This invention relates to an electrical breaking module equipped with a magnetic blow-out device, said breaking module comprising a non-magnetic, electrically insulating housing at least one fixed contact and one moving contact, said moving contact being designed to move relative to said fixed contact between a closed position and an open position and vice versa along a path defining a breaking plane, said fixed contact and said moving contact defining between them a breaking zone extending into said breaking plane, in which an electric arc extends at its origin, in particular when the electrical circuit is opened, said breaking module comprising at least one breaking chamber delimited by the inner walls of said housing and comprising said breaking zone for managing said electric arc with a view to breaking the current, and said magnetic blow-out device comprising at least one magnetic field source arranged in said breaking chamber opposite said breaking zone.
The invention also relates to an electrical breaking apparatus comprising at least one control module and said electrical breaking module defined above.
Magnetic blow-out of the arc is a principle commonly used in breaking technologies to manage the arc that arises, in particular, when an electrical circuit is opened, with the aim of improving breaking performance and preserving the integrity of the fixed and moving contacts of the breaking module. The magnetic field, which may be generated by any type of magnetic field source, enables the arc to be displaced as soon as it arises, and stretched rapidly to accelerate cooling until it is extinguished. Cooling the arc plasma increases its impedance, which in turn increases the arc voltage during breaking. Breaking direct current (DC) requires the breaking module to generate more voltage than the mains voltage to be broken. This is why the magnetic blow-out principle is particularly well suited to DC breaking. However, a high arc voltage is also of interest when breaking alternating current (AC), as it enables the current to be limited during breaking, thereby reducing arc damage and even shortening the arc time through a limiting effect. As a result, the magnetic blow-out principle is just as interesting for DC currents as for AC currents.
The applicant's publication FR 3 006 101 A1 proposes an electrical breaking module equipped with a non-polarized magnetic blow-out device, which has the advantage of operating independently of the direction of the current in said breaking module. For this purpose, the magnetic blow-out device includes a magnetic field source, such as a permanent magnet, arranged in such a way that the breaking response is unchanged regardless of the current direction. Placing the magnet in front of the breaking zone allows the arc to be blown out to a large extent. Magnetic blow-out results in a lengthening of the arc and an arc column that licks the insulating inner walls of the housing. Together, these two phenomena tend to cool the arc plasma, increasing its impedance. As a result, the arc voltage rises sharply, making it possible to break higher DC voltages.
However, the quest for improved breaking performance is omnipresent.
EP 2 980 821 A1 proposes a magnetic blow-out solution that is unsatisfactory for many reasons. The single central magnet is far from the breaking zone, resulting in a high magnetic field loss in the breaking zone and making magnetic blow-out difficult. The magnetic arms that extend the central magnet generate a concentration and distortion of the magnetic field, which is counterproductive for arc blow-out. The electromotive force induced by the magnetic field on the arc is not directed towards the arms, but perpendicular to them, which is also counterproductive for arc blow-outs. In addition, the magnetic arms leave a large volume of air around the breaking zone, allowing the arc to recoil and reform or reclash between the fixed and moving contacts, which is dangerous for equipment and people.
And publication WO 2012/110523 A1 proposes a solution for extinguishing the arc not by magnetic blow-out but by creating arc confinement imposed by mechanical displacement, commonly known as a guillotine. This principle of arc management is very violent in terms of the arc plasma, and may generate significant overvoltages that are harmful or even dangerous to the electrical mains you wish to interrupt.
Disclosure of the Invention
The aim of this invention is to improve the magnetic blow-out device described in the applicant's publication by proposing a solution that further accelerates arc plasma cooling, with a view to generating even more arc voltage when the current is interrupted, while retaining a non-polarized breaking solution that can be easily adapted to different configurations of electrical breaking apparatus, and enabling the choice of less efficient and therefore less expensive magnets.
To this end, the invention relates to an electrical breaking module of the kind indicated in the preamble, characterized in that said magnetic blow-out device further comprises at least one non-magnetic and electrically insulating deflector, arranged in said breaking chamber to form a physical obstacle in the path of the electric arc when it is magnetically blown, and occupy the major part of the space existing between said breaking zone and said housing, so as to create in the narrow gap remaining between the insulating walls of said deflector and those of said housing, at least one arc confinement zone in which said electric arc, when magnetically blown, is deflected and constrained to promote its cooling and extinction.
The addition of the non-magnetic deflector in the breaking chamber has the effect of immediately deflecting the arc plasma path in the direction of the induced electromagnetic force, stretching the blown arc as far as possible from the breaking zone to avoid recladding, and constraining it in a narrow gap between insulating walls to promote cooling and accelerate extinction.
Alternatively, said breaking chamber may extend on either side of said breaking plane, symmetrically or not, and said deflector may also extend on either side of said breaking plane, symmetrically or not, to define at least two arc confinement zones in opposition to said breaking plane.
In a preferred embodiment of the invention, said at least one magnetic field source can be oriented to generate at least one magnetic excitation vector substantially parallel to said breaking plane so that the induced electromagnetic force displaces and stretches said electric arc in a direction substantially perpendicular to said breaking plane towards the housing and into said at least one arc containment zone.
According to the selected embodiments, the deflector may be movable and integral with the movable contact, or fixed and integral with said housing.
In addition, said deflector may be made up of a plurality of fins or plates spaced apart and oriented substantially perpendicular to said breaking plane. It may also be made of a solid or openwork monoblock.
In the preferred form of the invention, said deflector can have a C-shaped cross-section, substantially symmetrical with respect to the breaking plane, comprising two lugs separated by a central opening designed to free a passage for the relative movement of said movable contact or said fixed contact depending on whether said deflector is fixed or movable.
The said magnetic blow-out device may also comprise at least one carcass arranged to channel the magnetic flux induced by the said at least one magnetic field source, this carcass may or may not be integrated into the housing and arranged around at least the said magnetic field source and the said deflector.
Alternatively, said at least one field source may be static and integral with said housing, or mobile and integral with said mobile contact. In addition, said movable contact may be rotatable about said central axis or translatable parallel to said breaking plane.
If the electrical breaking module comprises two fixed contacts symmetrical with respect to a central axis or median plane of said housing, and a moving contact common to the two fixed contacts defining two symmetrical breaking zones, then it advantageously comprises two symmetrical breaking chambers, and at least two non-magnetic, electrically insulating deflectors, each arranged in one of the breaking chambers.
This invention and its advantages will become clearer in the following description of several non-limiting example embodiments, with reference to the appended drawings, in which:
In the illustrated embodiments, the identical elements or parts bear the same reference numbers. Furthermore, terms having a relative meaning, such as vertical, horizontal, right, left, front, rear, above, below, etc., are to be interpreted under normal conditions of use of the invention, and as represented on the figures. Furthermore, the geometrical positions indicated in the description and claims, such as “perpendicular”, “parallel”, “symmetrical”, are not limited to the strict sense defined in geometry, but extend to geometrical positions which are close, i.e., which accept a certain tolerance in the technical field considered, without influencing the result obtained. This tolerance is notably introduced by the adverb “sensibly”, without this term necessarily being repeated before each adjective.
With reference to the figures, the electrical breaking apparatus 1 according to the invention may be interchangeably any of the following: a cutoff switch, a switch-disconnector, a contactor, a switch, a changeover switch, a circuit breaker, or any other similar breaking apparatus. It is designed to be mounted on a DIN rail, a base plate or any suitable mounting bracket. It can be designed to break low-voltage direct current (i.e., below 1500V), such as in photovoltaic or similar applications, or medium-voltage direct current, such as 2000V or 3000V for special applications, without these values and examples being limitative. It can also be used to break alternating current in all types of industrial, tertiary and domestic applications, regardless of the nominal supply voltage.
The electrical breaking apparatus 1 may or may not be based on a modular architecture. If the apparatus is modular, then with a single control module 2 it can control one or more breaking modules 3, 3′, for example one to eight breaking modules, without this number being limitative. The control module 2 is not part of the invention and will not be described. Only the breaking module 3 forms part of the invention and will be described in detail, it being specified that it can form an integral part of said electrical breaking apparatus when the latter is not modular. The term “module” should therefore not be interpreted in a restrictive sense.
Each breaking module 3, 3′ forms a switch pole, which can interchangeably be a single switch pole with one fixed contact CF and one moving contact CM, or a double switch pole with two fixed contacts CF and one common moving contact CM. In all cases, the moving contact CM is arranged to move relative to the fixed contact(s) CF between a closed position and an open position and vice versa on a path defining a breaking plane P. The relative movement of the moving contact CM can interchangeably be rotary or linear. In addition, the fixed CF and movable CM contacts can interchangeably be sliding, pressure or any other type of compatible electrical contact.
The electrical breaking apparatus 1, hereinafter also referred to as breaking apparatus 1 or apparatus 1, according to the invention and as illustrated in
Also with reference to
The fixed contact CF and the moving contact CM define between them respectively two breaking zones Z, in which an electric arc E extends, particularly when the electrical circuit is opened. The electric arc E is represented schematically by a cord in
The breaking module 3 comprises two breaking chambers 9, which are delimited by the inner walls of the housing 5 and each comprise one of the breaking zones Z. Breaking chambers 9 are used to manage the electric arc E in order to quench the current. In the example shown, the breaking chambers 9 are diametrically opposed with respect to the central axis A and symmetrical with respect to the median plane coinciding with the breaking plane P. This example is not limitative, since asymmetrical breaking chambers can be envisaged, without calling into question either the operation or the non-polarity of the magnetic blow-out devices 10.
The breaking module 3 also includes a magnetic blow-out device 10 for the electric arc E. In the example shown, the magnetic blow-out device 10 comprises two static magnetic field sources 11, each arranged close to and opposite a switch-off zone Z. The fact that they are each located opposite a breaking zone Z makes it possible to create a maximum magnetic field directly in the breaking zone and a virtually constant magnetic field throughout the breaking chamber 9 for optimum magnetic blow-out of the electric arc E. The magnetic field sources 11 are isolated from the said breaking zone Z by the inner walls of the housing 5. In the example shown, each magnetic field source 11 is oriented to generate a magnetic excitation vector M substantially parallel to the breaking plane P. Thus, the electromagnetic force F induced by each magnetic field source 11 moves and stretches the corresponding electric arc E in a direction substantially perpendicular to the breaking plane P towards the bottom of parts 5a, 5b of housing 5, and this independently in one direction or the other depending on the polarity of the magnetic field source 11 and/or said current. However, the invention is also suitable for magnetic blow-out devices which may have a different architecture, offering both non-polarized and polarized breaking, and blow-outs of the arc towards other walls of the housing 5.
The magnetic field source 11 may consist of one or more permanent magnets, or any other equivalent system capable of generating a magnetic excitation vector, such as one or more electrically powered coils. In the examples shown, the magnetic field source 11 consists of a permanent magnet with a flat, parallelepiped shape, without this shape being limitative. The numerical reference 11 will be used interchangeably to designate the magnetic field source and the magnet(s). In fact, it is possible to design a magnetic field source 11 whose shape is adapted to the architecture of the breaking module, which may be curved, as in the case of a rotary breaking apparatus, for example. In this case, it may consist of a plurality of parallelepiped permanent magnets arranged side by side on a curved line, or of a permanent magnet molded into a curved shape. The characteristics of the permanent magnet, as well as its technical effects on the blow-out and stretching of the electric arc, are described in particular in the applicant's publication FR 3 006 101 A1, and will not be detailed in this application.
The magnetic blow-out device 10, in accordance with the invention, differs from that described in the above-mentioned publication in that a non-magnetic, electrically insulating deflector 20 is present in said breaking chamber 9. This deflector 20 is designed and arranged to occupy, fill or fulfill a major part of the breaking chamber 9, i.e., the space existing between the breaking zone Z and the housing 5, and to leave one or more narrow spaces or gaps between the insulating walls of said deflector and those of said housing. The deflector 20 thus forms an entirely non-magnetic physical obstacle, interposed in the path of the blown arc, and reduces to a minimum the volume of air remaining in said breaking chamber 9. At least one of the remaining narrow spaces or gaps then constitutes an arc confinement zone 21, in which the electric arc E when magnetically blown is deflected and constrained to promote its cooling and extinction. This arc confinement zone 21 is mainly located at a distance from and in line with the breaking zone Z in the direction of the electromotive force F.
In the example shown in
The inner walls of housing 5 have a shape substantially complementary to the shape of deflector 20, for example lugs 22, with a defined clearance to create said arc confinement zones 21. Thus, the inner walls of housing 5 also have a geometric shape that is substantially symmetrical with respect to the breaking plane P in the example shown, without this example being limiting. As already mentioned, the symmetry of the chambers 9 with respect to the aforementioned breaking plane P guarantees equivalent breaking performance, whatever the polarity of the magnets 11 and the direction of the current, if the magnets are also arranged symmetrically with respect to the aforementioned breaking plane P. The same result is possible if the chambers 9 are not symmetrical if the magnets 11 are also arranged non-symmetrically. In all cases, non-polarized operation of the magnetic blow-out device 10 is guaranteed.
When the electrical circuit is opened and the moving contact CM leaves the fixed contact CF, an electric arc E is established in the breaking zone Z between the fixed contact CF and the moving contact CM, and flows through the central opening 23 of the deflector 20 (see
This new breaking principle offers a gain in breaking performance, as it enables a high arc voltage to be achieved. It also makes it possible to reduce the magnetic field required and to use magnets 11 of lower quality and cost, such as ferrite-type magnets or similar, instead of high-quality, rare-metal and expensive magnets such as neodymium iron boron.
In addition, the breaking principle described above can be easily adapted to a variety of different applications, some examples of which are described below.
The movable deflector 20, as described with reference to
These examples of deflector 20, 20′ are of course not limitative, and other modes of implementation and/or geometric shapes are possible insofar as they form non-magnetic physical obstacles in the path of the blown electric arc E, which occupy and fill the breaking chambers 9 to reduce to a minimum the volume of air remaining in narrow spaces, baffles and/or exhaust columns, having the effect of constraining and deflecting the path of the arc plasma and therefore of the electric arc between non-conducting walls. The deflector 20, 20′ can also be made of a one-piece openwork part, not shown, for example with slots, orifices, pores or the like running through it to allow the arc plasma to expand in the direction of the electromotive force F and towards the confinement zones 21, 21′.
The breaking principle of the invention also applies to so-called linear breaking modules 3′, as opposed to the rotary breaking modules 3 described above. With particular reference to
The linear breaking module 3′ also includes two symmetrical breaking chambers 9, in line with two breaking zones Z, a magnetic blow-out device 10 with two symmetrical magnets 11 facing each of the breaking zones Z, and two symmetrical deflectors 20 mounted on the linear carriage 8′. These deflectors 20 also have the same configuration as the deflectors 20 of
In addition, and in all the variants described, the magnetic blow-out device 10 can be amplified by the addition of a ferromagnetic or similar housing 12, the effect of which is to channel and concentrate magnetic field M induced by magnet 11 of magnetic blow-out device 10 in each breaking chamber 9. In the example shown in
The magnetic blow-out device 10, when used in double breaking modules 3, 3′, as shown in the various
This invention is of course not limited to the embodiments described, but extends to any modifications and variants obvious to a person skilled in the art, within the limits of the appended claims. In addition, all or some of the technical characteristics of the above-mentioned embodiments and variants may be combined with each another. Furthermore, the arrows M and F, which respectively represent the magnetic excitation vector in the figures, generated by each magnetic field source 11 and the corresponding induced electromagnetic force, may be oriented differently as a function of both the polarity of said magnetic field source 11 and the direction of the current flowing in each breaking chamber 9, without thereby departing from the protective scope of the invention.
Number | Date | Country | Kind |
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2105345 | May 2021 | FR | national |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2022/062695 | 5/10/2022 | WO |
Publishing Document | Publishing Date | Country | Kind |
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WO2022/243119 | 11/24/2022 | WO | A |
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10176945 | Domejean | Jan 2019 | B2 |
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20200286692 | Kolmonen | Sep 2020 | A1 |
Number | Date | Country |
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211719469 | Oct 2020 | CN |
2980821 | Feb 2016 | EP |
3006101 | Nov 2014 | FR |
WO2012110523 | Aug 2012 | WO |
Entry |
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Translation of CN211719469 (Original document published Oct. 20, 2020) (Year: 2020). |
Number | Date | Country | |
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20240234043 A1 | Jul 2024 | US |