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A heat pulse technique for measuring water flow in soil
Tyson Ochsner
USDA-ARSSoil and Water Management Research Unit
St. Paul, MN
Application of the heat pulse technique
Upstream sensor
Heater
Downstream sensor
1 cm
The heat transfer occurs by conduction and convection.
Heat transfer equations
2
2
2
2
x
TV
y
T
x
T
t
T
C
CJV ww
where Jw is the water flux.
• The governing heat transfer equation is
• The solution of this governing equation leads to a simple relationship between water flux and the temperature increase ratio.
u
d
ww T
T
CxJ ln
0
We tested the technique in the lab using packed columns of sand, sandy loam, and silt loam soil.
Laboratory experiments
Time (s)
0 20 40 60 80 100
Td
/ Tu
0.0
0.5
1.0
1.5
2.0
2.5
3.0
0.2 0.40.91.72.65.39.617.727.037.2
Heat pulse signals converted to Td/Tu
The temperature increase ratio increases with flow rate.
Sand
Flux (cm h-1)
u
d
ww T
T
CxJ ln
0
Flux measured at outlet (cm h-1)
0 10 20 30 40
Est
ima
ted
flu
x b
ase
d on
ln T
d / T
u (c
m h
-1)
0
10
20
30
40SandSandy loamSilt loam
Resulting water flux estimates
Strong linear relationship between flux measured by the sensor and that measured at the column outlet.
Soil typeSlope
(S)Intercept
Std. Err.
r2
cm hr-1 cm hr-1
Sand 0.765 0.605 0.390 0.998
Sandy loam 0.232 0.452 0.125 0.998
Silt loam 0.400 2.88 0.071 0.999
Linear regression results
Regression results indicate good precision and linearity, but the slopes are less than one.
u
d
ww T
T
Cxb
aJ ln
0
Sb
a 1
abVx
T
T
u
d 0expx
TbV
y
T
x
Ta
t
T
2
2
2
2
Linking theory and measurements
Choosing a = 1/S and b = 1 leads to an “enhanced conduction” model.
Choosing a = 1 and b = S leads to a “reduced convection” model.
Original theory Enhanced conduction Reduced convection
Silt loam
16.1 cm h-1
Time (s)
0 20 40 60
Tem
pera
ture
Inc
reas
e (K
)
0.0
0.4
0.8
1.2
Time (s)
0 20 40 60
Sandy loam
36.5 cm h-1
Tem
pera
ture
Inc
reas
e (K
)
0.0
0.4
0.8
1.2
Time (s)
0 20 40 60 80
Sand
37.2 cm h-1
Tem
pera
ture
Inc
reas
e (K
)
0.0
0.4
0.8
1.2
Td
Tu
Modeled Td
Modeled Tu
Results
• The smallest flux detected with the heat pulse technique was 0.12 cm hr-1.
• The relationship between heat pulse flux estimates and the outflow flux was linear up to 40 cm hr-1.
• The standard heat transfer model over-predicted the sensitivity of the heat pulse sensor to water flux.
• A reduced convection model accounted for the discrepancies between the measured data and the standard model.
Closing statements
• “Uncorrected” heat pulse measurements are fairly accurate in sand.
• Theoretical over-predictions of instrument response to convective heat transfer are common.
• A reliable procedure for correcting heat pulse measurements is needed.
• The heat pulse approach for measuring soil water flux warrants further development.
Acknowledgements
• Collaborators are Robert Horton, Gerard J. Kluitenberg, and Quanjiu Wang.
• This work was conducted at Iowa State University.