A dynamic thermal flow sensor for simultaneous measurement of thermal conductivity and flow velocity of gases

被引:27
作者
Cubukcu, Ali Sukru [1 ,3 ]
Romero, Diego F. Reyes [1 ]
Urban, Gerald A. [1 ,2 ]
机构
[1] Univ Freiburg, Dept Microsyst Engn IMTEK, Lab Sensors, D-79110 Freiburg, Germany
[2] Univ Freiburg, Freiburg Inst Adv Studies, D-79104 Freiburg, Germany
[3] Aselsan AS, Micro Nano Devices Design Dept, TR-06011 Ankara, Turkey
关键词
Thermal flow sensor; Flow simulation; Fluid thermal properties; Fluid-independent flow sensor; FLUID;
D O I
10.1016/j.sna.2013.12.007
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
080906 [电磁信息功能材料与结构]; 082806 [农业信息与电气工程];
摘要
Through finite element modeling and experiments, we describe individual influences of gas flow velocity (v) and thermal conductivity (lambda) on temperature amplitude and phase measurements from a dynamic MEMS thermal flow sensor that employs AC heating at 200 Hz. We further describe the relationships among the temperature phase, time-of-flight, and time-of-diffusion proposing a new boundary layer definition based on the existing flow and thermal boundary layer theories. The sensor has five primary thermistors made of amorphous germanium for high sensitivity. Four of these are symmetrically distributed around four central heater elements on a thermally isolating diaphragm where the fifth is in the center. Simulations and experimental results show that phase shifts (time lags) of temperature between thermistors primarily depend on lambda, and negligibly on v below a velocity limit. Simulation results also suggest that the influences of density (rho) and specific heat capacity (c(p)) on these phase shifts are relatively small or even negligible. Thus, lambda can be accurately determined independent of the flow velocity for gases of similar rho.c(p) product, up to 1 m/s under the set flow boundary conditions. Hence, simultaneous determination of thermal conductivity and flow velocity is expected to be feasible with this sensor under these circumstances, which, in turn, allows medium-independent flow sensing for a such selected set of gases. Experimental results show that the measurement resolution and maximum inaccuracy of lambda within the prescribed flow conditions are approximately equal to 2.445% and 3.18 + 4.20% (nonlinearity + velocity dependence) of the actual thermal conductivity, respectively. (C) 2014 Elsevier B.V. All rights reserved.
引用
收藏
页码:73 / 87
页数:15
相关论文
共 41 条
[1]
AirLiquide, OCT RC318 ONL GAS EN
[2]
Anemometer based on Seebeck effect [J].
Al Khalfioui, M ;
Michez, A ;
Giani, A ;
Boyer, A ;
Foucaran, A .
SENSORS AND ACTUATORS A-PHYSICAL, 2003, 107 (01) :36-41
[3]
[Anonymous], 1994, Handbook of Thermal Conductivity of Liquids and Gases
[4]
[Anonymous], 1996, Statistical mechanics
[5]
Beigelbeck R., 2008, 2008 IEEE Sensors, P518, DOI 10.1109/ICSENS.2008.4716491
[6]
Bonne U., 2008, COMPREHENSIVE MICROS, P375
[7]
THERMALLY EXCITED RESONATING MEMBRANE MASS-FLOW SENSOR [J].
BOUWSTRA, S ;
KEMNA, P ;
LEGTENBERG, R .
SENSORS AND ACTUATORS, 1989, 20 (03) :213-223
[8]
BRACE JG, 1989, IEEE 1989 ULTRASONICS SYMPOSIUM : PROCEEDINGS, VOLS 1 AND 2, P573, DOI 10.1109/ULTSYM.1989.67049
[9]
Cubukcu A., 2009, 10 INT C THERM MECH, P1
[10]
Cubukcu A., 2008, 9 INT C THERM MECH M, P1