TheCS500 TEMPERATURE AND RELATIVE HUMIDITY PROBE is
warranted by CAMPBELL SCIENTIFIC, INC. to be free from defects in
materials and workmanship under normal use and service for twelve (12)
months from date of shipment unless specified otherwise. Batteries have no
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CS500 Table of Contents
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2. Calibration for Temperature.......................................................................6
3. Calibration for Relative Humidity...............................................................6
4. Wiring for CR1000 and CR10X Examples................................................. 7
5. CR10(X) Wiring for Example 1..................................................................9
i
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CS500 Temperature and Relative
Humidity Probe
1. General
The CS500 Temperature and Relative Humidity probe contains a Platinum
Resistance Temperature detector (PRT) and a Vaisala INTERCAP® capacitive
relative humidity sensor.
The -L option on the model CS500 Temperature and Relative Humidity probe
(CS500-L) indicates that the cable length is user specified. This manual refers
to the sensor as the CS500.
2. Specifications
Operating Temperature: -40°C to +60°C
Storage Temperature: -40°C to +80°C
Probe Length: 6.8 cm (2.66 in.)
Probe Body Diameter: 1.2 cm (0.47 in.)
Filter: 0.2 µm Teflon membran e
Filter Diameter: 1.2 cm (0.47 in.)
Housing Material: ABS Plastic
Power Consumption: < 2 mA
Supply Voltage: 7 to 28 VDC
Settling Time after power is switched on: 1 second
2.1 Temperature Sensor
Sensor: 1000 Ω PRT, DIN 43760B
Temperature Measurement Range: -40°C to +60°C
Temperature Output Signal range : 0 to 1.0 VDC
1
CS500 Temperature and Relative Humidity Probe
Temperature Accuracy:
1.6
1.2
0.8
0.4
o
( C)
0
-0.4
Error
-0.8
-1.2
-1.6
-20-400
2.2 Relative Humidity Sensor
Sensor: INTERCAP
Relative Humidity Measurement Range: 0 to 100% non-condensing
RH Output Signal Range: 0 to 1.0 VDC
Accuracy at 20°C
unspecified (0 to 10% Relative Humidity)
±3% RH (10 to 90% Relative Humidity)
±6% RH (90 to 100% Relative Humidity)
2040 60
Temperature( C)
®
o
3. Installation
Temperature Dependence of Relative Humidity Measurement:
1.5
1.0
o
0.5
C
0
-0.5
( %RH/ )
-1.0
-1.5
Temperature Dependence
10 20 30 40 50 60 70 80 90 100
60 C
-40 C
RH (%)
o
o
Typical Long Term Stability: Better than 1% RH per year
Response Time (at 20°C, 90% response to a steep change in humidity):
15 seconds with membrane filter
The CS500 must be housed inside a solar radiation shield when used in the
field. The 41303 6-Plate Radiation Shield (Figure 1) mounts to a CM6/CM10
tripod or UT10 tower. The CS500 is held within the 41301 by a mounting
clamp (Figure 2).
The 41003 10-Plate Radiation Shield (Figure 3) mounts to a CM6/CM10
tripod. The UT12VA 12-Plate Radiation Shield mounts to a UT10 or UT30
tower with the UT018 horizontal mounting arm.
2
NOTE
CS500 Temperature and Relative Humidity Probe
The CS500 is held in place, within the 41003 or UT12VA Radiation Shield, via
an adapter, Model 41381. The 41381 adapter is threaded onto the bottom of
the CS500 (Figure 4). The 41004 12-Plate Radiation Shield, used with 207
probes, can be converted to a 41002 with P/N 6638.
®
The black outer jacket of the cable is Santoprene
rubber. This
compound was chosen for its resistance to temperature extremes,
moisture, and UV degradation. However, this jacket will support
combustion in air. It is rated as slow burning when tested
according to U.L. 94 H.B. and will pass FMVSS302. Local fire
codes may preclude its use inside buildings.
FIGURE 1. CS500 and 41301 Radiation Shield
on a CM6/CM10 Tripod Mast
3
CS500 Temperature and Relative Humidity Probe
Mounting Clamp
FIGURE 2. CS500 and 41303 Radiation Shield
FIGURE 3. CS500 and 41003 Radiation Shield
on a CM6/CM10 Tripod Mast
4
CS500 Temperature and Relative Humidity Probe
Tripod Mast
41003 10-Plate Radiation Shield
Lock nut tightens against adapter
CS500
Internal threads secure the CS500 to adapter
41381 Adapter
FIGURE 4. Radiation Shield, CS500, and 41381 Adapter
Connections to Campbell Scientific dataloggers are given in Table 1. The
probe is measured by two single-ended analog input channels, one for
temperature and one for relative humidity.
CAUTION
Always connect the Green lead to the datalogger first,
followed by the Black, Brown, and Clear leads. Connect
the Red (Power) lead last.
5. Example Programs
This section is for users who write their own datalogger programs. A
datalogger program to measure this sensor can be created using Campbell
Scientific’s Short Cut Program Builder Software. You do not need to read this
section to use Short Cut.
The temperature and relative humidity signals from the CS500 are measured
using two single-ended analog measurements (Instruction 1).
The probe output scale is 0 to 1000 millivolts for the temperature range of 40°C to +60°C and for the relative humidity range of 0 to 100%. Tables 2 and
3 provide calibration information for temperature and relative humidity.
3:4SE Channel;Brown wire (SE 4), Green wire (G)
4:3Loc [ RH_pct ]
5:.1Mult;See Table 3 for alternate multipliers
6:0Offset
;Limit the maximum relative humidity to 100%.
;
03: If (X<=>F) (P89)
1:3X Loc [ RH_pct ]
2:3>=
3:100F
4:30Then Do
04: Z=F (P30)
1:100F
2:0Exponent of 10
3:3Z Loc [ RH_pct ]
CR7 (5000 mV)
05: End (P95)
6. Long Lead Lengths
Long lead lengths cause errors in the measured temperature and relative
humidity. The approximate error in temperature and relative humidity is
0.35°C and 0.35% per 100 feet of cable length, respectively.
When long lead lengths are required and the above errors in temperature and
relative humidity are unacceptable, use the HMP45C temperature and humidity
probe.
Understanding the following details are not required for the general operation
of the CS500 with Campbell Scientific’s dataloggers. The signal reference and
the power ground (black) are the same lead in the CS500. When the CS500
temperature and relative humidity are measured, both the signal reference and
power ground are connected to ground at the datalogger. The signal
reference/power ground lead serves as the return path for 12 V. There will be a
voltage drop along this lead because the wire itself has resistance. The CS500
draws approximately 2 mA when it is powered. The wire used in the CS500
(P/N 9720) has resistance of 17.5 Ω/1000 feet. Using Ohm’s law, the voltage
drop (V
), along the signal reference/ power ground lead, is given by Eq. (1).
d
V
IR
d =∗
=∗
mA ft
21751000
=
mV ft
351000
8
. Ω
(1)
This voltage drop will raise the apparent temperature and relative humidity
because the difference between the signal and signal reference, at the
datalogger, has increased by V
relative humidity is 0.35
respectively.
7. Absolute Humidity
The CS500 measures the relative humidity. Relative humidity is defined by the
equation below:
CS500 Temperature and Relative Humidity Probe
. The approximate error in temperature and
d
°C and 0.35% per 100 feet of cable length,
e
RH
100
=∗(2)
e
s
where RH is the relative humidity, e is the vapor pressure in kPa , and e
is the
s
saturation vapor pressure in kPa. The vapor pressure, e, is an absolute measure
of the amount of water vapor in the air and is related to the dew point
temperature. The saturation vapor pressure is the maximum amount of water
vapor that air can hold at a given air temperature. The relationship between
dew point and vapor pressure, and air temperature and saturation vapor
pressure are given by Goff and Gratch (1946), Lowe (1977), and Weiss (1977).
When the air temperature increases, so does the saturation vapor pressure.
Conversely, a decrease in air temperature causes a corresponding decrease in
saturation vapor pressure. It follows then from Eq. (2) that a change in air
temperature will change the relative humidity, without causing a change in
absolute humidity.
For example, for an air temperature of 20°C and a vapor pressure of 1.17 kPa,
the saturation vapor pressure is 2.34 kPa and the relative humidity is 50%. If
the air temperature is increased by 5°C and no moisture is added or removed
from the air, the saturation vapor pressure increases to 3.17 kPa and the relative
humidity decreases to 36.9%. After the increase in air temperature, the air can
hold more water vapor. However, the actual amount of water vapor in the air
has not changed. Thus, the amount of water vapor in the air, relative to
saturation, has decreased.
Because of the inverse relationship between relative humidity and air
temperature, finding the mean relative humidity is meaningless. A more useful
quantity is the mean vapor pressure. The mean vapor pressure can be
computed on-line by the datalogger (Example 1).
TABLE 5. CR10(X) Wiring f or Example 1
DescriptionColorCR10(X)
TemperatureBlackSE 3 (2H)
Relative HumidityBrownSE 4 (2L)
Signal & Power Refer enceGreenG
PowerRed12 V
ShieldClearG
9
CS500 Temperature and Relative Humidity Probe
Example 1. Sample CR10(X) Program that Computes Vapor Pressure
and Saturation Vapor Pressure
3:4SE Channel;Brown wire (SE 4), Green wire (G)
4:2Loc [ RH_frac ]
5:.001Mult;See Table 3 for alternate multipliers
6:0Offset
CR7 (5000 mV)
CR7 (5000 mV)
;Limit the maximum value of relative humidity
;to 1 (expressed as a fraction).
;
03: If (X<=>F) (P89)
1:2X Loc [ RH_frac ]
2:3>=
3:1F
4:30Then Do
04: Z=F (P30)
1:1F
2:0Exponent of 10
3:2Z Loc [ RH_frac ]
05: End (P95)
;Compute the saturation vapor pressure in kPa.
;The temperature must be in degrees Celsius.
;
06: Saturation Vapor Pressure (P56)
1:1Temperature Loc [ T_C ]
2:3Loc [ e_sat ]
10
;Compute the vapor pressure in kPa.
;Relative humidity must be a fraction.
;
07: Z=X*Y (P36)
1:3X Loc [ e_sat ]
2:2Y Loc [ RH_frac ]
3:4Z Loc [ e ]
8. Maintenance
CS500 Temperature and Relative Humidity Probe
The CS500 Probe requires minimal maintenance. Check monthly to make sure
the radiation shield is free from debris. The white screen at the tip of the probe
should also be checked for contaminants.
When installed in close proximity to the ocean or other bodies of salt water
(e.g., Great Salt Lake), a coating of salt (mostly NaCl) may build up on the
radiation shield, sensor, filter and even the chip. NaCl has an affinity for water.
The humidity over a saturated NaCl solution is 75%. A buildup of salt on the
filter or chip will delay or destroy the response to atmospheric humidity.
9. References
The filter can be rinsed gently in distilled water. If necessary, the chip can be
removed and rinsed as well. Do not scratch the chip while cleaning.
The offset and gain on the CS500 electronics can not be adjusted as part of a
recalibration. Replace the RH chip as needed.
Goff, J. A. and S. Gratch, 1946: Low-pressure properties of water from -160°
to 212°F, Trans. Amer. Soc. Heat. Vent. Eng., 51, 125-164.
Lowe, P. R., 1977: An approximating polynomial for the computation of
saturation vapor pressure, J. Appl. Meteor., 16, 100-103.
Weiss, A., 1977: Algorithms for the calculation of moist air properties on a
hand calculator, Amer. Soc. Ag. Eng., 20, 1133-1136.
11
CS500 Temperature and Relative Humidity Probe
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12
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