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handbook of modern sensors

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190 5 Interface Electronic Circuits<br />

5.6 Ratiometric Circuits<br />

A powerful method for improving the accuracy <strong>of</strong> a sensor is a ratiometric technique,<br />

which is one <strong>of</strong> the most popular methods <strong>of</strong> signal conditioning. It should be emphasized,<br />

however, that the method is useful only if a source <strong>of</strong> error has a multiplicative<br />

nature but not additive; that is, the technique would be useless for reducing, for instance,<br />

thermal noise. On the other hand, it is quite potent for solving such problems<br />

as the dependence <strong>of</strong> a sensor’s sensitivity to such factors as power-supply instability,<br />

ambient temperature, humidity, pressure, effects <strong>of</strong> aging, and so forth. The technique<br />

essentially requires the use <strong>of</strong> two <strong>sensors</strong>, <strong>of</strong> which one is the acting sensor, which<br />

responds to an external stimulus, and the other is a compensating sensor, which is<br />

either shielded from that stimulus or is insensitive to it. Both <strong>sensors</strong> must be exposed<br />

to all other external effects which may multiplicatively change their performance.<br />

The second sensor, which is <strong>of</strong>ten called reference, must be subjected to a reference<br />

stimulus, which is ultimately stable during the lifetime <strong>of</strong> the product. In many practical<br />

systems, the reference sensor must not necessarily be exactly similar to the acting<br />

sensor; however, its physical properties, which are subject to instabilities, should be<br />

the same. For example, Fig. 5.34A shows a simple temperature detector, where the<br />

acting sensor is a negative temperature coefficient (NTC) thermistor R T . A stable<br />

reference resistor R 0 has a value equal to the resistance <strong>of</strong> the thermistor at some<br />

reference temperature, (e.g., at 25 ◦ C). Both are connected via an analog multiplexer<br />

to an amplifier with a feedback resistor R. The output signals produced by the sensor<br />

and the reference resistor respectively are<br />

V N =− ER<br />

R T<br />

, (5.39)<br />

V D =− ER<br />

R 0<br />

.<br />

It is seen that both voltages are functions <strong>of</strong> a power-supply voltage E and the circuit<br />

gain, which is defined by resistor R. That resistor as well as the power supply may be<br />

the sources <strong>of</strong> error. If two output voltages are fed into a divider circuit, the resulting<br />

signal may be expressed as V 0 = kV N /V D = kR 0 /R T , where k is the divider’s gain.<br />

The output signal is not subject to either power-supply voltage or the amplifier gain.<br />

It depends only on the sensor and its reference resistor. This is true only if spurious<br />

variables (like the power supply or amplifier’s gain) do not change rapidly; that is,<br />

they must not change appreciably within the multiplexing period. This requirement<br />

determines the rate <strong>of</strong> multiplexing.<br />

A ratiometric technique essentially requires the use <strong>of</strong> a division. It can be performed<br />

by two standard methods: digital and analog. In a digital form, output signals<br />

from both the acting and the reference <strong>sensors</strong> are multiplexed and converted into<br />

binary codes in an A/D converter. Subsequently, a computer or a microprocessor<br />

performs the operation <strong>of</strong> a division. In an analog form, a divider may be a part <strong>of</strong> a<br />

signal conditioner or the interface circuit.A“divider” (Fig. 5.35A) produces an output

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