Poiseuille number correlation for high speed micro-flows

被引:34
作者
Hong, Chungpyo [1 ]
Asako, Yutaka [2 ]
Lee, Jae-Heon [3 ]
机构
[1] Tokyo Univ Sci, Dept Mech Engn, Noda, Chiba 2788510, Japan
[2] Tokyo Metropolitan Univ, Dept Mech Engn, Hachioji, Tokyo 1920397, Japan
[3] Hanyang Univ, Dept Mech Engn, Seoul 133791, South Korea
关键词
D O I
10.1088/0022-3727/41/10/105111
中图分类号
O59 [应用物理学];
学科分类号
摘要
The Poiseuille number, the product of a friction factor and the Reynolds number (f center dot Re) for a quasi-fully developed high speed flow in a micro-channel of Re < 2300 and Mach number Ma < 0.7, was obtained numerically. The numerical methodology is based on the arbitrary-Lagrangian-Eulerian (ALE) method. Two-dimensional compressible momentum and energy equations with no-slip and slip boundary conditions were solved for constant wall temperatures that are lower or higher than the inlet temperature. The channel height ranges from 10 to 100 mu m and the channel aspect ratio is 200. The stagnation pressure, p(stg), is chosen such that the exit Mach number ranges from 0.1 to 0.7. The outlet pressure is fixed at atmospheric conditions. In the case of fast flow for both no-slip and slip boundary conditions, the value of f center dot Re is higher than 96 due to compressibility effects. However, in the case of slow flow for slip boundary conditions (Ma(out) < 0.3), the value of f center dot Re is slightly lower than 96 due to rarefaction effects, even the flow is accelerated. The f center dot Re correlation for slip boundary conditions is obtained from that for no-slip boundary conditions and incompressible theory as a function of the Mach number and the Knudsen number. The f center dot Re correlation obtained for no-slip boundary conditions is also compared with that obtained for slip boundary conditions. The values of f center dot Re obtained for no-slip and slip boundary conditions almost coincide within 3% for the channel height in the range 10-100 mu m.
引用
收藏
页数:10
相关论文
共 18 条
[1]   Rarefaction, compressibility, and viscous heating in gas microfilters [J].
Ahmed, I ;
Beskok, A .
JOURNAL OF THERMOPHYSICS AND HEAT TRANSFER, 2002, 16 (02) :161-170
[2]  
Ameel TA, 1997, MICROSCALE THERM ENG, V1, P303
[3]  
[Anonymous], LA8095 LOS AL SCI LA
[4]   Effect of compressibility on gaseous flows in micro-channels [J].
Asako, Y ;
Pi, TQ ;
Turner, SE ;
Faghri, M .
INTERNATIONAL JOURNAL OF HEAT AND MASS TRANSFER, 2003, 46 (16) :3041-3050
[5]   Rarefaction and compressibility effects in gas microflows [J].
Beskok, A ;
Karniadakis, GE ;
Trimmer, W .
JOURNAL OF FLUIDS ENGINEERING-TRANSACTIONS OF THE ASME, 1996, 118 (03) :448-456
[6]   Numerical method for predicting three-dimensional steady compressible flow in long microchannels [J].
Chen, CS .
JOURNAL OF MICROMECHANICS AND MICROENGINEERING, 2004, 14 (07) :1091-1100
[7]  
Churchill SW, 1988, VISCOUS FLOWS PRACTI
[8]   Size effect on microscale single-phase flow and heat transfer [J].
Guo, ZY ;
Li, ZX .
INTERNATIONAL JOURNAL OF HEAT AND MASS TRANSFER, 2003, 46 (01) :149-159
[9]   Numerical modeling of three-dimensional compressible gas flow in microchannnels [J].
Jain, V ;
Lin, CX .
JOURNAL OF MICROMECHANICS AND MICROENGINEERING, 2006, 16 (02) :292-302
[10]   Numerical simulation of wall roughness on gaseous flow and heat transfer in a microchannel [J].
Ji, Y ;
Yuan, K ;
Chung, JN .
INTERNATIONAL JOURNAL OF HEAT AND MASS TRANSFER, 2006, 49 (7-8) :1329-1339