Bondable Resistance Temperature Sensors
and Associated Circuitry
Readout Methods
One method of reading temperature with
TG
temperature sensors
is to connect the sensor to a Wheatstone resistance
bridge, and convert the resistance readings to
equivalent temperatures with the tables given in this
publication. But, the leadwires can cause two
different errors in a Wheatstone bridge. First, the
resistance of the leads, which can be appreciable
with remote gages, produces an initial offset error,
and desensitizes the arm of the bridge containing the
temperature sensor. The second error is the result of
resistance change in the leads caused by temperature
variations. Except under unusual conditions, errors
of this type are very small. In cases where long
leadwires are necessary, special calibration
techniques or compensation systems can be used (Ref.
1
and
2
).
A variation of the above method is capable of
providing accurate compensation for leadwire
resistances with a three-wire system. The circuit is
shown below, in which a precision decade box is used
in place of one resistor in the Wheatstone bridge.
Three-wire null-balance circuit for TG sensor.
The decade box in this circuit is varied to keep the
output at null, and the indicated decade resistance
is therefore the same as the sensor resistance.
Provided leads 1 and 3 are of the same length and
size, resistance changes in the leadwire circuit
caused by temperature changes common to all wires
will not create errors in the reading. Three-wire
compensation is effective in this case because this
is a true null-balance system in which the bridge arm
adjacent to the sensor (the decade box) is always set
to the sensor resistance at the time of readout.
Excitation power can be either dc or ac, depending
on the null indicator chosen. Excessive excitation
can create errors due to self-heating in the sensor,
but this error is easily avoided or corrected as
discussed
later
.
A more sophisticated readout system, which
eliminates the need for manual rebalance, is shown
below. This arrangement eliminates leadwire errors by
use of a four-wire system.
Four-wire circuit for TG sensor.
If the digital voltmeter has a high enough input
impedance, the readings will be a known function of
sensor resistance, regardless of resistance change in
any of the leadwires. A current level of one mA will
allow the voltmeter to read sensor resistance in
terms of mV (50.0 ohms reads as 50.0 mV).
(continued...)
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