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Of course, it turned out that the machine could not play chess at all Instead, it provided cramped quarters for a human chess player who in turn ran the machinery that made the Turk move One very complex automaton wasn t an android, but a duck Jacques Vaucanson created this avian automaton in 1738 and then went on tour with it At the price of a week s wages, audiences were invited to see this creation move around, adjust its wings, preen, drink water, and even eat food, digest it, and then defecate All of this required thousands of moving parts within both the duck and its large base And yet, automata were just a hobby of Vaucanson s He sold his collection in 1743 and went on to direct the stateowned silk-mills in France.



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Hydrodynamic thrust bearings are also used in reverse osmosis applications wherein the grease or oil is replaced with a process lubricant A tilting-pad design is chosen because it has a sufficient load capacity, compactness and efficiency FMC Technologies, Houston, uses the bearing shown in Figure 634 for such applications up to 5,000 hours without any sign of wear Several bearing manufacturers are currently testing various new materials, which can lead to hydrodynamic bearings having a better performance Waukesha, for instance, has found

solid polymer pads [15]





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Among other innovations, he developed a way to weave silk brocade using a machine guided by perforated cards Owing to hostility among the weavers of the time, his advances in factory automation were ignored for decades In 1804, Joseph-Marie Jacquard improved and reintroduced the technique and was later credited with its invention While the automatic loom was still despised by weavers, who went as far as burning down automated factories,.

that polymer bearings provide an alternative in both oil-lubricated applications and those lubricated by a process fluid A polymer based on polyether-ether-ketone (PEEK), which combines excellent surface properties with a high working temperature, has been introduced Basically, this new range of polymer materials is capable of higher operating temperatures up to 250 C (480 F), high load capability, corrosion resistance and a high electrical resistivity (better than 109 m) [15]

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The analysis of hydrodynamic journal and thrust bearings is usually tedious and is fully dependent on the shape of the pad for thrust bearings The analysis involves the extensive use of the principles of fluid mechanics and derivation of Reynolds equation For journal bearings, several approximations may be applied such as the full Sommerfeld solution, half Sommerfeld solution and Reynolds Boundary condition For the purpose of introduction, these mathematical analyses are not included Reference can be made to the work of Hamrock titled Fundamentals of Fluid Film Lubrication [1] For certain applications, the operating temperature and the type of lubricant are crucial in determining the viscosity of the lubricant under consideration Figure 635 shows the viscositytemperature curves for typical SAE (Society of Automotive Engineers) numbered oils A simplified approach to obtain the friction of a hydrodynamic sliding journal bearing has been analysed by Petroff in whose equation the shaft is assumed to be concentric [13] This is only possible when the radial load action on the bearing is negligible, the viscosity of the lubricant is infinite and the speed of the journal is infinite This however is seldom possible Petroff s equation gives a good approximation even when the criteria are not fully satisfied By referring to a vertical shaft shown in Figure 636, it is assumed that there is no eccentricity between the bearing and the journal, and hence no wedging action and no lubricant flow in the axial direction [5] The absolute viscosity is given by =

Fig. 5-8.

Rearranging the previous equation, the friction force in a concentric journal bearing is then given as AU F= where F is the friction torque/shaft radius = Tf /RI, A, the pDL = 2pRL, U, the (pDn = 2pRn (n is in revolutions/sec, rps) and H is the c (c = radial clearance = (bearing diameter shaft diameter) 2) Substituting and solving for the friction torque gives Tf 2 RL2 Rn = R C 2 4 nLR 3 Tf = C

Fig 635: Viscosity versus temperature curves for a typical SAE graded oil [4]

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