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If you test the voltage from the positive rail to the ground rail, you will get a value something like 9 V. It won t be exactly 9 V, since the voltage across batteries changes with time and their charge. If you get a negative voltage reading, make sure the black probe goes to the black, ground, wire. With the circuit hooked up you can test it from two di erent perspectives. Try putting the positive probe on the 9 V rail (A) and the ground probe at the junction (B). When R2 is in bright light the AB voltage is nearly 9 V. In the dark, AB is about 4.5 V. Looking at the circuit from the perspective of BC, with the positive probe at B, you get readings near zero for bright light and again about 4.5 V in the dark. The circuit was designed to work in the BC mode, as indicated by the output lines in Fig. 5-25. In this mode, equation (5-8) is in e ect. Plug in the di erent values for R1 and R2 (R1 at 10 k and R2 at 10 k and 100 k ) and see how the math works. When you reverse your measurement, like when you did the AB test, you also have to turn the equation upside down: R1 5-11 Vout Vin R1 R2 Now add the second voltage bridge as shown in Fig. 5-26. Since R3 equals R4, the voltage at their junction is half of the input voltage. Now test the



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This value is applicable for diatomic gases with a ratio of specific heats of 14 For other classification of gases, the critical ratio may be different The gauge pressure ratio at which the feed holes become choked can be obtained for air from the ensuing equation and from Figure 738 For atmospheric exhaust conditions, air bearings have choked feed holes at Kgo = 04 at a supply pressure in excess of 55 lbf/in2 gauge Thus, a higher supply pressure at a higher value of Kgo is often recommended Kgo =





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If the consideration of choked feed holes permits, for an optimum radial load capacity, a gauge pressure ratio of 04 should be used However, if small clearances are employed for limiting gas consumption and for achieving a high stiffness, the difficulty in producing small feed holes and avoiding hole blockage become the limiting factors In the analysis of flow through feed holes, it is assumed that there is no pressure loss upstream of the throat, and the pressure immediately downstream of the jet is the static pressure at the throat of the jet For a nozzle of the same throat diameter as that of the jet, the following equation expresses the relationship between the supply pressure and the static pressure at the throat

Fig. 5-26.

Fig 738: The journal bearing design choice of the gauge pressure ratio [3]

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voltage between these two dividers. It is unlikely that the result is zero in the dark. We need to add a trim potentiometer to help calibrate the circuit. Figure 5-24 shows this trim potentiometer in parallel with R3 and R4. You could simply replace R3 and R4 with the potentiometer; however, you get more sensitive calibration results if you build the circuit as shown. The top half of the trim pot is in parallel with R3 and the bottom half is in parallel with R4. Look back at equation (5-6) and see what this means for the total resistance of that voltage divider. One question that should have crossed your mind is, how do you choose the values for R1, R3, and R4 I m glad you asked. Trial and error plays a part. However, if you use your multimeter to test the photoresistor, you will nd that its resistance drops to about 10 k in full light. I used this minimum resistance as the rating for the other resistors. What kind of results would you get if R1 were 1 k 100 k Try these values out in equation (5-8) and see what happens. Try This: Take your resistors and design several di erent series and parallel circuits. Using Ohm s Law, calculate what the resistance across the circuit should be. Now build the circuit and measure it! How close are your results to the calculations Is it within the tolerance of the resistors

where Pd is the static pressure at the throat, v the velocity at the throat, ao the speed of sound at the supply pressure conditions and g is the ratio of specific heats for the gas The mass flow through the jet is given as m = CD rd A where CD is the coefficient of discharge, rd the density at the throat and A is the cross-section area of the throat It is always assumed in theory that in each slot around an eccentric journal bearing, the gas flows axially from the plane of the feed hole to the end of the bearing The pressure distribution in the bearing and corresponding load capacity shown in Figure 739 takes into consideration the changes

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