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Wheatstone Bridge

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The <strong>Wheatstone</strong> <strong>Bridge</strong><br />

The <strong>Wheatstone</strong> <strong>Bridge</strong> consists of a dc voltage source, four resistors and a detector. The<br />

detector is a type of ammeter called a galvanometer.<br />

The galvanometer is used to detect the condition i g = 0 . When the circuit satisfies the condition<br />

i = 0<br />

g<br />

we say that “the bridge is balanced”.<br />

Because the galvanometer is a type of ammeter, v g = 0 . (It’s always true that v g = 0 , whether<br />

the bridge is balanced or not. When the bridge is balanced it is also true that i = 0 .) Apply KVL<br />

to the top mesh of the bridge to get<br />

R i −v− Ri = 0 ⇒ Ri = Ri<br />

(1)<br />

2 2 g 1 1 1 1 2 2<br />

Apply KVL to the bottom mesh of the bridge to get<br />

vg + Rmim − R3i3 = 0 ⇒ R3i3 = Rmim When the bridge is balanced i = 0 . Apply KCL to node b of the balanced bridge to get<br />

g<br />

i = i + i = ⇒ i = i<br />

(3)<br />

1 g 3 0<br />

Apply KCL to node c of the balanced bridge to get<br />

1 3<br />

i + i = i ⇒ i = i<br />

(4)<br />

2 g m 2 m<br />

Using equations 3 and 4 to substitute for the currents in equation 2 gives<br />

g<br />

(2)<br />

R3i1= Rmi2 (5)<br />

1


Dividing equation 5 by equation 1 gives<br />

Now and solving for R m we get<br />

R3 m R<br />

= (6)<br />

R R<br />

1 2<br />

R2<br />

Rm = R3<br />

(6)<br />

R<br />

Typically, 1 R and 2 R are fixed resistors and 3 R is a variable resistor. R m is the resistance that<br />

is being measured. R 3 is adjusted until the detector indicates that the bridge is balanced. Then<br />

the value of R m is determined using equation 6.<br />

Example<br />

Consider using a <strong>Wheatstone</strong> bridge having R 1 = 200 Ω and R 2 = 2000 Ω to measure a<br />

resistance R m . The bridge is balanced by adjusting 3 R until R 3 = 250 Ω . What is the value of<br />

R m ?<br />

Solution<br />

From equation 6<br />

R2<br />

2000<br />

Rm= R3=<br />

250 = 2500 Ω<br />

R 200<br />

1<br />

Example<br />

Consider using a <strong>Wheatstone</strong> bridge having R 1 = 200 Ω and R 2 = 2000 Ω to measure a<br />

resistance, R m , of a temperature sensor. Suppose the resistance of the temperature sensor, R m ,<br />

in Ω, is related to the temperature T, in °C, by the equation<br />

R = 1500 + 25T<br />

m<br />

The bridge is balanced by adjusting 3 R until R 3 = 250 Ω . What is the value of the temperature?<br />

Solution<br />

From equation 6<br />

Next, the temperature in °C is given by<br />

R2<br />

2000<br />

Rm= R3=<br />

250 = 2500 Ω<br />

R 200<br />

1<br />

m 1500 R − 2500 −1500<br />

1000<br />

T = = = = 40 ° C<br />

25 25 25<br />

1<br />

2


Example<br />

Consider using a <strong>Wheatstone</strong> bridge having R 1 = 200 Ω and R 2 = 2000 Ω to measure a<br />

resistance, R m , of a temperature sensor. Suppose the resistance of the temperature sensor, R m ,<br />

in Ω, is related to the temperature T, in °C, by the equation<br />

R = 1500 + 25T<br />

m<br />

The temperature is expected to vary over the range 0 to 100 °C. Over what range must R 3 vary<br />

in order for the bridge to measure temperature over the range 0 to 100 °C?<br />

Solution:<br />

Solve equation 6 for R 3 :<br />

When T = 0 °C, Ω and 1500 R =<br />

m<br />

When T = 100 °C, ( )<br />

m<br />

2<br />

R1<br />

R3 = Rm<br />

(7)<br />

R<br />

R1<br />

200<br />

R3= Rm=<br />

1500 = 150 Ω<br />

R 2000<br />

R = 1500 + 25 100 = 4000 Ω and<br />

R1<br />

200<br />

R3= Rm=<br />

4000 = 400 Ω<br />

R 2000<br />

2<br />

R 3 could be implemented as a 150 Ω resistor in series with a 250 Ω potentiometer:<br />

2<br />

3

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