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The Wheatstone Bridge Figure 4.10 Using Kirchhoff’s Voltage Law: Using Kirchhoff’s Current Law:

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Presentation on theme: "The Wheatstone Bridge Figure 4.10 Using Kirchhoff’s Voltage Law: Using Kirchhoff’s Current Law:"— Presentation transcript:

1 The Wheatstone Bridge Figure 4.10 Using Kirchhoff’s Voltage Law: Using Kirchhoff’s Current Law:

2 What is the Wheatstone bridge equation if another resistor, R x, is added in parallel with R 1 ? RxRx

3 One advantage of using two resistors in parallel in one leg of the WB is that the added resistor can be located remotely from the actual WB, such as in a flow. Here, that resistor can serve as a sensor. RxRx

4 When E o = 0, the WB is said to be ‘balanced’ → When the WB is balanced and 3 of the 4 resistances are known, the 4 th (unknown) resistance can be found using the balanced WB equation. The is called the null method.

5 Now consider the case when all 4 resistors are the same initially and, then, one resistance, say R 1, is changed by an amount  R. This is called the deflection method. Often,  R is associated with a change in a physical variable.

6 In-Class Example Figure 4.18 RTD:  RTD = 0.0005 / ºC; R = 25  at 20.0 ºC Wheatstone Bridge: R 2 = R 3 = R 4 = 25  E i =  5 V Amplifier: Gain = G Multimeter: 0 V to 10 V range (DC) Experimental Operating Range: 20 ºC to 80 ºC

7 Cantilever Beam with Four Strain Gages When F is applied as shown (downward), R 1 and R 4 increase by  R (due to elongation), and R 2 and R 3 decrease by  R (due to compression). Here,  R is directly proportional to the strains. Figure 4.11 From solid mechanics, for a cantilever beam, both the elongational strain,  L, and the compressive strain,  C, are directly proportional to the applied force, F. Figure 6.2

8 The Cantilever Beam with Four Gages The WB equation This instrumented cantilever beam system is the basis for many force measurement systems (like force balances and load cells. becomes


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