This application is related to disconnect switches.
A disconnect switch is utilized to disconnect power sources from an electrical system. In a direct current (DC) system, for example, a photovoltaic disconnect switch may be used to disconnect multiple DC power sources from the electric system that is supplied by photovoltaic cells in one or more photovoltaic modules. The Underwriters Laboratory (UL) standard requirement for certification of a photovoltaic disconnect switch are for the device to operate at an overload of 200 percent of the rated current of the switch and to pass an endurance test at the rated current.
However, opening the contacts of a disconnect switch under a DC load creates an arc between the stationary contact, (e.g., line side), and movable contact, (e.g., load side), of the switch. Current industry devices attempt to suppress this arc by connecting two poles of a three pole disconnect switch in series and by using arc grids (e.g., deion plates) to suppress the arc. This series connection creates additional break points in the circuit when the switch is opened, which add to the overall resistance of the circuit, thereby causing the arc to be rapidly extinguished. Additionally, arc grids in some cases break the arc into smaller arcs and cool the arc, which raises the arc voltage and aids in extinguishing the arc.
However, the current devices allow only one line/load combination to be wired through a three pole disconnect switch. When wiring the current devices in a three (3) line/load configuration with no additional series connection, they are not able to meet the necessary number of operations under overload and endurance conditions as required by the UL rating body.
Additionally, arc grids alone work well only when they remain relatively cool. The arc in general rises with natural convection into the arc grids. When the temperature of the arc grids increase during endurance, the heat of the grids begin to repel the arc. This repulsion acts to constrain and shorten the path of the arc. The increase in arc voltage is not achieved and the arc remains active after the disconnect switch is completely open. This failure to rapidly extinguish the arc results in additional heat being built up in the system and the eventual melting of the disconnect switch, since the arc itself may be at a temperature of 20,000 Degrees Kelvin.
It would therefore be beneficial to provide a disconnect switch that does not use arc grids to extinguish the arc.
A disconnect switch is disclosed. The disconnect switch includes a case having a movable contact, a stationary contact and a plurality of magnets. The movable contact is adapted to move from a first closed position where it is in physical contact with the stationary contact to a second open position. The magnets are located at predefined locations and in predefined orientations about the axis of movement of the movable contact, whereby upon the movement of the movable contact from the first position to the second open position, a current arc created by the movable contact is extinguished.
By utilizing a combination of magnets to extinguish an arc, instead of utilizing an arc grid, space is opened up for the arc to lengthen and cool.
Referring now to the drawings, wherein like reference numerals refer to similar components across the several views,
Disposed within the cover 110 are magnets 150, (designated 1501, 1502, and 1503). Additionally, the cover 110 includes vents to release heat. Again, for purposes of example, three magnets 150 are shown, however, it should be noted that a greater or lower number of magnets may be included, depending on the desired application.
Referring now collectively to
As each movable contact 130 rotates about its axis from a first position where it is in physical contact with its respective stationary contact 140 to a second, open, position, an arc “A” is formed along the path of the movable contact 130 in breaking its physical contact with its respective stationary contact 140. A magnetic field MA is generated by the current flow of each arc. As the arc A proceeds along its path, it is first attracted by the magnetic fields Mm produced by magnets 150, stretching and lengthening the path of the arc by acting on the Arc's magnetic field. That is, the magnetic fields Mm of magnets 1501, 1502 and 1503 first attract the arc A, stretching and lengthening the path of the arc by acting on the Arc's magnetic field. As the movable contact 130 moves past the magnets 1501 and 1503, the arc A is repelled. The combination of attracting and repelling the arc A increases its voltage above the system voltage, (e.g., 600V and higher), which aids in extinguishing the arc. In addition, the magnetic fields of the magnets deflect the arc plasma, which causes an additional increase in the arc voltage. This effect may be referred to as the “Hall” effect. Since ions may be many times heavier than electrons, (e.g., 10,000 times heavier), as the electrons are pushed out of the plasma stream, the stream ceases to be a good conductor and extinguishes. The arc is also cooled through the vents of the cover 110 through convection.
In this embodiment, disposed within the base 1020 are three magnets (10501, 10502, and 10503), while disposed within the cover 1010 are five magnets (10504, 10505, 10506, 10507, and 10508). Additionally, the cover 1010 includes vents to release heat. Again, for purposes of example, eight magnets 1050 are shown, however, it should be noted that a greater or lower number of magnets may be included, depending on the desired application.
Referring now collectively to
Disposed within the cover 1010 are magnets 10504, 10505, 10506, 10507, and 10508 substantially parallel to the axis of the paths of the movable contacts 1030. Magnets 10505 and 10508 each have their north poles facing to the left and the south poles facing to the right in the view of
As each movable contact 1030 rotates about its axis from a first position where it is in physical contact with its respective stationary contact 1040 to a second, open, position, an arc “A” is formed along the path of the movable contact 1030 in breaking its physical contact with its respective stationary contact 1040. A magnetic field MA is generated by the current flow of each arc. As the arc A proceeds along its path, it is attracted immediately upon creation by the magnetic fields Mm produced by magnets 10505 and 10508, stretching and lengthening the path of the arc by acting on the Arc's magnetic field, due to the magnets' locations proximate to the stationary contacts 1040.
Also, as the arc A proceeds along its path, it is first attracted by the magnetic fields Mm produced by magnets 10501, 10502, 10503, 10504, 10506, and 10507, stretching and lengthening the path of the arc by acting on the Arc's magnetic field, and then repelled by their magnetic fields as the movable contact 1030 moves past the magnets 10501, 10502, 10503, 10504, 10506, and 10507. The combination of attracting and repelling the arc A increases its voltage above the system voltage, (e.g., 600V and higher), which aids in extinguishing the arc. In addition, the magnetic fields of the magnets deflect the arc plasma, which causes an additional increase in the arc voltage. This effect may be referred to as the “Hall” effect. Again, since the ions may be many times heavier than the electrons, as the electrons are pushed out of the plasma stream, the stream ceases to be a good conductor and extinguishes. The arc is also cooled through the vents of the cover 1010 through convection. In addition, the magnets 10501, 10502, 10503, 10504, 10506, and 10507 twist the arc to further aid in the extinguishing of the arc.
The above embodiments provide a disconnect switch, for example a photovoltaic disconnect switch, that rapidly stretch, attract, repel, and twist an arc generated during the breaking of contact between a movable contact in the switch with a stationary contact in order to extinguish the arc. The arc is thereby extinguished before the contacts are fully open allowing the disconnect switch to operate at higher voltages, such as 600V and higher, and break current higher than rated current, (e.g., twice rated current), at that voltage. Additionally, the above embodiments provide for the breaking of multiple independent sources in a single disconnect switch. Although the disconnect switches 100 and 1000 are described as including a separate cover and base portion, it should be noted that the switches 100 and 1000 may be formed as a single case unit. In addition, example magnets 150 may be formed of a material such as a grade 35 Neodymium-Iron-Boron (NdFeB), having a coating in accordance with the American Society for Testing and Materials (ASTM) standard B689-97, although other types of magnets may be used.
The foregoing embodiments have been shown and described for the purposes of illustrating the structural and functional principles of the embodiments, as well as illustrating the methods of employing the embodiments and are subject to change without departing from such principles. All modifications to the embodiments are therefore encompassed within the spirit of the following claims.
This application claims the benefit of U.S. Provisional Patent Application Nos. 61/303,123, filed on Feb. 10, 2010 and 61/314,805, filed on Mar. 17, 2010, both of which are incorporated by reference herein as if fully set forth.
Number | Name | Date | Kind |
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4367448 | Nishizako | Jan 1983 | A |
Number | Date | Country | |
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20110193664 A1 | Aug 2011 | US |
Number | Date | Country | |
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61303123 | Feb 2010 | US | |
61314805 | Mar 2010 | US |