High rotational velocity and/or large mass in rotary motion can cause damaging impact at the end of stroke. Deceleration and absorption of rotating system energy can be achieve with cushions, external shock absorbers or fluid circuit devices which reduce speed as the actuator approaches the end of travel.
Cushions are the simplest design alternative, but consideration must be given to the cushion energy absorption capacity. Exceeding rated cushion capacity can reduce actuator life or result in severe actuator damage. To determine if a cushion is suitable for the application, calculate the total energy that must be absorbed and compare with the cushion capacity rating.
Ek = Energy of mass in motion (kinetic energy)
Ek = 1/2 J w2
Ep = Propelling energy of actuator
Ep = PpCtqd
Eg = Gravitational energy of lifting or lowering weight
Eg = W raqdsinfbar
Total Energy, where: Et = Ek + Ep +/- Eg
Eg is added if weight is falling or subtracted if weight is rising
Note: If weight is rotating in horizontal plane, the gravitational energy is zero.
Two 50 lb parts are positioned diameterically opposed on a 150 lb rotary transfer table which swings through 180° in a horizontal plane. The table radius is 50 in and the radius to the parts is 40 in. Rotational velocity of the table as it enters the cushion deceleration is 80°/sec or (80+57.3) 1.40 rad/sec. An Ohio Oscillator model H19 actuator operating at 1,500 psi has been selected to propel the load.

Ek = 1/2 J w2
Moment of Inertia: J = Jtable + Jload

Ep = PpCtqd
Torque Factor (Ct) for Model H19 (1.8 lb-in/psi)
Deceleration Arc (qd) for Model H19 (0.29 radians)
Ep = PpCtqd = (1500 psi) (1.8 lb-in/psi) (0.29 rad) = 783 lb-in
Eg = 0 for horizontal rotation
Et = Ek + Ep +/- Eg
Et = 883 + 783 + 0 lb-in = 1666 lb-in
Total energy to be absorbed in the example is 1666 lb-in. The cushion capacity, properly adjusted, of Model H19 is 1950 lb-in. which is adequate to absorb the deceleration requirement.
Caution: See caution note on Rotary Formulas
A material handling rollover mechanism transfers a 200 lb machine part through 180° in a vertical plane from a 9 o'clock to a 3 o'clock position. The radius arm to the part grippers is 40 in and the effective weight and radius of the arms and grippers can be approximated by two 40 in long rods weighing 70 lb a piece. Rotational velocity of the mechanism as it enters the cushion deceleration arc is 40°/sec or (40/57.3) 0.70 rad/sec. An Ohio Oscillator model H67 actuator operating at 2,000 psi has been sellected to propel the load.

Ek = 1/2 J w2
Moment of Inertia J = Jarm + Jload

Ep = PpCtqd
Torque Factor (Ct) for Model H67 (6.0 lb-in/psi)
Deceleration Arc (qt) for Model H67 (.034 rad)
Ep = Pp Ct qd = (2,000 psi) (6.0 lb-in/psi) (0.34 rad) = 4080 lb-in
Eg = W raqdsinfbar
W ra = (200 lb)(40 in) + 2(70 lb) 1/2(40 in) = 10,800 lb-in.
Deceleration Arc (qd) for model H67 (0.34 rad or 19.6°

Et = Ek + Ep +/- Eg
Et = 250 + 4080 + 3635 lb-in = 7965 lb-in
Total energy to be absorbed in the example is 7965 lb-in. The cushion capacity of Model H67 is 7100 lb-in. this is inadequate to absorb the deceleration requirement.
When the energy developed exceeds the capacity of the cushion, consider the following:
CAUTION: Cushion needle adjustment is a crucial factor in achieving optimum cushion performance. If the needle valve setting is too far open, cushion capacity will be reduced or rendered ineffective; if set too tight, cushion action will generate shock and pressure spikes in excess of actuator rating.