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By referring to Figure 764, it can be seen that for a design clearance of 05 10 3 in the jet diameter is 10 10 3 in when b/a is 3 A correction is required since the figure is plotted based on 50 lbf/in2 The multiplication factor is obtained from the vertical axis at the intersection of a supply pressure of 75 lbf/in2 with the curve of Figure 765 (a) The corrected diameter is given as 12 (10 10 3) = 0012 in The influence of pressure, temperature and gas properties on the optimum jet diameter and mass flow is similar to that of the journal bearings, and the related figures can be applied for the design of thrust bearings In this case, multiple jets will be arranged, feeding into a circular groove of radius given by c2 = 10 075 = 075 c = 0866 in The number of feed holes will be determined in the limit by the smallest size that can be drilled Figure 765 (b) shows the variation in feed hole diameter with the number of feed holes The practical choice of most designers would lie between eight and 16 and possibly the best compromise between considerations of aerostatic instability and manufacturing difficulty would be to use 12 feed holes of a 72 10 3 in diameter The final drawing is as shown in Figure 766 Figure 767 and Figure 768 clearly show the use of aerostatic bearings in the work spindle and the grinding spindle, respectively Both the spindles employ aerostatic journal bearings and aerostatic thrust bearings to obtain the various advantages of ultra-precision applications

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The dots shown in the two gures indicate the polarity of the coupling between the coils If the dots are at the same end of the coils, the voltage induced in coil 2 by a current in coil 1 has the same polarity as the voltage induced by the same current

Genetic drift in small populations: q 0.5. After time passes, the populations of gure 20.5 begin to diverge in their allelic frequencies. Time is measured in population size (N), showing that the effects of random genetic drift are qualitatively similar in populations of all sizes; the only difference is the timescale. (From M. Kimura, Solution of a process of random

genetic drift with a continuous model, Proceedings of the National Academy of Sciences, USA, 41:144-50, 1955. Reprinted by permission.)

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in coil 1; otherwise, the voltages are in opposition, as shown in the lower part of Figure 166 Thus, the presence of such dots indicates that magnetic coupling is present between two coils It should also be pointed out that if a current (and therefore a magnetic eld) were present in the second coil, an additional voltage would be induced across coil 1 The voltage induced across a coil is, in general, equal to the sum of the voltages induced by self-inductance and mutual inductance

Linear Variable Differential Transformer (LVDT)

Any population that has the a allele lost or xed will be permanently removed from the process of random genetic drift. Without mutation to bring one or the other allele

Hybrid gas bearings combine the principle of aerodynamic and aerostatic bearings They also combine higher load capacities due to the external pressure of an aerostatic bearing with additional aerodynamic

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The linear variable differential transformer (LVDT) is a displacement transducer based on the mutual inductance concept just discussed Figure 167 shows a simpli ed representation of an LVDT, which consists of a primary coil, subject to AC excitation (vex ), and of a pair of identical secondary coils, which are connected so as to result in the output voltage vout = v1 v2 The ferromagnetic core between the primary and secondary coils can be displaced in proportion to some external motion, x, and determines the magnetic coupling between primary and secondary coils Intuitively, as the core is displaced upward, greater coupling will occur between the primary coil and the top secondary coil, thus inducing a greater voltage in the top secondary coil Hence, vout > 0 for positive displacements The converse is true for negative displacements More formally, if the primary coil has resistance Rp and self-inductance Lp , we can write di = vex dt and the voltages induced in the secondary coils are given by iRp + Lp v 1 = M1 v 2 = M2 so that vout = (M1 M2 ) di dt

where M1 and M2 are the mutual inductances between the primary and the respective secondary coils It should be apparent that each of the mutual inductances is dependent on the position of the iron core For example, with the core at the null position, M1 = M2 and vout = 0 The LVDT is typically designed so that M1 M2 is linearly related to the displacement of the core, x Because the excitation is by necessity an AC signal (why ), the output voltage is actually given by the difference of two sinusoidal voltages at the same frequency, and is therefore itself a sinusoid, whose amplitude and phase depend on the displacement, x Thus, vout is an amplitude-modulated (AM) signal, similar to the one discussed in Focus on Measurements: Capacitive Displacement Transducer in 4 To recover a signal proportional to the actual displacement, it is therefore necessary to use a demodulator circuit, such as the one discussed in Focus on Measurements: Peak Detector for Capacitive Displacement Transducer in 8

The McGraw Hill Companies, 2001

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