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Machinery Reliability Audits arid Reviews   99

                  values comparable to the bearing stiffnesses. This information will show how  sensi-
                  tive the rotor  critical speeds and  responses  are to pedestal  stiffnesses. Generally,
                  pedestal stiffnesses may  vary from approximately  1 million to 20 million Ib/in. The
                  horizontal stiffnesses are usually less than the vertical stiffnesses; therefore, the hori-
                   zontal critical speeds will be lower than the vertical. Pedestal stiffnesses are impor-
                  tant in the analysis of  large rotors such as induced draft fans where the pedestal and
                  foundation stiffnesses will be lower than typical bearing stiffnesses.


                  Special Lateral Response Analyses
                    Liquid Pump Lcrteral Response Analyses. Pump rotordynamics are dependent on a
                  greater number of design variables than are many other types of rotating equipment.
                  Besides the journal  bearing and shaft characteristics, the dynamic characteristics of
                   the seals and the impeller-diffuser interaction can have significant effects on the crit-
                  ical speed location, rotor unbalance sensitivity, and rotor ~tability.~~’~
                    For modeling purposes, seals can be treated as bearings in the sense that direct and
                  cross-coupled stiffness and damping properties can be calculated based on the seal’s
                  hydrostatic and hydrodynamic properties. Seal clearances, geometry, pressure drop,
                  fluid properties, inlet swirl, surface roughness, and shaft speed are all important in
                  these calculations. Since the pressure drop across seals increases approximately with
                  the square of the pump speed, the seal stiffness also increases with the square of the
                  speed. This increasing stiffness effect is often thought of as a “negative” mass effect,
                  which is usually referred  to as the “Lomakin effect”  or the  “Lomakin  mass.””  In
                  some cases the theoretical Lomakin mass or stiffness effect can be of sufficient mag-
                  nitude to prevent the critical speed of  the rotor from ever being coincident with the
                  synchronous speed.
                    The accurate prediction of the stiffness and damping properties of seals for differ-
                  ent geometries  and operating  conditions  is a subject of  ongoing  re~earch.’~.’~ The
                  basic theories presented by Black14 have been modified to account for finite length
                  seals, inlet  swirl, surface roughness, and other important parameters. However,  a
                  universally accepted procedure to accurately predict seal properties is not  available
                  for all  the types  of  seals  in use today.  This  is  particularly  true for grooved  seals.
                  Unless  seal effects are correctly  modeled, calculated critical speeds can be signifi-
                  cantly different from actual critical speeds.
                    Grooved  seal designs  used in commercial pumps have been tested recently,  and
                  techniques have been developed whereby the seal geometry can be specified and the
                  characteristics calculated for specific assumptions with regard to inlet swirl, groove
                  design,  et^.'**'^
                    The rotordynamic analysis of  an eight-stage centrifugal pump using  serrated
                   (grooved) seals was discussed by Tisong and will be used to illustrate a design audit of
                   a pump.” The first step in  a rotordynamic analysis of  a pump is to model the basic
                  rotor, using the lumped parameter techniques. A sketch of the rotor with the location of
                  the seals and bearings is given in Figure 3-15. Note that the pump shaft is analyzed as
                   a rotor with 11 bearings (2 cylindrical bearings, 8 impellers, and the balance piston).
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