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in which a ground reference is established for example, by connecting the signal low lead to a case or housing A oating signal source is one in which neither signal lead is connected to ground; since ground potential is arbitrary, the signal source voltage levels (signal low and signal high) are at an unknown potential relative to the case ground Thus, the signal is said to be oating Whether a sensor can be characterized as a grounded or a oating signal source ultimately depends on the connection of the sensor to its case, but the choice of connection may depend on the nature of the source For example, the thermocouple described in Section 151 is intrinsically a oating signal source, since the signal of interest is a difference between two voltages The same thermocouple could become a grounded signal source if one of its two leads were directly connected to ground, but this is usually not a desirable arrangement for this particular sensor In analogy with a signal source, a measurement system can be either groundreferenced or differential In a ground-referenced system, the signal low connection is tied to the instrument case ground; in a differential system, neither of the two signal connections is tied to ground Thus, a differential measurement system is well suited to measuring the difference between two signal levels (such as the output of an ungrounded thermocouple) One of the potential dangers in dealing with grounded signal sources is the introduction of ground loops A ground loop is an undesired current path caused by the connection of two reference voltages to each other This is illustrated in Figure 158, where a grounded signal source is shown connected to a groundreferenced measurement system Notice that we have purposely denoted the signal source ground and the measurement system ground by two distinct symbols, to emphasize that these are not necessarily at the same potential as also indicated by the voltage difference V Now, one might be tempted to tie the two grounds to each other, but this would only result in a current owing from one ground to the other, through the small (but nonzero) resistance of the wire connecting the two The net effect of this ground loop would be that the voltage measured by the instrument would include the unknown ground voltage difference V , as shown in Figure 158 Since this latter voltage is unpredictable, you can see that ground loops can cause substantial errors in measuring systems In addition, ground loops are the primary cause of conducted noise, as explained later in this section.

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The design of an aerostatic bearing involves matching the various load and stiffness requirements with bearing clearance, orifice design, air supply pressure and flow rate Table 72 provides some guidelines for the design of aerostatic journal bearings Relative values are given for each parameter It is found that two air bearings with feeding at the quarter station give the best performance in terms of load capacity, stiffness and angular stiffness However, the air flow rate is comparatively much higher Figure 741 shows the operation of work and grinding spindles in the Moore ultra-precision machine [29] Most of the air bearings in the work spindle from various manufacturers are almost similar in terms of performance and dimension The same can be said about the grinding spindle which is shown in Figure 742 It is found that there are different approaches to design the aerostatic journal bearing in either the work or the grinding spindle However, Powell s approach seems to be accurate and comprehensive Therefore, the design of an aerostatic journal bearing similar to those used in ultra-precision machines will be explained based on an example adapted from Design of Aerostatic Bearings by JW Powell [3] Example: Design of an Aerostatic Journal Bearing An air-lubricated journal bearing must be designed to carry a load of 100 lbf (445 N) at an eccentricity ratio of 05 Its radial stiffness should exceed 400,000 lbf/in (70,000 N/mm) A workshop airline is available at a 75 lbf/in2 (51675 kPa) gauge The airflow should not exceed 050 scfm (00142 m3/min)

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an additional production line The total electrical load in the building is 23 kW The nameplates on the various loads give the minimum and maximum voltages below with the related full-load current: VS = 450 V VL min = 446 V IL FL = 515 A VL max = 463 V IL FL = 496 A

It is often desirable in genetic studies to know whether a relationship exists between two given characteristics in a series of individuals. For example, is there a relationship between height of a plant and its weight, or between scholastic aptitude and grades, or between a phenotypic measure in parents and their offspring If one increases, does the other also An example appears in table 18.3; the same data set is graphed in gure 18.11, in what is referred to as a scatter plot. A relation does appear between

The building is sited a distance d from the transformer bank which can be modeled as an ideal source (see Figure P241) If d = 85 m, determine the AWG of the smallest conductors which can be used in a rubber-insulated cable used to supply the load

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The building is sited a distance d from the transformer bank which can be modeled as an ideal source (Figure P243) The cable must have AWG 4 or larger conductors to carry a current of 5157 A without overheating Determine the maximum length d of a rubber-insulated cable with AWG 4 conductors which can be used to connect the source to the load

where sx and sy are the standard deviations of x and y, respectively. To calculate the correlation coef cient, we need to de ne and calculate the covariance of the two variables, cov(x, y). The covariance is analogous to the variance, but it involves the simultaneous deviations from the means of both the x and y variables: cov(x, y) (x x)( y n 1 y)

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Slocum s performance comparison of load, flow rate stiffness and tilt stiffness for typical journal bearing geometries and arrangements modified with station locations [1]

(18.5)