This patent relates to actuators, such as the type of actuators used in controlling high-power circuit breakers, circuit switchers, fault interrupters, disconnectors, grounding devices, and the like, and more particularly, to a high speed electromagnetic actuator.
High speed operation and actuation is necessary or desirable in many types of power distribution equipment. Typical applications include providing fault protection of sensitive loads while ensuring substantially continuous electrical services. Providing continuous electrical service in the presence of a fault often involves quickly transferring the load from a primary source (usually a utility) to a secondary source (a separate source or utility or a local source such as a generator). High speed fault clearing is desirable to minimize voltage disturbances for other loads on the same feeder. This technique is especially prevalent in transmission systems and closed loop distribution systems.
Electromagnetic devices have seen application as actuators for high speed operation of power distribution equipment. Electromagnetic actuators used in circuit breakers and other power distribution equipment may employ one or more solenoids with ferromagnetic stators and armatures expending energy stored or created in the magnetic circuit to perform mechanical work. A small class of electromagnetic actuators uses repulsive forces to drive the load. In this type of actuator, a current with a high rate of change flows through a coil inducing opposing current in an adjacent conductive plate. The opposing currents repel each other driving the plate away from the coil. Achieving the high rate of change requires high voltages; achieving significant forces requires high current. These factors require large capacitive power supplies. In addition, the current in the coil and plate cannot reach their peak value at the same time, reducing the maximum possible force.
An electromagnetic actuator is capable of providing a high speed driving force, for example, for driving the contacts of a circuit breaker or similar power distribution equipment. The electromagnetic actuator may use electromagnetic forces for motion and a permanent magnet for latching. A velocity proportional feedback device, or other suitable structure, may provide component speed control. An electromagnetic actuator in accordance with one more of the herein described embodiments may minimize the number of moving parts while providing reliable and consistent performance.
In accordance with one or more of the herein described embodiments, an electromagnetic actuator may use a separate coil supplying an opposing current, while the moving element is directly powered. Directly powering the moving element may reduce the requirements for current, voltage and current and/or voltage rate-of-change permitting use of a smaller power supply. Separate coils may further allow for precise control of actuator motion by permitting different supply voltages, firing times and capacitor supplies. The coils may be identical or of different designs. The coils may be connected in parallel or series and may be powered separately. Lower current and voltages allow for economical construction using circuit elements typically specified for solenoid-type actuators.
The electromagnetic actuator may incorporate a return spring arrangement. One or more permanent magnets may be employed to hold the moving element in place at both ends of its motion. The retaining force may be overpowered by the coil generated repulsive force and/or the latching magnet flux may be reversed by applying a current to an adjacent coil.
A velocity proportional feedback device, such as a hydraulic damper or dash-pot, may be provided. Alternative type velocity control devices include pneumatic dampers or an additional electromagnetic coil, e.g., a voice-coil. The velocity control device may operate to control the speed of the moving element throughout its stroke. Referring to
Referring to
In the actuator first position, the moving coil 110/armature 104 and opening coil 106 are adjacent to one another, as shown. The moving coil 110 is held in place by a plunger 118 of the magnetic latch 120, which rests on a latch stator 122. The permanent magnet 124, which may be ring-shaped, remains in contact with the stator 122. The plunger 118 is threaded to the armature 104 and secured with a locknut 126. The armature 104 pushes on the compliance spring 119, which in turn pushes on the drive shaft 128 through a washer 130 and retaining ring 132. The drive shaft 128 applies pressure to a driven element, such as a circuit breaker contact, through a ferrule 134 that is threaded into the drive shaft 128.
To provide an operating force in a first direction, for example, to provide an opening force on the circuit breaker contact, the moving coil 110 and the first coil 106 may be energized in parallel. The electromagnetic force from the opposing currents (the Lorentz force) drives the two apart. The first coil 106 is fixed, so the moving coil 110 moves from a first position in the first direction toward the second coil 108. After the moving coil 110 has moved a short distance from the first coil 106, it strikes the flange 136 of the drive shaft 128. This impact initiates motion of the drive shaft 128 in the first direction. For example, when used in conjunction with a circuit breaker, the impact provides energy to break any contact welds. After a brief period of bounce, the spring 138 pushes the moving coil 110 and drive shaft 128 to the second position. In the second position, the armature 104 rests against a linear bearing 140 and the shaft flange 136 rests against the bottom of the armature 104. To provide an operating force in a second direction, opposite the first direction, the second coil 108 and the moving coil 110/armature 104 start adjacent each other. Once energized, the opposing currents initiate travel from the second position in the second direction, for example, to drive the contacts of the circuit breaker closed. The armature bobbin 116 quickly travels to the latched position with the plunger 118 held against the face of the stator 122. The drive shaft 128 is retarded by a velocity-feedback device 142, e.g., a hydraulic damper, and is driven more slowly to the closed position by the compressed compliance spring 119.
Movement of the drive shaft 128, and hence movement of a component or components of a coupled device, is controlled by the velocity feedback device 142, which may be a hydraulic damper. The velocity-feedback device 142 produces a force proportional to velocity that opposes the movement of the coupled device. The hydraulic damper may include a housing defining a cup portion 144 and one face of the stationary first coil bobbin 114. The hydraulic damper is filled with an appropriate fluid, such as silicone fluid, and sealed with o-rings 146. Force is generated and transmitted to the coupled device through a flange 148 on the drive shaft 128 that acts like a piston within the cup 144. The relation between the force and velocity may be controlled by the geometry of the flange 148, the cup 144 and the properties of the fluid.
In general, the design is intended to be self-aligning. Alignment to the drive shaft 128 is provided by the o-rings 146 and the bearing 140 in the second coil bobbin 114. Provisions may also be made in the drive shaft 128 for connections to the coupled device as well as to for a travel indicator. Additionally, the actuator 100 may be retained within a frame or housing (not depicted) and may include suitable electrical connections for coupling to a power supply and/or a controller.
Referring to
As seen in
Referring to
The spring 260 is compressed between an end of the armature 204 and a pocket 266 in the stator 264 in the second position. The spring rate of the spring 260 and the compliance spring 219 and their corresponding deflections are chosen such that the total energy stored in the springs is the same in either the first or second positions.
The actuators 100 and 200, as described above, contained no magnetic materials in the vicinity of the coils. The magnetic field generated by each coil was identical to that produced in open air. An alternate actuator 300, depicted in
The actuators 100 or 200 typically fired two coils at once: either the first or the second coil 106 and 108 and the moving coil 110. These coils were adjacent at the beginning of the stroke, and repelled each other. The unfired coil, either coil 106 or 108 may be fired near the end of the stroke to attract the moving coil 110, as will be described below. This coil, however, could not add significant flux across the moving coil until it approached. By adding steel parts to channel the flux, more flux from the far coil can pass across the moving coil early in the stroke. Also, if the stationary coils have the same current, and the stroke is short (≦2.5 cm, 1 inch), the total radial component of flux across the moving coil will be nearly constant for the whole stroke; as flux from one coil drops off, the other picks up.
The design of the actuator can be tailored for different purposes. The chart of
The coil stators 322 and 368 and output shaft 328 are made of mild steel. An outer mild-steel tube 370 has also been added to channel flux from the stationary coils 306 and 308. This constitutes the constant force, curve 402, form of the actuator 300. More force can be generated by making the armature 304 and flanges 372 from mild steel and adding a mild-steel collar 374 to the moving coil 310. This configuration produces the non-linear force curve, curve 400.
As noted above in connection with
The circuit 600 is described with reference to the actuator 100, but it should be understood that the circuit 600 may be used in conjunction with an actuator in accordance with any one or more of the herein described embodiments of actuators or modifications thereof. Bipolar transistors 602 and 604 couple to the first coil 106 and the second coil 108. The transistors 602 and 604 permit a current flow in the main channel that is proportional to the current in the gate. For discrete control, the transistor gate current may be derived directly from the position transducer 606 and the inverse thereof 608. To ensure complete cutoff of the coil current, each transistor gate may further be controlled by a field effect transistor (FET) 610. The FETs 610 are normally open, closing in response to an OPEN or CLOSE signal from a suitable controller, allowing gate current to flow. A bi-directional IGBT bridge 612 couples to drive the moving coil 110.
As shown in
If the position transducer 606 output is linear with position, the signal will be linear growing in value as the plunger 118 comes to rest at the second position. The second coil 108 current will begin at a maximum, repelling the moving coil 110, because their currents are opposite. As the moving coil 110 travels to the second coil 108 current will be reduced and the first coil 106 current will increase, attracting the armature 110, because the currents are in the same direction. Inductance of the coils prevents the currents from exactly mimicking the position signal.
The linear transducer may be inefficient because the effects of the stationary coils 106 and 108 are equal at the midpoint of travel. This can be remedied by using a non-linear position transducer. One option is to have a Hall-Effect sensor embedded in the face of the permanent magnet stator 122. As the air gap is reduced, the magnet flux will increase in response to the reduced reluctance. This effect is non-linear. The result is the second coil 108 repelling the moving coil 110 for a much greater percentage of the stroke. The first coil 106 does not begin to attack until the end of the stroke, when its contribution is most effective.
The system could be still more efficient if current dropped off entirely during the middle of the stroke.
Referring to
With additional reference now to
The current in each of the stationary closing coil 108 and opening coil 106 is controlled by single IGBTs 901 and 902. Additional MOSFETs 907 and 908 are added on the low voltage side of these coils to facilitate the use of commercially available driver ICs (not depicted). Current in the moving coil 110 is controlled using an H-bridge 912 composed of four IGBTs 903, 904, 905, and 906. Use of the H-bridge 912 allows the direction of the current in the moving coil 110, and thus the motion of the output, to be controlled independently of the direction of its windings.
While the present disclosure is susceptible to various modifications and alternative forms, certain embodiments are shown by way of example in the drawings and the herein described embodiments. It will be understood, however, that this disclosure is not intended to limit the invention to the particular forms described, but to the contrary, the invention is intended to cover all modifications, alternatives, and equivalents defined by the appended claims.
It should also be understood that, unless a term is expressly defined in this patent using the sentence “As used herein, the term ‘______ ’ is hereby defined to mean . . . ” or a similar sentence, there is no intent to limit the meaning of that term, either expressly or by implication, beyond its plain or ordinary meaning, and such term should not be interpreted to be limited in scope based on any statement made in any section of this patent (other than the language of the claims). To the extent that any term recited in the claims at the end of this patent is referred to in this patent in a manner consistent with a single meaning, that is done for sake of clarity only so as to not confuse the reader, and it is not intended that such claim term by limited, by implication or otherwise, to that single meaning. Unless a claim element is defined by reciting the word “means” and a function without the recital of any structure, it is not intended that the scope of any claim element be interpreted based on the application of 35 U.S.C. §112, sixth paragraph.
This application claims the benefit of U.S. Provisional Application No. 60/741,518 filed Dec. 1, 2005.
Number | Date | Country | |
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60741518 | Dec 2005 | US |