Page 312 - Intro Predictive Maintenance
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Failure-Mode Analysis    303

            Because this is a friction-driven motion, the cage turns much slower than the inner
            race of the bearing. Generally, the rate of rotation is slightly less than one-half of the
            shaft speed. The FTF is calculated by the following equation:

                                            1  È   BD ˘
                                      FTF =   f r 1 -
                                            2  Î Í  PD˚ ˙

            Ball-Spin Frequency. Each of the balls or rollers within a bearing rotates around its
            own axis as it rolls around the bearing races. This spinning motion is referred to as
            ball spin, which generates a ball-spin frequency (BSF) in a vibration signature. The
            speed of rotation is determined by the geometry of the bearing (i.e., diameter of the
            ball or roller, and bearing races) and is calculated by:

                                    1  PD    È  Ê  BD ˆ 2    ˘
                                                           2
                               BSF =      ¥  f r 1 -   ¥ cos b ˙
                                             Í
                                    2  BD    Î  Ë  PD ¯      ˚
            Ball-Pass Outer-Race. The ball or rollers passing the outer race generate the ball-pass
            outer-race frequency (BPFO), which is calculated by:

                                         n    Ê  BD       ˆ
                                 BPFO =   ¥  f r 1 -  ¥ cosb
                                         2    Ë  PD       ¯
            Ball-Pass Inner-Race. The speed of the ball/roller rotating relative to the inner race
            generates the ball-pass inner-race rotational frequency (BPFI). The inner race rotates
            at the same speed as the shaft, and the complete set of balls/rollers passes at a slower
            speed. They generate a passing frequency that is determined by:

                                        n    Ê   BD       ˆ
                                  BPFI =  ¥  f r 1 +  ¥ cosb
                                        2    Ë   PD       ¯

            Defect Frequencies

            Rolling-element bearing defect frequencies are the same as their rotational frequen-
            cies, except for the BSF. If there is a defect on the inner race, the BPFI amplitude
            increases because the balls or rollers contact the defect as they rotate around the
            bearing. The BPFO is excited by defects in the outer race.

            When one or more of the balls or rollers have a defect such as a spall (i.e., a missing
            chip of material), the defect impacts both the inner and outer race each time one
            revolution of the rolling element is made. Therefore, the defect vibration frequency is
            visible at two times (2¥) the BSF rather than at its fundamental (1¥) frequency.

            14.2.2 Bearings: Sleeve (Babbitt)
            In normal operation, a sleeve bearing provides a uniform oil film around the supported
            shaft. Because the shaft is centered in the bearing, all forces generated by the
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