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Online proceedings - EDA Publishing Association

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dipping method, hydrodynamic transmission of the fluid in a<br />

microenvironment is used to drive the motion of the<br />

biomolecules. Tabeling et al. [10] mentioned that when a fluid<br />

flows through a square-shaped downward concave slot, the<br />

fluid causes a degree of swirling flow in the corner of the slot,<br />

and the side length ratio of the square-shaped slot influences the<br />

flow state of the fluid in the slot. Bruus et al. [11] also observed<br />

that the fluid created a swirling flow in the corner of the<br />

square-shaped slot when the Reynolds number of the<br />

microchannel increased. In this study, we first applied the<br />

special structure present in the microenvironment to cause the<br />

internal fluid to swirl in multiple directions, to increase the<br />

chaos of the fluids in the microenvironment. Next, by the<br />

traction force of the chaotic fluid flow, we drove the motion of<br />

the biomolecules, raised the evenness and the coverage rate of<br />

adhesion of the biomolecules to the sensing field, reducing the<br />

time for adhesion of the biomolecules to the sensing field, and<br />

improving the efficiency and sensibility of the microbial sensor.<br />

Finally, we used the plant virus TYMV to test the effect of the<br />

adhesion of TYMV on the sensing surface of the<br />

microenvironment.<br />

II.<br />

2.1 Sensing Principle<br />

SENSING PRINCIPLE AND SIMULATION<br />

The virus, TYMV, [12] is a tymovirus of the family<br />

Tymoviridae. TYMV are propagated in cabbage leaves and<br />

stored at -20 ℃ . The structure of TYMV is simulated by<br />

RasMol, a computer program written for molecular graphics<br />

(Fig. 1) and 400 amino groups on the TYMV surface is found.<br />

These amino groups can be easily linked with antibodies and<br />

quantum dots. The TYMV we used were obtained from the<br />

Graduate Institute of Biotechnology, National Chung Hsing<br />

University, Taiwan. This TYMV had Alexa Fluor 594 applied<br />

to it to examine the virus distribution under a confocal<br />

microscope. The other type of fluorescent we used was NCD-4<br />

(N-Cyclohexyl-N-4-Dime-thylamino naphthyl carbodiimide).<br />

This can also be linked with TYMV by the thiol groups on the<br />

TYMV. We used the self-assembled monolayers (SAMs) and<br />

the linker to achieve the goal of affixing the virus to the sensing<br />

surface in the microfluidics channel. The kind of SAMs used in<br />

this paper were MUA (11-mercaptoundecanoic acid). At one<br />

end of the chemical structure of MUA are thiol groups which<br />

can be attached on the gold film of the sensing surface. At the<br />

other end of the MUA is a carboxyl functional group. This<br />

functional group can form a connection between the linker and<br />

MUA. The linker layer we used was EDC<br />

(1-Ethyl-3-[3-dimethylaminopropyl]<br />

carbodiimide<br />

Hydrochloride) and NHS (N-hydroxysuccinimide). After EDC<br />

interacts with MUA, TYMVs will be captured by designed<br />

SAMs. The compound NHS is used to prevent EDC layer<br />

hydrolysis. Therefore, we can achieve a connection between the<br />

virus and the sensing surface. After the virus with quantum dots<br />

was anchored to the sensing surface of the microfluidics<br />

channel, a confocal microscope was used to monitor the surface<br />

of the silicon membrane. A laser beam with a wavelength of<br />

615 nm was passed through an aperture and was focused by an<br />

objective lens onto a small focal volume on the sensor surface.<br />

A mixture of emitted fluorescent lights (594 nm) and reflected<br />

11-13 <br />

May, 2011, Aix-en-Provence, France<br />

<br />

laser lights from the quantum dots were then reobtained by the<br />

objective lens. A photodetection device was used to transforme<br />

the reflected light signal. The results of the confocal<br />

microscopy measurement are shown in Fig. 10(a). Only a few<br />

TYMV with quantum dots were observed on the silicon<br />

membrane and the coverage rate of TYMV was poor. Also,<br />

some large molecules or particles were stuck on the surface<br />

which might result from the aggregation of MUA, EDC, or<br />

NHS by the dipping method. This result is unfavorable if<br />

researchers want to detect viruses at extremely low<br />

concentrations in the solution.<br />

(a)<br />

(b)<br />

Fig. 1 (a) Structure of TYMV (b) amine functional groups of TYMV<br />

2.2 Microfluidics Theory<br />

When TYMV is in a microenvironment, because it cannot<br />

infect any cells and parasitize on them, the virus does not exist<br />

in a living state but in a form of chemical compound. We<br />

therefore regard it as a small particle without life. When the<br />

liquid in the microenvironment is static, the virus particles can<br />

only move by diffusion of Brownian motion caused by the<br />

continuous collision of the media molecules in the<br />

microenvironment. The coefficient of diffusion signifies the<br />

movement capability of the virus by diffusion. Through the<br />

coefficient of diffusion we can understand the movement speed<br />

of the virus in static liquid. Table 1 [13] shows the coefficients<br />

of diffusion of the different viruses in various sizes in water<br />

under room temperature.<br />

Table 1 Different virus diffusion coefficient<br />

Diameter of<br />

Virus<br />

virus (nm)<br />

Diffusion<br />

coefficients (m 2 /s)<br />

Poliovirus [13] 25 1.72×10 –11<br />

Turnip Yellow Mosaic Virus [12] 31.8 1.35×10 –11<br />

Hepatitis B virus [13] 42 1.02×10 –11<br />

Adenovirus [13] 75 5.72×10 –12<br />

Human Immunodeficiency Virus [13] 120 3.58×10 –12<br />

When the virus is in a microenvironment where the medium<br />

is water, assuming the average displacement from the starting<br />

point to the terminal point is 5 mm, and the temperature is 293<br />

K, the time required for adhesion of each virus is shown in Fig.<br />

2. From the figure, we see that 230 hours is required for the<br />

movement of the virus by diffusion. Therefore, if we apply the<br />

diffusion effect as the mechanism of TYMV for adhering to the<br />

sensing surface, the action time is extremely long and the<br />

adhesion efficiency is poor. To solve the aforementioned<br />

obstacles, our study utilizes a microenvironment to drive the<br />

movement of the TYMV, and thus raise the adhesion efficiency<br />

of the TYMV.<br />

367

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