The3WHB10K 3-WIRE HALF BRIDGE TERMINAL INPUT MODULE
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
warranty. CAMPBELL SCIENTIFIC, INC.'s obligation under this warranty is
limited to repairing or replacing (at CAMPBELL SCIENTIFIC, INC.'s option)
defective products. The customer shall assume all costs of removing,
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INC. CAMPBELL SCIENTIFIC, INC. will return such products by surface
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3WHB10K Table of Contents
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3-1. 3-Wire Half Bridge Used to Measure PRT .............................................2
3-1. 3WHB10K Connections to Campbell Scientific Dataloggers.................2
4-1. Excitation Voltage for 100 Ohm PRT in 3WHB10K Based on
Maximum Temperature and Input Voltage Range...............................3
i
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3WHB10K 3-Wire Half Bridge Terminal
H
L
AG
H
L
AG
H
L
G
Input Module
1. Function
Terminal input modules connect directly to the datalogger's input terminals to
provide completion resistors for resistive bridge measurements, voltage
dividers, and precision current shunts.
FIGURE 1-1. Terminal Input Module
2. Specifications
10 kOhm Completion Resistor
Tolerance @ 25°C
Temperature coefficient
0°-60°C
-55°-125°C
Power rating @ 70°C 0.25 W
Vx
H
L
or AG
FIGURE 2-1. Schematic
±0.01%
±4 ppm/°C
±8 ppm/°C
10 kΩ
H
L
G
1
3WHB10K 3-Wire Half Bridge Terminal Input Module
3. Wiring
Datalogger
Vx
10 kΩ
H
L
or AG
or G
FIGURE 3-1. 3-Wire Half Bridge Used to Measure PRT
TABLE 3-1. 3WHB10K Connections to
Function
Excitation Black Wire E1 EX1 Excitation 1
V1 Reference H SE1 SE1 1H
V2 Sense L SE2 SE2 1L
Ground G AG
Label/Lead
Sh ie ld
Campbell Scientific Dataloggers
CR10X,
CR510
H
L
G
CR23X,
CR1000,
CR800, CR850,
CR3000
A
B
21X, CR7,
CR9000X
4. Programming Examples
The following examples simply show the two instructions necessary to 1)
make the measurement and 2) calculate the temperature. The result of the 3wire half bridge measurement as shown is R
PRT algorithm to calculate temperature.
All the examples are for a 100 Ohm PRT in the 3WHB10K. The excitation
voltages used were chosen with the assumption that the temperature would not
exceed 50°C. Table 4-1 lists excitation voltage as a function of maximum
temperature and the input voltage ranges used with the different dataloggers.
Calculation of optimum excitation voltage is discussed in Section 5.1.
The multiplier shown is for a 100 Ohm PRT. The multiplier for a 1000 Ohm
PRT is 10.
The advantages of the 3-wire half bridge over other measurements that correct
for lead wire resistance such as a 4-wire half bridge, are that it only requires 3
lead wires going to the sensor and takes 2 single-ended input channels,
whereas the 4-wire half bridge requires 4 wires and 2 differential channels.
5
3WHB10K 3-Wire Half Bridge Terminal Input Module
The result of the 3-wire half bridge instruction is equivalent to the ratio of the
PRT resistance, R
to the resistance of the 10 k fixed resistor, Rf.
s
The RTD Instruction (16) computes the temperature (°C) for a DIN 43760
standard PRT from the ratio of the PRT resistance at the temperature being
measured (R
) to its resistance at 0°C (R0). Thus, a multiplier of Rf/R0 is used
s
with the 3-wire half bridge instruction to obtain th e desired intermediate, R
= (R
R
x Rf/Ro). When Rf = 10,000 and R0 = 100, the multiplier is 100; when
s/Rf
is 1000 the multiplier is 10.
0
The fixed resistor must be thermally stable. Over the -55° to 85°C extended
temperature range for the datalogger, the ±4 ppm/°C temperature coefficient
would result in a maximum error of ±0.04°C at 60°C. The
±8 ppm/°C temperature coefficient would result in a maximum error of
±0.13°C at -55°C.
5.1 Excitation Voltage
R
s
R
f
s/R0
The best resolution is obtained when the excitation voltage is large enough to
cause the signal voltage to fill the measurement voltage range. The voltage
drop across the PRT is equal to the current, I, multiplied by the resistance of
the PRT, R
measure a temperature in the range of -10 to 40°C, the maximum voltage drop
will be at 40°C when R
voltage that can be used when the measurement range is ±25 mV, we assume
V2 equal to 25 mV and use Ohm's Law to solve for the resulting current, I.
V
is equal to I multiplied by the total resistance:
x
If the actual resistances were the nominal values, the 25 mV range would not
be exceeded with V
resistances and to leave a little room for higher temperatures, set V
2.1 volts.
5.2 Calibrating a PRT
The greatest source of error in a PRT is likely to be that the resistance at 0°C
deviates from the nominal value. Calibrating the PRT in an ice bath can
correct this offset and any offset in the fixed resistor in the Terminal Input
Module.
, and is greatest when Rs is greatest. For example, if it is desired to
s
=115.54 Ohms. To find the maximum excitation
s
I = 25 mV/R
= 25 mV/115.54 Ohms
s
= 0.216 mA
V
= I(Rs+Rf) = 2.18 V
x
= 2.18 V. To allow for the tolerances in the actual
x
equal to
x
6
With the PRT at 0°C, R
reciprocal of the multiplier required to calculate temperature, R
. Thus, the above result becomes R0/Rf, the
s=R0
f/R0
making a measurement with the PRT in an ice bath, errors in both R
can be accounted for.
. By
and R0.
s
3WHB10K 3-Wire Half Bridge Terminal Input Module
To perform the calibration, connect the PRT to the datalogger and program the
datalogger to measure the PRT with the 3-wire half bridge as shown in the
example section. For a 100 Ohm PRT use a multiplier of 100; for a 1000 Ohm
PRT use a multiplier of 10. Place the PRT in an ice bath (@ 0°C; R
Read the result of the bridge measurement. The reading is R
equal to R
since Rs=R0. The correct value of the multiplier, Rf/R0, is the
0/Rf
multiplier used divided by this reading. For example, if, with a 100 Ohm PRT,
the initial reading is 0.9890, the correct multiplier is: R
101.11.
5.3 Compensation for Wire Resistance
The 3-wire half bridge compensates for lead wire resistance by assuming that
the resistance of wire A is the same as the resistance of wire B (Figure 3-1).
The maximum difference expected in wire resistance is 2%, but is more likely
to be on the order of 1%. The resistance of R
actually R
For example, assume that a 100 Ohm PRT is separated from the datalogger by
500 feet of 22 awg wires. The average resistance of 22 AWG wire is 16.5 Ohms
per 1000 feet, which would give each 500 foot lead wire a nominal resistance of
8.3 Ohms. Two percent of 8.3 Ohms is 0.17 Ohms. Assuming that the greater
resistance is in wire B, the resistance measured for the PRT (R
the ice bath would be 100.17 Ohms, and the resistance at 40°C would be 115.71.
The measured ratio R
temperature computed by Instruction 16 from the measured ratio would be about
0.1°C lower than the actual temperature of the PRT. This source of error does
not exist in a 4-wire half bridge where a differential measurement is used to
directly measure the voltage across the PRT.
plus the difference in resistance of wires A and B.
s
is 1.1551; the actual ratio is 115.54/100 = 1.1554. The
s/R0
).
s=R0
, which is
s/Rf
= 100/0.9890 =
f/R0
calculated with Instruction 7, is
s
= 100 Ohms) in
0
7
3WHB10K 3-Wire Half Bridge Terminal Input Module
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8
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