Page 267 - Machinery Component Maintenance
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Balancing of  Machinery  Components   249

                  their supporting structure. If the structure is rigid, the force is larger than
                  if the structure is flexible (except at resonance). In practice, supporting
                  structures are neither entirely rigid nor entirely flexible but somewhere
                  in between. The rotor-bearing support offers some restraint, forming a
                  spring-mass system with damping, and having a single resonance fre-
                  quency. When the rotor speed is below this frequency, the principal iner-
                  tia axis of the rotor moves outward radially. This condition is illustrated
                  in Figure 6-8A.
                    If  a  soft  pencil  is held  against the  rotor,  the  so-called high  spot  is
                  marked at the same angular position as that of the unbalance. When the
                  rotor speed is increased, there is a small time lag between the instant at
                  which the unbalance passes the pencil and the instant at which the rotor
                  moves out enough to contact it. This is due to the damping in the system.
                  The angle between these two points is called the "angle of lag." (See Fig-
                  ure 6-8B.) As the rotor speed is increased further, resonance of the rotor
                  and its supporting structure will occur; at this speed the angle of lag is
                  90". (See Figure 6-8C.) As the rotor passes through resonance, there are
                  large vibration amplitudes and the angle of lag changes rapidly. As the
                  speed is increased further, vibration subsides again; when increased to
                  nearly twice resonance speed, the angle of lag approaches 180 degrees.
                  (See Figure 6-8D  .) At speeds greater than approximately twice resonance
                  speed, the rotor tends to rotate about its principal inertia axis at constant
                  amplitude of  vibration; the angle of lag (for all practical purposes) re-
                  mains  180".
                    In Figure 6-8 a soft pencil is held against an unbalanced rotor. In (A) a
                  high spot is marked. Angle of  lag between unbalance and high spot in-
                  creases from 0" (A) to 180" in (D) as rotor speed increases. The axis of
                  rotation has moved from the shaft axis to the principal axis of inertia.
                    Figure 6-9 shows the interaction of rotational speed, angle of lag, and
                  vibration amplitude as a rotor is accelerated through the resonance fre-
                  quency of  its suspension system.

                  Correlatlng CG Displacement with Unbalance

                    One of the most important fundamental aspects of balancing is the di-
                  rect relationship between the displacement of center-of-gravity of a rotor
                  from its journal axis, and the resulting unbalance. This relationship is a
                  prime consideration in tooling design, tolerance selection, and determi-
                  nation of balancing procedures.
                    For a disc-shaped rotor, conversion of CG displacement to unbalance,
                  and vice versa, is relatively simple. For longer workpieces it can be al-
                  most as simple, if  certain approximations are made.  First,  consider a
                  disc-shaped rotor.
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