Throughout history, engineers have used actuators to move objects providing rotary or linear motion. A rotary actuator is simply a gearing system that either increases or decreases the rotational speed of a prime mover, typically a hydraulic motor, an internal combustion engine, a turbine engine, or an electric motor, to provide a desired level of rotational speed and torque at an output. Examples of rotary actuators include: gearboxes, transmissions, differentials, Rotac® actuators, and rotary electro-mechanical actuators. Linear actuators are machines designed to provide force and linear displacement to an object. Some examples of linear actuators include: rack & pinion actuators, hydraulic rams, ball screw actuators, and crank arm actuators.
Historically, hydraulic/pneumatic motors and hydraulic/pneumatic rams have been the primary source of power for both linear and rotary actuators. Hydraulic systems offer many advantages to the designer including: high power density, accurate position control, low inertia (for high frequency response), and overload protection (via pressure relief valves).
More recently, engineers have replaced hydraulic/pneumatic actuation systems with electro-mechanical actuation systems. Electro-mechanical actuators (“EMA”), which typically include a motor, a gear box and an actuator, offer increased efficiency over their hydraulic and pneumatic counterparts and are less prone to leakage.
When designing small, high power density EMAs, a designer is faced with a problem caused by the rotational inertia associated with the EMAs electric motor. In order to create an EMA with a large force capability, the designer must create an electric motor that is capable of producing a large torque, or must create a gear train that reduces the motor's output torque requirement. If the designer chooses to create a motor with a large torque capability, its rotor will contain a significant amount of rotational inertia. If the designer chooses to utilize a gear reduction system to decrease the motor's output torque requirement, thereby reducing the motor's physical size and rotational inertia, the motor will be required to operate at a faster speed. The inertia of the motor, as felt by the output of the actuator, will be proportional to the motor's inertia multiplied by the gear reduction ratio squared.
The inertia of the EMA motor becomes extremely important when sizing the gear train and/or the actuator structure if, for instance, the actuator hits an internal stop at full speed, or if the actuated structure hits a stop at the end of its travel at full speed. In this scenario, the rotational inertia of the motor will tend to cause the actuator to continue driving through its stop, or through the structure's end stop, causing significant damage to the EMA, or its supporting structure. If the stops and structures are strong enough to maintain their integrity, the next weakest link, most likely the actuator or the gear train driving the actuator will be damaged.
Historically, the gear train and the EMA's stops are overbuilt to handle an intense torque spike associated with the rapid deceleration of the EMA's motor as the actuator hits its stops, and the internal shafting flexes as the motor spins down. This design approach tends to cause the actuator to become significantly larger and heavier than it would otherwise have to be.
Another method to handle the scenario described above is to incorporate a slip clutch in the driveline between the EMA's motor and the EMA's output. Incorporating a slip clutch in the driveline allows the EMA's output to nearly instantaneously stop, while the motor decelerates, with the stored energy of the rotating motor rotor being absorbed by the slip clutch's friction material. This type of system works well, however, it again adds components to the EMA that add size, cost, weight, and reduce the actuator's overall reliability.
According to a non-limiting embodiment, an apparatus has a first motor for moving an actuator, an engaged brake for dissipating a torque spike in the EMA, and a gear attaching the motor to the actuator to cause the actuator to move and attaching to the engaged brake whereby the torque spike overcomes stiction in the engaged brake so that the torque spike is dissipated in the engaged brake.
According to a further non-limiting embodiment, an apparatus has a first motor for moving an actuator, a second motor for moving the actuator, the second motor moving the actuator upon a failure of the first motor, an engaged brake attaching to the second motor for dissipating torque spikes in the system, and a gear attaching the first and second motor to the actuator to cause the actuator to move and to the engaged brake whereby the torque spikes overcome stiction in the engaged brake so that the torque spike is dissipated in the engaged brake.
According to yet another non-limiting embodiment, an apparatus dissipates torque spike in therein and has a first motor for moving an actuator, a first brake for selectively braking the motor, a second brake that is engaged, the second brake dissipating torque spikes in the system, and a gear attaching the first motor to the actuator to cause the actuator to move and to the second brake whereby the torque spikes overcome stiction in the engaged brake so that the torque spike is dissipated in the engaged brake.
Referring to the Figure, a non-limiting schematic embodiment of an EMA 10 is shown. The EMA comprises a pair of motors 15, 20 a pair of brakes 25, 30 each brake being associated with a motor, a differential 35, an impeller such as linear actuator 40, such as a ball screw, a position sensor 45, and an attachment 50 that attaches to a load (not shown). The linear actuator 40 has an internal stop 47 shown as a collar.
The EMA shows a pair of motors 15, 20 because some applications require redundancy. If one motor fails, the other may be used. In this application, one motor 15 operates while the other motor 20 does not. In the non-operating motor 20, the brake 30 associated with it, is engaged in a non-energized state as will be discussed hereinbelow. If the motor 15 fails, motor 20 will then operate and the brake 30 will be disengaged in an energized state and does not provide braking torque on the motor unless desired.
Each motor is attached to the differential gear train as follows: motor output shaft 55 has a gear 60 mounted thereon that attaches to gear 65 that attaches to a brake gear 70. Gear 65 is mounted on shaft 75 that has a reduction gear 80 mounted thereon. For motor 15, the reduction gear 80 meshes to gear 85 on the differential 35. For motor 20, the reduction gear 80 meshes to gear 90 on the differential 35.
Referring to
Referring back to
During operation, operating motor 15 rotates to move motor output shaft 55, gear, 60, gear 65, shaft 75, reduction gear 80, gear 85, first input shaft 125, first sun gear 135, first planetary gear 145, shaft 165, differential output gear 155, ball screw gear 170 and ball screw actuator 40. The electromagnet 120 of the brake 25 is actuated so that the clapper plate 110 is drawn away from the brake plate 100 so that shaft 95 and brake gear 70 may rotate freely as the motor operates.
While the motor 15 operates, the electromagnet 120 of the brake 30 is not actuated so that the clapper plate 110 is pushed against the brake plate 100 thereby not allowing the shaft or the gear 70 mounted thereon to rotate. If the gear 70 does not rotate the gear 65 does not rotate and the motor 20 via gear 60 and shaft 55 do not rotate. Also, if gear 65 does not rotate, reduction gear 80, gear 90, shaft 130, and second sun gear 140 do not rotate. However, because planetary gear 150 is attached to differential output gear 155 that rotates due to the motor 15 input as mentioned hereinabove, planetary gear 150 may still rotate around the second sun gear 140.
If the actuator 40 hits its internal stop 47 with motor 15 spinning at full speed, a sudden torque spike, caused by the nearly instantaneous stopping of the actuator 40, is absorbed by the EMA 10. Because gear 170 can no longer rotate to extend the linear actuator beyond the stop and the drive path provided by the motor 15 can also not continue to rotate, the kinetic energy stored in the EMA passes through the second planetary gear 150, the previously stationary second sun gear 140, shaft 130, reduction gear 80, shaft 75, gear 65, gear 70 and shaft 95 to cause clapper plate 110 and brake plate 100 of brake 30 to exceed its maximum static torque rating, e.g., that force that causes the brake and clapper plates to stick together and not rotate or stiction. As brake 30 begins to slip, the stored energy associated with motor 15 rotational speed and rotational inertia will be dissipated by the friction material 105 on brake plate 100.
The EMA illustrated in
This EMA allows for the dual use of the differential and brake system, associated with the dual redundant architecture of the EMA, to create a light weight, and mechanically simple mechanism that has the ability to dissipate the stored energy associated with the rotational inertia and rotational speed of the operating motor 15.
The foregoing description is exemplary rather than defined by the limitations within. Various non-limiting embodiments are disclosed herein, however, one of ordinary skill in the art would recognize that various modifications and variations in light of the above teachings will fall within the scope of the appended claims. It is therefore to be understood that within the scope of the appended claims, the invention may be practiced other than as specifically described. For that reason the appended claims should be studied to determine true scope and content.
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