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Pressure from each hole is p felt over a chord of width D sin N Pd5 F r5 p N W F r2 Pd2 Fr2 Pd1 Fr1 Pd5 Pa Pd3 Fr3 Pd1



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Let s look at one last type of resistor the light bulb. Yes, light bulbs are resistors. They get hot, so hot that they glow white. When you heat up your electric oven, it creates light too, but mostly in the red and infrared (below red, as heat) range. See if you can nd a 60-watt light bulb in your house. Clean the contacts on it and use your multimeter to nd the resistance across the bulb. In my bulb, I recorded a resistance of 19 . Using Ohm s Law (equation (5-2)), and the knowledge that American house voltage is about 110 V, we calculate that this bulb should draw about 5.7 amps. Using the de nition of power (equation (5-4)) we see that this translates into 627 watts. That s not right! In fact, that s ten times what it should be. This is because resistors do not have the same resistance under all conditions. Most metals, for example, increase their resistance as they heat up. A light bulb drawing almost 6 amps is going to heat up a lot, and fast. Doing the math backwards, we calculate that the hot resistance of the bulb should be closer to 200 .





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Fig 739: The load capacity of an aerostatic journal bearing the axial flow model [3]

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]

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The effect of dispersion is clear in short bearings and in bearings with fewer numbers of jets per row In short bearings, the lubricant does not have sufficient time to fill the whole bearing before being exhausted This drawback does not exist in circumferential slot feeding Initially, it is assumed that there is no non-axial flow However, in practice, the circumferential pressure distribution causes the gas to flow around the bearing [3] This reduces both the pressure difference across the shaft and the load capacity The analysis is usually done using a computer program However, Shires has deduced a semi-empirical correction factor for non-axial flow in which the constant was derived from a series of experimental results by Robinson [33] The correction factor also makes some allowance for dispersion effect

This was a long chapter, but we had a lot of material to cover. First, we looked at schematics. These are the diagrams that we use to describe electronic circuits, the language of electronics. A schematic is an abstract thing, an idea only. To make it real, we need to build the circuit using actual components. This construction can take place on circuit boards of di erent types, in the air, or in temporary breadboard arrangements. There are new skills involved in circuit building, namely soldering. Though there isn t much call for soldered circuits in this book, when you buy kits or move on to more advanced projects you will need to know how to solder things together. And even here, there will be times when you may want to solder new wires onto a component so it will t into your breadboard circuit. Our rst component was the resistor, a deceptively simple part. With it, however, we were able to build a Wheatstone Bridge that explores many of the features of electricity and resistance. We were given a chance to explore both Ohm s Law and the rules governing resistors in parallel circuits. With your new knowledge you are better prepared to look at schematics and know what they mean, as well as to build the circuits described within them.

cosh(636 l / D ) 1 L 2l sinh(636 l / D ) + tanh 636 D CL = 0315 L l C Lo D

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