Page 219 - Tribology in Machine Design
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204  Tribology in machine design

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                                                                   2
                                 Equation (5.65) gives p = 1.22 x 10 N/m , which is a safe value for white
                                 metal. Assuming an inlet temperature of 40 °C, eqn (5.66) yields


                                As can be seen from the reference to Fig. 5.22, oil 2 meets this condition to a
                                close approximation and the solution is complete. In a practical case,
                                however, it may be necessary to use oil 3 at some other point in the system of
                                which the bearing is a part and, to avoid the necessity for two oils in one
                                machine, this oil may also be used in the bearing. Because the viscosity will
                                be greater, the bearing will operate at a lower eccentricity and a higher
                                temperature than when lubricated by oil 2. The exact values of eccentricity
                                and temperature will depend on the viscosity-temperature characteristics of
                                oil 3 and can be determined by the iterative process shown in Fig. 5.23.
                                  Assuming a trial value of eccentricity of 0.5, the corresponding value of
                                         2   2
                                 (p/Hco)(c/r) (D/L)  is 1.55 from which the viscosity can be estimated at
                                 0.075 Pa s. This value of [t produces a temperature rise of 53°C, so the
                                operating temperature is 40 + 53 = 93°C. From Fig. 5.22 this gives a
                                viscosity of 0.02 Pa s. The estimates of viscosity are not in agreement and
                                therefore the assumption of 0.5 for eccentricity ratio is insufficiently
                                accurate. A better approximation is obtained by taking the mean of the two
                                estimates of viscosity. Thus, a new value for n is 0.0475Pas and the
                                corresponding eccentricity is 0.6 which in turn determines the temperature
                                rise of 30 °C. The temperature rise of 30 °C, taken in conjunction with the
                                assumption of 40 °C for the inlet temperature, gives an effective operating
                                temperature of 70 °C. Reference to Fig. 5.22 gives the viscosity of oil 3 at this
                                temperature as about 0.048 Pa s which is in good agreement with the
                                assumed mean. It will be sufficient for most purposes, therefore, to accept
                                that the result of using oil 3 in the bearing will be to reduce the eccentricity
                                ratio to 0.6 and to increase the operating temperature to 70 °C.
                                   If agreement within acceptable limits had not been achieved at this stage,
                                further iteration would be carried out until the desired degree of accuracy is
                                attained. It is clear therefore that the method presented is very convenient
                                when a computer is used to speed-up the iteration process.

     5.6 Journal bearings       Hydrodynamically lubricated journal bearings are frequently used in
     for specialized            rotating machines like compressors, turbines, pumps, electric motors and
     applications               electric generators. Usually these machines are operated at high speeds and
                                therefore a plain journal bearing is not an appropriate type of bearing to
                                cope with problems such as oil whirl. There is, therefore, a need for other
                                types of bearing geometries. Some of them are created by cutting axial
                                grooves in the bearing in order to provide a different oil flow pattern across
                                the lubricated surface. Other types have various patterns of variable
                                clearance so as to create pad film thicknesses which have more strongly
                                converging and diverging regions. Various other geometries have evolved
                                as well, such as the tilting pad bearings which allow each pad to pivot about
                                some point and thus come to its own equilibrium position. This usually
                                results in a strong converging film region for each pad.
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