Chapter 2
Using the Module
2-2
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The Wheatstone bridge is the electrical equivalent of two parallel voltage divider circuits. R
1
and R
2
compose one voltage divider circuit, and R
4
and R
3
compose the second voltage
divider circuit. The output of a Wheatstone bridge is measured between the middle nodes of
the two voltage dividers. A physical phenomena, such as a change in strain or temperature
applied to a specimen, changes the resistance of the sensing elements in the Wheatstone
bridge, resulting in a bridge output voltage that is proportional to the physical phenomena.
The output voltage of the bridge scales with the excitation voltage. However, the ratio of the
bridge output (
V
CH
) and the excitation voltage (
V
EX
) remains fixed over variations in
excitation voltage, and it is this unitless ratio (
V
CH
/
V
EX
) that is of interest. To accurately
measure the ratiometric output of a bridge based sensor both the bridge output voltage (
V
CH
)
and the excitation voltage must be known. Determination of the excitation voltage can be
accomplished by either using an accurate voltage source or by measuring it. The
NI PXIe-4330/4331 uses circuitry that continuously measures the excitation voltage and
applies it as a reference to its analog-to-digital converter (ADC). In this way, variations in the
excitation voltage are compensated for, and the module returns data as a ratio of the bridge
output voltage and the excitation voltage.
Connection Options to Correct for Resistance Errors
The basic Wheatstone bridge in Figure 2-1 shows the excitation voltage impressed directly
across the bridge. However, field wiring used to connect sensors to measurement devices have
a non-zero resistance, and this resistance can create errors in bridge circuit measurements.
The NI PXIe-4330/4331 provides two mechanisms to correct for these errors: remote sensing
and shunt calibration.
Remote Sensing
Remote sensing continuously and automatically corrects for errors in excitation leads, and
generally is most appropriate for half- and full-bridge sensors. Moreover, its use is most
critical in applications that employ long wires and/or small gauge wires, as these have
greater resistance. The resistance in the wires that connect the excitation voltage to the bridge
causes a voltage drop, which is a source of gain error. The NI PXIe-4330/4331 includes
remote sensing to compensate for this gain error. Connect remote sense inputs of the
NI PXIe-4330/4331 to the excitation voltage wires of the sensor as close to the bridge circuit
as possible. Refer to the full-bridge diagram in Figure 2-2 for an illustration of how to connect
remote sense wires.