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Figure 29 depicts various symbols for voltage sources that will be employed throughout this book Note that the output voltage of an ideal source can be a function of time In general, the following notation will be employed in this book, unless otherwise noted A generic voltage source will be denoted by a lowercase v If it is necessary to emphasize that the source produces a time-varying voltage, then the notation v(t) will be employed Finally, a constant, or direct current, or DC, voltage source will be denoted by the uppercase character V Note that by convention the direction of positive current ow out of a voltage source is out of the positive terminal The notion of an ideal voltage source is best appreciated within the context of the source-load representation of electrical circuits, which will frequently be referred to in the remainder of this book Figure 210 depicts the connection of an energy source with a passive circuit (ie, a circuit that can absorb and dissipate energy for example, the headlights and light bulb of our earlier examples) Three different representations are shown to illustrate the conceptual, symbolic, and physical signi cance of this source-load idea

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quantity measured by the sensor (eg, temperature, ow rate) Other classi cations are also possible Table 151 presents a partial classi cation of sensors grouped according to the variable sensed; we do not claim that the table is complete, but we can safely state that most of the engineering measurements of interest to the reader are likely to fall in the categories listed in Table 151 Also included in the table are references to the Focus on Measurements boxes that describe sensors elsewhere in this book A sensor is usually accompanied by a set of speci cations that indicate its overall effectiveness in measuring the desired physical variable The following de nitions will help the reader understand sensor data sheets: Accuracy: Conformity of the measurement to the true value, usually in percent of full-scale reading Error: Difference between measurement and true value, usually in percent of full-scale reading Precision: Number of signi cant gures of the measurement Resolution: Smallest measurable increment Span: Linear operating range Range: The range of measurable values Linearity: Conformity to an ideal linear calibration curve, usually in percent of reading or of full-scale reading (whichever is greater) Motion and Dimensional Measurements The measurement of motion and dimension is perhaps the most commonly encountered engineering measurement Measurements of interest include absolute position, relative position (displacement), velocity, acceleration, and jerk (the derivative of acceleration) These can be either translational or rotational measurements; usually, the same principle can be applied to obtain both kinds of measurements These measurements are often based on changes in elementary properties, such as changes in the resistance of an element (eg, strain gauges, potentiometers), in an electric eld (eg, capacitive sensors), or in a magnetic eld (eg, inductive, variable-reluctance, or eddy current sensors) Other mechanisms may be based on special materials (eg, piezoelectric crystals), or on optical signals and imaging systems Table 151 lists several examples of dimensional and motion measurement that can be found in this book Force, Torque, and Pressure Measurements Another very common class of measurements is that of pressure and force, and the related measurement of torque Perhaps the single most common family of force and pressure transducers comprises those based on strain gauges (eg,.

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in the clearance value due to different eccentricities The value calculated will be more than in practice due to the effects of dispersion and non-axial flow that distort the pressure distribution as seen in Figure 736 The effect of dispersion is clear in short bearings and bearings with fewer numbers of jets per row As the flow diverges from around the feed jet, the theoretical load is reduced by a factor known as the load dispersion coefficient, Cw, given by [32]

This value (V or s2) is called the variance. Observe that the atter the distribution is, the greater the variance will be. The variance is one of the simplest measures we can calculate of variation about the mean. You might wonder why we simply don t calculate an average deviation from the mean rather than an average squared deviation. For example, we could calculate a measure of variation as (x n x) 1

Sensors Resistive potentiometers Strain gauges Differential transformers (LVDTs) Variable-reluctance sensors Capacitive sensors

The McGraw Hill Companies, 2001

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