis,

which describe how chemical factors attract or repel cell migrate along the direction

of chemical gradient. Human neutrophils migrate to the place with the highest

concentration of interleukin-8 (IL-8) and demonstrate different behaviors to different

gradient patterns (Li Jeon, Baskaran et al. 2002). Venular and arterial endothelial cells

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show different reactions to the gradient of fibroblast growth factor 2 (FGF2) and

different gradient strengths of vascular endothelial growth factor A 165 (VEGFA165)

could induce human umbilical vein endothelial cells (HUVECs) to generate different

chemotaxis responses (Barkefors, Le Jan et al. 2008).

Astrocyte has been observed to migrate toward hypotonic region under an

osmotic gradient (Saadoun, Papadopoulos et al. 2005), and that observation might be

involved with the water flow through aquaporins (AQPs) on the cell membrane

(Papadopoulos, Saadoun et al. 2008) Some other experiments also show that the

osmolarity play a role in controlling cell motility (Loitto, Karlsson et al. 2009). A

theoretical study proposes that the osmotic gradient can induce water flux to facilitate

the cell motility (Jaeger, Carin et al. 1999). Although the mechanism is still not clear,

the osmotic gradient might be a fundamental mechanical stimulation to guide cell

migration.

Substrate stiffness is another important mechanical stimulation that has been

shown to control the differentiation of mesenchymal stem cells (Engler, Sen et al.

2006) and cell migration. 3T3 fibroblast (Lo, Wang et al. 2000), vascular smooth

muscle cells (Wong, Velasco et al. 2003; Isenberg, DiMilla et al. 2009) and

macrophages (Nemir, Hayenga et al. 2010) have been demonstrated that they would

migrate to stiffer region from softer region of the substrata. This phenomenon is

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durotaxis, and the most common material to study how cell response to substrata

biophysical signals is polyacrylamide (PA) gel (Gribova, Crouzier et al. 2011). The

preparation and characteristics of polyacrylamide gel are well established and studied

(Tse and Engler 2010).

Although these studies have shown deep insights to explain the relation between

one specific signal and cell migration, there are still few have built an environment

providing dual or multiple gradient cues simultaneously. Understanding the cell

behaviors under a more in vivo-like situation will further extend our knowledge to cell

migration and have more reliable information for medical application. However, this

idea is mainly limited by the nature that one method can usually generate only one

well-controlled signal. One of the approaches to overcome this challenge with

microfluidics is designing a functional channel-geometry to generate shear stress

gradients in one cell culture chamber, thus it can cooperate with chemical gradient to

guide cell migration at the same time (Park, Yoo et al. 2009). Despite their many

benefits, there are a number of small, but important, problems. For example, the two

stimulations could not be controlled independently since the chemical gradient is also

influenced by the flow profile. Another weakness is that the real flow velocity is very

difficult to be measured for the flow direction is not simply straight. Moreover, the

properties of substrata still could not be changed while these signals are also critical to

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guide cell migration.

In this study, we propose a new approach that integrates two different systems

into a dual cues device which can generate substrate stiffness and osmotic gradients

simultaneously. The two systems in this device are: (1) a gradient-compliant PA gel

which is responsible for the first mechanical cue, the substrate stiffness gradient, and

(2) a microfluidic system which can generate the second mechanical cue, the osmotic

gradient. Sucrose is selected here to adjust the osmolarity of the cell culture media,

and it has been used before to study the effect of hypertonic stress on C2C12 cells

(Alfieri, Bonelli et al. 2006). The design of the microfluidic system can be divided

into two sides: (1) the source side which continues to provide cell culture media with

highest sucrose concentration to the cell culture chamber in the microfluidics, and (2)

the free side which allows the cell culture chamber to access the bulk solution without

sucrose. The gradient is built through the diffusion of sucrose from source side to free

side and can be maintained for long term cell culture studies. To develop our dual

cues device, we have created two new steps to embed the PA gel in the microfluidic

system and protect the gel from damages during the conventional

poly(dimethylsiloxane) (PDMS) microfluidics fabrication process.

The C2C12 mouse myoblast is an appropriate candidate to be investigated with

osmotic and stiffness gradients. This cell line has been shown that the expression of

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AOP5 is regulated by differentiation and hypertonic stress (Hwang, Lee et al. 2002).

The morphology of C2C12 cells is found to depend on substrate stiffness (Engler,

Griffin et al. 2004). However, the effects of these mechanical cues on C2C12 cell

migration are still not clear.

We hypothesize that C2C12 cell migration can be influenced by both stiffness

and osmotic gradients and the two signals can facilitate with each other to guide cell

migration. So far, we have successfully performed C2C12 cell culture in our device.

We also cultured C2C12 cells with a high osmolarity cell culture medium in the

culture dish, and analyzed cell migration on a gradient-compliant PA gel. These

results provide important information for further experiments to test our hypotheses.

The device presented in this study might be the first one to embed a

gradient-compliant PA gel in a microfluidic system, and this device has the potential

to be used to study cell migration under two different stimulations which is more

close to the in vivo system. The first stimulation is stiffness gradient, and the second

one can be osmotic gradients or theoretically, chemical gradients if the solute is

replaced with chemoacttractants, thus making the device more flexible to be adopted

for other studies.

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Chapter 2. Materials and Methods

2.1 Device design and operation principle

The main components of the device are shown in Fig 2.1, a. The microfluidic

channel includes the main channels and inlet channels (Fig 2.1, b), and their main

function is to provide fresh cell culture medium, remove the waste produced by the

cells and generate osmotic gradients. Polyacrylamide (PA) gel is used to provide

stiffness gradient. The Glas_1 is used to hold PA gel and overcome the challenge that

PA prepolymer solution is difficult to polymerize on PDMS. The square groove on

PDMS substrate is for Glass_1 and PA gel to be embedded in. The main function of

Glass_2 is holding PDMS substrate to ensure the surface of groove on PDMS

substrate is smooth, it’s more important for thin PDMS substrate (i.e. less than 600

μm). The inlet is connected with a syringe pump, and the outlet is a one side of the

main channel (Fig 2.1, c). The important dimension of each component is shown in

Fig 2.1, d.

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Fig. 2.1: Schematic of the dual mechanical cues device (not to scale). (a) Main

components and their functions (in square bracket) of the device. (b) Perspective view

of the top layer, the inlet channels and the main channel. (c) Positions of inlet and

outlet, the blue circle represents the syringe pump. (d) Cross section view of the A to

A’ line in (c).

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The operation principle of the dual mechanical cues device is illustrated in Fig

2.2. The region where inlet channels connected to the main channel is the source side

for high osmolarity cell culture media (high concentration of sucrose), and the outlet

of the main channel is connected to the bulk solution where is sucrose-free cell culture

media (Fig 2.1, a and Fig 2.2, a). Because the flow velocity driven by the syringe

pump is small (≒1×10-9 m/sec) in the main channel , the distribution of sucrose

would be similar with the result from diffusion, thus creating a concentration gradient

in the direction from inlet to outlet. The cell migration experiment is performed in the

cell culture chamber composed of the main channel and a compliant-gradient PA gel.

The direction of the two stimulations, stiffness and osmotic gradients, in the cell

culture chamber is shown in Fig 2.2, b, and they are perpendicular with each other.

However, it is flexible to change the relative direction between them dependent on the

requirement of different experiments. Fig 2.2, c shows the concept about how the two

signals simultaneously stimulate a cell in the cell culture chamber. The cell can not

only sense the osmolarity difference between the front and the back, but also stiffness

difference between the left side and the right side of the cell.

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Fig. 2.2: Schematic of device operation, dual gradients and signals sensed by the cell

(not to scale). (a) The whole device, except the inlet tube, is immersed in the standard

cell culture media. (b) The color changes indicate the intensity distribution from

maximum to minimum of the two stimulations in the cell culture chamber. (c)

Enlarged dashed-line box in the middle of (b) shows the two different gradient signals

sensed by the cell attached on the PA gel.

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2.2 Fabrication of microfluidic system

2.2.1 Photolithography

The microfluidic channels (Fig 2.1, a) was fabricated by soft lithography. The

first step was to build the master mold by photolithography (Fig 2.3). We used silicon

wafer as the substrate for photoresist (PR), SU8-2050. The wafer was cleaned with

buffered oxide etch (BOE) to remove the native oxide to promote the adhesion of PR

on the substrate (Fig 2.3, a). The PR (shown in yellow in Fig 2.3) was poured on the

wafer and spin at 1600 rpm to have a thin-film with thickness of 100 μm (Fig 2.3, b).

After the spin coating process, bake PR at 65℃ for 5 minutes then 95℃ for 20

minutes on a hotplate and finally leave PR to cool to room temperature (Fig 2.3, c).

Right after soft bake, use UV light to expose the PR under a photomask to transfer the

pattern from the mask to PR (Fig 2.3, d). The energy used in the exposure process is 7

mJ/cm2 and the exposure time is 35 sec. Then replace the wafer to the hotplate for

post exposure bake process, bake the PR at 65℃ for 5 minutes then 95℃ for 10

minutes and finally leave PR to cool to room temperature. The shape of patterns

should appear after the baking process (Fig 2.3, e). After post exposure bake, immerse

PR in the Microchem’s SU-8 developer, and develop PR for 7 minutes (or until the

non-pattern PR is removed) with an ultrasonic bath (Fig 2.3, f). Then rinse the PR

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with fresh developer solution, isopropyl alcohol (IPA) and deionized water

sequentially. Air dry with nitrogen, then bake the PR at 150℃ for 2 minutes (Fig 2.3,

g). Silanize the product with dichlorodimethylsilane (DCDMS) in a desiccator

overnight to form a thin film on PR and wafer (red film in Fig 2.3, h). That film could

prevent PR from damage during fabricating PDMS replica. After these processes, we

had a silanized master mold of the microfluidic channels.

Fig. 2.3: Fabrication process of master mold. (a) Clean the surface of the silicon wafer.

(b) Spin coat the SU8-2050 PR (yellow drop) on the silicon wafer. (c) Soft bake. (d)

Exposure PR. (e) Post exposure bake. (f) Develop. (g) Hard bake. (h) Silanize the

SU-8 precursor.

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2.2.2 Soft lithography

The second step of soft lithography is shown in Fig 2.4. Pour Sylgard 184

(PDMS prepolymer: curing agent in 10:1 by weight) on the master mold and cure it at

60℃ for at least two hours (Fig 2.4, a). Remove the PDMS replica from master mold

(Fig 2.4, b) and punch a hole on the replica for inlet, then autoclave it at 120℃ for 30

minutes (Fig2.4, c) to promote the polymerization of PDMS and decrease

uncrosslinked oligomers, which might be toxic to cells (Hanson, Cui et al. 2011). The

PDMS replica or microfluidic channels were ready to be used in the integration

process (Fig 2.8, c).

Fig. 2.4: Fabrication process of PDMS replica. (a) Pour the mixture of PDMS

prepolymer and curing agent (10:1 by weight) on the silanized master mold, then cure

it at 60℃. (b) Replace the PDMS replica from the master mold. (c) Punch a hole for

inlet, then autoclave the PDMS replica for 15 min.

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2.3 Gradient-compliant polyacrylamide gel

2.3.1 Polymerization of the polyacrylamide gel

The preparation of gradient-compliant PA gel is slightly modified from Engler’s

protocol (Tse and Engler 2010). Briefly, the PA prepolymer solution was polymerized

between two coverslips (Fig 2.5). One of the coverslip was modified with

glutaraldehyde to enhance PA gel to attach on coverslip, and this modification is

especially important for gradient-polymerized PA gel. The other coverslip was

modified with dichlorodimethylsilane (DCDMS) to make the surface hydrophobic to

smooth the surface of the PA gel. The PA prepolymer solution was composed of 10%

acrylamide (w/v ratio), 0.3% bis-acrylamide, 0.4% acrylic acid, 0.5% Irgacure 2959

(photoinitiator) and deionized water. The intensity of the stiffness gradient can be

controlled through exposure time, mask opacity, the concentration of Irgacure 2959

and UV power.

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Fig. 2.5: Polymerization of PA gel. The PA prepolymer solution sits in between GA

activated coverslip and DCDMS activated coverslip, then polymerize the prepolymer

solution with UV light (wavelength = 365nm) filtered with a photomask, thus

generating a non-uniform polymerization in the PA prepolymer solution.

2.3.2 Functionalization of the polyacrylamide gel

The PA gel could be further modified to functionalize the surface with extra

cellular matrix proteins, for example, fibronectin (Fig 2.6). The method of protein

conjugation was through carbodiimide-mediated cross-linking (Kandow, Georges et al.

2007). However, we used 1-(3-(dimethylamino) propyl)-3-ethyl-carbodimide

methiodide (ETC) instead of 1-ethyl-3-(3-dimethyllaminopropyl) carbodiimide

hydrochloride (EDC). Because the molecular weight between ETC and EDC is

different, from our experience, the appropriate concentration of ETC is 40.3 mg/ml.

The concentration of fibronectin is 100μg/ml.

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Fig. 2.6: Protein conjugation with PA gel. The ETC (yellow) can react with acrylic

acid (red) of PA gel to form an unstable intermediate, which can react with the protein

(green), thus conjugating the protein on the PA gel.

2.3.3 Characterization of the polyacrylamide gel

We used immunofluorescence to verify a uniform density of fibronectin

conjugation among the gradient-compliant PA gel. The primary antibody

(anti-fibronectin) was diluted with PBS (4% BSA) in 1:400, and the secondary

antibody (anti-rabbit) was diluted with PBS (4% BSA) in 1:600. The fluorescent

images were analyzed by Image J.

The measurement of PA gel stiffness was kindly assisted by Bioceramics and

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Composites Lab in institute of biomedical engineering, national Taiwan university.

We used TR800PB probe with spring constant about 0.615 N/m to 0.731 N/m, and the

Possion ratio of PA gel was defined as 0.42 (Engler, Rehfeldt et al. 2007).

2.4 Fabrication and characterization of the dual mechanical cues device

2.4.1 Fabrication of PDMS substrate

Besides the microfluidic channels, we also used soft lithography to make another

PDMS replica, the PDMS substrate for holding Glass_1 (Fig 2.1, a). The process is

shown in Fig 2.7. We used laser ablation to trim a transparency film to a square (5.1

mm x 5.1 mm), then attached it on the glass with 3M double tape. It is the master

mold for the groove in the PDMS substrate. Poly (methyl methacrylate) (PMMA) was

used here as a spacing to define the thickness of PDMS substrate. PDMS prepolymer

solution was poured on the master mold, then we placed a DCDMS modified glass

dish on the PMMA. The extra PDMS solution was squeezed out by applying a force

on the glass, then the whole setup was placed in an oven to cure the PDMS. This

smoothing process enables the surface of groove on the PDMS to be flat after bonding

to Glass_2, thus increasing the success rate of bonding between Glass_1 and PDMS

substrate.

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Fig. 2.7: Planarization of PDMS substrate. The master mold of PDMS substrate is

fabricated by attaching customized PMMA spacing and transparency film with 3M

double tape to the glass slide. Then use standard PDMS replication process and

pressurized glass dish to smooth top surface of the PDMS replica.

2.4.2 Integration of the PA gel and the microfluidic channels

The integration process of the PA gel and the microfluidic system (Fig 2.8)

started from assembling Glass_1, PDMS substrate and Glass_2. We used oxygen

plasma bonding method and it would render the PDMS surface to be hydrophilic.

Therefore, we had to cover the non-bonding area with 3M tape to retain their

hydrophobicity, which prevented chemical solutions spreading from the groove during

the surface modification process of Glass_1. The PA polymerization process was

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similar with the description in section 2.3.1. During this process, the extra silane on

the DCDMS-modified coverslip had to be removed, or it would transfer to the PDMS

surface and make these areas unable to be activated by air plasma. The final bonding

process (Fig 2.8, c) was completed as fast as possible to decrease the possibility to

dehydrate the PA gel, and we also use a customized coverslip (5 mm x 5mm) to

protect the PA gel from reactive ion species. The fastest bonding condition (18W, 890

mtorr, 33 sec) we had was achieved through performing the air plasma activation

under higher process pressure. The device was filled with deionized water to prevent

the PA gel from dehydration, some bubbles might appear during this process. After

sterilizing the device with UV light, we immersed it in deionized water overnight to

remove bubbles, then injected the ETC solution through the inlet to perform the

protein-PA gel conjugation process (section 2.3.2). The functionalized device was

ready to be used in cell culture experiments or kept in PBS at 4℃.

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Fig. 2.8: Fabrication process for integrating microfluidic system with PA gel.

(a) Use oxygen plasma to activate Glass_1, PDMS substrate and Glass_2 except

non-groove area of the PDMS substrate (protected by 3M tape). Bond PDMS

substrate and Glass_2 first, and then bond Glass_1 to the surface of the groove. After

completing the bonding process, re-activate Glass_1 with oxygen plasma again. (b)

Modify the Glass_1 surface and then polymerize the PA prepolymer solution on the

glass. (c) Treat the microfluidic channel and the product from step (c) with air plasma

except the PA gel area, and bond them together. (d) Leave the device at room

temperature for at least 30 minute to enhance the bonding effect.

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2.4.3 Quantification of the concentration gradient

We used trypan blue (Mw=872.88 Da) as the solute to observe the color

gradient to simulate the sucrose (Mw=342.3 Da ) gradient in the cell culture

chamber . We captured the images continuously from A to A’ (Fig 3.4) with a phase

contrast microscope. The gray intensity of each image was analyzed by Image J. We

defined the average intensity of the final 100 point as the background (IB). The gray

intensity of each data point (except the final 100 points) subtracted from IB to IC. The

minimum of IC was defined as IM, and the normalized concentration of each point was

defined as:

Normalized concentration=IC IM

2.5 Osmotic gradients simulation

In our study, we used sucrose to control osmolarity, thus the osmolarity

difference sensed by a cell is proportional to the concentration gradient of sucrose. To

predict the concentration gradient and the flow velocity profile in the cell culture

chamber (Fig 2.2), we used COMSOL Multiphysics 4.2a to simulate these

distributions in a two-dimensional simulation. In the two simulations below, the fluid

was defined as incompressible flow and neglect inertial term. The diffusion

coefficient of sucrose was defined as 5 x 10-10 m2/s for free flow media. All the results

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were presented in the equilibrium state except the concentration-time dependent

change (Fig 3.3, b).

For the top view to the cell culture chamber, we coupled two physical models,

laminar flow and transport of diluted species, to perform the sucrose concentration

and flow profile in the free flow area. The normal inflow velocity was 1 x 10-7 m/s,

the inflow concentration was 200 mM, and the outflow concentration was 0 mM since

we assumed that the solutes disappeared quickly as they accessed to the bulk area.

The mesh settings was physics-controlled mesh consisted of 2012 elements (normal).

The characteristics of water were generated from the default setting in COMSOL

Multiphysics.

For a more specific simulation to our device, we used the other two physical

models, Brinkman equations and species transport in porous media. This model

construction could give us a more realistic prediction since the substrate in the cell

culture media was PA gel, a porous medium. We built the whole model according to

COMSOL model gallery (model ID: 170). In Brinkman equations, the fluid properties

were generated from the default setting of water, while the porous matrix properties

were user defined. The porosity of porous medium gel was defined as 0.3 between

solid (0) and free flow (1), and permeability was defined as 1 x 10-14 m2 (Grattoni,

Al-Sharji et al. 2001). The porosity of free flow area was defined as 1, and

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permeability was defined as 1 m2. For setting species transport in porous media, we

defined the porosity of PA gel as 0.3, and bulk density 1000 kg/m3 to represent water.

The diffusion coefficient of sucrose in porous media was defined as 1 x 10-10 m2/s,

which was smaller than that in free flow media. The other parameters were defined as

in the previous case, and the mesh settings was physics-controlled mesh consisted of

5125 elements (coarser).

2.6 Cell culture and cell migration analysis

The cell line used in our studies was C2C12 mouse myoblast cells. The cells

were kept in the conventional incubator (37℃, 5%CO2) and supplied with cell culture

media (10% FBS and 1% antibiotics in Dulbecco’s Modified Eagle’s Medium). For

cell culture test in the device, the cells were delivered to the cell culture camber by

pipeting the cell suspension (106 cells/ml) several times in front of the outlet. When

culturing cells in high osmolarity culture media, we added sucrose to increase the

osmolarity and had the cell density relatively low (2000 cells/cm2) to decrease the

possibility of cell-cell contact.

For cell migration experiments, the cell density on the PA gel was 1850 cells/cm2.

The cells were cultured at conventional incubator for 24 hours before cell migration

tracking. During the cell migration tracking, the cells were cultured at a customized

cell culture chamber on a motor stage of the microscopy. The environment was kept

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as in a conventional incubator.

To analyze the cell migration on a gradient-compliant PA gel, we tracked the

cells by a phase contrast microscope. Six fields from the hard regions to the soft

regions were chose and captured at 20 min intervals over 8hrs through CCD digital

camera. Cells that came into contact with each other were excluded from tracking. We

used a Labview program to identify the centroids of the cells, and the data were

transferred to the excel format, which can be the imported to Image J

(chemotaxis_tool) for further analysis. The windrose plots were showed for

qualitative results of cell migration path. The tactic index (TI) was used to

quantitatively describe how strongly the cell migration was influenced by the

stimulation (Isenberg, DiMilla et al. 2009; Sochol, Higa et al. 2011).

TI=X L

X: mean displacement along gradient direction; L: total path length

TI would be 0 if the cell migration was unbiased, and 1 if it was fully biased.

After being incubated for 48hrs, cells were fixed and stained with

4’,6-diamidine-2’-phenylindole dihydrochloride (DAPI) to count the number of cells

in different places on the PA gel. All the statistical analyses were performed with t-test

except one sample t test for tactic index.

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Chapter 3. Results and Discussion

3.1 The integrated PA gel-microfluidic device

A photograph of our device is shown in Fig 3.1, and a picture of the photomask

is also shown below it to demonstrate the microfluidic channel design more clearly.

The long inlet channels are designed to increase the hydraulic resistance in these

channels, and that high resistance can increase the flow stability in the source side of

the cell culture chamber. This will be important to have uniform concentrations along

the direction perpendicular to the input flow. The whole device is transparent, which

is an advantage for cell-research users because this will be compatible to their daily

instrument, for example, the phase contrast microscope. However, the thickness (1

mm) of the PDMS substrate will be an issue if the user wants to study cell organelles

or cytoskeletons. The possible solution for the thickness issue will be further

discussed in chapter five. Air bubbles appear sometimes in the device during injecting

deionized water into the cell culture chamber by connecting the inlet to the syringe.

However, it does not affect the performance of the device since the bubbles will

disappear easily when we immerse it in the deionized water overnight. The device can

be kept in sterilized deionized-water for over one week before the functionalization

process of the PA gel.

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Fig. 3.1: A photograph of the assembled device and the mask design of the

microfluidic channels.

Some of the misalignments were shown in Fig 3.2. The possibility of

misalignments during bonding process can be largely decreased though designing

lock and key structures to the microfluidic channels and the PDMS substrate,

respectively. Another misalignment is caused by that the PA gel were not fully cover

the Glass_1 (Fig 3.2, c). PDMS might lead to this consequence because it can

interfere with the polymerization of PA gel. To our knowledge, there is no appropriate

explanation to this phenomenon, thus making this issue much difficult to be solved.

Despite of this issue, the device is still capable to generate a stable concentration

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gradient when the input flow is slow enough to make the solute can only move

through diffusion in the cell culture chamber.

Fig. 3.2: Top-view phase contrast images of the cell culture chamber in the device. (a),

(b) and (c) indicate the misalignments of the device. Red arrows mean the distance

between the edge of microfluidic channels and the edge of the PDMS substrate. Blue

arrows: microfluidic channels and Glass_1. Green arrow: Glass_1 and PA gel. (d) The

surface of the PA gel in the device.

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3.2 Concentration gradients generation and analysis

3.2.1 Simulation of the sucrose concentration gradient

The simulation results are shown in Fig 3.3. There are eight inlet ports to the cell

culture chamber, and these eight point sources form a line source to supply the solute

to diffuse into the cell culture chamber. The line source will be more appropriate to

generate uniform concentration gradient along different position of y-axis. The arrow

surface also shows the velocity field is uniform in the cell culture chamber. The data

suggests that the device needs six to ten hours to have a stable gradient (Fig 3.3, b) by

computing the gradients change along the white arrow (Fig 3.3, a) in a time dependent

study. From these simulations, we also noted that the highest concentration in the

source side of cell culture chamber is slightly lower (e.g. 190 mol/m3) than the inflow

setting (e.g. 200 mol/m3). In fact, when the position of the inlet was set much far from

the cell culture chamber, this concentration drop between the inlet and source side

would be more significant (e.g. 200 mol/m3 to 65 mol/m3, data not shown). That can

be an important reference to decide what the concentration would be in the inlet to

generate the gradients we need in the cell culture chamber.

Considerate the cell culture chamber is constructed from free flow area (the main

channel in Fig 2.1, b) and porous media (PA gel), we analyzed the concentration

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distribution in the cross section area (Fig 3.3, c). There is no significant difference in

the concentration distribution between free flow area and porous media when we set

the thickness of the two layers are equal to 100 μm. However, the flow velocity

profiles in these two areas are quite different caused by the low permeability (10-14 m2)

of the PA gel. The highest flow velocity in the free flow area is about 0.15 μm/sec

(Fig 3.3, d), but it is almost zero in the porous media. It might explain that the

fluorophore still existed in the PA gel after wash the whole cell culture chamber with

deionized water several times. The velocity profile is similar with other simulation

work for free flow-porous media (COMSOL model gallery, Model ID: 170).

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Fig. 3.3: Simulation of concentration gradient and data plots. (a) Top-view of the

concentration gradients in the cell culture chamber. (b) A time-dependent change of

the concentration gradient along the white arrow in (a). (c) A cross section view of the

concentration gradients in the cell culture chamber. (d) Perpendicular velocity profile

along the black arrow in (c).

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3.2.2 Trypan blue concentration gradient

The concentration gradient of trypan blue generated by our device is shown in

Fig 3.4. This color gradient existed for over than 36 hours. The concentration gradient

upon the PA gel (AÆA’) is plotted on the right figure. Despite the experimental result

dose not fit much to the simulation result, they give the same trend. Besides the

structure defects described in section 3.1 (Fig 3.2, a, b and c), the non-well controlled

flow rate might also lead to this consequence. The syringe pump can generate flow

rate below than 0.1μL/hr, which is slow enough to have a concentration gradient in

the cell culture chamber from the simulation work. However, we often failed to

generate concentration gradients in the real operation. In some fluorescent

experiments, the whole bulk area (Fig 2.2, a) emitted fluorescence after operating the

device at a flow rate of 0.053μL/hr for 24 hours. The fluorescent intensity of the bulk

area was larger than the intensity of the PA gel area. That might be explained by the

flow was not slow enough to have a more diffusion-like solute distribution. In the

case shown in fig 3.4, we used a passive pump to generate the flow, but the protocol

to operate passive pump has not been established. A more sophisticated method to

control the flow velocity might be a priority.

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Fig. 3.4: A photograph of the trypan blue concentration gradient generated by the

device. The data plot (right) describes the concentration gradient from A to A’ (left),

which is the width of the PA gel.

3.3 Characterization of the gradient-compliant PA gel

3.3.1 Stiffness gradient

The gels used here were polymerized on a coverslip (18 x 18 mm2), and the only

different parameter of these two gels is exposure time: 8 minutes (Fig 3.5, a) and 7.5

minutes (Fig 3.5, b). The data plots suggest that there might be a saturation zone in

the hardest region. The measurement of the soft region is difficult to get accurate data.

Therefore, the linear stiffness gradient only exists in the middle region (more than

one-fourth of the total area). The strength of the gradients (4.43 kPa/mm and 3.51

kPa/mm) should be enough to induce durotaxis for vascular smooth muscle cells

(Wong, Velasco et al. 2003). However, it should be careful to apply these data to have

a quantitative analysis with regard to the relationship between stiffness gradients and

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cell migration. It is difficult to establish an effective protocol to measure the soft

material like PA gel with an atomic force microscope. Furthermore, PA gel may not be

a purely elastic substrate and some data processing will be necessary to provide more

accurate information (Isenberg, DiMilla et al. 2009). Even with this quantitative

analysis issue, the gradient polymerization method is still easy and robust to generate

gradient-compliant PA gel.

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Fig. 3.5: Stiffness measurement of the gradient-compliant PA gels. The distance

between two measured points is 1 mm, and the measurement was conducted

continuously from the hard region to the soft region. The data is the average elasticity

of each point. (a) Exposure time: 8 minutes. (b) Exposure time: 7.5 minutes.

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3.3.2 Fibronectin densities

There is no significant difference of the fluorescence among different positions

on the gradient-compliant PA gel. For comparison, the uniform-gradient PA gel is also

showed. These results suggest that the difference of stiffness or polymerization degree

would not affect the protein conjugation to the PA gel. The fluorescent intensity

profile is similar with other research (Isenberg, DiMilla et al. 2009).

Fig. 3.6: Fibronectin densities of the PA gels. Data are shown in Mean ± SD.

3.4 C2C12 cell culture and analysis

3.4.1 Cell culture in the integrated PA gel-microfluidic device

We have cultured C2C12 cells in four different devices (Fig 3.7). Three of four

are successful, and the one (device 4) failed to culture cells might have a

non-functionalized PA gel. This assumption is lead by two observations. First, there

are cells attached on Glass_1 in device 4, thus the ECM protein and other conditions

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(pH, temparature..etc.) must function appropriately. Second, even the rough surface in

device 3 doesn’t affect cell culture much. The cause of failed ETC-fibronectin

reaction should come from inappropriate bonding between microfluidic channel and

PDMS substrate. As mentioned in section 2.4.2, the DCDMS might transfer to the

surface of PDMS substrate and make bonding failed in the containminated area.

When injecting the reactants into the failed-bonding device with a syringe, the flow

will leak out the device through these failed-bonding regions, which are lower

hydraulic resistance channels. This leakage can also be found when the failed-bonding

device was tested with fluorescent dye. If the DCDMS transfer issue is addressed

properly, the device is easy to perform cell culture with only slightly changes of

functionalization of PA gel and cell culture protocol.

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Fig. 3.7: Cell culture after seeding for 24 hours in the devices. Only device 4 failed to

have a normal cell culture result.

3.4.2 Cell culture in the high osmolarity cell culture medium

After culturing the C2C12 cells in the conventional culture dish with high

osmolarity cell culture medium for 7 hours, most of the cells still did not spread out

(Fig 3.8, 200mM). The osmolarity of DEME we used is 332-352 mM/kg, thus the

osmolarity of the cell culture medium with high concentration sucrose would be about

532-552 mOsm. The osmolarity more than 500 mOsm may decrease the cell viability

(Alfieri, Bonelli et al. 2006). However, some of the cells can spread out after exposing

to hypertonic environment for 26 hours, though the average cell area is still smaller

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than control group (Fig 3.9). The effect of high osmolarity on cell morphology,

projection area, perimeter and circularity ratio, would be much clear by comparing

with the results of control group (p<0.001). The findings are different from other

studies which show that hypertonic stress didn’t induce significant morphological

differences of C2C12 cells or even induced an opposite response (Hwang, Lee et al.

2002; Van Donkelaar, Daniels et al. 2003). Non-confluent cell culture or single cell

culture might be important for C2C12 to have a different response under hypertonic

stress. Moreover, this cell morphology changes between different time periods of

hypertonic stimulation may imply C2C12 cells can sense and adapt to the hypertonic

environment. Therefore, it is possible that C2C12 cells can respond to an osmotic

gradient. A quantitative description of cell morphology is shown in table 1.

Fig. 3.8: Cell culture with or without high concentration sucrose.

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Fig. 3.9: Quantitative analysis of C2C12 cell morphology changes under hypertonic

stress.Treat C2C12 cells treated with hypertonic medium significantly induce

morphological changes. The morphological differences between experimental groups

(7hr and 26hr) imply a compensatory mechanism to the hypertonic stress

Table 1: Quantitative description of C2C12 cell morphology under different

hypertonic stress. Area (μm2), perimeter (μm), Ctrl=Control group.

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3.4.3 Cell migration on a gradient-compliant PA gel

The windrose plots (Fig 3.10) qualitatively show C2C12 cells migration path on

a gradient-compliant PA gel. We divide the cell tracking points into two categories,

one is harder region (hard in Fig 3.10) where the elasticity of the substrate is large

than 12 kPa, and the other is softer region (mid and soft in Fig 3.10) where the

elasticity of the substrate is small than 12 kPa. The preferred migration directions of

C2C12 cells are opposite in the two regions. However, the quantitative analysis (Fig

3.11) shows only C2C12 cells from the hard region have a significant TI value

compared to zero (no biased). The mean of TI in hard region is 0.22 (table 2) which

represents a strong biased migration driven by stiffness gradient (Isenberg, DiMilla et

al. 2009; Sochol, Higa et al. 2011). The cell migration difference is similar with

previous studies, which demonstrated that cell migration speed is faster on a softer

substrate (Lo, Wang et al. 2000; Wong, Velasco et al. 2003).

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Fig. 3.10: Windrose plot of cell migration path and positions of cell tracking on a

gradient-compliant PA gel.

Fig. 3.11: Quantitative analysis of C2C12 cell migration speed and TI.

Table 2: Quantitative description of C2C12 cell migration speed and TI.

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The cell number distribution among different position is shown in fig 3.10. This

data showed a trend that the cell would accumulate at harder region. Consider the

average migration speed of C2C12 cells is about 30μm/hr (Table 1), the trend might

be more significant if we culture the cells for more days (e.g. one week). The

distribution is also important to evaluate whether the C2C12 cell can respond to

stiffness gradient.

Fig. 3.12: Distribution of cell numbers along a gradient-compliant PA gel.

The gel was equally separated into eight columns, and each column was further

separated into ten rows. Therefore, there are ten data points in each column. The

number in the x-axis represents each column sequentially from the hard region to the

soft region. The cell numbers were described in Mean ± SEM of the ten data points in

each column.

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3.5 Evaluation of 2D and 3D hydrogel-microfluidic integration systems

Besides embedding a 2D gel in a microfluidic system, fabricating a 3D gel in the

microfluidic channels would be another design strategy, such as the device developed

by Kamm’s group (Chung, Sudo et al. 2009; Chung, Sudo et al. 2010). In brief, the

prepolymer solution can fill in specific channels and polymerize to form a 3D scaffold.

This would be easy and intuitive to embed a hydrogel in the microfluidic system.

However, the micro-pillar structure design (to confine gel in a specific region) or a

customized micro-injection tool would increase the fabrication complexity. The main

advantage of Kamm’s device would be a 3D cell culture environment and co-culture.

Despite the co-culture can not be operated in the single cell level, the interaction

between two groups of cell can still provide insightful information to cell behavior

research.

Two important issues to this device would be stiffness control and cell tracking

technique. For most materials used in 3D structure, such as collagen, the

biomechanical cues are coupled to some biochemical cues. If the polymerized degree

of collagen gel were changed, the porosity or pore size of the gel would also be

different. Therefore, the cell would also sense different density of the ECM protein

besides stiffness difference. For cell tracking, it can not be performed as easy as in 2D

surface. Sometimes the cell has to carry fluorescent protein for live image tracking.

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The total distance of cell migration is also hard to measure, thus a projected length is

used in most cases. Although we only take two examples to compare (table 3), the

strengths and weaknesses listed should be appropriate to represent general cases.

Table 3: A comparison table of 2D and 3D hydrogel-microfluidic integrated systems.

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Chapter 4. Conclusion and Future works

We have successfully developed a unique fabrication process to integrate a

gradient-compliant PA gel into a microfluidic system. Most of the characteristics of

the gradient-compliant PA gel have been evaluated. The ability to generate

concentration gradients through our device has also been demonstrated. In theory, this

integrated PA gel-microfluidics device could generate two well-controlled mechanical

cues simultaneously to guide cell migration. The C2C12 cell experiments also provide

important information for further experimental design to test our hypotheses.

To fully demonstrate the potential of our device, there are three important future

works. First of all, establish a protocol or a solid approach to well control the inlet

flow. It is especially important since we need the flow to be slow enough such that the

movement of solutes will be similar with random walk. Passive pump or osmotic

pump (Park, Hwang et al. 2007) are possible solutions and good references to control

very slow speed flow. The challenge would be learning about these two approaches.

Secondly, eliminate the structure defects. These defects will interfere with the

control to the concentration gradients, thus increasing the complexity of quantifying

the relationship between signals and cell migration. Besides the lock and key design

described before, fabricate the master mold of PDMS substrate through

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photolithography will also be useful. The difficulty would be familiar with multi-layer

SU-8 photoresist processing to construct the spacing in fig 2.7. Another good

approach is to fabricate thin-film PDMS substrate (Jo, Van Lerberghe et al. 2000).

Besides eliminating structure defects, we can replace the groove with a hole, thus

removing the cost of customized Glass_1. It may also enable our device be capable to

be studied with high power objective lens. The difficulty would be establishing an

effective protocol to reproduce the thin-film PDMS substrate.

Finally, use other cell types to evaluate the performance of our device. For

example, VSMC cells, which has been shown that they would respond to stiffness

gradient. Another example, the astrocyte, which has been demonstrated that it prefers

to migrate to the hypotonic region. Although it may increase the cost of the reagents

for cell culture, we can benefit from shortening the time to confirm our device

function well. That will certainly accelerate the optimization of this dual cues device.

For C2C12 cell migration studies, we can evaluate TI value to verify the impacts

of stiffness and osmotic gradients on guiding cell migration. The migration speed

difference between single cue and dual cues (e.g. osmotic and stiffness gradients in

parallel) would be an appropriate approach to test the facilitation between the two

signals.

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Gardel, M. L., I. C. Schneider, et al. (2010). "Mechanical integration of actin and adhesion dynamics in cell migration." Annual review of cell and developmental biology 26: 315-333.

Grattoni, C. A., H. H. Al-Sharji, et al. (2001). "Rheology and permeability of crosslinked polyacrylamide gel." Journal of colloid and interface science 240(2):

601-607.

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properties." J. Mater. Chem. 21(38): 14354-14366.

Hanson, L., L. Cui, et al. (2011). "A microfluidic positioning chamber for long‐term live‐cell imaging." Microscopy Research and Technique 74(6): 496-501.

Hwang, S. M., R. H. Lee, et al. (2002). "Expression of aquaporin-5 and its regulation in skeletal muscle cells." Experimental & molecular medicine 34(1): 69.

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Li Jeon, N., H. Baskaran, et al. (2002). "Neutrophil chemotaxis in linear and complex gradients of interleukin-8 formed in a microfabricated device." Nature biotechnology 20(8): 826-830.

Lo, C. M., H. B. Wang, et al. (2000). "Cell movement is guided by the rigidity of the substrate." Biophysical journal 79(1): 144-152.

Loitto, V. M., T. Karlsson, et al. (2009). "Water flux in cell motility: expanding the mechanisms of membrane protrusion." Cell motility and the cytoskeleton 66(5):

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Papadopoulos, M., S. Saadoun, et al. (2008). "Aquaporins and cell migration."

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Park, J. Y., C. M. Hwang, et al. (2007). "Gradient generation by an osmotic pump and the behavior of human mesenchymal stem cells under the fetal bovine serum

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Park, J. Y., S. J. Yoo, et al. (2009). "Simultaneous generation of chemical

concentration and mechanical shear stress gradients using microfluidic osmotic flow comparable to interstitial flow." Lab Chip 9(15): 2194-2202.

Saadoun, S., M. C. Papadopoulos, et al. (2005). "Involvement of aquaporin-4 in astroglial cell migration and glial scar formation." Journal of cell science 118(24):

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Sochol, R. D., A. T. Higa, et al. (2011). "Unidirectional mechanical cellular stimuli via micropost array gradients." Soft Matter.

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數據

Fig. 2.1: Schematic of the dual mechanical cues device (not to scale). (a) Main
Fig. 2.2: Schematic of device operation, dual gradients and signals sensed by the cell
Fig. 2.3: Fabrication process of master mold. (a) Clean the surface of the silicon wafer
Fig. 2.4: Fabrication process of PDMS replica. (a) Pour the mixture of PDMS
+7

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