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Calibration and Temperature Correction of Heat Dissipation Matric Potential Sensors

A. L. Flint*,a, G. S. Campbellb, K. M. Elletta and C. Calissendorffc

a U.S. Geological Survey, Placer Hall, 6000 J Street, Sacramento, CA 95189
b Decagon, Inc., 950 NE Nelson Ct., Pullman, WA 99163
c 1111 Myrtle Dr., Burlington, WA 98233



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Fig. 1. Matric potential data as a function of dimensionless temperature rise for seven Campbell Scientific Inc. (CSI) 229-L sensors and several early heat dissipation sensors. The dashed line is a nonlinear fit to a van Genuchten-type model and the solid line is the same model scaled to -1000 MPa, both described in the text.

 


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Fig. 2. Ratio of temperature change for a dry ceramic matrix ({Delta}Td) to measurements of temperature change {Delta}T in equilibrium with different relative humidities (h). The line is a quadratic fit to the data and is described in the text.

 


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Fig. 3. Thermal conductivity data from heat dissipation sensor ceramic as a function of saturation of the ceramic. The line is computed from the thermal conductivity model described in the text.

 


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Fig. 4. Slope of T* versus Ti (s*) as a function of T*. Squares are measurements from the Washington State University (WSU) heat dissipation sensors and triangles are measurements from the USGS heat dissipation sensors. The line is the thermal conductivity model response described in the text.

 


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Fig. 5. Soil temperature and corresponding matric potential values for a heat dissipation sensor, uncorrected and corrected for temperatures. Also show are uncorrected matric potential values for when soil temperatures were between 19 and 21°C.

 


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Fig. 6. Matric potential data for heat dissipations sensors in a desert soil in the northern Mojave Desert, relative to the atmospheric water potential indicating near air-dry soil in the top 20 cm, indicating the need for the extended range in the calibration equation.

 





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