Page 223 - Tribology in Machine Design
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208   Tribology in machine design

                                  Another important consideration for tilting pad bearings is the radial
                                 location of the pad pivot point. It may be moved so that the pad centres-of-
                                curvature do not coincide at a point at the centre of the bearing. This is a
                                preload factor essentially the same as described for elliptical, three-, and
                                 four-lobe bearings. A preload factor of less than zero (the pad centre-of-
                                curvature between the pad and bearing centre) creates a pad which will tend
                                to dig the leading edge into the shaft. This is sometimes called pad lock-up.
                                 Lock-up can be prevented by placing a small bevel on the pad leading edge,
                                which produces a small converging wedge effect, but negative preloads
                                should be avoided.
                                  Tilting pad bearings are very widely used to stabilize machines which
                                have subsynchronous vibration. Because the pads are free to follow the
                                shaft, the forces produced in the bearing are not capable of driving the shaft
                                in an unstable mode. Their disadvantages include high cost, high horse-
                                power loss and installation problems. Tilting pad journal bearings have
                                been widely adapted, particularly in cases where they are not readily
                                accessible and maintenance of alignment is important.
                                  Referring to Fig. 5.29, it is assumed that when the journal is under load
                                the film thickness becomes slightly reduced on those pads towards
                                which the load is directed, and correspondingly increased on the opposite
                                side of the bearing, i.e. eccentricity e is in the line of action of the load. Sup-
                                pose that the centre of breadth of each pad is located by the angle 0
                                measured from the position of maximum film thickness. Denoting
                                        A = the mean film thickness for a pad at angle 0,
                                        c = the radial clearance when the journal is placed centrally
                                          without load, and using the notation as for a normal journal
                                          bearing,


                                If P is the normal load on the pad per unit length of journal at angle 0




                                and the upward vertical component of P is




                                where z is a dimensionless constant,







                                and


                                As in the Reynolds theory we may neglect the effect of tangential drag in
                                estimating the load carried, so that, if N is the number of pads and Q the
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