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Procedia Engineering 00 (2014) 000–000

www.elsevier.com/locate/procedia

“APISAT2014”, 2014 Asia-Pacific International Symposium on Aerospace Technology,

APISAT2014

Experimental Investigation on flow Characteristics of Gas in Microchannels

Zhang Kai, Zheng Guanghua*, Du Fenglei

Northwestern Polytechnical University, Xi’an, China

Abstract

An experimental apparatus is developed for further study of flow characteristics in microchannels, compressible gas—air, is used as a work fluid. The experimental study were performed in copper micro tubes and plexiglass tubes with the diameters 0.2mm, 0.3mm, 0.4mm,0.5mm and 1.0mm, and the roughness less than 3%. The results show that the material of micro-tubes does not affect the experimental results; transition from laminar to turbulent flow occurred at critical Reynolds number about 1100 in the tubes with diameter 0.2mm, the critical Reynolds numbers are respectively about 1300,1600,1800 in the tubes with diameters 0.3mm, 0.4mm and 0.5mm, so the conclusion show the descending direction of the critical Reynolds number with the decreasing tube diameters, and the phenomena of transition in advance from laminar to turbulent flow is apparently observed. At the same time, the larger the diameter, the Reynolds number increases, the pressure drop increases even faster. And the results do not change with the change of tube number

.

© 2014 The Authors. Published by Elsevier Ltd.

Peer-review under responsibility of Chinese Society of Aeronautics and Astronautics (CSAA).

Keywords: micro-channel; resistance coefficient; flow characteristics; early transition

1.

Introduction

In recent years, as the electronics, machinery and other fields are developing in the direction of miniaturization and micromation, the flow and heat transfer characteristics in micro-channels are explored by scholars at home and abroad. Microscale flow has significant research value for it is widely use in micro-electromechanical systems

(MEMS), aerospace and other fields[1].

* Corresponding author. Tel.: +86-13227769820; fax: +86-029-88495911.

E-mail address: zhengguanghua@nwpu.edu.cn

1877-7058 © 2014 The Authors. Published by Elsevier Ltd.

Peer-review under responsibility of Chinese Society of Aeronautics and Astronautics (CSAA).

2 Zhang Kai / Procedia Engineering 00 (2014) 000–000

In Hsieh et al[2], the flow resistance of nitrogen through a silicon micro-channel in with 200µm width, 200µm depth, and 24mm length was measured to be consistently smaller than that predicted by the conventional incompressible theory. In Wang Ying et al[3], experimental investigation of polar liquid distilled water and absolute ethyl alcohol in copper micro-tubes has been reported. The diameters of micro-tubes are 231.91µm, 250.88µm,

297.14µm and 210.8µm 9. For laminar flow (Re<1600), friction factors for all micro-tubes have a good agreement with the predicted by the classical theory. In Zhang Tiantian et al[4] , when the Re is in a small value, friction constant is consistent with theoretical predictions no matter how length the tube is. In Ergu et al[5], the water flows through the silicon micro-channel was measured to be consistently higher than that predicted by the conventional incompressible theory.

In this paper, the phenomena of transition in advance in tiny pipeline has been revealed using the compressible fluid - air as the working medium. The conclusions have important significance for further revealing the characteristics of compressible flow in micro-channels.

2.

The Experimental Device

The experimental apparatus used in this study is shown in Figure 1. All the experiments are carried out in a clean room. The experimental apparatus consists of a compressor, a filter, the micro-channel test section, four thermocouples, two pitot tube, two (coarse and fine) pressure regulators, three pressure sensor, a gas mass flow meter, two data acquisition card, a spherical switch, the power supply and a computer.

1 Compressor 10 Pressure sensor

2 Filter 11 Data acquisition card

3 Coarse pressure regulator 12 Spherical switch

4 Fine pressure regulator 13 Gas mass flow meter

6 Pitot tube 14 Power supply

7 Micro-channel test section 15 Computer

8 Thermocouple

Fig.1. The schematic diagram of the experimental system

Zhang Kai / Procedia Engineering 00 (2014) 000–000 3

Fig. 2 Micro-tube SEM image, (a) d=0.5mm, (b) d=0.2mm

In order to get the friction factors of air flow in the micro-tube in this experiment, temperature, pressure and flow rate are needed. The gas is supplied from the compressor and flows through the filter, two pressure regulator. Then the gas goes into the test section. Temperatures of inlet and outlet chambers are measured with thermocouples. After leaving the outlet chamber, the gas passes through the gas mass flow meter connected to the out chamber with a pipe. Pressures of inlet and outlet chambers are measured with pressure sensors. All the data are collected by the data acquisition cards, and finally displayed on the computer.

The micro-tube is scanned by the SEM before the experiment. Fig.2 is the images of the micro-tubes which are enlarged 200 times.

3.

Experimental Results and Analysis

3.1.

Friction Constant and Reynolds

For this experiment the working gas is compressible, so the friction constant can be expressed as[6]

: f comp

 d l

 p

2

1

 p

2

2

RT

 

2

2 ln

 p

1 p

2

( 1 )

The relationship between Reynolds and friction constant of different diameter copper micro-tube can be seen in figure 3. The friction constant for laminar decreases rapidly with the increase of the Reynolds number, and in the turbulent region, the friction constant decreases slowly as the Reynolds number increases. The critical point of laminar flow and turbulent flow is the junction region areas of these two different decreasing trend. We can regard the turning point as the point of the critical Reynolds number, and we can see that the results of the experiment performed in the tube with 0.2mm show that transition from laminar flow to turbulent flow occurs at critical

Reynolds number about 1100 .While the critical Reynolds number of 0.3mm tube is about 1300, and the number of

0.4mm is about 1600, the number of 0.5mm is about 1800, the number of 1.0mm is about 2100 . The conclusion shows that with decreasing diameter, the critical Reynolds number decreases. So transition in advance apparently in the tiny channels.

The relationship between Reynolds and friction constant of different numbers of plexiglass glass micro-tube and copper micro-tube with the diameter 0.3mm can be seen in figure 4. There are almost the same experimental results

4 Zhang Kai / Procedia Engineering 00 (2014) 000–000 between plexiglass glass micro-tube and copper micro-tube when they have the same working conditions. So the relationship between the friction constant and the Reynolds number is mainly affected by the diameter of tube.

Fig.3. The relationship between Reynolds and friction constant of different diameter copper micro-tube

Fig.4. The relationship between Reynolds and friction constant of different numbers of plexiglass micro-tube and copper micro-tube

3.2.

Pressure Drop and Reynolds

In figure 5, as the flow rate and the Reynolds number increases, the flow resistance grows with increasing pressure drop

P. And Reynolds and ΔP approximate as a linear proportional relationship when the Reynolds is small. When the Reynolds number is same, with decreasing diameter, the pressure drop increases. The pressure drop increases slowly as the Reynolds number increases when the Reynolds is small. But at a certain interval, the pressure drop and Reynolds number deviated from the straight line, so the interval can be regarded as the transition zone.

The figure revealed in the tube with 1.0mm show that transition from laminar to turbulent flow occurs at critical

Reynolds numbers about 2300, almost with the conventional channel. While the critical Reynolds numbers of

0.2mm about 1200, the critical Reynolds number about diameter of 0.3mm, 0.4mm, 0.5mm is both less than 2000, so transition in advance in the tiny channel.

Zhang Kai / Procedia Engineering 00 (2014) 000–000 5

Fig.5. The relationship between Reynolds and pressure drop of different diameter copper micro-tube

4.

Conclusion

Transition in advance occurs in the tiny channel, and with decreasing diameter, the critical Reynolds number decreases.

With increasing Reynolds number and diameter, the pressure drop increases faster.

The material of the micro tubes does not affect the flow characteristics of the gas in micro-tube.

References

[1]TAO Ran, QUAN Xiao-bo, XU Jian-zhong. Several questions in research of microscale flow [J]. Journal of Engineering Thermophysics,

2001, 22 ( 5 ): 575-577.

[2]Hsieh S S, Tsai H H, Lin C Y, Huang C F, Chien C M. Gas flow in a long micro channel [J]. International Journal of Heat and Mass Transfer,

2004, 47 ( 17/18 ): 3877-3887

[3]WANG Ying, DLAO Yan-hua, ZHAO Yao-hua. Experimental study of frictional characteristics on rectangular microtubes [J]. Journal of

Engineering Thermophysics, 2009, 30 ( 5 ): 841-843

[4]ZHANG Tian-tian, JIA Li, LI Cheng-wen. Experimental study on gas flow characteristics in microchannels[J]. Journal of Engineering

Thermophysics, 2009, 30 ( 5 ): 854-856

[5]Ergu O B, Sara O N, Yapici S, Arzutug M E. Pressure drop and point mass transfer in a rectangular microchannel[J]. International

Communications in Heat and Mass Transfer, 2009, 36 ( 6 ): 618-623

[6]TANG Gui-hua, TAO Wen-quan, HE Ya-ling, WANG Qiu-wang. Experimental study and ansysis of frictional characteristics on gas flow in microchannels[J]. Journal of Engineering Thermophysics, 2004, 25 ( 6 ): 1125-1127

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