CIRCUIT BREAKER

Abstract: A circuit breaker in which arc shielding members (14, 15) are provided for predetermined contacts (4, 11; 3, 8) among a plurality of contact pairs arranged in parallel, so that the arc will take place between predetermined contacts when the contacts (4, 11; 3,8) are opened. The arc shielding members (14, 15) are made of a material having resistivity greater than that of the conductors (10, 2) to which the contacts (4, 11; 3, 8) are attached. The arc shielding members (14, 15) work to effectively inject metallic particles of contact material into the arc, so that the arcing voltage is rapidly raised and so that the feet of the arc will not spread to the conductors (10, 2) in the vicinities of the contacts (4, 11; 3, 8).

Description: The present invention relates to a circuit breaker and more specifically to a novel circuit breaker comprising current carrying contacts and a pair of arcing contacts in which arc shielding members are selectively provided for the arcing contacts, and the arcing voltage established across the contacts is quickly raised by the arc shielding members, in order to effectively extinguish the arc. The DE-A-2 218 420 shows a circuit breaker with a fixed conductor and a movable contact provided with pairs of main or current carrying contacts and a pair of arcing contacts. US-A-3 402 273 further discloses a circuit breaker in which the peripheries of the current carrying contacts are surrounded by fibre insulator sheets. This circuit breaker, however, relates to three separate current phases and each phase is broken by one pair of contacts only, which actually means, that there are no separate main and arcing contacts. In view of this prior art it is the object of the invention to provide a circuit breaker with enhanced breaking performance. With a circuit breaker consisting of a fixed conductor and a movable conductor being provided with pairs of current carrying contacts and a pair of arcing contacts, which in use, lag on opening behind the opening of said pairs of current carrying contacts, this object can be obtained in that in addition there are provided arc shielding members being made out of a material having a resistivity higher than that of the conductors, these arc shielding members being attached to the conductors so as to surround the peripheries of only the pair of arcing contacts. The provision of arc shielding members surrounding the two opposing arcing contacts has the particular advantage that the two feet of the arc forming between the arcing contacts during the process of opening the circuit breaker are held in a well defined area, while in addition the additional weight due to the arc shield member surrounding the movable arcing contact can be kept low, so that the opening sped of the circuit breaker is not affected to a notable degree. Preferred ways of carrying out the invention are described below with reference to the drawings, in which: Fig. 1a is a sectional plan view of a general circuit breaker to which the present invention can be applied; Fig. 1b is a sectional side view of the circuit breaker along line b-b of Fig. 1a; Fig. 2 is a schematic diagram illustrating the behaviour of an arc established across the contacts of the circuit breaker of Fig. 1a; Fig. 3a is a sectional plan view of a circuit breaker according to an embodiment of the present invention; Fig. 3b is a sectional side view of the circuit breaker along line b-b of Fig. 3a; Fig. 4a is a perspective view of an arc shielding member which is used for a movable arcing contact of the embodiment of Fig. 3a; Fig. 4b is a perspective view of an arc shielding member which is used for a fixed arcing contact of the embodiment of Fig. 3a; Fig. 5 is a schematic diagram illustrating the function of an arc shielding member employed for the circuit breaker of the present invention; Fig. 6 is a plan view illustrating the general function of the arc extinguishing board or plate; Fig. 7 is a sectional plan view of a circuit breaker according to another embodiment of the present invention; Fig. 8 is a perspective view of the arc shielding member used for the embodiment of Fig. 7; In the drawings, the same reference numerals denote identical or corresponding portions. A general circuit breaker to which the present invention can be adapted will be described below with reference to Figs. 1a and 1b. The circuit breaker comprises an enclosure 1 made of an insulating material, a fixed conductor 2 of which the one end is connected to the power-supply side and which penetrates through a lower portion of the enclosure 1, a pair of fixed main contacts 3 attached to the upper surface of the fixed conductor 2, and a fixed arcing contact 4 which is located midway between the fixed main contacts 3 on the upper surface of the fixed conductor 2. The fixed conductor 2 and contacts 3, 4 constitute a fixed contactor 5. A pair of movable main conductors 6 are attached to an operation mechanism 7 to be actuated thereby. Movable main contacts 8 are attached to lower free ends of the movable main conductors 6. The movable main conductors 6 and the movable main contacts 8 constitute movable main contactors 9a which are opposed to the fixed contactor 5, thereby to constitute two contactor pairs 9a, 5 for carrying current. There is further provided a movable arcing conductor 10 which is located between the two movable main conductors 6, and which is fastened to the operation mechanism 7. The movable arcing conductor 10 is also actuated by the operation mechanism 7. A movable arcing contact 11 is attached to the free lower surface of the movable arcing conductor 10. The movable arcing conductor 10 and the movable arcing contact 11 constitute a movable arcing contactor 9b which is opposed to the fixed arcing contact 4, thereby to constitute an arcing contact pair 4, 11 for treating the arcing that develops when the contacts are opened. There are further provided arc extinguishing boards or plates 12 for quenching the arc that is developed between the movable arcing contact 11 and the fixed arcing contact 4 when the movable arcing contact 11 is opened, and an outlet port 13 through which the arc or hot gas produced in the enclosure 1 will escape. In the thus constructed circuit breaker, if now the movable main contacts 8 and the fixed main contacts 3 are in contact, i.e., if the main contact pairs for carrying current are closed, the electric power is supplied from the power supply side to the load side via the fixed conductor 2, fixed main contacts 3, movable main contacts 8, and movable main conductors 6. Under this condition, if a heavy current such as short-circuit current flows through the closed circuit, the operation mechanism 7 works to turn the movable main conductors 6 and the movable arcing conductor 10 with their ends as fulcrums, whereby the movable main contacts 8 and the movable arcing contact 11 are separated from the fixed main contacts 3 and the fixed arcing contact 4. In this case, the circuit breaker has been constructed so that the pair of arcing contacts 4, 11 are opened while lagging behind the pairs of the main contacts 3, 8. Therefore, the arc A develops between the fixed arcing contact 4 and the movable arcing contact 11 only, and an arcing voltage is generated between the fixed arcing contact 4 and the movable arcing contact 11. The arcing voltage increases depending upon the distance by which the movable arcing contact 11 is separated from the fixed arcing contact 4. At the same time, the arc A is attracted by the magnetic force toward the arc extinguishing boards 12. Consequently, the arcing voltage is further raised. The arc A is extinguished at a moment when the arc current reaches a zero point; then, the breaking is finished. During the operation of breaking, a large amount of energy is generated between the movable arcing contact 11 and the fixed arcing contact 4 by the arc 8 within short periods of time, i.e., within several milliseconds. Accordingly, the temperature of gas in the enclosure 1 rises, and the pressure abruptly increases. The gas of high temperature and high pressure, however, is released into the open air through the outlet port 13. The circuit breaker which performs the breaking operation as mentioned above, should have a high arcing voltage. That is, high arcing voltage restrains the arc current that flows during the breaking operation, and reduces the current that flows through the circuit breaker. Therefore, the circuit breaker which generates a high arcing voltage has high performance for protecting various electric machines and equipment inclusive of wiring with which the circuit breaker is connected in series. In the circuits which include a plurality of circuit breakers connected in series, furthermore, the region of selective or cooperative breaking or the region of simultaneous breaking can be expanded. In the conventional circuit breakers of this type, therefore, the movable main contactors 9a and the movable arcing contactor 9b are operated to separate the contact pairs at high speeds in order to realize a high arcing voltage, or the arc A is stretched by utilizing the magnetic force of the arc extinguishing boards. However, limitation is imposed on the arcing voltage, and satisfactory performance for limiting the current is not obtained. Here, the arcing voltage across the fixed contact and the movable contact will be explained below prior to illustrating the circuit breaker of the present invention. In general, the arc resistance has the following relation: R = ρ I S where R denotes the arc resistance (Ω), ρ denotes arc resistivity (Ω · cm), / denotes the arc length (cm), and S denotes the sectional area of the arc (cm²). In the arc of a current of several kA and of a length of shorter than 50 mm, however, the arcing space is occupied by the particles of contact material emitted from the contacts. The particles of contact material are emitted in a direction at right angles with the surface of contacts. Further, the particles when emitted are heated to nearly the boiling point of the contact material. Moreover, as soon as they are injected into the arcing space, the particles receive electrical energy, are placed in the high-temperature and high-pressure conditions, become electrically conductive, and flow (fly) away from the contact of high speed while being expanded in accordance with the pressure distribution in the arcing space. Thus, the arc resistivity ρ and the sectional area S of the arc in the arcing space are determined by the quantity of particles to contact material and by the direction of emission. Therefore, the arcing voltage is also determined by the behaviour of particles of contact material. The behaviour of particles of electrode material will be explained below with reference to a conventional circuit breaker shown in Fig. 2. As mentioned above, the arc A in the circuit breaker of Figs. 1a and 1b occurs between the fixed arcing contact 4 and the movable arcing contact 11 only. Therefore, Fig. 2 illustrates the pair of arcing contacts only, with the same reference numerals as those of Figs. 1a and 1b denoting the same portions. A denotes the arc, planes X denote opposing surfaces on which the contacts 4 and 11 will come into contact with each other, and planes Y denote portions of contact surfaces and conductor surfaces which establish electrically contacting surfaces in addition to the opposing surfaces X. Further, dot-dash chain lines Z1 denote contours of arc A, and symbols a, b and c schematically represent particles of contact material emitted from the contacts 4, 11, wherein a denotes particles emitted from the central portions of the opposing surfaces X, b denotes particles of contact material emitted from the surfaces Y, and c denotes particles of contact material emitted from the periphery of the opposing surfaces X midway between the regions from where the particles a and b were emitted. After emitted, the particles flow (fly) as indicated by arrows m, n and O1. Particles a, b and c of contact material emitted from the contacts 4 and 11 are heated to the boiling point of the contact material, i.e., heated to about 3,000°C and up to a temperature at which they become electrically conductive, i.e., to 8,000°C, or further up to about 20,000°C. Consequently, the particles absorb the energy from the arcing space; i.e., temperature in the arcing space decreases, and arc resistance increases. Here, the amount of energy which the particles a, b and c absorb from the arcing space is determined by the positions and paths of emission of the particles a, b and c that are emitted from the contacts 4 and 11, and the degree of temperature rise is determined by the amount of energy absorbed. In the conventional circuit breaker as will be obvious from Fig. 2, therefore, the particles a of contact material emitted from the central portions of the opposing surfaces X absorb large amounts of energy from the arcing space. However, the particles b emitted from portions Y of the contact surfaces and the conductor surfaces absorb the energy from the arcing space in amounts less than the amounts absorbed by the particles a . Further, the particles c emitted from the periphery of the opposing surfaces X absorb the energy in amounts midway between those absorbed by the particles a and b . In other words, large amounts of energy are absorbed in a region where the particles a flow, and the temperature in the arcing space is decreases and, hence, the arc resistivity ρ is increased. In the regions where particles b and c flow, however, the energy is not absorbed in large amounts. Therefore, the tempertaure in the arcing space is decreased less, and the arc resistivity ρ increases little. Moreover, since the arc A develops from the opposing surfaces X and from the contact surfaces Y, the sectional area of the arc increases, and the arc resistance decreases. The flow of energy from the arcing space by the particles a, b and c of contact material corresponds to the electrical energy injected into the arcing space. Therefore, if the particles b and c of contact material are injected in increased amounts into the arcing space, the temperature in the arcing space can inevitably be reduced greatly, whereby the arc resistivity ρ can be increased to greatly increase the arcing voltage. In consideration of the above-mentioned events, the present invention contemplates to provide a circuit breaker having good currentlimiting performance, by permitting particles of contact material generated across the contacts to be injected into the arcing space in increased amounts, so that the arcing voltage is strikingly increased. Figs. 3a and 3b illustrate an embodiment of the present invention, in which the portions corresponding to those of Figs. 1a and 1b are denoted by the same reference numerals. In the embodiment of the present invention, the pair of arcing contacts 4 and 11 are provided with arc shielding members 14 and 15 which are composed of flat plates having fitting holes 16, 17 that fit to the contacts 4, 11, as shown in Figs. 4a and 4b. The arc shielding members 14, 15 are placed on the conductors 10, 2 so as to surround the peripheries of the contacts 4, 11. The arc shielding members are made of a material having resistivity greater than that of the conductors 10, 2. Examples of the high-resistance material include organic or inorganic electrical insulating materials, ceramics, nichrome, nickel, iron, copper-nickel, copper-manganese, coppermanganin, iron-carbon, iron-nickel and iron-chromium. The arc shielding members 14, 15 in the form of plates can be fastened to the corresponding conductors 2, 10. Alternatively, the arc shielding members can be formed by coating the fixed conductor 2 and the movable arcing conductor 10 with a high-resistance material, such as ceramic material, by the plasma-jet melt injection, so as to cover the periphery of the fixed arcing contact 4 and the movable arcing contact 11. The latter method makes it possible to cheaply and easily form the arc shielding members. In particular, the weight is not increased and the moment of inertia remains small on the side of the movable arcing contactor 9b. Therefore, the movable arcing contactor 9b can be opened at high speeds to obtain increased arcing voltage. In the embodiment of the present invention, the arc shielding members are formed in the shape of plates in order to squeeze the arc, as will be mentioned later. Operation of the above embodiment will be explained below with reference to Fig. 5, in which the same reference numerals as those of Figs. 1 to 4b denote the corresponding portions; Z2 denotes the contours of the arc A which is compressed by the arc shielding members 14, 15; O2 denotes the flow of particles c of contact material along paths different from those of the conventional circuit breaker owing to the provision of the arc shielding members 14, 15; and the hatched areas Q denote the space where the pressure is increased as compared to that of the conventional circuit breaker without arc shielding members, since the pressure produced by the arc A is reflected by the arc shielding members 14, 15. The particles of contact material between the contacts behave as mentioned below. That is, the pressure in space Q never becomes greater than the pressure in the arcing space, but is very high compared with a structure without the arc shielding members 14, 15. Therefore, a considerably high pressure established in space Q by the arc shielding members 14, 15 works to restrain the spread of arcing space and to confine it to a narrow region. This means that the flow paths m and n of particles a, c emitted from the opposing surfaces X are confined to the arcing space. Therefore, the particles of contact material emitted from the opposing surfaces X are effectively injected into the arcing space, whereby large amounts of particles effectively injected into the arcing space absorb the energy in amounts very greater than that absorbed in the conventional breaker. Therefore, the arcing space is markedly quenched, the arc resistivity ρ, i.e., the arc resistance R, is remarkably increased, the arcing voltage is strikingly increased, and very good current-limiting performance is obtained. The arcing phenomenon in the circuit breaker has been explained already with reference to Fig. 5, in which an excess of current flows relative to the rated current of the breaker, i.e., an excess of current greater than, for example, 5000 A flows through the circuit breaker having a rated current of, for example, 100 A. However, when a current of smaller than 600 A flows through the circuit breaker having a rated current of 100 A, the breaking performance at a point of current zero becomes a problem, i.e., the insulation recovery force in the arcing space at a point of current zero becomes a problem rather than the current-limiting performance which restrains the circuit current by increasing the arcing voltage. This results from the following reasons. The breaking current If is given by a relation, If = V/Z where If: breaking current V: circuit voltage Z: circuit impedance When a small current is flowing, however, it means that the circuit impedance is considerably greater than the arc resistance, and the current is limited very little by the arc. Therefore, a point of current zero takes place at a moment which is determined by the impedance of the circuit. If under such a condition the circuit has a large impedance and a large inductance, the circuit has a high instantaneous value of voltage at the point of current zero. To break the circuit, therefore, insulation in the arcing space must be recovered for a voltage differential between the circuit voltage and the arcing voltage. When the circuit is to be broken by a heavy current, i.e., when the circuit has a small impedance, the current is greatly limited by the arc, the point of current zero changes greatly depending upon the degree of current limitation, the point of current zero is reached when the insulation by the arc is recovered sufficiently, and the circuit is broken predominantly by the recovered insulation by the arc. As illustrated in the foregoing, the breaking of small currents often requires more severe breaking performance than the breaking of heavy currents. The force of insulation recovery in space is greatly affected by the quenching of heat in the positive column of arc. To effectively quench the heat in the positive column, the positive column of arc is stretched for small currents, and the heat is directly absorbed by the cooling member. The arc extinguishing board (plate) 12 mentioned earlier serves as means to fulfill this purpose. The arc extinguishing board 12 is usually made of a magnetic material in such a shape as to attract and stretch the arc. Fig. 6 illustrates a relation between the arc and the arc extinguishing board, wherein the arc A occurs relative to the arc extinguishing board 12, and the current flows in a direction perpendicular to the surface of the paper from the front surface to the back surface of the paper. The magnetic field established by the arc A is indicated by symbol m . In this setup, the magnetic field around the arc is distorted as it is affected by the arc extinguishing board 12 made of magnetic material; the magnetic flux in the space close to the arc extinguishing board 12 becomes extremely low. Owing to the electromagnetic force, therefore, the arc is drawn toward the direction indicated by F, i.e., toward the direction attracted by the arc extinguishing board. Thus, the arc A is stretched, and the heat is obsorbed by the magnetic member, and the insulation in the positive column recovers more quickly. Figs. 7 and 8 illustrate a further embodiment, in which the feet of arc are moved from the contacts toward the arc extinguishing board so that it will exhibit the effect more conspicuously. The arc shielding members 14, 15 according to this embodiment have arc guiding paths 18, 19 consisting of grooves. The arc guiding paths 18, 19 extend away from the contacts 4, 11, i.e., toward the arc extinguishing board 12 in Fig. 7. The conductors 2, 10 are exposed to the bottom portions of the arc guiding paths 18, 19; i.e., the arc guiding paths 18, 19 have electric conductivity greater than the arc shielding members 14, 15. The circuit breaker of this embodiment operates in the same manner as that of Figs. 1a and 1b, and this operation is therefore not explained in detail. In this embodiment, however, since the arc extinguishing board 12 composed of a magnetic material is located near the port 13 for releasing the arc, and since the arc shielding members 14, 15 are provided with arc guiding paths 18, 19, the arc moves toward the outlet port 13, and the positive column of arc stretches greatly as compared with the conventional device. Consequently, the positive column comes into direct contact with the arc extinguishing board 12, whereby the heat is absorbed in large amounts. Therefore, the insulation recovers quickly at a point of current zero, and the circuit breaker exhibits a breaking performance which is very superior to the circuit-breaking performance of the conventional circuit breaker.

Claims: 1.Circuit breaker consisting of a fixed conductor (2) and a movable conductor (6, 10) being provided with pairs of current carrying contacts (3, 8) and a pair of arcing contacts (4, 11), which in use, lag on opening behind the opening of said pairs of current carrying contacts (3, 8), characterized in that in addition there are provided arc shielding members (14, 15) being made out of a material having a resistivity higher than that of the conductors (2, 6, 10), these arc shielding members (14, 15) being attached to the conductors (2, 10) so as to surround the peripheries of only the pair of arcing contacts (4, 11).

Inventors: HISATSUNE, FUMIYUKI, TERACHI, JUNICHI, YAMAGATA, SHINJI, YAMAMOTO, KIYOMI, YOSHIYASU, HAJIMU
Applicants: MITSUBISHI DENKI KABUSHIKI KAISHA
Application year: 1982
Main classification: H01H73
IPC codes: H01H1, H01H9