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Table of Contents
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1. General Description....................................................1
3-1. SI-111 mounted onto a CM204 crossarm via the CM220....................2
3-2. SI-111 mounted onto a CM204 crossarm via the CM230....................2
Tables
5-1. Wiring for Example Programs .............................................................3
i
SI-111 Precision Infrared Radiometer
NOTE
Prior to November 2008, the SI-111 was named the IRR-P. Only
the name changed.
1. General Description
The SI-111 is an infrared temperature sensor that provides a non-contact means
of measuring the surface temperature of an object. It senses the infrared
radiation being emitted by the target. The SI-111 can be widely used for
measurements of leaf, canopy, and average surface temperature. With contact
sensors, it is difficult to avoid influencing the temperature, maintain thermal
contact, and provide a spatial average.
By mounting the infrared sensor at an appropriate distance from the target, it
can be used to measure an individual leaf, a canopy, or any surface of interest.
The SI-111 is an infrared temperature sensor that includes a thermopile for
measuring a millivolt output dependent on the target to sensor body
temperature difference. A thermistor measures the temperature of the sensor
body. The sensor body temperature is used to reference the target temperature.
2. Specifications
Input Power:
Absolute Accuracy:
Uniformity:
Repeatability:
Mass:
Dimensions:
Response Time:
Target Output Signal:
Body Temperature
Output Signal:
Optics:
Wavelength Range:
Field of View:
Operating
Environment:
2.5 V excitation for thermistor
*
±0.2°C @ –10° to 65°C
±0.5°C @ –40° to 70°C
±0.1°C @ –10° to 65°C
±0.3°C @ –40° to 70°C
±0.05°C @ –10° to 65°C
±0.1°C @ –40° to 70°C
190 grams
6.3 cm long by 2.3 cm diameter
Less than 1 second to changes in target
temperature
60 μV per °C difference from sensor body
0 to 2500 mV
Germanium lens
8 to 14 micrometers
22° half angle
Highly water resistant, designed for
continuous outdoor use; operating range is
–55° to 80°C, 0 to 100% RH
**
*
Where target temperature is within 20°C of sensor body temperature.
**
Where target temperature is greater than 20°C of sensor body temperature.
1
SI-111 Precision Infrared Radiometer
3. Installation
The field of view for infrared sensors is calculated based on the geometry of
the sensor and lens. However, optical and atmospheric scatter and unwanted
reflections from outside the field of view may influence the measurement.
Under typical conditions, 95 to 98 percent of the IR signal is from the field of
view and 2 to 5 percent is from the area surrounding the field of view. If the
target surface is small, for example a single leaf, try to mount the sensor close
enough that the surface extends beyond the field of view.
NOTE
Remove green cap from the SI-111 before mounting to a
crossarm, mast, or user-supplied support.
The SI-111 is often mounted to a CM202, CM204, or CM206 crossarm, a
tripod or tower mast, or a user-supplied pole via a CM220 right angle mount
(see FIGURE 3-1) or CM230 adjustable inclination mount. The CM230 allows
the sensor to be pointed at the surface of interest. When using the CM230, fix
the declination of the sensor by tightening the U-bolt that mounts on the mast
or crossarm. The inclination is then adjusted with the other U-bolt and nuts
(see FIGURE 3-2). A hole threaded for a standard tripod camera mount screw
(1/4 inch diameter; 20 threads per inch) can be used to mount the sensor to a
user-supplied support.
2
FIGURE 3-1. SI-111 mounted onto a CM204 crossarm via the CM220
FIGURE 3-2. SI-111 mounted onto a CM204 crossarm via the CM230
4. Wiring
g
SI-111 Precision Infrared Radiometer
5. Example Programs
The example datalogger programs measure the SI-111’s thermistor to obtain
the SI-111 sensor body temperature and measure the SI-111’s thermopile to
obtain the target-to-sensor body temperature difference.
After measuring the thermopile and thermistor outputs, the sensor body
temperature is used to reference the target temperature.
Wiring for the example programs is shown in TABLE 5-1. The actual channels
used need to be adjusted for the actual installation and application.
NOTE
Coefficients used to calculate the slope (m) and intercept (b) are
specific to individual SI-111 sensors. The unique coefficients for
each individual sensor are provided on the calibration sheet
shipped with the sensor.
Target Temperature:
Red Differential High
Black Differential Low
Clear Analog Ground
Sensor Body Temperature:
Green Single-Ended
Blue Analog Ground
WhiteVolta
e Excitation
TABLE 5-1. Wiring for Example Programs
Sensor/Lead Description CR10X CR1000
SI-111 Thermopile
Red Diff. High 2H 2H
Black Diff. Low 2L 2L
Clear Analog Ground AG
SI-111 Thermistor
Green SE 1 1
Blue Analog Ground AG
White Excitation E1
Target Temp
Sensor Temp
VX1 or
EX1
3
SI-111 Precision Infrared Radiometer
5.1 CR1000 Example Program
This example CR1000 program measures the sensor every 5 seconds and
outputs a sample once every 60 seconds. The actual measurement rate and
output intervals need to be adjusted for the actual installation and application.
Explanation of Variables and Constants Used in the Program
PanelT = datalogger panel temperature
BattV = datalogger battery voltage
SBTempC = sensor body temperature in degrees Celsius
SBTempK = sensor body temperature in Kelvin
TargmV = mV output of thermopile infrared detector (dependent on temperature difference between
target and sensor body)
m = slope of equation relating target and sensor body temperatures to mV output of thermopile
b = intercept of the equation relating target and sensor body temperatures to mV output of thermopile
TargTempK = target temperature in Kelvin
TargTempC = target temperature in degrees Celsius
mC2 = polynomial coefficient (C2) used to calculate slope (m)
mC1 = polynomial coefficient (C1) used to calculate slope (m)
mC0 = polynomial coefficient (C0) used to calculate slope (m)
bC2 = polynomial coefficient (C2) used to calculate intercept (b)
bC1 = polynomial coefficient (C1) used to calculate intercept (b)
bC0 = polynomial coefficient (C0) used to calculate intercept (b)
NOTE
All calibration coefficients are sensor-specific; those listed below
are examples and must be changed based on the sensor being
used.
'CR1000 Series Datalogger Program for Measuring Apogee Model SI-111 Infrared Radiometer
'Declare public variables
Public PanelT, BattV, SBTempC, SBTempK, TargmV, m, b, TargTempK, TargTempC
'Declare constants (replace the listed values with coefficients received with sensor)
Const mC2 = 82213
Const mC1 = 7841000
Const mC0 = 1419700000
Const bC2 = 13114
Const bC1 = 185020
Const bC0 = -17215000
'Define data table (table is outputting data every 60 seconds)
DataTable (IRR,1,-1)
DataInterval (0,60,Sec,10)
Minimum (1,BattV,FP2,0,False)
Sample (1,PanelT,FP2)
Average (1,TargmV,FP2,False)
Average (1,SBTempC,FP2,False)
Average (1,TargTempC,FP2,False)
EndTable
'Main program (program is making a measurement every 5 seconds)
BeginProg
Scan (5,Sec,0,0)
PanelTemp (PanelT,_60Hz)
Battery (BattV)
'Instruction to measure sensor body temperature (green wire to SE1, white wire to EX1, blue
wire ‘to ground)
Therm109 (SBTempC,1,1,Vx1,0,_60Hz,1.0,0)
4
SI-111 Precision Infrared Radiometer
'Instruction to measure mV output of thermopile detector (red wire to 2H, black wire to 2L,
clear ‘wire to ground)
VoltDiff (TargmV,1,mV2_5,2,True ,0,_60Hz,1.0,0)
'Calculation of m (slope) and b (intercept) coefficients for target temperature calculation
m = mC2 * SBTempC^2 + mC1 * SBTempC + mC0
b = bC2 * SBTempC^2 + bC1 * SBTempC + bC0
'Calculation of target temperature
SBTempK = SBTempC + 273.15
TargTempK = ((SBTempK^4) + m * TargmV + b)^0.25
TargTempC = TargTempK - 273.15
This example CR10X program measures the sensor once a second and outputs
the average values once an hour. The actual measurement rate and output
intervals need to be adjusted for the actual installation and application.
Explanation of Labels Used in the Program
mV_thrm = mV output of the thermistor
1_mV_thrm = first step in converting the mV output of the thermistor to resistance
2_mV_thrm = second step in converting the mV output of the thermistor to resistance
R_thrm = resistance of the thermistor
InR_thrm = natural log of the resistance of the thermistor
Scaled_R = intermediate step in converting the natural log of the resistance to temperature
SH_Coeff = application of the Steinhart and Hart coefficients to convert the scaled resistance to the
reciprocal of temperature
SB_Temp_K = sensor body temperature in Kelvin
SB_Temp_C = sensor body temperature in degrees Celsius
mV_tpile = mV output of the thermopile (dependent on the temperature difference between the
target and the sensor body)
m_slope = slope of the equation relating target and sensor body temperature to mV output of the
thermopile
b_inter = y-intercept of the equation relating target and sensor body temperature to mV output of the
thermopile
Exponent1 = exponent used to raise the sensor body temperature to the 4th power
Exponent2 = exponent used to calculate the 4th root of the sum of the terms used to calculate the
target temperature
1_SB_4Pow = first calculation step; sensor body temperature (Kelvin) raised to the fourth power
2_mVxm = second calculation step; mV output of the thermopile multiplied by m (slope)
3_Sum1 = third calculation step; sum of calculation steps one and two
4_Sum2 = fourth calculation step; the sum of calculation step 3 and b (intercept)
T_Temp_K = target temperature in Kelvin; calculated by adding the temperature difference between
the target and sensor body to the sensor body temperature
T_Temp_C = target temperature in degrees C
5
SI-111 Precision Infrared Radiometer
;{CR10X}
*Table 1 Program
01: 1 Execution Interval (seconds)
;Instruction string to measure the resistance of the thermistor and calculate the sensor body
;temperature. See the Instruction Manual for Campbell Scientific Model 109 Temperature Probe for
;details.
1: AC Half Bridge (P5)
1: 1 Reps
2: 25 2500 mV 60 Hz Rejection Range ;the range should at least match the excitation
3: 1 SE Channel
4: 1 Excite all reps w/Exchan 1
5: 2500 mV Excitation
6: 1 Loc [ mV_thrm ]
7: 1.0 Mult
8: 0.0 Offset
2: Z=1/X (P42)
1: 1 X Loc [ mV_thrm ]
2: 2 Z Loc [ 1_mV_thrm ]
3: Z=X+F (P34)
1: 2 X Loc [ 1_mV_thrm ]
2: -1.0 F
3: 3 Z Loc [ 2_mV_thrm ]
4: Z=X*F (P37)
1: 3 X Loc [ 2_mV_thrm ]
2: 24900 F
3: 4 Z Loc [ R_thrm ]
5: Z=LN(X) (P40)
1: 4 X Loc [ R_thrm ]
2: 5 Z Loc [ InR_thrm ]
6: Z=X*F (P37)
1: 5 X Loc [ InR_thrm ]
2: 0.001 F
3: 6 Z Loc [ Scaled_R ]
8: Z=1/X (P42)
1: 7 X Loc [ SH_Coeffs ]
2: 8 Z Loc [ SB_Temp_K ]
6
SI-111 Precision Infrared Radiometer
9: Z=X+F (P34)
1: 8 X Loc [ SB_Temp_K ]
2: -273.15 F
3: 9 Z Loc [ SB_Temp_C ]
;Instruction to measure the mV output of the thermopile.
10: Volt (Diff) (P2)
1: 1 Reps
2: 21 2.5 mV 60 Hz Rejection Range
3: 2 DIFF Channel
4: 11 Loc [ mV_tpile ]
5: 1.0 Mult
6: 0.0 Offset
;Calculation of m (slope) coefficient for target temperature calculation. Each sensor has unique
;C0, C1, and C2 values. Refer to the calibration sheet shipped with the sensor to obtain the correct
;values for your sensor.
12: Z=X*F (P37)
1: 12 X Loc [ m_slope ]
2: 99999 F
3: 12 Z Loc [ m_slope ]
;Calculation of b (intercept) coefficient for target calculation. Each sensor has unique C0, C1, and
;C2 values. Refer to the calibration sheet shipped with the sensor to obtain the correct values for
;your sensor.
14: Z=X*F (P37)
1: 13 X Loc [ b_inter ]
2: 99999 F
3: 13 Z Loc [ b_inter ]
7
SI-111 Precision Infrared Radiometer
;Target temperature calculation based on m and b coefficients.
15: Z=F x 10^n (P30)
1: 0.4 F
2: 1 n, Exponent of 10
3: 14 Z Loc [ Exponent1 ]
16: Z=F x 10^n (P30)
1: 0.025 F
2: 1 n, Exponent of 10
3: 15 Z Loc [ Exponent2 ]
17: Z=X^Y (P47)
1: 8 X Loc [ SB_Temp_K ]
2: 14 Y Loc [ Exponent1 ]
3: 16 Z Loc [ 1_SB_4Pow ]
18: Z=X*Y (P36)
1: 11 X Loc [ mV_tpile ]
2: 12 Y Loc [ m_slope ]
3: 17 Z Loc [ 2_mVxm ]
19: Z=X+Y (P33)
1: 16 X Loc [ 1_SB_4Pow ]
2: 17 Y Loc [ 2_mVxm ]
3: 18 Z Loc [ 3_Sum1 ]
20: Z=X+Y (P33)
1: 13 X Loc [ b_inter ]
2: 18 Y Loc [ 3_Sum1 ]
3: 19 Z Loc [ 4_Sum2 ]
21: Z=X^Y (P47)
1: 19 X Loc [ 4_Sum2 ]
2: 15 Y Loc [ Exponent2 ]
3: 20 Z Loc [ T_Temp_K ]
22: Z=X+F (P34)
1: 20 X Loc [ T_Temp_K ]
2: -273.15 F
3: 21 Z Loc [T_Temp_C ]
;Output average values once an hour
23: If time is (P92)
1: 0 Minutes (seconds -- ) into a
2: 60 Interval (same units as above)
3: 10 Set Output Flag High (Flag 0)
24: Real Time (P77)
1: 1220 Year, Day, Hour/Minute (midnight = 2400)
25: Average (P71)
1: 1 Reps
2: 21 Loc [ T_Temp_C ]
8
*Table 2 Program
02: 0.0 Execution Interval (seconds)
*Table 3 Subroutines
End Program
6. Maintenance
A primary source of inaccurate measurements for any radiation sensor is
blocking of the optical path to the detector. The window in the Apogee’s
infrared sensor is inset and protected, but it can become partially blocked in
three ways:
1. Spiders can make a nest in the entrance. We recommend using a cotton
2. Calcium deposits can accumulate on the window if irrigation water sprays
SI-111 Precision Infrared Radiometer
swab to apply a spider repellent around the entrance to the aperture (not on
the sensor window itself).
up on the head. These typically leave a thin white film on the surface and
can be removed with a dilute acid like vinegar. Calcium deposits cannot
be removed with solvents such as alcohol or acetone.
3. Dust and dirt can be deposited in the aperture in windy environments and
are best cleaned with deionized water, rubbing alcohol, or in extreme
cases, acetone.
Clean the inner threads and sensor window using a cotton swab dipped in the
appropriate solvent. It is important to use only gentle pressure on the window
to avoid scratching the thin optical coating on the window. Let the solvent do
the cleaning, not mechanical force. The cleaning should be repeated with a
second, fresh cotton swab to ensure a completely clean window. Sensors can
go for many months and stay clean in some environments, but frequent
cleaning is needed in other environments.