The transient response and frequency response of a constant-temperature platinum film gage are computationally modeled for application to heat flux measurement. The probe consists of a thin platinum film (sensor) deposited on a Pyrex substrate, and coated with aluminum oxide. The probe is exposed to a convective environment, and the power required to maintain the sensor at a constant temperature is a direct indication of the local, instantaneous heat transfer rate. In application, the probe is mounted in a heated, high thermal conductivity material, creating an isothermal heat transfer surface. A two-dimensional numerical model was developed to represent the sensor, the Pyrex substrate and the coating. Ideally, the probe would be operated with the platinum at identically the same temperature as the isothermal surface. In the present study, the effects of non-ideal operating conditions, resulting in differences between the sensor and surface temperature, are examined. Frequency response characteristics are presented in a nondimensional form. The results of this modeling effort clearly indicate the importance of precise control over the sensor temperature in employing the present method for heat flux measurement. With the sensor temperature equal to the isothermal surface temperature, the probe calibration is insensitive to the heat transfer rate over a wide range of heat transfer coefficients. However, a 0.5°C difference between the sensor and surface temperatures yields a change in the calibration of approximately 20 percent over a range of heat transfer coefficient of 500 W/m2K. At an input frequency of 10 Hz and an average heat transfer coefficient of 175 W/m2K, amplitude errors increase from 3 percent to 35 percent as the temperature difference changes from zero to 1°C. These results are useful guide to calibration, operation, and data reduction in active heat flux measurement.

1.
Beasley
D. E.
, and
Figliola
R. S.
,
1988
, “
A Generalised Analysis of a Local Heat Flux Probe
,”
Journal of Physics E: Scientific Instruments
, Vol.
21
, pp.
316
322
.
2.
Diller, T. E., 1993, “Advances in Heat Flux Measurements,” Advances in Heat Transfer, Vol. 23, Academic Press, San Diego, CA, pp. 279–369.
3.
Figliola
R. S.
,
Swaminathan
M.
, and
Beasley
D. E.
,
1993
, “
A Study of the Dynamic Response of a Local Heat Flux Probe
,”
Measurement Science and Technology
, Vol.
4
, pp.
1052
1057
.
4.
Figliola
R. S.
, and
Swaminathan
M.
,
1996
, “
Boundary Condition Influences on the Effective Area of a Local Heat Flux Probe
,”
Measurement Science and Technology
, Vol.
4
, pp.
1052
1057
.
5.
Liang
P. W.
, and
Cole
K. D.
,
1992
, “
Conjugated Heat Transfer from a Rectangular Hot-Film with the Unsteady Surface Element Method
,”
AIAA J. of Thermodynamics and Heat Transfer
, Vol.
6
, pp.
349
355
.
6.
Park
C. H.
, and
Cole
K. D.
,
1994
, “
Unsteady Heat Transfer from a Thick-Film Sensor
,”
AIAA J. of Thermodynamics and Heat Transfer
, Vol.
8
, pp.
797
799
.
7.
Park, C. H., and Cole, K. D., 1996, “One Point Calibration of a Glue-on Shear Stress Sensor,” Proceedings of at the 1996 IMECE, Atlanta, GA, paper 96-WA/HT-19.
This content is only available via PDF.
You do not currently have access to this content.