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Rolling Element, Hydrodynamic and Hydrostatic Bearings Volumetric flow, Q capillary and orifice inflow restrictor For design conditions, the volumetric flow for both capillary and orifice restrictors are similar: Ps Q = Ro (1 + ) 225 Q = 553 (1 + 1 ) Q = 0203 in3 s 1 330 10 6 m3 s 1 Pumping power, Pp capillary and orifice inflow restrictor Pp = QPs Pp = 0203 225 517 W Pp = 458 in lbf s 1 For the 10 pads, the total pumping power is multiplied by the number of pads: nPp = 458 10 nPp = 458 in lbf s 1 nPp 007 hp 517 W Friction force, FL and Friction Power, Pf rectangular pad



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Summary

The friction force is mainly due to the shearing of the fluid film The force is proportional to the viscosity, relative sliding speed, land area and inversely proportional to the clearance: v 2 2 ( a + b ) c 4c2 + 08584r(int) FL = h FL =

FL = 795 lbf 354 N The friction power is obtained by multiplying the friction force with the sliding speed Pf = FLn Pf = 795 50 Pf = 398 in lbf s 1 449 W For the 10 pads, the total friction power is multiplied by the number of pads nPf = 398 10 nPp = 06 hp 449 W Criterion of the Operating Temperature The average temperature rise per pass of the oil through the system of bearing pads, neglecting heat losses is given by p1 + P f / Q t F 152





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In this chapter we continued to lay down a foundation of concepts for our later work. We started with passive control, a form of control where you don t have to do anything to manage it. From there we looked at some active control concepts, starting with openloop control where the controller doesn t have any con rmation, or feedback, as to what the system is doing. A more powerful form of control is closed-loop control, where feedback is used to adjust the system. Feedback doesn t imply fancy sensors, electronics, or computers. Very simple systems use feedback to good e ect, and these simple principles can be used in more complicated systems as well. Whenever you can make it work, simple mechanisms are better than complex ones less likely to break, easier to understand, and more likely to work throughout the life of the system.

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where P and Q are the summations of the contributions of the individual pads of a bearing system, p1 = [lbf in 2], Pf = [J s 1] and Q = [in3 s 1]:

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its improved e ciency led to its ultimate acceptance and led the way into the industrial revolution. In the nineteenth century improved manufacturing techniques brought simple automata to the masses, typically in the form of toys, fancy clocks, and other novelties. Clockwork mechanical toys were popular well into the twentieth century. Today the springs, gears, and cams in toys have been replaced by tiny motors and electronic controls. The skills and techniques developed by the automata makers during the Renaissance provided a foundation for the industrial revolution that followed. Today, you can still nd automata for sale. Automata are now in the domain of the artist and pieces from modern craftsmen and artists can be found for as little as a few dollars, up to hundreds or thousands of dollars. Another use for these magical machines is entertainment. Walt Disney introduced mechanical actors in the displays of his amusement park and christened them Audio-Animatronics. This cumbersome name is normally shortened to simply animatronics. Animatronics are machines driven by motors and hydraulics and synchronized with an audio track to give the full illusion of life. From the simplest Egyptian trick with water to the modern miracles of Disney s animatronics, these machine all share one characteristic. They can only reproduce a preset sequence of motions.

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