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Variables, x and y (x = the midparent average of the two parents in wing length in fruit ies in millimeters; y = the offspring measurement)

characteristic: R(x) = 100ex where x is a normalized displacement The nonlinear resistor is to be used to measure the displacement x in the circuit of Figure P249

VT (V )

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Thus equipped, if a cause-and-effect relationship does exist between the two variables, we can predict a y value given any x value. We can either use the formula y a bx or graph the regression line and directly determine the y value for any x value. We now continue our examination of the genetics of quantitative traits.

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Precision Engineering not restrict the bearing length Ultimately, the completed design of the whole spindle is shown in Figure 743 Here the work spindle consists of both aerostatic journal and thrust bearings From Table 710, it is seen that for externally pressurized gas bearings, a thrust face must be provided to carry the axial load This is even more critical when designing the grinding spindle, as the forces will be concentrated in the axial direction Most bearings have linear operating characteristics up to an eccentricity ratio of 05 as can be seen from Figure 75 Thus, this permits an accurate estimation of the radial stiffness for values below an eccentricity of 05 In addition, higher

a If the total length of the resistor is 10 cm, nd an expression for vout (x) b If vout = 4 V, what is the distance, x

+ V _ S + V _

y 2 2 2.2 2 2.2 2.2 1.9 2.2 2.5 92.7 x n (x n s2 x 2.51 x)2 1 0.44

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A differential measurement system is often a way to avoid ground loop problems, because the signal source and measurement system grounds are not connected to each other, and especially because the signal low input of the measuring instrument is not connected to either instrument case ground The connection of a grounded signal source and a differential measurement system is depicted in Figure 159

x 2.2 2.3 2.3 2.4 2.4 2.4 2.4 2.4 2.4

+ V _ S + V _

Fig 742: An aerostatic grinding spindle [29]

Differential Floating Ground-referenced measurement (nonreferenced) signal system source measurement system (a) (b)

x 2.9 2.9 2.9 3 3 3 3.1 3.2 3.2 3.2

Figure 1510 Measuring signals from a oating source: (a) differential input; (b) single-ended input

If the signal source connected to the differential measurement system is oating, as shown in Figure 1510, it is often a recommended procedure to reference the signal to the instrument ground by means of two identical resistors that can provide a return path to ground for any currents present at the instrument An example of such input currents would be the input bias currents inevitably present at the input of an operational or instrumentation ampli er The simple concepts illustrated in the preceding paragraphs and gures can assist the user and designer of instrumentation systems in making the best possible wiring connections for a given measurement Noise Sources and Coupling Mechanisms Noise meaning any undesirable signal interfering with a measurement is an unavoidable element of all measurements Figure 1511 depicts a block diagram of the three essential stages of a noisy measurement: a noise source, a noise coupling mechanism, and a sensor or associated signal-conditioning circuit Noise sources are always present, and are often impossible to eliminate completely; typical sources of noise in practical measurements are the electromagnetic elds caused by uorescent light xtures, video monitors, power supplies, switching circuits, and high-voltage (or current) circuits Many other sources exist, of course, but often the simple sources in our everyday environment are the most dif cult to defeat

y 2.7 2.7 3 2.8 2.8 2.9 3 2.4 2.8 2.9

Figure 1511 also indicates that various coupling mechanisms can exist between a noise source and an instrument Noise coupling can be conductive; that

2.52 y )2 1 0.32

Fig 743: A typical ultra-precision aerostatic spindle and drive system [2]

sy (x x ) (y n 1 y)

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