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Similarly, this can be repeated for other gauge pressure ratios Therefore, the following can be obtained: at l/L = 1/4, Kg = 08; Airflow = 045 scfm (00127 m3/min) The mass flow is independent of the number of jets and is inversely proportional to the lengthto-diameter ratio and the feed hole station The correction factor for different length-to-diameter ratios and location of the rows of jets are given in Figure 752 For the one-eighth station feeding, a correction can be made based on Figure 752 (b) The value of 2 is read from the vertical axis of the intersection of l/L (0125) and the curve The correction value is multiplied by the airflow at l/L (025) at l/L = 1/8, Kg = 06; Airflow = 0840 scfm (00238 m3/min) at l/L = 1/8, Kg = 08; Airflow = 1326 scfm (00375 m3/min) The choices of the one-eighth station feedings are not possible at the available flow rate Thus, the final choice will be two rows of eight feed holes at the quarter station From Figure 745, the intersection of the feed hole diameter with the diametrical clearance will give the gauge pressure ratio, which may be interpolated The best diameter is the one that gives a lower gauge pressure ratio A feed hole diameter of 50 10 3 in is to be preferred since it provides the lowest gauge pressure ratio and Fig 752: Variation of the mass flow with the bearing geometry [3] airflow However, feed holes of a larger diameter up to 60 10 3 in can be used without jeopardizing the performance of the aerostatic bearing The final design is summarized in Table 73 and illustrated in Figure 753 The performance is scaled down taking into consideration a safety factor Slot Feeding Slot-fed bearings can help in overcoming the effect of dispersion and non-axial flow that are dominant in reducing the load capacity and stiffness for the jet-fed bearings Circumferential feed slots can.

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Comments: In Figure 1552 the Schmitt trigger output is compared to that of a comparator without noise protection Note that a common comparator would be triggered twice in the presence of noise Focus on Computer-Aided Tools: The Electronics Workbench solution of this example may be found in the accompanying CD-ROM

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The Op-Amp Astable Multivibrator This section describes an op-amp circuit useful in the generation of timing, or clock, waveforms In the previous discussion, it was shown how it is possible to utilize positive feedback in a Schmitt trigger circuit A small fraction of the large output saturation voltage was used to delay the switching of a comparator to make it less sensitive to random uctuations in the input signal A very similar circuit can be employed to generate a square-wave signal of xed period and amplitude This circuit is called an astable multivibrator, because it periodically switches between two states without ever reaching a stable state The circuit is shown in Figure 1553 in a somewhat simpli ed form The analysis of the circuit is similar to that of the Schmitt trigger, except for the presence of both negative and positive feedback connections We start by postulating that the op-amp output is saturated at the positive supply saturation voltage One can easily verify that, in this case, the noninverting terminal voltage is R2 vout (1539) v+ = R2 + R 3

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cessive trait. A true-breeding ebony female (ee) is mated with a true-breeding wild-type male that has been irradiated. Among the wild-type progeny is a single ebony male. Explain this observation. Answer: The cross is ee e e , and all F1s should be e e (wild-type). The use of irradiation alerts us to the possibility of chromosomal breaks, as well as simple mutations. What type of chromosomal aberration would allow a recessive trait to appear unexpectedly A deletion, which creates pseudodominance when there is no second allele, is a good possibility. The male in question could have gotten the ebony allele from its mother and no homologous allele from its father. Alternatively, the wild-type allele from the father could have mutated to an ebony allele.

and that the voltage at the inverting input is equal to the voltage across the capacitor, vC One can write an expression for the inverting terminal voltage, v , by noting that the capacitor charges at a rate determined by the feedback resistance and by the capacitance, according to the time constant: = R1 C (1540)

Final design dimensions: Diameter Length Diametrical Clearance Feeding Feed Hole Diameter Radial Load Capacity Radial Stiffness Airflow 2 in (508 mm) 3 in (762 mm) 0001 in (00254 mm) Two rows of eight simple orifices at the quarter station 50 10 3 in (0127) mm 107 lbf (at e = 05), 14552 N 428 000 lbf / in (0 < e < 05), 74900 N/mm 035 scfm (00099 m3/min)

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Since the current owing into the inverting terminal is negligible, the inverting input voltage is in effect given by v (t) = vC (t) = Vsat (1 e t/ ) (1541)

A sketch of the inverting input voltage as a function of time is shown in Figure 1554 The behavior of this op-amp multivibrator is best understood if the differential voltage, = v + v , is considered Assuming that the capacitor starts charging at t = 0 from zero initial charge and that vout is saturated at +Vsat , one can easily show that this condition will be sustained for as long as remains positive However, as the capacitor continues to charge, v will eventually grow larger than v + , and will become negative Since v+ = R2 Vsat R2 + R 3 (1542)

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