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A properly wired, grounded, and shielded sensor connection is a necessary rst stage of any well-designed measurement system The next stage consists of any signal conditioning that may be required to manipulate the sensor output into a form appropriate for the intended use Very often, the sensor output is meant to be fed into a digital computer, as illustrated in Figure 151 In this case, it is important to condition the signal so that it is compatible with the process of data acquisition Two of the most important signal-conditioning functions are ampli cation and ltering Both are discussed in the present section Instrumentation Ampli ers An instrumentation ampli er (IA) is a differential ampli er with very high input impedance, low bias current, and programmable gain that nds widespread application when low-level signals with large common-mode components are to be ampli ed in noisy environments This situation occurs frequently when a lowlevel transducer signal needs to be preampli ed, prior to further signal conditioning (eg, ltering) Instrumentation ampli ers were brie y introduced in 12 (see Example 124), as an extension of the differential ampli er You may recall that the IA introduced in Example 124 consisted of two stages, the rst composed of two noninverting ampli ers, the second of a differential ampli er Although the design in 12 is useful and is sometimes employed in practice, it suffers from a few drawbacks, most notably the requirement for very precisely matched resistors and source impedances to obtain the maximum possible cancellation of the common-mode signal If the resistors are not matched exactly, the commonmode rejection ratio of the ampli er is signi cantly reduced, as the following will demonstrate The ampli er of Figure 1516 has properly matched resistors (R2 = R2 , RF = RF ), except for resistors R and R , which differ by an amount R such that.

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Weight of Parent Beans 15 65 75 55 65 45 55 35 45 25 35 15 25 Totals 5 8 5 6 2 1 4 11 13 1 30 Weight of Progeny Beans (centigrams) 20 25 30 2 9 20 36 37 3 107 35 3 14 37 139 58 12 263 40 16 51 101 278 133 29 45 37 79 204 498 189 61 50 71 103 287 584 195 38 55 104 127 234 372 115 25 977 60 105 102 120 213 71 11 622 306 135 52 24 9 2 65 75 66 76 69 20 70 45 34 34 20 2 75 19 12 17 4 80 12 6 3 3 85 3 5 1 90 2 n Mean SE 0.43 0.41 0.27 0.18 0.30 0.52 0.13

v'b R iS R2 v _

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494 58.47 609 54.37 1,138 51.45 2,238 48.62 835 46.83 180 46.53 5,491 50.39

where (Po Pa) is expressed in lbf/in For example, the information in Figure 744 is valid for e = 05 and a supply pressure gauge of 100 lbf/in2 A diameter of 2 in is given with a load capacity of 100 lbf From the figure, a length of 3 in which will give a load value (145 lbf, on interpolation of curve 100 lbf and 150 lbf) that is higher than the load capacity at the intersection of the length and accordingly the diameter is chosen For a supply pressure gauge of less than 100 lbf/in2, a correction factor is required (as indicated before) Therefore, for the available supply pressure gauge that is 75 lbf/in2, the corrected load capacity is

R = R + R Let us compute the closed-loop gain for the ampli er As shown in Example 124, the input-stage noninverting ampli ers have a closed-loop gain given by A= vb v 2R2 = a =1+ vb va R1 (154)

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To compute the output voltage, we observe that the voltage at the noninverting terminal is v+ = RF RF + R + R va (155)

(156)

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