Electronics Resistive Sensors and Bridge Circuits

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Electronics Resistive Sensors and Bridge Circuits Wilfrid Laurier University September 27, 2012

Switches in voltage dividers One of the simplest forms of voltage divider is where one of the elements is a switch. A switch can be thought of as a resistor which can have a value of either zero or infinity. Following is an illustration of a voltage divider where one element is a switch.

V in R 1 I V out = V in ( ) R2 R 1 +R 2 R 2 I True if I out 0

V in R 1 R 1 = I = 0 V 2 = V out = 0 R 2 I

V in R 1 R 1 = I = 0 V 2 = V out = 0 R 2 I

V in R 1 R 1 = 0 V 1 = 0 V 2 = V out = V in R 2 I

V in R 1 R 1 = 0 V 1 = 0 V 2 = V out = V in R 2 I

So if one of the elements is a switch, the output varies between 0 and V in. If either resistor in a voltage divider is variable, then a range of output voltages is possible.

V in R 1 I V out = V in ( ) R2 R 1 +R 2 R 2 I True if I out 0

Resistive sensors Resistive sensors A resistive sensor is a resistor which changes according to some physical change in its environment. Some examples would be: Potentiometer; the resistance varies with physical movement Photoresistor; the resistance varies with light Thermistor; the resistance varies with heat Strain gauge (or gage); the resistance varies with stress or compression Force-dependent resistor; the resistance varies with applied pressure

Resistive sensors Here s an example of how a strain gauge works.

Resistive sensors Resistance R = ρ L A

Resistive sensors Resistance (Ω) (Low temperature; R max ) (High temperature; R min ) Temperature ( C) This is the resistance/temperature curve for a thermistor.

Resistive sensors If we want to put this variable resistor in a voltage divider, then we need to choose the other resistor. To make the output vary over as large a range as possible as the variable resistor goes from R min to R max, it turns out we want to choose the other resistor, R so that R = R min R max

Balancing a Wheatstone Bridge A common type of circuit is a Wheatstone bridge. It is really a pair of voltage dividers using a common voltage source. It s usually operated with the output voltage at or close to zero.

Balancing a Wheatstone Bridge R 1 R 3 V in V out R 2 R 4 This is a Wheatstone bridge.

Balancing a Wheatstone Bridge R 1 R 3 V in V out R 2 R 4 Here it s redrawn to show the two voltage dividers.

Balancing a Wheatstone Bridge R 1 R 3 V in V out R 2 R 4 Here s one voltage divider.

Balancing a Wheatstone Bridge R 1 R 3 V in V out R 2 R 4 Here s the other voltage divider.

Balancing a Wheatstone Bridge Often a Wheatstone bridge is used with one resistor variable, such as a resistive sensor. Knowing the other resistors allows the variable one to be easily determined. The circuit is very sensitive to small changes in the variable resistor.

Balancing a Wheatstone Bridge R 1 R v V in V A V out V B R 2 R 4 The variable resistor could be in any of the four positions; this is one example.

Balancing a Wheatstone Bridge Balancing a Wheatstone Bridge When the bridge is balanced, V o = 0 or V A = V B. (This will happen when R 1 R 2 = Rv R 4.) For our diagram R 1 R 2 is the reference branch, and R v R 4 is the evaluation branch. If R v increases, V B will decrease, and vice versa. For optimum performance, all resistors should be of the same order of magnitude. If using a resistive sensor, use a meter to measure resistance of sensor to get a correct order of magnitude.

Balancing a Wheatstone Bridge R R v = R + R V in V A V out V B R R If resistors are chosen to be equal, except for R v, then the output voltage will vary with changes in R v.

Balancing a Wheatstone Bridge Specifically, V A = V R 2R = V /2 R V B = V 2R+ R = V R+ R/2 R/2 2R+ R = V /2 V R/2 2R+ R V /2 V R/2 2R If no current flows between A and B then V A V B V R 4R which can be rearranged to give R (V A V B ) V 4R So we can determine R. (This approximation is true as long as R << R)