Vacuum circuit interrupter

The present invention relates to a circuit interrupter of the vacuum type, and more particularly, to a noise free vacuum circuit interrupter which eliminates the noise generated by the current therethrough.
Power vacuum switches have, in general, found extensive application in switching power lines in power substations and also in large scale power equipment. A conventional power vacuum switch comprises, as will later be described with reference to the drawing, fixed and movable electrodes which are disposed in substantial alignment with each other, and the latter is moved toward or away from the former for respectively making closing and opening the switch contacts. In such a conventional construction, when the switch is closed, an alternating current flows through the power switch and thereby noise is generated by the alternating magnetic field generated by the alternating current.
Recently with growth in population of concurbation and the increase of building density the need for electric power has rapidly increased. However it is always very difficult to eliminate the noise of a vacuum power interrupter. Accordingly, efforts have been directed to reduce the noise generated.
Referring first to FIG. 1, there is shown a conventional vacuum type circuit interrupter. In FIG. 1, reference numeral 10 shows a highly evacuated envelope. Reference numeral 12 denotes a tubular insulating housing, and reference numerals 14 and 16 are a pair of metallic end caps. Reference numerals 18 and 20 illustrates metallic tubes, and 22, 24 are insulating tubes. Moreover, reference numerals 26 and 28 are metallic tubes for connecting the insulating tubes 22 and 24. Reference 20 shows a stationary contact fastened to a stationary supporting rod 34, and reference numeral 32 is a movable contact secured to a movable rod 36.
In the conventional vacuum circuit interrupter shown in FIG. 1, each of shields 42, 44 and 46 and a disc 48 is, generally, made of a nonmagnetic material such as an austetinic stainless steel. On the other hand, each of the central metallic tubes 26 and 28 is made of a ferromagnetic material such as Fe-Ni-Co alloy or Fe-Co alloy because it is preferable to use a metal of which the coefficient of thermal expansion is equal approximately to that of the insulating tubes 22 and 24. The magnetodistortion is generated by the alternating current magnetic field caused by the alternating current which flows between the stationary contact 30 and the movable contact 32, because the tubes 26 and 28 are made of a ferromagnetic material. Under these conditions, an important problem encountered is that the metallic tubes 18, 20, 26 and 28 generate mechanical noise which is caused by the vibration of the metallic tubes, particularly when the alternating current in the order of 200 to 300 amperes flows through the vacuum circuit interrupter.
In more detail, the metallic tubes 18, 20, 26 and 28 forms a magnetic circuit when the alternating magnetic flux is induced by the alternating current flowing through the supporting rod 34 and the operating rod 36. The magnetic field intensity H or the magnetizing force F due to the current supplied thereto is represented by
H=I/2.pi.r(AT/m)
where I is the supplied current and r is the distance from the current path to the metallic tubes 18, 20, 26 and 28 which corresponds to a radius of the metallic tubes.
As will be soon from equation (1), the alternating magnetic field intensity in each metallic tube is about 6400 AT/m, when the supplied current I is 300 A, and the radius r of the metallic tube was is 0.075 m. Magnetodistortion appears in the ferromagnetic metallic portions such as the metallic tubes 18, 20, 26 and 28 due to the alternating magnet field H which is induced therein by the alternating current. From the induction of the magnetodistortion, the metallic tubes are vibrated by the expanding and contradiction thereof and, as a result, the noise is generated. In this case, the noise level was 70 dB at a point P shwn in FIG. 1 when the current frequency was 50 Hz. The measurement was carried out by the A-characteristic of a compromise noise meter, and the background noise was 44 dB. Moreover, the background noise was 69 to 72 dB under the same measuring condition as that of the above case, when the radius of the metallic tubes was 0.08 m. Accordingly, reduction of the noise generated from the vacuum circuit interrupter is extremely desirable, particularly when the interrupter is used in a crowded urban environment.
It is, accordingly, an object of the present invention to provide an improved vacuum circuit interrupter which over comes the above described drawbacks, namely, a vacuum circuit interrupter which eliminates the noise generated by current which flows therethrough.
More specifically, an object of the present invention is to provide a vacuum circuit interrupter which can avoid the generation of the vibrating noise due to the alternating magnetic field generated by current which flows through the circuit interrupter.

BRIEF DESCRIPTION OF THE DRAWINGS
Additional objects and advantages will become apparent upon consideration of the following description when taken in conjunction with the accompanying drawings. In the accompanying drawings like parts in each of the several figures are identified by the same reference character, and:
FIG. 1 is an elevation sectional view of the conventional vacuum circuit interrupter.
FIG. 2 is a fragmentally sectional elevation view of the vacuum circuit interrupter.
FIG. 3 is a cross-sectional view taken along line III--III of FIG. 2.
FIG. 4 is a graph showing a characteristic of an alloy of Fe-Ni-Co.
FIG. 5 is a graph showing a histerises loop of a ferromagnetic material.
FIG. 6 is a fragmental sectioned view of a modification of the interrupter of FIG. 3.
FIG. 7 is a fragmental sectioned view of a further modification of the interrupter of FIG. 3.
FIG. 8 is a fragmental sectioned view showing other embodiment of the present invention.
FIG. 9 is a fragmentary sectional view illustrating further embodiment of the present invention.
FIG. 10 show a fragmental view of further embodiment of the vacuum circuit breaker in accordance with the present invention.
FIG. 11 is a fragmental view of a modification of the vacuum circuit breaker of FIG. 10.
FIG. 12 is a fragmental view of the vacuum circuit interrupter of other embodiment of the present invention.
FIG. 13 is a fragmental sectioned view of the vacuum circuit breaker in accordance with further embodiment of the present invention.
FIG. 14 is a cross-sectional view of the vacuum circuit interrupter in accordance with the present invention.
FIG. 15 is a cross-sectioned view of a modification of the vacuum circuit interrupter of FIG. 14.
FIG. 16 is a cross-sectioned view of a modification of the vacuum circuit interrupter of FIG. 15.
FIG. 17 is a fragmental sectioned view of other modification of the vacuum circuit interrupter of the present invention.
FIG. 18 is a cross-sectioned view of the vacuum circuit interrupter of further modification of FIG. 16.
FIG. 19 is a fragmental sectioned view of the vacuum circuit interrupter in accordance with further embodiment of the present invention.
FIG. 20 is an elevational perspective view of a modification of a magnetic flux generating member and,
FIG. 21 is an elevational perspective view of further modification of a magnetic flux generating member.

Referring to the drawings, particularly to FIGS. 2 and 3, there is shown a vacuum circuit interrupter embodying the present invention. This vacuum circuit interrupter comprises a highly evacuated envelope 50. This envelope 50 comprises a tubular insulating housing 12 and a pair of metallic end caps 14 and 16 located at opposite ends of the insulating housing 12. The end caps 14 and 16 are jointed to the insulating housing 12 by vacuum tight seals in the form of metallic tubes 18 and 20.
The insulating housing 12 comprises two short tubular sections 22 and 24, each of a suitable glass or ceramic. It should be noted that the number of the sections is not restricted to two; other embodiments of the present invention may have a different number. These tubular insulating sections are disposed collinearly and are jointed together by metallic glass-to-metal seals between the insulating sections.
Disposed within the envelope 50 are two contacts movable relative to each other, shown in their fully contacted position. The upper contact 30 is a stationary contact, and the lower contact 32 is a movable contact. The stationary contact 30 is suitably brazed to the lower end of a conductive supporting rod 34, which is integrally jointed at its upper end to the metallic end plate 14. The movable contact 32 is suitably brazed to the upper end of a conductive operating rod 36, which is vertically movable to effect opening and closing of the interrupter.
For permitting vertical motion of the operating rod 36 without impairing the vacuum inside the envelope 50, a suitable bellows 38 is provided around the operating rod 36. A cup-shaped shield 40 surrounds the bellows 38 and protects it from being bombarded by arcing products.
The interrupter can be operated by driving the movable contact 32 upward and downward to close and open the power line. When the contacts are engaged, current can flow between opposite ends of the interrupter via the path 36, 32, 30 and 34.
Circuit interruption is effected by driving the contact 32 downward from the closed contacts position by suitable operating means (not shown). This downward motion establishes an arc between the contacts. Assuming an alternating current circuit, this arc persists until about the time a natural current zero is reached, at which time it vanishes and is thereafter prevented from reigniting by the high dielectric strength of the vacuum. A typical arc is formed during the circuit interrupting operation. For protecting the insulating housing 50 from the metallic vapors, a series of shield 42, 44 and 46 are provided. The main shield 42 is supported on the tubular insulating housing by means of an annular metallic disc 48. This disc 48 is suitably jointed at its outer periphery to the central metallic tubes 26 and 28 and at its inner periphery to shield 42. The shields 18 and 20, which are of metal, cooperate with the metallic end plates 14 and 16.
In the vacuum circuit interrupter as constructed above, each of the shields 42, 44 and 46 and the disc are, generally, made of a non-magnetic material such as an austenitic stainless steel. On the other hand, each of the metallic tubes 18, 20, 26 and 28 is a ferromagnetic material such as an Fe-Ni-Co alloy or Fe-Co alloy, because it is preferable to use a metal of which the coefficient of thermal expansion is equal to that of the insulating tubes 22 and 24.
An important feature of the invention is that, as is shown in FIG. 2, a magnet field means 52 is provided on each of the metallic tubes 18, 20, 26 and 28 in order to apply a magnetic field to metallic tube. The magnetic field applying means 52 comprises a magnetic flux generating member 56 for generating a magnetic flux to be applied to the metallic tubes, and a mounting means 54 for mounting the magnetic flux generating member 56 to the envelope 50.
As is best shown in FIG. 3, four sets of magnetic field applying means 52 are circumferentially arranged on the peripheral surfaces of metallic tubes 18, 20, 26 and 28. Each of the magnetic field applying means 52 comprises a magnetic flux generating member 56 consisting of a permanent magnet 58 for generating the matnetic flux to be applied to the ferromagnetic portion of the housing 12, a mounting member 54 including a pair of yokes 54a and 54b which are of curved shape.
The yokes 54a and 54b are made of a high magnetic permeability material such as silicon steel, pure iron, or a permalloy. Each base portion of the yokes 54a and 54b is secured to the outer peripheral surface of the metallic tube 26 by a suitable adhesive. The permanent magnet 58 is a conventional permanent magnet which is made of a hard magnetic material such as rare earth-cobalt, platinum-cobalt, a ferlite or an alnico. The permanent magnet 48 is secured between end portions of the opposite yokes 54a and 54b by suitable adhesive agent.
In this embodiment, the permanent magnet 58, is a cuboid 14 mm.times.15 mm.times.15 mm, and has magnetic flux density of the order of 0.91-0.98 Wb.m.sup.-2 which corresponds to 9100-9800 G, and coercivity .sub.I H.sub.C of 5.01.times.10.sup.5 -5.81.times.10.sup.5 Am-1 (6300-7300 G). Naturally, the coercivity .sub.I H.sub.C is sufficiently large that the permanent magnet 58 is not demagnetized by the alternating magnet field of intensity Hp=I/2.pi.r exerted on the metallic tubes 18, 20, 26 and 28 by a normal current flow I (e.g. 3000 A), when the magnetic polarization is zero. Moreover, the permanent magnet 58 is provided with a sufficient coercivity .sub.I H.sub.C not to be demagnetized even by the magnetic field generated by an overcurrent an order of magnitude larger (commonly, for example 10-80 KA). As is shown in FIG. 3, four magnets 58 are circularly arranged with like poles adjacent. Under these conditions, magnetic paths are formed in closed loops each of which consists of a yoke 54a, a portion of the metallic tube, a yoke 54b and the permanent magnet 58. Lines of magnetic flux lie along the magnetic path, and thereby the magnetic field is constantly applied from the permanent magnets 58 to the metallic tubes 18, 20, 26 and 28. The magnetic field intensity of the permanent magnets 58 is set such that the magnetic field in the metallic tubes is the saturation state or approximately the saturation state and such that substantially no magnetodistortion is coused influenced by the alternating magnetic flux supplied to the metallic tubes when the normal alternating current flows through the interrupter.
FIG. 4 shows a characteristic of a magnetic substance which is made of Fe-Ni-Co alloy. It is generally known that the relative distortion .lambda.(=.DELTA.1/1) increases and finally saturates in accordance with the increment of the magnetic field intensity H .phi.rsted, as is shown by a curve l.sub.1 of FIG. 4. Here l is the length of the magnetic substance. It is also known that magnetization of the magnetic material is saturated when the magnetic field intensity H is more than 50 .phi. (.phi.rsted). The magnetic material expands and shrinks at right angles to the direction of the magnetic field H to absord the variation in the length l. In addition, it is known that apparent magnetic reluctance R becomes large, that is, the magnetic permiability .mu.s becomes approximately equal to that of air (.mu.s=1) when the magnetic flux in a magnetic circuit reaches the saturation state or approximately the saturation state.
According to the vacuum circuit interrupter shown in FIGS. 2 and 3, the metallic tubes 18, 20, 26 and 28 are made of the alloy of Fe-Co-Ni and the variation ratio of the magnetodistortion becomes zero when the amplitude of the alternating magnetic field is .+-.75 .phi. by the application of the magnetic field due to the normal current flow of the interrupter. Accordingly, fluctuation of the magnetic field intensity can be kept within the range 50-200 .phi., as is best shown in FIG. 4, by application of a magnetic field intensity of 125 Oe from the permanent magnets 58 to the metallic tubes 18, 20, 26 and 28, and thereby the magnetodistortion of each metallic tube is completely restricted. By the restriction of magnetodistortion, vibration of the metallic tubes is eliminated and thereby generation of the vibration noise is also completely prevented.
In the vacuum circuit interrupter shown in FIGS. 2 and 3, the vibration generated from the metallic tubes was 44-45 dB in a measurement of the A-characteristic of a compromise noise meter, under the condition that background noise was 44 dB, when the radius of the metallic tubes was 0.008 m and the normal current flow was 3000 A, of which frequency was 50 Hz. Accordingly, it is understood that the vibration noise is perfectly eliminated.
As is shown by a histerises loop l.sub.2 of FIG. 5, it is known that the magnetic flux density B is approximately saturated when the magnetic field intensity H is about 2.5 Oe in the ferromagnetic material composed of the alloy of Fe-Ni-Co. The magnetic flux B is approximately constant, even when the magnetic field intensity H varies within the range from 77.5 Oe to 2.5 .phi. under the measuring conditions that the current which flows through the interrupter is 3000 A and that the distance r is 0.08 m. Consequently, the magneto-distortion is extremely eliminated, and thereby the vibration noise is completely reduced by the application of magnetic fields from the permanent magnets 58 to the metallic tubes 18, 20, 26 and 28.
FIG. 6 shows the modification of the magnetic field applying means employed in the present invention. In this embodiment, a plurality of magnetic field applying members 52 are provided on the inner side of metallic tubes 18, 20, 26 and 28. In more detail, the magnetic field applying means 52 comprises a plurality of magnetic flux generating members 56 for supplying the magnetic flux to the metallic tubes 18, 20, 26, and 28 and a plurality of mounting members 54 for mounting the magnetic flux generating members 56. The magnetic flux generating member 56 comprises a permanent magnet 58. The mounting member comprises a pair of curved yokes 54a and 54b. The base portion of each of the yokes 54a and 54b is secured to the inner surface of the metallic tubes 18, 20, 26 and 28. The permanent magnet 58 of the magnetic flux generating member 56 is supported and secured between end portions of the yokes 54a and 54b by suitable adhesive, as in the above described embodiment. In addition, the permanent magnets are also arranged coaxially with respect to the metallic tubes so that like poles are adjacent.
FIG. 7 shows an another more effective embodiment of the invention. In the embodiment of FIG. 7, a plurality of magnetic field applying means 52 are provided on both the outer and inner peripheral surface of on metallic tubes 18, 20, 26 and 28. Pair of curved yokes 54a and 54b are symmetrically secured to the outer peripheral surface and the inner peripheral surface of each metallic tube. Accordingly, a plurality of magnetic flux generating means 56 are circumferentially arranged on both of outer and inner peripheral surfaces of the metallic tube. The permanent magnets are also arranged coaxially with respect to the metallic tube so that like poles are adjacent.
FIG. 8 shows a modification of the magnetic field applying means of FIG. 3. In the vacuum circuit interrupter of FIG. 8, magnetic field applying members 52 are provided on an outer surface of the metallic tube spaced apart at predetermined intervals. In more detail, a pair of yokes 54a and 54b of the mounting member are fastened to the outer surface of the metallic 18, 20, 26 and 28. The permanent magnets 58 of the magnetic flux generating means 56 are provided between end portions of yokes 54a and 54b so that opposite poles are adjacent permanent magnet 58.
In accordance with the vacuum circuit interrupter of FIG. 8, the metallic tubes 18, 20, 26 and 28 are magnetized by the magnetic flux circutation through the magnetic path formed by yokes 54a and 54b, the permanent magnet 58 and a portion of the metallic tubes 18, 20, 26 and 28 and by magnetic leakage flux 60 between the adjacent magnetic field applying members 52. A magnetic path is formed by the permanent magnet 58, the yokes 54a, a portion of metallic tube and the yoke 54b. The magnetic flux passes through the magnetic path to magnetize the metallic tube, and the leakage flux 60 is added to the adjacent magnetic field applying member 52 to increase the magnetization of the metallic tube.
Although the permanent magnet 58 is secured by the pair of yokes 54a and 54b in the above embodiments of FIGS. 3, 6, 7 and 8, the invention is not limited to this technique and a C-shaped permanent magnet or a circular are shaped permanent magnet can be employed instead of the permanent magnet 58 and the yokes 54a and 54b.
FIG. 9 illustrates another embodiment of the present invention, a magnetic field applying means 52 comprises a magnet flux generating member 56 for supplying the magnetic flux to metallic tubes 18, 20, 26 and 28, and a mounting member for mounting the magnetic generating member 56. The magnetic flux generating member 56 comprises at least one permanent magnet 58. The mounting member comprises a ring-shaped yoke 62. The permanent magnet 58 is encluded in the ring-shaped yoke 62. The yoke 62 is supported by the suitable supporting means (not shown). Lines of magnetic flux are generated from the permanent magnet 58. A portion of the lines of magnetic flux passes through the yoke 62, and other portions of the lines of magnetic flux leak from a main magnetic path which includes the permanent magnet 58 and the yoke 62 to outer and inner portions thereof. The metallic tube 18, 20, 26 and 28 are magnetized by leakage flux from the permanent magnet 58 such that the magnetic field of the metallic tube is approximately saturated, and thereby the magnetodistortion of the metallic tube reaches the saturation state, even if further magnetic field is added to the metallic tube by the current flowing through the circuit interrupter.
In to the vacuum circuit interrupter shown in FIG. 9, vibration noise was reduced to 43-45 dB under the same measuring conditions as that of the interrupter shown in FIG. 1. Although the magnetic field applying means 52 is provided in the outer side of the metallic tube in the embodiment of FIG. 9, similar operations and effects can be obtained by means of providing a magnetic field applying means which comprises a ring-shaped yoke in which a suitable number of permanent magnets are interposed to the inner side the metallic tube or to both of the inner and the outer sides of the metallic tube.
FIG. 10 illustrates a further embodiment of the vacuum circuit interrupter in accordance with the present invention. In this embodiment, a magnetic field applying means 52 comprises an electro magnet 66. The electro-magnet 66 includes an approximately C-shaped yoke 64 and a lead wire wound over the yoke 64. As is best seen in FIG. 10, a plurality of C-shaped yokes 64 are provided in alignment with the circumference, of the outer surface of metallic tubes 18, 20, 26 and 28 and the wire 66 is wound on each of the yoke 66.
In the vacuum circuit interrupter of FIG. 10, magnetic flux is generated by supplying current to the wire 66 in the direction indicated by arrow A. Each of the metallic tubes 18, 20, 26 and 28 is magnetized by the induced magnetic flux from the electro-magnet, and thereby the magnetodistortion of the metallic tubes is prevented, in spite of the additional magnetic flux due to the current of the circuit interrupter.
In this exemplary embodiment, the plurality of electric magnet can be provided at any places of the metallic tube such as, for example, the inner surface, or both surfaces of the metallic tube. In this case, similar operations and advantages as in the case of FIG. 10 may be obtained.
FIG. 11 is an illustraties vacuum circuit interrupter which embodies the present invention. In the embodiment of FIG. 11, a magnetic field applying means 52 comprises a magnetic flux generating member 56 including a ring-shaped yoke 68 provided coaxially on the outer side of metallic tube, and a suleniod coil formed by winding a wire 66 on the yoke 68. When an current is supplied to the solenoid coil as is shown by an arrow B, the magnetic flux generating member 56 generates magnetic flux as is shown by arraws C. The metallic tubes are magnetized by leakage flux from the electro magnet which consists of the yoke 68 and the lead wire 66 wound on the yoke 68, so that the magnetic density of the metallic tubes are always in the saturation state. In the vacuum circuit breaker of FIG. 11, the background noise was about 50-54 dB, when the measurement was carried out in the same conditions as in the case of the first embodiment.
FIG. 12 shows an other embodiment of the invention. In this embodiment, the difference, from the above described embodiments is that magnetic field is applied to metallic tubes in a direction parallel to the main current path of the vacuum circuit breaker. In more detail, a plurality of permanent magnets 58 are arranged circularly spaced apart at a desired distance from each other on an outer peripheral surface of the metallic tube 18. The metallic tube 18 is magnetized in the longitudinal direction thereof. Each of the permanent magnets 58 is fastened to the outer surface of the metallic tube 18 by means of mounting members 54 in the form of a pair of yokes. Additionally, magnetic field applying means 52 of the above described various embodiments are also applicable to the vacuum circuit interrupter of FIG. 12.
FIG. 13 shows a possible embodiment of the present invention. In the vacuum circuit interrupter shown in FIG. 13, the apparent magnetic reluctance of the metallic tubes increased by making the magnetic flux reach saturation state. In more detail, at least one magnetic field applying means 52 is provided on the outer surfaces of the metallic tubes in order to avoid the harmful influences of an alternating magnetic field produced by current of the vacuum circuit interrupter. A magnetic flux generating member 56 comprises a permanent magnet 58 provided on an outer surface of the metallic tube 18. One end of the permanent magnet 58 is secured to the outer surface of the metallic tube 18 by means of adhesive.
In the circuit interrupter of FIG. 13, lines of magnetic flux from the permanent magnet 58 interlinks with a portion of the metallic tube 18. By the interlinkage of the magnetic flux with the metallic tube 18, the metallic tube 18 is magnetized so that the magnetic flux density is saturated to decrease the vibration noise due to the alternating magnetic field induced by the current flow of the vacuum circuit interrupter.
It is known that the apparent magnetic reluctance increases as mentioned above, when the magnetic flux density in a portion of the magnetic circuit reaches the saturation state or approximately the saturation state. Accordingly, the magnetic reluctance R of the portion of the magnetic circuit can be represented by following equation
R=ls/.mu.o.multidot..mu.s(A Wb.sup.-1) (1)
where r is the radius of the metallic tube, l is a cross sectional area of the metallic tube, .mu.o=4.pi..times.10.sup.-7 (H/M) is the permeability in the vacuum and .mu.s is the relative permeability of the metallic tube. Magnetic-motive force F is represented by the following (equation), when the current flowing through the vacuum interrupter is I.
F=nI(AT), (n=1) (2)
.phi.=F/R(Wb) (3)
where .phi. is the magnetic flux.
Since the relative permeability is approximately equal to 1 and the sectional area is S, the resulting magnetic flux is:
B.sub.1 =P/S(WbM.sup.-2) (4)
(1Wb/M.sup.2 =10.sup.4 G).
Further the resulting magnetic flux density is obtained by substituting the equations (1), (2) and (3) to the equation (4):
B1=F/R.S=4.pi.(10.sup.-7)/l(Wb/m.sup.2) (5)
When the magnetic field applying density is not provided on the metallic tube, the resulting magnetic flux density is:
B2=4.pi.(10.sup.-7.mu.)I/2.pi.r(Wb/m.sup.2) (6)
Consequently, the following relation is obtained:
(B1/B2)=(1/.mu.).multidot.(2.mu.r/1) (7)
The relative permeability of the alloy of Fe-Ni-Co was 173, and the resulting ratice of B1 and B2 was therefore.
(B1/B2)=(1/173).multidot.[.mu.150(10.sup.-3)/15(10.sup.-3)]=0.18,
when the diameter was 150 mm (r=75 mm), the length l of the magnetized portion of the metallic tube was 15 mm, and the current flow I was 3000 Arms. Accordingly, it can be understood that the alternating magnetic field induced by the current I in the metallic tube is reduced to about 1/5 when the portion (1=15 mm) of the metallic tube is magnetized such that the magnetic flux density of the metallic tube is saturation state or about saturation state. It is further to be understood that the vibration of the metallic tube due to the magnetadistortion is eliminated and thereby the noise due to the vibration of the metallic tube is reduced.
Moreover, the following experimental data were obtained by measuring by means of the A-characteristic of a compromise noise meter under the condition that the background noise was 44 dB. Namely, the noise generated due to the vibration of the vacuum circuit interrupter was 51 dB at the place spaced apart 1.0 m from the vacuum circuit interrupter, when the radius of the vacuum circuit interrupter was 0.075 m and when the current flow I was 3000 A and its frequency was 50 Hz. Accordingly, the eliminated noise was about 19 dB with respect to the conventional vacuum circuit interrupter.
In the embodiment of FIG. 13, the permanent magnet 58 has a coersive force so that the magnet 58 is not demagnetized by the magnetic field intensity H=80.times.10.sup.-3 =4.25.times.10.sup.5 (AT/m)=5340 (Oe), due to the peals value of 2.5 times of the maximum over current 80 KArms. The permanent magnet 58 is also substituted by a permanent magnet having the coersive force so as not to be demagnetized in accordance with the maximum value of the overcurrent.
FIG. 14 is illustrative of one effective modification of the vacuum circuit interrupter. In the vacuum circuit interrupter of FIG. 14, a plurality of magnetic flux generating member 56 are secured to a metallic tube 18 in order to increase the apparent magnetic reluctance of the metallic tube. In more detail, four permanent magnets 28 are provided spaced apart equidistantly from each to an outer surface of the metallic tube 18.
In accordance with the vacuum circuit breaker shown in FIG. 14, the noise due to the vibration was 46 dB under the same measuring condition as in the case of FIG. 13.
FIG. 15 is illustrative of one possible modification of the vacuum circuit interrupter in accordance with the present invention. In the modification shown in FIG. 15, the vacuum circuit breaher further comprises a magnetic flux by-passing member in the form of a yoke 70 for leading lines of magnetic flux. In this embodiment, a plurality of permanent magnets 28 are secured to the outer surface of a metallic tube 18 spaced apart at a predetermined distance from each. In this case, one of the permanent magnet 58 is secured to the metallic tube 18 so that a position magnetic polarity is positioned to the metallic tube side, and other is fastened to the metallic tube 18 so that a negative polarity (S) is located to the metallic tube side. The yoke 70 is bridged and secured between the adjacent magnets 58.
According to the vacuum circuit interrupter of FIG. 15, the lines of magnetic flux produced from each of the magnet 58 are by-passed to the adjacent magnet by way of the yoke 70, and thereafter the magnetic flux circulates through the other magnet 58, a portion of the metallic tube 18. Consequently, the amount of leakage magnetic flux is reduced by the aid of the yoke 70, and, as a result the apparent magnetic reluctance is effectively increased.
In accordance with the above described embodiment, the generated noise was 48 dB under the same measuring conditions as in the case of the vacuum circuit interrupter of FIG. 14.
FIG. 16 shows an effective modification of the vacuum circuit interrupter of FIG. 15. The vacuum circuit interrupter shown comprises a plurality of closed magnetic circuits which includes a pair of permanent magnets 58 which are directly secured to the outer surface of a metallic tube 18 and a magnetic flux bridging segment in the form of a yoke 70. The pair of permanent magnets 58 are directly secured to the outer surface of the metallic tube 18 such that adjacent magnets have opposite polarity. Four closed magnetic loops are formed around the circumferential direction and, accordingly the apparent magnetic reluctance is further increased. In this embodiment, the noise induced from the interrupter was 44 dB in the same measuring condition as that of the above embodiment. It is, accordingly, understood that the noise is completely reduced.
FIG. 17 is illustrative of another embodiment of the present invention. The interrupter shown is substantially similar to that of FIG. 10, and this magnetic field applying member 52 can also make the magnetic reluctance of a portion of the metallic tube 18.
In the above description of the embodiments of FIGS. 3, 6-9, and 13-16, the detailed explanation has been in terms of permanent magnets 58 formed by sintering of ordinary ferromagnetic material, but the present invention is not limited to such conventional permanent magnets 58. For example, permanent magnets formed by resin binding of ordinary ferromagnetic material may be used. Alternatively, a rare earth-cobalt powder alloy such as samarium-cobalt may be bound with flexible plastic or rubber and formed into substantially rectangular shape to form a so-called plastic or rubber magnet. Again, the power alloy may be formed as a film on paper or the like, magnetized, and used as a flexible magnet. If permanent magnets of this resin bound or flexible type are used, then compared with conventional magnets, various advantages are obtained. For example, in the manufacturing state, in the forming of connections, particularly problems with defects near the poles of the magnets are avoided. In the ninth to twelfth embodiments, where the poles of the magnets are joined to connecting rings it is possible to ensure a good connection.
FIG. 18 shows a further embodiment of the vacuum circuit interrupter of the present invention. The vacuum circuit interrupter shown comprises a magnetic flux generating means 56. The magnetic flux generating means 56 comprises four permanent magnets 58 provided on the outer surface of metallic tube 18, evenly spaced apart and a circular magnetic flux bridging sequent in the form of a circular yoke 74. Four closed magnetic circuits are formed by the pair of permanent magnets 58 and the circular magnetic flux bridging sequent 74.
According to the vacuum circuit interrupter shown in FIG. 18, lines of magnetic flux are effectively circulated by way of each pair of magnets 58, a portion of the yokes 74 and the portion of the metallic tube 18. Accordingly, the magnetic flux density and the magnetic distortion are extremely enhanced.
FIGS. 19 to 21 show other possible embodiment of the vacuum circuit interrupter of the present invention. In the vacuum circuit interrupter shown in FIG. 10 a magnetic field applying means 52 comprises a magnetic flux generating member 56 which consists of a plurality of flexible permanent magnets 58b provided on the outer surface of the metallic tube 18 and a ring-shaped yoke 76 for securing the permanent magnets 58b to the outer surface of the metallic tube 18. The permanent magnets 58b are, respectively, positioned such that the magnetic polarity of adjacent magnets is opposite. Each of the permanent magnets 58b is magnetized in the thickness direction thereof.
In the vacuum circuit interrupter of FIG. 19, lines of magnetic flux circulate in a magnetic path formed by permanent magnet 58b, a portion of the metallic tube 18, a portion of the yoke and an adjacent permanent magnet 58b. By the magnetic flux existing in the metallic tube 18, the metallic tube 18 is magnetized to increase the apparent magnetic reluctance of the metallic 18.
FIGS. 20 and 21 show other examples of the magnetic flux generating member 56 employed in the vacuum circuit breaker of FIG. 19. The magnetic flux generating member 56 of FIG. 20 consists of a plurality of permanent magnets 58b formed by magnetizing a ferromagnetic plate in alternating thickness directions. Moreover, the magnetic flux generating member 56 of FIG. 21 consists of a permanent magnet 58b formed by magnetizing ferromagnetic plate in its thickness direction.
According to the present invention as described above, two end plates are sealed to the ends of an evacuated insulated tube and form magnetic paths. Within the evacuated tube a fixed and a movable electrode are provided so as to be connected or separated, and to form a vacuum interrupter. A magnetic field applying means is provided so as to saturate or substantially saturate the magnetic flux distortion of the metallic tube. Thus it is possible to reduce substantially or eliminate noise caused by vibration of the metallic tubes due to magnetic distortion. Moreover, if resin bound magnets or flexible magnets are used as permanent magnets for the magnetic field applying means, breakages and defects can be avoided and furthermore the vacuum interrupter can be made more easily and cheaply.
Since, moreover, a magnetic field applying means is provided such that the magnetic flux intensity in at last one portion of the metallic tubes is at saturation level, or near saturation level, suppression or elimination of vibration noise caused by the effect of the alternating magnetic field on the metallic tube can be achieved with a means for applying a magnetic field using fewer permanent magnets or electromagnets.

Number	Date	Country
54-34608	Mar 1979	JPX
54-46261	Apr 1979	JPX
54-522231[U]JPX	Apr 1979	JPX

Number	Name	Date	Kind
3372258	Porter	Mar 1968
3920942	Yanagisawa	Nov 1975

Vacuum circuit interrupter

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Abstract

Description

Claims

Priority Claims (3)

US Referenced Citations (2)