Outputs from measurement sensors that take the form of voltage signals can be measured using the voltage indicating and test instruments discussed in the last chapter. However, in many cases, the sensor output does not take the form of an electrical voltage. Examples of these other forms of sensor output include translational displacements and changes in various electrical parameters such as resistance, inductance, capacitance and current. In some cases, the output may alternatively take the form of variations in the phase or frequency of an a.c. signal.
For sensor outputs that are initially
in some non-voltage form, conversion to a measurement signal that is in a more
convenient form can be achieved by various types of variable conversion element
in the measurement system. Bridge circuits are a particularly important type of
variable conversion element, and these will be covered in some detail.
Following this, the various alternative techniques for transducing the outputs
of a measurement sensor will be covered.
7.1 Bridge circuits
Bridge circuits are used very
commonly as a variable conversion element in measurement systems and produce an
output in the form of a voltage level that changes as the measured physical
quantity changes. They provide an accurate method of measuring resistance,
inductance and capacitance values, and enable the detection of very small
changes in these quantities about a nominal value. They are of immense
importance in measurement system technology because so many transducers measuring
physical quantities have an output that is expressed as a change in resistance,
inductance or capacitance. The displacement-measuring strain gauge, which has a
varying resistance output, is but one example of this class of transducers.
Normally, excitation of the bridge is by a d.c. voltage for resistance
measurement and by an a.c. voltage for inductance or capacitance measurement.
Both null and deflection types of bridge exist, and, in a like manner to
instruments in general, null types are mainly employed for calibration purposes
and deflection types are used within closed-loop automatic control schemes.
7.1.1 Null-type, d.c. bridge
(Wheatstone bridge)
A null-type bridge with d.c.
excitation, commonly known as a Wheatstone bridge, has the form shown in Figure
7.1. The four arms of the bridge consist of the unknown resistance Ru,
two equal value resistors R2 and R3 and a variable
resistor Rv (usually a decade resistance box). A d.c. voltage Vi
is applied across the points AC and the resistance Rv is varied
until the voltage measured across points BD is zero. This null point is usually
measured with a high sensitivity galvanometer.
To analyse the Whetstone bridge,
define the current flowing in each arm to be I1 ...I4 as
shown in Figure 7.1. Normally, if a high impedance voltage-measuring instrument
is used, the current Im drawn by the measuring instrument will be
very small and can be approximated to zero. If this assumption is made, then,
for Im = 0:
I1 = I3
and I2 = I4
Looking at path ADC, we have a
voltage Vi applied across a resistance Ru + R3
and by Ohm’s law:
I1 = Vi/(Ru + R3)
Similarly for path ABC:
I2 = Vi/(Rv + R2)
Now we can calculate the voltage drop
across AD and AB:
VAD = I1Rv
= ViRu/(Ru + R3) ; VAB = I2Rv =
ViRv/(Rv + R2)
By the principle of superposition,
V0 = VBD
= VBA + VAD = - VAB + VAD
Thus:
V0
= - ViRv/(Rv + R2) + ViRu/(Ru
+ R3) (7.1)
At the null point V0 = 0,
so:
Ru/(Ru
+ R3) = Rv/(Rv + R2)
Inverting both sides:
(Ru + R3)/Ru
= (Rv + R2)/Rv i.e.
R3/Ru = R2/Rv or Ru = R3Rv/R2 (7.2)
Thus, if R2 = R3,
then Ru = Rv. As Rv is an accurately known
value because it is derived from a variable decade resistance box, this means
that Ru is also accurately known.
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