ARC RESTRICTING DEVICE FOR CIRCUIT BREAKER

Abstract: The present invention combines the provision of arc shields (6, 7) surrounding the contacts (202, 302) of a circuit breaker with a magnetic driving means (8) to raise the arc voltage of an arc drawn across the contacts (202, 302) and to effectively drive the arc, whereby the performance of the circuit breaker is improved.

Description: The invention relates to a circuit breaker according to the preamble of one of the claims 1 to 3. Such circuit breakers are already known from the documents US-A-3 155 801 and US-A-2 555 799, where circuit breaking devices are described, in which an arc formed between two contacts is urged by a magnetic field to move across arc runners towards an arrangement of plates extinguishing the arc. However, the arc struck across the contacts spreads to the conductor on which the contacts are mounted so that it is difficult to adequately raise the arc voltage; even if magnetic driving means are incorporated to extinguish the arc extinguishing is not effected efficiently. Further from US-A-3 402 273 it is already known to provide the conductors of a circuit breaker with arc shields surrounding the contacts of the two contactors. The DE-A-1 199 363 further shows the provision of a permanent magnet used at a magnetic driving means. The DE-A-1 207 027 however, teaches the provision of a C-shaped magnetic means surrounding the stationary conductor in the area of its contact, while the particular conductor has an U-shaped configuration. Finally within the book ′Starkstromtechnik II′ by Arnold Einsele, Berlin, 1960, it is stated on page 76 that circuit breakers can be provided with a specific contact system, so that an electric coil forming the magnetic driving means can be activated only during the circuit interruption by means of the arc. Considering this prior art it is the object of the present invention to provide a circuit breaker of simple construction which allows the interruption of a large current in a very efficient way. Three different ways of carrying out the invention are specified within the characterizing clause of the claims. While the US-A-3 155 801 teaches the usage of a magnetic driving means formed by two blow out coils embedded in the faces of the side walls of the arc chamber whereby the blow out coils force the arc in direction of two arc runners arranged in the V-shaped configuration, the US-A-3 402 273 teaches the provision of arc shields used for producing a certain amount of gas which is supposed to shorten the arc estinguishment. Within the frame work of the present invention, however, the arc shields surrounding the two contacts are used in order to stabilize and position the feet of the arc produced during the switching operation. In view of this fact the magnetic driving means can react only on the middle portion of the formed arc because the feet of the arc are held in position by the provided arc shields. Due to this situation the produced arc is stretched to a large extend, which facilitates the extinguishment of the arc within the extinguishing plate assembly. Within the various claims different ways are shown how the magnetic driving means can be built in such a way that a very efficient operation of the ciruit breaker can be obtained. Preferred ways of carrying out the invention are described in detail below with reference to drawings, in which: Figure 1a is a sectional plan view of a conventional circuit breaker to which this invention is applicable; Figure 1b is a sectional side view of the circuit breaker taken along line b-b of figure 1a; Figure 1c is a perspective view showing the operation of the circuit breaker of figure 1a; Figure 2 is a model diagram showing the behaviour of an electric arc struck across the gap between the contacts of the circuit breaker of figure 1a; Figure 3a is an exploded perspective view of an embodiment of a circuit breaker according to this invention; Figure 3b is a perspective view showing the operation of the circuit breaker of figure 3a; Figure 4 is a model diagram showing the effects of the arc shields provided in the circuit breaker of figure 3a; Figure 5 is a model diagram showing the general effects of arc extinguishing plates; Figure 6a is an exploded perspective view of another embodiment of a circuit breaker according to this invention; Figure 6b is a perspective view showing the operation of the circuit breaker of figure 6a; Figure 7a is an exploded perspective view of a circuit breaker showing another embodiment; Figure 7b is a perspective view showing the operation of the circuit breaker of figure 7a; Figure 8a is an exploded perspective view of a circuit breaker showing another embodiment; and Figure 8b is a perspective view showing the operation of the circuit breaker of figure 9a. In the drawings, like symbols denote identical or corresponding parts. A conventional circuit breaker to which this invention is applicable will be described with reference to figures 1a, 1b and 1c. An enclosure 1 is made of an insulating material and forms the housing for a switching device, and is provided with a gas exhaust port 101. A stationary contactor 2 housed in the enclosure 1 comprises a stationary rigid conductor 201 which is rigidly fixed to the enclosure 1, and a stationary-side contact 202 which is mounted on an electrically contacting surface of the stationary rigid conductor 201. A movable contactor 3 which is adapted to engage the stationary contactor 2 comprises a movable rigid conductor 301 which makes or breaks contact with the stationary rigid conductor 201, and a movable-side contact 302 which is mounted on an electrically contacting surface of the movable rigid conductor 301 in opposition to the stationary-side contact 202. An operating mechanism 4 operates to move the movable contactor 3 in or out of contact with the stationary contactor. An arc extinguishing plate assembly 5 functions to extinguish an electric arc A struck upon the separation of the movable-side contact 302 from the stationary-side contact 202, and it is so constructed that a plurality of arc extinguishing plates 501 are supported by frame plates 502. The operating mechanism 4 is well known in the art, and is described, for example, in US-A-3,599,130. As appears from this patent, the operating mechanism includes a reset mechanism. In the case where the movable-side contact 302 and the stationary-side contact 202 are contacting, current flows from a power supply side onto a load side along a path from the stationary rigid conductor 201, to the stationary-side contact 202, to the movable-side contact 302 and to the movable rigid conductor 301. When in this state an overcurrent, such as a short-circuit current, flows through the circuit, the operating mechanism 4 operates to separate the movable-side contact 302 from the stationary-side contact 202. At this time, an arc A appears across the gap between the stationary-side contact 202 and the movable-side contact 302, and an arc voltage develops thereacross. The arc voltage rises as the distance of separation of the movable-side contact 302 from the stationary-side contact 202 increases. Also, the arc A is drawn toward the arc extinguishing plate assembly by the magnetic force, and the length of the arc is stretched by the arc extinguishing plates 501, further raising the voltage. Thus the arc current reaches the current zero point to extinguish the arc A, so that the interruption is completed. During such interrupting operation, large quantities of energy are generated by the arc A across the gap between the movable-side contact 302 and the stationary-side contact 202 in a short period of time of the order of several milliseconds. In consequence, the temperature of the gas within the enclosure 1 rises abruptly, as does the pressure thereof, and the high temperature and pressure gas is emitted into the atmosphere through the exhaust port 101. A circuit breaker operates as explained above when breaking an overcurrent, but the performance capability expected of a circuit breaker in such operation is that the arc voltage be high, whereby the arc current flowing during the interruption operation is suppressed, and the magnitude of the current flowing through the circuit breaker is reduced. Accordingly, a circuit breaker which generates a high arc voltage offers a high level of protection to the electric equipment, including the electrical wiring disposed in series therewith. Heretofore, in circuit breakers of this type, separating the contacts at high speed or stretching the arc by means of magnetic force were used as means for attaining a high arc voltage, but in these cases, there was a certain limit to the rise in arc voltage, such that satisfactory results could not be achieved. Now, the behaviour of the arc voltage, etc., across the gap between the stationary-side and movable-side contacts 202 and 302 of the circuit breaker of figures 1a, 1b and 1c will be explained. In general, the arc resistance R (Ω) is given by the following expression: where: ρ: arc resistivity (Ω · cm) I: arc length (cm) S: arc sectional area (cm²) In general, in short arc A with a large current of at least several kA and an arc length / of at most 50 mm, the arc space is occupied by particles of metal from the rigid conductors on which the arc has its foot. Moreover, the emission of metal particles from the rigid conductors occurs orthogonally to the rigid conductor surfaces. At the time of the emission, the metal particles have a temperature close to the boiling point of the metal used in the rigid conductors, and whether they are injected into the arc space or not, they are injected with electrical energy, rising further in temperature and pressure, and taking on conductivity, and they flow away from the rigid conductors at high speed while expanding in a direction conforming with the pressure distribution in the arc space. The arc resistivity ρ and the arc sectional area S in the arc space are determined by the quantity of metal particles produced and the direction of emission thereof. Accordingly, the arc voltage is determined by the behaviour of such metal particles. This behaviour of the metal particles is explained in conjunction with figure 2. In figure 2, the stationary-side contact 202 and the movable-side contact 302 include surfaces X, the opposing surfaces of the contact surfaces when the respective contacts 202 and 302 are in contact, and surfaces Y, the electrically contacting surfaces of the contacts other than the surfaces X and a portion of the surfaces of the rigid conductor. A contour Z indicated by a dot-and-dash line in figure 2 is the envelope of the arc A struck across the gap between the contacts 202 and 302. Further, metal particles a, b and c are typically representative of the metal particles which are respectively emitted from the surfaces X and Y of the contactors 2 and 3, with the metal particles a coming from the vicinity of the centre of the surfaces X, the metal particles b coming from the surfaces Y, portions of the surfaces of the contacts and of the surfaces of the rigid conductors, and the metal particles c coming from the peripheral vicinity or region of the opposing X surfaces located between the points of origin of the metal particles a and b . The paths of the respective metal particles a, b and c subsequent to emission respectively extend along the flow lines shown by the arrows m, n and o . Such metal particles a, b and c emitted from the contactors 2 and 3 have their temperature raised from approximately 3,000°C, the boiling point of the metal of the contactors, to a temperature at which the metal particles take on conductivity, i.e., at least 8,000°C, or to the even higher temperature of approximately 20,000°C, and so energy is taken out of the arc space and the temperature of the arc space lowers, the result of which being to produce arc resistance. The quantity of energy taken from the arc space by the particles a, b and c increases with the rise in the temperature, and the degree of rise in temperature is determined by the positions and emission paths in the arc space of the metal particles a, b and c emitted from the contactors 2 and 3. However, in figure 3, the particles a emitted from the vicinity of the centre of the opposing surfaces X take a large quantity of energy from the arc space, but the particles b emitted from the surfaces Y on the contacts and rigid conductors, compared to the particles a, take little energy from the arc space, and further the particles c emitted from the peripheral portion of the opposing surfaces X take out only an intermediate amount of energy approximately midway between the amounts of energy taken by the particles a and b. That is to say, within the range in which the particles a flow, it is possible to take out large quantities of energy and to lower the temperature of the arc space, and hence to increase the arc resistivity ρ, but within the range in which the particles b and c flow, large quantities of energy are not taken out, and so the lowering of the temperature in the arc space is also small, and so no increase in the arc resistivity is achieved. Moreover, since the arc is produced from both the opposing surfaces X and the contactor surfaces Y, the cross-sectional area of the arc increases, and the arc resistance is consequently lowered. This energy outflow from the arc space due to the contact particles is proportional to the electrically injected energy, and so if the quantity of particles a produced between the contacts 202 and 302, injected into the arc space were increased, the temperature in the arc space would, of course, be greatly lowered, with the result that the arc resistivity could be increased, and the arc voltage greatly raised. A circuit breaker according to this invention breaks through the limits that existed with regard to the increase in arc voltage in conventional circuit breakers as hereinabove described, and by increasing the quantity of metal particles generated between the contacts and injected into the arc space, and by magnetically stretching the arc, it is possible to greatly raise the arc voltage. That is to say, in the embodiment of the present invention shown in figures 3a and 3b, a stationary contactor 2 and a movable contactor 3 respectively comprise a stationary rigid conductor 201 and a movable rigid conductor 301, to the respective ends of which are affixed a stationary-side contact 202 and a movable-side contact 302. The respective contactors 2 and 3 are disposed in mutual opposition such that the contacts 202 and 302 thereon can make or break a circuit. Further disposed on the respective rigid conductors 201 and 301 in a manner so as to surround the periphery of the contacts 202 and 302 are arc shields 6 and 7, respectively, formed of a high resistivity material of a resistivity higher than that of the rigid conductors 201 and 301. The high resistivity material of which the arc shields 6 and 7 are formed may, for example, be an organic or inorganic insulator, or a high resistivity metal such as copper-nickel, copper-manganin, manganin, iron-carbon, iron-nickel, or iron-chromium, etc. A blow-out coil 8 is connected at its one end to the stationary conductor 201, and at its other end to a portion 203 of the conductor insulated from the rigid conductor 201 by an insulator block 204. This blow-out coil 8 forms a single-winding coil that is disposed laterally of the area where the contacts open and close, and when a current flows, the blow-out coil 8 creates a magnetic flux that intersects the arc at right angles, the magnetic flux being wound in a direction that drives the arc in the direction of the arc extinguishing plate assembly 5 provided in the vicinity of the contacts. Further, the size of the blow-out coil 8 should be sufficient to encompass the stationary-side contact 202 and the movable-side contact 302 in both the open and closed circuit states, as viewed from the direction D in figure 3. The movable rigid conductor 301 is operated by the operating mechanism 4 to make or break contact with the stationary rigid conductor 201. The operation of the circuit breaker of the above-described construction is substantially the same as that of the earlier described prior device, so explanation thereof is omitted, but the behaviour of the metal particles between the contacts differs from that of the prior device, and so explanation thereof now follows. In figure 4, mutually opposing contacts 202 and 302 are respectively fixed to a stationary rigid conductor 201 and a movable rigid conductor 301 on which arc shields 6 and 7 are respectively provided so as to surround the periphery of the respective contacts and to oppose the arc space, as described above. In figure 4, X, a, c and n denote the same items as in figure 3, and the dot-and-dash line Z o indicates the envelope of the space of arc A contracted by the abovementioned arc shields, the arrow O o indicates the flow lines of the contact particles c that with the arc shields flow in a different path to that of the prior device, and the intersecting oblique lines (hatched areas) Q indicate the space in which the pressure generated by the arc A is reflected by the arc shields 6 and 7, raising the pressure which was lowered in the prior device without the arc shields 6 and 7. The metal particles between the contacts in the circuit breaker of this invention behave as follows. The pressure values in the space Q cannot exceed the pressure value of the space of the arc A itself, but much higher values are exhibited, at least in comparison with the values attained when the arc shields 6 and 7 are not provided. Accordingly, the relatively high pressure in the space Q produced by the arc shields 6 and 7 acts as a force to suppress the spread of the space of the arc A, and the arc A is confined to a small area. In other words, the flow lines of the contact particles a and c emitted from the opposing surfaces X are narrowed and confined to the arc space. Thus, the metal particles a and c emitted from the opposing surfaces X are effectively injected into the arc space with the result that a large quantity of effectively injected metal particles a and c take a quantity of energy out of the arc space of a magnitude that greatly exceeds that taken out in the prior art, thus markedly cooling the arc space and hence causing a marked increase in the arc resistivity ρ, i.e. the resistance R, substantially raising the arc voltage. However, as stated above, a blow-out coil 8 is provided together with the arc shields 6 and 7, and the magnetic flux produced by the blow-out coil 8 serves as a driving force acting on the arc A so the arc A, of which the resistance has become great as described above, further stretches the positive column, and is cooled by the arc extinguishing plates 501, and so the arc voltage across the contactors 2 and 3 is greatly raised. In the event of an excess current flowing in relation to the rated current of a circuit breaker, e.g. when an excess current of 5,000 A or more flows with respect to a rated current of 100 A, the arc extinguishing phenomenon as described with reference to figure 4 will take place, but with a relatively small overcurrent of for example 600 A or less with regard to a rated current of 100 A, such as may occur with normal use, it is the interruption performance at the current zero point, i.e. the restoration of the insulation of the arc space at the current zero point that becomes more of a problem than the current limiting performance of raising the arc voltage and suppressing the circuit current. This is for the following reason. The interruption current If is expressed by: If = V/Z wherein: V: Circuit Voltage Z: Circuit Impedance. However, with the aforementioned relatively small current, the circuit impedance is very much larger than the arc resistance, and there is virtually no current limiting due to the arc. Accordingly, the current zero point occurs at a time point determined by the circuit impedance. In these circumstances, if the circuit impedance is large and the inductance is great, the momentary value of the circuit voltage at the current zero point is high, and to render interruption possible, the insulation of the arc space with regard to the difference in voltage between the abovementioned circuit voltage and the arc voltage, must be restored. On the other hand, when breaking large currents, i.e. when the circuit impedance is small, current limiting by the arc is great, and even at the current zero point it varies greatly in accordance with the degree of current limiting reaching the zero point at the time when the arc insulation restoration power is sufficient; it is therefore possible to effect interruption following the lead of the arc insulation restoration power. As explained above, in some instances small current interruption can be much more demanding with regard to interruption performance than large current interruption. The arc space insulation restoration power is greatly affected by the cooling of the heat of the arc positive column. In order to achieve cooling with regard to the heat of the positive column, it has long been the practice, with regard to small currents, to absorb the heat directly by stretching the arc positive column and by means of a cooling member. Arc extinguishing plates are an example of such means, and are generally constructed of a magnetic material formed so as to easily draw and stretch the arc. The relationship between the abovementioned arc and the arc extinguishing plates is shown in figure 5, wherein an arc A exists with respect to the arc extinguishing plates 501, the current flows vertically on the paper in a direction from the front surface towards the rear surface. A magnetic field m is generated by the arc A, and the magnetic field in the periphery of the arc A is distorted by the effects of the arc extinguishing plates 501, the magnetic flux in the space rear the magnetic members becoming ragged, and the magnetic field is ultimately drawn by the electromagnetic force in the direction F in figure 5, i.e. the direction towards the arc extinguishing plates. In this way, the arc is stretched, heat is absorbed by the arc extinguishing plates 501, and the insulation restoration power of the positive column is made great. Another embodiment of the present invention is shown in figures 6a and 6b, this embodiment shifting the arc in the direction of the arc extinguishing plates to further increase the effectiveness of the abovementioned arc extinguishing plates. In this embodiment, the arc shields 6 and 7 are formed with slits 601 and 701, respectively, extending outwardly from the contacts 202 and 302. These slits 601 and 701 expose portions of the rigid conductors 201 and 301 in communication with the contacts 202 and 302. The slits 601 and 701 are open-ended in the direction of the arc extinguishing plates 501, so the arc A is led by these slits 601 and 701 in the direction of the arc extinguishing plates 501, thus even more effectively stretching the arc positive column. As the result of this, the arc positive column makes direct contact with the arc extinguishing plates 501, whereby a large quantity of heat is absorbed, adequately cooling the arc to enable raised insulation power with regard to small currents. Figures 7a and 7b illustrate another embodiment of the present invention wherein a permanent magnet is employed as the magnetic field generating means, and in so far as a magnetic field of a fixed directionally is generated, it is particularly suited to direct current (DC) circuit breakers. On the two sides of the arc extinguishing plates 501 are disposed a pair of magnetic flux plates 9, formed of a magnetic material, that flank the contacts 202 and 203. A permanent magnet 10 is suspended between the magnetic flux plates 9, the outer periphery of the permanent magnet 10 being covered by an insulating tube to protect the magnet 10 against burning by the arc. The magnetic poles of the permanent magnet 10 adjoin to the magnetic flux plates 9, and their polarity is disposed such that the vector sum of the magnetic flux between the magnetic flux plates 9 and the arc current across the gap between the contacts 202 and 302 coincides with the direction towards the arc extinguishing plate 501. The basic operation of the circuit breaker of the construction described above is substantially similar to that of prior devices, so description thereof is omitted. As stated above, the present embodiment is provided with magnetic flux plates 9 suspending a permanent magnet 10, assembled in such a manner that the vector sum of the magnetic flux between the magnetic flux plates 9 and the arc current coincides with the direction towards arc extinguishing plates 501. Thus the arc positive column is subject to a strong driving force driving it in the direction of the arc extinguishing plates 501. As a result, the arc, of which the resistivity has been made large by the arc shields 6 and 7, is further stretched, and is then transected and cooled by the arc extinguishing plates, and so the arc voltage across the contactors 2 and 3 is greatly raised. In this embodiment, the provision of slits 601 and 701 in the arc shields 6 and 7 respectively, does, of course, provide the same improvement with regard to interruption performance with relatively small currents, as described with respect to the embodiment illustrated in figures 6a and 6b. Figures 8a and 8b show yet another embodiment wherein a construction substantially similar to that of the embodiment illustrated in figures 6a and 6b is employed, with the addition a second contact 205 to form an excitation circuit for the blow-out coil 8. That is to say, in the present embodiment, a second contact 205 is disposed at the open end side of the slit 601 provided in the arc shield 6 on the stationary contactor 2, i.e. the arc extinguishing plates 501 side, and is fixed to the stationary rigid conductor 201 via an insulating plate 206. The blow-out coil 8 has one end joined to the second contact 205 and the other end joined to the stationary rigid conductor 201, and forms a coil of one winding on the outside of the side plate 502 of the arc extinguishing plate assembly 5. Accordingly, when a large excess current flows in the circuit breaker and the operating mechanism 4 operates to separate the movable-side contact 302 from the stationary-side contact 202, an arc is drawn, but as explained with regard to figure 4, the arc is confined by the arc shields 6 and 7, and the rise in the arc voltage creates a current limiting effect, and then due to the magnetic force of the arc current one portion of the arc travels along the slit 601 in the stationary-side arc shield 6, in the direction of the arc extinguishing plates 501, and when it reaches the second contact 205, the blow-out coil 8 is inserted into the current circuit. Thus, the blow-out coil 8 is excited, the arc A is stretched in the direction of the arc extinguishing plates 501, and is cooled and extinguished thereby. That is to say, in a circuit breaker according to this embodiment, a second contact 205 is provided in proximity to the arc extinguishing plates 501, and when the arc shifts to the contact 205 the blow-out coil 8 is excited, whereby the length of the arc is rapidly and greatly stretched in the direction of the arc extinguishing plates 501, and so the cooling and extinguishing effects of the arc extinguishing plates 501 can be effectively exploited. Further, the provision of the second contact 205 also has the effect of enabling wear of the stationary-side contact 202, the arc shield 6 and the portion of the stationary rigid conductor 201 exposed by the slit 601 to be substantially prevented.

Claims: 1. A circuit breaker provided with a pair of contactors (2, 3) each comprising a rigid conductor (201, 301) with a contact (202, 303) affixed thereto operating to make or break an electrical circuit, the conductor (201) being a stationary conductor, said breaker comprising magnetic driving means for generating a magnetic field influencing the formation of an arc drawn across the contacts of said contactors and an assembly (5) of arc extinguishing plates (501) for extinguishing said arc, characterized by the combination of the following features the two contacts (202, 302) are surrounded by arc shields (6, 7) having a resistivity greater than that of the conductors (201, 301), thereby stabilizing and positioning the feet of the arc (A) during the switching operation, the magnetic driving means (8) are positioned in such a way, that the magnetic force generated by them bends and stretches the middle portion of the arc (A) towards the extinguishing plates (501) of the extinguishing plate assembly (5), wherein the magnetic driving means are formed by a single loop coil (8) placed on the outside of one of the frame plates (502) of the extinguishing plate assembly (5) and having ends which are connected to the stationary conductor (201, 203) being interrupted by an insulator block (204), (Fig. 3a, b). 2. A circuit breaker provided with a pair of contactors (2, 3) each comprising a rigid conductor (201, 301) with a contact (202, 303) affixed thereto operating to make or break an electrical circuit, said breaker comprising magnetic driving means for generating a magnetic field influencing the formation of an arc drawn across the contacts of said contactors and arc extinguishing plates (501) for extinguishing said arc, characterized by the combination of the following features the two contacts (202, 302) are surrounded by arc shields (6, 7) having a resistivity greater than that of the conductors (201, 301) thereby stabilizing and positioning the feet of the arc (A) during the switching operation, the magnetic driving means (9) are positioned in such a way, that the magnetic force generated by them bends and stretches the middle portion of the arc (A) towards the extinguishing plates (501) of the extinguishing plate assembly (5), wherein the magnetic driving means (9) are formed by a permanent magnet (10), both ends of which are connected to magnetic flux plates (9), which are attached to the outside of the two frame plates (502) of the extinguishing plate assembly (5), (Fig. 7a, b). 3. A circuit breaker provided with a pair of contactors (2, 3) each comprising a rigid conductor (201, 301) with a contact (202, 303) affixed thereto operating to make or break an electrical circuit, said breaker comprising magnetic driving means for generating a magnetic field influencing the formation of an arc drawn across the contacts of said contactors and arc extinguishing plates (501) for extinguishing said arc, characterized by the combination of the following features the two contacts (202, 302) are surrounded by arc shields (6, 7) having a resistivity greater than that of the conductors (201, 301) thereby stabilizing and positioning the feet of the arc (A) during the switching operation, the magnetic driving means (8) are positioned in such a way, that the magnetic force generated by them bends and stretches the middle portion of the arc (A) towards the extinguishing plates (501) of the extinguishing plate assembly (5) wherein the magnetic driving means are formed by a single loop coil (8) placed on the outside of one of the frame plates (502) of the extinguishing plate assembly (5) and having ends which are connected to the stationary conductor (201) and an auxiliary contact (205) being attached to the stationary conductor (201) by means of an insulator plate (206), the arc shield (6) surrounding the main contact (201) of the stationary contact (202) being provided with a slit (601) leading to the auxiliary contact (205), (Fig. 9a, b).

Inventors: HISATSUNE, FUMIYUKI, TERACHI, JUNICHI, WADA, YUUICHI, YAMAGATA, SHINJI, YAMAMOTO, KIYOMI, YOSHIYASU, HAJIMU
Applicants: MITSUBISHI DENKI KABUSHIKI KAISHA
Application year: 1982
Main classification: H01H9
IPC codes: H01H9