VACUUM INTERRUPTER

TECHNICAL FIELD

The present invention relates to a vacuum interrupter having a fixed electrode and a moving electrode in an insulation enclosure maintaining a vacuum to break and connect a circuit.

BACKGROUND ART

A conventional vacuum interrupter serves to interrupt a high current flowing through an electric circuit by switching the state between a fixed electrode and a moving electrode from a closed state to an open state when, for example, an accident occurs. The current interruption causes an arc discharge between the fixed electrode and the moving electrode.

In order to extinguish the arc discharge, each of the fixed electrode and moving electrode has a contact portion protruding relative to the central portion, and slits dividing the contact portion into a plurality of circular segment portions, each slit having one end point adjacent to the central portion and the other end point adjacent to the circumferential edge of the contact portion.

The vacuum interrupter further includes a magnetic body disposed along the surface of and around the circumferential edge of a fixed stem supporting the fixed electrode, and a magnetic body disposed along the surface of and around the circumferential edge of a moving stem supporting the moving electrode.

Such a structure allows a Lorentz force to act on the arc discharge, thereby efficiently driving the arc discharge to rotate along the circumferential edge of the electrodes and extinguishing the arc discharge (PTL 1, for example).

CITATION LIST
Patent Literature

PTL 1: Japanese Patent Laying-Open No. 2014-127280

SUMMARY OF INVENTION
Technical Problem

A conventional vacuum interrupter is designed as shown in FIG. 17. FIG. 17(a) is a front view of a surface of a moving electrode 101u that comes into contact with a fixed electrode 101d. FIG. 17(b) is a front view of a surface of fixed electrode 101d that comes into contact with moving electrode 101u. In FIG. 17(a), moving electrode 101u is shown upside down on the drawing sheet, for the sake of clear description of a current flowing from moving electrode 101u to fixed electrode 101d.

Description will now be given to a current flowing from moving electrode 101u to fixed electrode 101d in a closed state in which a contact portion 202 of moving electrode 101u is in contact with contact portion 202 of fixed electrode 101d.

When moving electrode 101u is in contact with fixed electrode 101d, a current flows through contact portions 202 of moving electrode 101u and fixed electrode 101d, with no current flowing through central portions 201 of moving electrode 101u and fixed electrode 101d, since contact portion 202 protrudes relative to central portion 201 in each of moving electrode 101u and fixed electrode 101d.

In moving electrode 101u, a current component Ivu flowing in the direction from top to bottom on the drawing sheet enters contact portion 202 in the vicinity of central portion 201. Current component Ivu then branches off into a current component Icu flowing circumferentially from the center side of moving electrode 101u.

Current component Icu flows from contact portion 202 of moving electrode 101u to contact portion 202 of fixed electrode 101d. This in turn causes a current component Icd flowing through contact portion 202 of fixed electrode 101d to the vicinity of central portion 201. Current component Icd then turns into a current component Ivd flowing out of fixed electrode 101d in the direction from top to bottom on the drawing sheet.

Current component Icd flowing through fixed electrode 101d causes a concentric magnetic flux Md. Likewise, current component Icu flowing through moving electrode 101u causes a concentric magnetic flux Mu.

On moving electrode 101u, magnetic flux Md forms a circumferential magnetic flux from the central portion 201 side, acting on current component Icu. This causes a Lorentz force Fu acting on moving electrode 101u in the direction from bottom to top on the drawing sheet.

Likewise, on fixed electrode 101d, magnetic flux Mu forms a circumferential magnetic flux from the central portion 201 side, acting on current component Icd. This causes a Lorentz force Fd acting on fixed electrode 101d in the direction from top to bottom on the drawing sheet.

That is, in a conventional vacuum interrupter, when a current is carried through the fixed stem and the moving stem while the interrupter is in a closed state, Lorentz forces act on fixed electrode 101d and moving electrode 101u, thereby causing a repulsive force in the direction toward an open state.

In order to prevent unintended separation between the fixed electrode and the moving electrode, the application of load (hereinafter referred to as “contact load”) is required. Accordingly, a conventional vacuum interrupter, which entails a repulsive force in the direction toward an open state, involves an increased contact load and upsizing and complication of the load application mechanism.

If contact portion 202 does not protrude relative to central portion 201 but is flush with central portion 201 in each of the fixed electrode and moving electrode, an arc discharge may occur in the vicinity of central portion 201 at the time of interruption operation when the vacuum interrupter switches from a closed state to an open state. Such an arc discharge occurring in the vicinity of central portion 201 is not acted on by a Lorentz force and thus cannot be extinguished.

The present invention has been made to solve a problem of upsizing and complication of the load application mechanism as described above. An object of the present invention is to provide a fixed electrode, a moving electrode, and their surrounding structures that can reduce the repulsive force.

Solution to Problem

A vacuum interrupter of the present invention includes a magnetic body disposed on a circumferential edge around a stem surface of at least one of a moving current-carrying stem and a fixed current-carrying stem. The magnetic body includes a lower magnetic permeance portion having a lower magnetic permeance than the other portion.

Advantageous Effects of Invention

The present invention can provide a small-sized, reliable vacuum interrupter without involving upsizing and complication of the reduction load application mechanism.

BRIEF DESCRIPTION OF DRAWINGS

FIG. 1 is a cross-sectional view of a vacuum interrupter 100 in embodiment 1 of the present invention.

FIG. 2 is a perspective view illustrating a part including a fixed electrode 5, a moving electrode 8, and their surrounding area of vacuum interrupter 100.

FIG. 3 shows front views illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100.

FIG. 4 shows a cross-sectional view illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100 in a closed state; and a front view illustrating a layout of a moving magnetic body 11 and a fixed magnetic body 10.

FIG. 5 is a perspective view illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100 in a closed state.

FIG. 6 shows front views illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100.

FIG. 7 shows graphs illustrating the temporal variations of parameters at the time of interruption operation of vacuum interrupter 100.

FIG. 8 shows front views illustrating the states of arc discharge on a contact surface 5f of fixed electrode 5 of vacuum interrupter 100 at the time of interruption operation.

FIG. 9 shows perspective views illustrating the states of arc discharge at the time of interruption operation of vacuum interrupter 100.

FIG. 10 is a cross-sectional view illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100 to describe the directions of current and magnetic flux.

FIG. 11 shows front views of fixed electrode 5 and fixed magnetic body 10 in a preferred example of embodiment 1.

FIG. 12 show front views illustrating the shapes of a fixed magnetic body 10A and a moving magnetic body 11A and the densities of the magnetic fluxes generated in a variation of embodiment 1.

FIG. 13 is a cross-sectional view illustrating a part including fixed electrode 5, moving electrode 8A, and their surrounding area in embodiment 2 of the present invention.

FIG. 14 shows a layout illustrating the areas of the parts where the solid part of moving magnetic body 11 overlaps with the solid part of fixed magnetic body 10, and shows a front view illustrating arc discharges on fixed electrode 5 in embodiment 3 of the present invention.

FIG. 15 is a cross-sectional view illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of a vacuum interrupter in embodiment 4 of the present invention.

FIG. 16 is a graph comparing the arc-driving forces with different widths ds.

FIG. 17 shows front views illustrating Lorentz forces acting in a conventional vacuum interrupter.

FIG. 18 is a perspective view illustrating a part including a moving magnetic body 11B, a fixed magnetic body 10B, and their surrounding area of a vacuum interrupter 110 in embodiment 5.

FIG. 19 is a side view illustrating moving magnetic body 11B and fixed magnetic body 10B of vacuum interrupter 110 in embodiment 5.

FIG. 20 is a perspective view illustrating a part including moving magnetic body 11, fixed magnetic body 10, and their surrounding area of vacuum interrupter 100 in embodiment 1.

FIG. 21 is a side view illustrating moving magnetic body 11 and fixed magnetic body 10 of vacuum interrupter 100.

FIG. 22 is a magnetic circuit diagram illustrating a magnetic circuit of vacuum interrupter 100.

FIG. 23 is a magnetic circuit diagram simplifying the circuit diagram of FIG. 22.

FIG. 24 is a perspective view illustrating a part including a moving magnetic body 11C, a fixed magnetic body 10C, and their surrounding area of a vacuum interrupter 120 in a variation of embodiment 5.

FIG. 25 is a side view illustrating moving magnetic body 11C and fixed magnetic body 10C of vacuum interrupter 120 in the variation of embodiment 5.

FIG. 26 is a perspective view illustrating a part including a moving magnetic body 11D, a fixed magnetic body 10D, and their surrounding area of a vacuum interrupter 130 in embodiment 6.

DESCRIPTION OF EMBODIMENTS
Embodiment 1

Embodiment 1 of the present invention will now be described in detail with reference to FIGS. 1 to 12.

First, with reference to FIGS. 1 to 3, a configuration of a vacuum interrupter 100 in embodiment 1 is described.

FIG. 1 is a cross-sectional view of vacuum interrupter 100 in embodiment 1 for practicing the present invention. FIG. 2 is a perspective view illustrating a part including a fixed electrode 5, a moving electrode 8, and their surrounding area of vacuum interrupter 100. FIG. 3 shows front views illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100.

In FIG. 1, the Y direction indicated by an arrow defines the direction from the back side to the front side on FIG. 1 sheet; the X direction indicated by an arrow defines the direction from left to right on FIG. 1 sheet; and the Z direction indicated by an arrow defines the direction from top to bottom on FIG. 1 sheet. The X, Y, and Z directions indicated by arrows in FIGS. 2 and 3 define the same directions as the X, Y, and Z directions in FIG. 1.

Also, where X, Y, and Z directions are defined in FIGS. 4 to 15 and 18 to 26, the X, Y, and Z directions define the same as those in FIG. 1.

With reference to FIGS. 1 and 2, a cylindrical insulation enclosure 1 is made of an insulating member, such as ceramic. Insulation enclosure 1 has a moving end plate 3 at its one end. Insulation enclosure 1 has a fixed end plate 2 at its other end.

A bellows 6, flexible in the Z direction, is attached to moving end plate 3 at one end of bellows 6. Bellows 6 has the other end having a bellows shield 12 attached thereto. Further, a moving current-carrying stem 7 is attached passing through bellows shield 12. Moving current-carrying stem 7 has moving electrode 8 at its end.

Moving end plate 3, bellows 6, bellows shield 12, moving current-carrying stem 7, and moving electrode 8 are electrically connected. Further, a solid part of a moving magnetic body 11 is disposed on the circumferential edge around the stem surface of moving current-carrying stem 7.

A fixed current-carrying stem 4 is attached to fixed end plate 2, such that fixed current-carrying stem 4 lies on an extension of the axis of moving current-carrying stem 7 and passes through fixed end plate 2. Fixed current-carrying stem 4 has fixed electrode 5 at its end.

Fixed end plate 2, fixed current-carrying stem 4, and fixed electrode 5 are electrically connected. Further, a solid part of a fixed magnetic body 10 is disposed on the circumferential edge around the stem surface of fixed current-carrying stem 4.

A contact surface 5f of fixed electrode 5 faces a contact surface 8f of moving electrode 8. The distance between contact surface 5f of fixed electrode 5 and contact surface 8f of moving electrode 8 is denoted as an inter-electrode distance g. The maximum value of inter-electrode distance g is denoted as a maximum distance gmax, which indicates the maximum value in the movable range of moving current-carrying stem 7.

Insulation enclosure 1 contains an arc shield 9 therein made of a conductive member, such as metal. Arc shield 9 covers fixed electrode 5 and moving electrode 8. When an arc discharge occurs between moving electrode 8 and fixed electrode 5, arc shield 9 can protect other regions from the metal vapor and metal particles scattering from moving electrode 8 and fixed electrode 5 due to the heat from arc discharge.

With reference to FIG. 3, the structure of fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100 will now be described in detail.

FIG. 3(a) is a front view at the connection between moving electrode 8 and moving current-carrying stem 7, taken along broken line A-A shown in FIG. 1. The Y direction is reversed to align with a later-described drawing with a current direction. FIG. 3(b) is a front view of contact surface 8f of moving electrode 8, with the Y direction also reversed. FIG. 3(c) is a front view of contact surface 5f of fixed electrode 5. FIG. 3(d) is a front view at the connection between fixed electrode 5 and fixed current-carrying stem 4 taken along broken line B-B shown in FIG. 1.

With reference to FIG. 3(a), a solid part of moving magnetic body 11 is disposed on the circumferential edge around a stem surface 7f of moving current-carrying stem 7. Moving magnetic body 11 has a notch 11n, a partial cut-out in the solid part. Moving magnetic body 11 has a tip 11t located at the end, on the outer peripheral side, of the boundary between the solid part and notch 11n.

With reference to FIG. 3(b), moving electrode 8 has slits 8s each having one end point adjacent to a central portion 8c indicated by a broken line, and having the other end point adjacent to an edge portion 8e. Slits 8s divide the outer periphery of moving electrode 8 into a plurality of circular segment portions 8a. The regions defined by slits 8s and circular segment portions 8a, one of which is enclosed by a dotted line in the drawing, are referred to as wings 8w. Each wing 8w has a tip 8t, which is the end of wing 8w on the outer peripheral side. In other words, slits 8s divide the region on the edge portion 8e side relative to central portion 8c, into a plurality of wings 8w.

In embodiment 1, moving electrode 8 has three slits 8s dividing the outer periphery of moving electrode 8 into three parts, thus creating three circular segment portions 8a and three wings 8w.

With reference to FIG. 3(c), fixed electrode 5 has slits 5s each having one end point adjacent to a central portion 5c indicated by a broken line, and having the other end point adjacent to an edge portion 5e. Slits 5s divide the outer periphery of fixed electrode 5 into a plurality of circular segment portions 5a. The regions defined by slits 5s and circular segment portions 5a, one of which is enclosed by a dotted line in the drawing, are referred to as wings 5w. Each wing 5w has a tip 5t, which is the end of wing 5w on the outer peripheral side. In other words, slits 5s divide the region on the edge portion 5e side relative to central portion 5c, into a plurality of wings 5w.

In embodiment 1, fixed electrode 5 has three slits 5s dividing the outer periphery of fixed electrode 5 into three parts, thus creating three circular segment portions 5a and three wings 5w.

With reference to FIG. 3(d), a solid part of fixed magnetic body 10 is disposed on the circumferential edge around a stem surface 4f of fixed current-carrying stem 4. Fixed magnetic body 10 has a notch 10n, a partial cut-out in the solid part. Fixed magnetic body 10 has a tip 10t located at the end, on the outer peripheral side, of the boundary between the solid part and notch 10n.

In embodiment 1, notch 11n of moving magnetic body 11 is 180 degrees rotationally displaced from notch 10n of fixed magnetic body 10 around the Z direction.

The operation of vacuum interrupter 100 will now be described.

The inside of vacuum interrupter 100 is kept at a vacuum of 1×10⁻³Pa or less so as to maintain a high vacuum. Switching can be made between a closed state in which moving electrode 8 is connected to fixed electrode 5, and an open state in which moving electrode 8 is separated from fixed electrode 5.

FIG. 1 is an open state in which moving electrode 8 is not connected to fixed electrode 5. In other words, it is a state in which contact surface 8f is not in contact with contact surface 5f.

When a pressure is externally applied to moving current-carrying stem 7 in the Z direction, moving current-carrying stem 7 moves to create a closed state in which moving electrode 8 is connected to fixed electrode 5. In other words, it is a state in which contact surface 8f is in contact with contact surface 5f.

That is, a movement of moving current-carrying stem 7 can switch from an open state to a closed state, or from a closed state to an open state.

With reference to FIGS. 4 to 10, the mechanism to extinguish an arc discharge occurring at the time of interruption operation will now be described.

First, with reference to FIGS. 4 to 6, description is given to the paths of current and the magnetic fields generated from the current in vacuum interrupter 100 in a closed state.

FIG. 4 shows a cross-sectional view illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100 in a closed state; and a front view illustrating a layout of moving magnetic body 11 and fixed magnetic body 10.

FIG. 4(a) is a cross-sectional view seen from the same direction as the cross-section shown in FIG. 1, with the directions of a current Id, a magnetic flux Mr, and leakage fluxes Mv and Mvr added therein.

FIG. 4(b) shows a layout of moving magnetic body 11 and fixed magnetic body 10 as seen from front in the Z direction, with the directions of leakage fluxes Mv and Mvr added therein.

The regions where the solid part of moving magnetic body 11 overlaps with the solid part of fixed magnetic body 10 are denoted as regions v1 and v2, which are located between moving magnetic body 11 and fixed magnetic body 10.

FIG. 5 is a perspective view illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100 in a closed state, with the directions of current Id, magnetic flux Mr, and leakage fluxes Mv and Mvr added therein.

FIG. 6, similar to FIG. 3, shows front views illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100, with the directions of current Id, magnetic flux Mr, and leakage fluxes Mv, Mvr, and Mp added therein.

FIG. 6(a), similar to FIG. 3(a), shows a front view at the connection between moving electrode 8 and moving current-carrying stem 7, with the directions of current Id, magnetic flux Mr, and leakage fluxes Mv, Mvr, and Mp added therein. FIG. 6(b), similar to FIG. 3(b), shows a front view of moving electrode 8, with the direction of current Id added therein. FIG. 6(c), similar to FIG. 3(c), is a front view of fixed electrode 5, with the direction of current Id added therein. FIG. 6(d), similar to FIG. 3(d), is a front view at the connection between fixed electrode 5 and fixed current-carrying stem 4, with the directions of current Id, magnetic flux Mr, and leakage fluxes Mv, Mvr, and Mp added therein.

Vacuum interrupter 100 is in a closed state, with current Id flowing from moving current-carrying stem 7 to fixed current-carrying stem 4. That is, current Id is flowing in the Z direction.

Since contact surface 8f of moving electrode 8 is in contact with contact surface 5f of fixed electrode 5 over the whole surface, current Id mainly flows from central portion 8c of moving electrode 8 through central portion 5c of fixed electrode 5.

That is, as compared with a conventional vacuum interrupter (described in PTL 1), current Id has no or little current component flowing through wings 8w and wings 5w. This reduces a repulsive force in the direction toward an open state between fixed electrode 5 and moving electrode 8.

Magnetic fluxes caused by a magnetomotive force from current Id will now be described.

First, current Id causes concentric magnetic fluxes around moving current-carrying stem 7 and fixed current-carrying stem 4. Among the magnetic fluxes, magnetic flux Mr is circulating through moving magnetic body 11 and fixed magnetic body 10.

Notch 11n of moving magnetic body 11 causes leakage fluxes. The leakage fluxes include: leakage flux Mp in the same direction as magnetic flux Mr; leakage flux Mv in the direction from moving electrode 8 to fixed current-carrying stem 4; and leakage flux Mvr in the direction from fixed current-carrying stem 4 to moving electrode 8.

Similarly, notch 10n of fixed magnetic body 10 causes leakage fluxes. The leakage fluxes include: leakage flux Mp in the same direction as magnetic flux Mr; leakage flux Mv in the direction from moving electrode 8 to fixed current-carrying stem 4; and leakage flux Mvr in the direction from fixed current-carrying stem 4 to moving electrode 8.

Leakage flux Mv mainly passes through region v2, whereas leakage flux Mvr mainly passes through region v1.

With reference to FIGS. 7 to 10, the mechanism will now be described for extinguishing an arc discharge occurring between contact surface 5f and contact surface 8f when vacuum interrupter 100 makes an interruption operation with current Id flowing.

FIG. 7 shows graphs illustrating the temporal variations of parameters at the time of interruption operation of vacuum interrupter 100.

FIG. 7(a) shows the temporal variation of inter-electrode distance g.

A magnetic field caused by leakage fluxes Mv and Mvr is defined as a parallel magnetic field. The average of the absolute values of the magnetic field intensities caused by leakage fluxes Mv and Mvr is defined as a parallel magnetic field intensity.

A magnetic field caused by magnetic flux Mr circulating inside moving magnetic body 11 or fixed magnetic body 10 is defined as a circulating magnetic field. The average of the absolute values of the intensities caused by magnetic flux Mr is defined as a circulating magnetic field intensity.

FIG. 7(b) shows the temporal variations of the parallel magnetic field intensity and the circulating magnetic field intensity.

At the zero time, vacuum interrupter 100 is in a closed state. Vacuum interrupter 100 then makes a mechanical operation of moving current-carrying stem 7.

When inter-electrode distance g reaches maximum distance gmax, the mechanical operation of moving current-carrying stem 7 is completed.

Meanwhile, an arc discharge occurs between contact surface 5f of fixed electrode 5 and contact surface 8f of moving electrode 8, which is then extinguished at time t3, thus annihilating the parallel magnetic field and the circulating magnetic field.

An arc discharge occurs at the point at which contact surface 8f is separated from contact surface 5f at the last moment in the interruption operation. Specifically, an arc discharge may occur at any position on contact surface (5f, 8f), according to the effect of microscopic asperities on contact surfaces 5f and 8f.

If contact portion 202 does not protrude relative to central portion 201 but is flush with central portion 201 in each of the fixed electrode and moving electrode as in a conventional vacuum interrupter (described in PTL 1), an arc discharge occurring at central portion 201 cannot be extinguished, as described above.

The mechanism for extinguishing an arc discharge will now be described. In the description, an arc discharge is assumed to occur at central portion (8c, 5c) since the present invention can effectively extinguish an arc discharge occurring at central portion (8c, 5c) at the time of interruption operation.

FIG. 8 shows front views illustrating the states of arc discharge on contact surface 5f of fixed electrode 5 of vacuum interrupter 100 at the time of interruption operation. Similarly, FIG. 9 shows perspective views illustrating the states of arc discharge of fixed electrode 5 and moving electrode 8 at the time of interruption operation.

FIGS. 8(a) and 9(a) show the state at time t1 shown in FIG. 7, FIGS. 8(b) and 9(b) show the state at time t2 shown in FIG. 7, and FIGS. 8(c) and 9(c) show the state at time t3 shown in FIG. 7.

FIG. 10 is a cross-sectional view illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of vacuum interrupter 100, with the directions of a current Ia, a magnetic flux Ma, and a Lorentz force Fa added therein to describe the directions of current and magnetic flux after an arc discharge moves to wings 5w.

With reference to FIGS. 7, 8(a), and 9(a), at time t1 immediately after the start of interruption operation, an arc discharge a1 from central portion 8c to central portion 5c has already occurred.

Since the magnetic permeance does not change inside fixed electrode 5 and moving electrode 8, the circulating magnetic field intensity remains almost unchanged.

As inter-electrode distance g is increased, the magnetic permeance between moving magnetic body 11 and fixed magnetic body 10 is decreased, thereby attenuating the parallel magnetic field intensity from the initial intensity to a magnetic field intensity value of ms1. Meanwhile, the circulating magnetic field intensity maintains a relatively high magnetic field intensity value of mg1.

With reference to FIGS. 7, 8(b), and 9(b), at time t2 after a lapse of a certain period of time from time t1, arc discharge a1 diffuses while moving from central portion 5c to wings 5w, thereby increasing its cross-sectional area (i.e., the area on contact surface 5f) as indicated by an arc discharge a2.

Such a change, peculiar to an arc discharge in a vacuum, is due to the property of arc discharge of moving to a place having a higher intensity of magnetic field parallel to the discharge current (parallel magnetic field). This phenomenon is considered to be because the charged particles (ions and electrons) of arc discharge move helically winding around a magnetic flux.

In other words, in embodiment 1, since regions v1 and v2 shown in FIG. 4(b) have a high parallel magnetic field intensity, arc discharge a1 moves to region v1 or v2.

The behavior of arc discharge a1 after moving to regions v1 and v2 and the mechanism of arc extinguishing depend on the magnitude of current Id to be interrupted.

Firstly, description is given to a behavior of arc discharge with a low current Id to be interrupted.

An arc discharge in a vacuum trapped by a parallel magnetic field diffuses over the whole surface of regions v1 and v2, which have a high parallel magnetic field intensity. Thus, the arc discharge is maintained at a lower current density than in no parallel magnetic field. Arc discharge a2 therefore does not cause an excessive temperature rise of fixed electrode 5 and moving electrode 8. Arc discharge a2 is thus extinguished while remaining diffused over the whole surface of regions v1 and v2. In this case, fixed electrode 5 and moving electrode 8 do not experience an excessive temperature rise and thus exhibit very little wear.

Secondly, description is given to a behavior of arc discharge with a high current Id to be interrupted.

An increase in current causes an increase in magnetomotive force, thereby increasing the magnetic flux density of circulating magnetic field flowing through fixed magnetic body 10 and moving magnetic body 11. When the magnetic flux density exceeds the saturated magnetic flux density intrinsic in the material of fixed magnetic body 10 and moving magnetic body 11, magnetic saturation is reached. This significantly decreases the magnetic permeability of fixed magnetic body 10 and moving magnetic body 11.

In this case, the magnetic flux is likely to move along the path passing through notch 11n and circulating through the same magnetic body, thus decreasing the intensities of leakage fluxes My and Mvr. That is, the parallel magnetic field intensity attenuates. Accordingly, arc discharge a2, which has been diffused over regions v1 and v2, cannot maintain the diffused state, thus moving to wings 5w as indicated by an arc discharge a3 in FIG. 8(c) and shifting to a state of high current density.

With reference to FIGS. 7, 8(c), and 9(c), arc discharge a3 will now be described in detail.

At time t3 after a lapse of a certain period of time from time t2, arc discharge a2 moves to wings 5w as indicated by arc discharge a3.

With reference to FIG. 10, current Ia caused by arc discharge a3 flows from moving current-carrying stem 7 to fixed current-carrying stem 4 as before the interruption operation.

When arc discharge a3 lies in wings 5w, current Ia flows in the direction along wings 8w of moving electrode 8. For the sake of brevity, the direction of current Ia along wings 8w is described as substantially coinciding with the Y direction.

Current Ia flows between moving electrode 8 and fixed electrode 5 as arc discharge a3, and then flows in the direction along wings 5w to reach fixed current-carrying stem 4. For the sake of brevity, the direction of current Ia along wings 8w is described as substantially coinciding with the direction opposite to the Y direction.

When flowing through wings 8w of moving electrode 8 in the Y direction, current Ia causes a concentric magnetic flux Ma around the direction of current Ia. Similarly, when flowing through wings 5w of fixed electrode 5 in the direction opposite to the Y direction, current Ia causes concentric magnetic flux Ma around the direction of current Ia. These magnetic fluxes are X-direction magnetic fluxes in the vicinity of arc discharge a3.

Further, Lorentz force Fa in the Y direction is applied to arc discharge a3. With Lorentz force Fa, arc discharge a3 circulates on contact surface 8f of moving electrode 8 and on contact surface 5f of fixed electrode 5, thereby being cooled and extinguished.

That is, arc discharge a1 originally generated at the central portion (8c, 5c) circumferentially diffuses by the action of the parallel magnetic field parallel to the discharge direction.

When current Id is low, the action of the parallel magnetic field continues and maintains the diffusion with low current density. This can curb a temperature rise of fixed electrode 5 and moving electrode 8, thus allowing arc discharge a2 to be extinguished.

When current Id is high, the parallel magnetic field cannot be maintained due to the magnetic saturation of the magnetic bodies, resulting in arc discharge a2 moving to wings 5w and then changing into a high current density state. However, due to Lorentz force Fa, produced by magnetic fluxes generated by current Ia flowing through moving electrode 8 and fixed electrode 5, arc discharge a2 circulates on contact surface 8f of moving electrode 8 and on contact surface 5f of fixed electrode 5, thereby being cooled and extinguished.

Since Lorentz force Fa acts due to current Ia in the direction along the wings (8w, 5w), Lorentz force Fa actually acts on arc discharge a3 in the direction rotating around a Z direction axis. For the sake of brevity, at times t1 to t3, the arc discharge, acted on by Lorentz force Fa, also moves in the direction rotating around a Z-direction axis.

As described above, vacuum interrupter 100 in embodiment 1 can, in a closed state, reduce a repulsive force in the direction toward an open state between fixed electrode 5 and moving electrode 8. This can prevent upsizing and complication of the load application mechanism.

Further, at the time of interruption operation, vacuum interrupter 100 can quickly extinguish arc discharge a1 occurring between fixed electrode 5 and moving electrode 8.

That is, according to embodiment 1, a small-sized, reliable vacuum interrupter can be provided.

With reference to FIG. 11, a preferred example of embodiment 1 will now be described.

FIG. 11 shows front views illustrating angles of rotation of fixed electrode 5 and fixed magnetic body 10. FIG. 11(a) shows the front of fixed electrode 5, where the center of fixed electrode 5 is defined as an origin O and where the clockwise angles with respect to the reference axis extending upward from origin O on the drawing sheet are defined as positive angles. Similarly, FIG. 11(b) shows the front of fixed magnetic body 10, where the clockwise angles with respect to the reference axis, the same as that of FIG. 11(b), are defined as positive angles.

With reference to FIG. 11(a), fixed electrode 5 has three wings 5w, as described above.

Angle θ1 is an angle defined by a line segment and tip 5t that the line segment first encounters when the line segment rotates around origin O from the reference axis in the positive direction. Similarly, angle θ2 is an angle defined by a line segment and tip 5t that the line segment encounters next to angle θ1 when the line segment rotates around origin O from the reference axis in the positive direction. Further, angle θ3 is an angle defined by a line segment and tip 5t that the line segment encounters next to angle θ2 when the line segment rotates around origin O from the reference axis in the positive direction.

Angles θ1, θ2, and θ3 are generically referred to as angle θn (n=1, 2, 3).

With reference to FIG. 11(b), angle (θc−Δθc) is an angle defined by a line segment and one tip 10t of notch 10n that the line segment first encounters when the line segment rotates around origin O from the reference axis of fixed magnetic body 10 in the positive direction. Similarly, angle (θc+Δθc) is an angle defined by a line segment and the other tip 10t of notch 10n that the line segment next encounters when the line segment rotates around origin O from the reference axis of fixed magnetic body 10 in the positive direction.

That is, angle θc is the angle defined by the center of notch 10n and the reference axis, and angle (2×Δθc) is the central angle of a circular segment defined by one tip 10t and the other tip 10t of notch 10n with origin O being a center.

In a more preferred example of embodiment 1, tips 5t of fixed electrode 5 preferably do not overlap with notch 10n of fixed magnetic body 10.

This is because such a configuration allows a stronger Lorentz force Fa to act on arc discharge a3 in the vicinity of tips 5t of fixed electrode 5, as compared with the case in which tips St of fixed electrode 5 overlap with notch 10n of fixed magnetic body 10.

In other words, tips 5t of fixed electrode 5 preferably overlap with the solid part of fixed magnetic body 10. Thus, in a more preferred example of embodiment 1, for each of angles θ1, θ2, and θ3, a condition of angle (θc−Δθc)>angle θn (n=1, 2, 3) or a condition of angle θn (n=1, 2, 3)>angle (θc+Δθc) be preferably satisfied.

For the same reason, tips 8t of moving electrode 8 preferably do not overlap with notch 11n of moving magnetic body 11. In other words, tips 8t of moving electrode 8 preferably overlap with the solid part of moving magnetic body 11.

With reference to FIG. 12, a variation of embodiment 1 will now be described.

FIG. 12 show front views illustrating the shapes of a fixed magnetic body 10A and a moving magnetic body 11A and the magnetic fluxes generated in the variation of embodiment 1. FIG. 12(a) shows the front of fixed magnetic body 10A in the variation of embodiment 1. FIG. 12(b) shows the front of fixed magnetic body 10A and moving magnetic body 11A in place in the variation of embodiment 1.

With reference to FIG. 12(a), fixed magnetic body 10A has three notches 10n equally spaced on the circumference. Similarly, moving magnetic body 11A also has three notches 11n equally spaced on the circumference.

With reference to FIG. 12(b), moving magnetic body 11A is 60 degrees rotationally displaced from fixed magnetic body 10A around a Z-direction axis, so that notches 11n do not overlap with notches 10n.

When current Id flows, leakage fluxes Mv and Mvr are generated at three locations, with leakage fluxes Mv and Mvr alternating. That is, parallel magnetic fields are formed. Thus, at the time of interruption operation, if arc discharge a1 occurs through central portion 8c of moving electrode 8 and central portion 5c of fixed electrode 5, it can be extinguished.

Thus, according to a more preferred example and variation of embodiment 1 as described above, vacuum interrupter 100 can, in a closed state, reduce a repulsive force in the direction toward an open state between fixed electrode 5 and moving electrode 8. This can prevent upsizing and complication of the load application mechanism.

Further, at the time of interruption operation, vacuum interrupter 100 can quickly extinguish arc discharge a1 occurring between fixed electrode 5 and moving electrode 8.

That is, according to embodiment 1, a small-sized, reliable vacuum interrupter can be provided.

Embodiment 2

Embodiment 1 has described a mode in which contact surface 8f of moving electrode 8 is a flat surface.

Embodiment 2 describes a mode in which contact surface 8f of moving electrode 8 has a protrusion 8x.

FIG. 13 is a cross-sectional view illustrating a part including fixed electrode 5, a moving electrode 8A, and their surrounding area. The other regions are the same as those of vacuum interrupter 100 in embodiment 1.

In FIG. 13, the same reference numbers or signs as those of FIGS. 1 and 2 designate the same or equivalent elements as those described in embodiment 1, and thus the detailed description of such elements is omitted.

With reference to FIG. 13, contact surface 8f of moving electrode 8A has protrusion 8x at central portion 8c. If contact surface 8f is a flat surface as described above, it may be difficult to predict where on contact surface 8f an arc discharge will initially occur. However, the interruption ability has to be ensured for any behavior of arc discharge located at any position on contact surface 8f. This may lead to a complicated design of moving electrode 8A, fixed electrode 5, moving magnetic body 11, and fixed magnetic body 10.

By providing protrusion 8x at central portion 8c of contact surface 8f of moving electrode 8A, the position on contact surface 8f at which the electrodes remain in contact to the last moment at the time of interruption operation can be limited to protrusion 8x. That is, the position where an arc discharge initially occurs can be limited to protrusion 8x, thus simplifying the design of moving electrode 8A, fixed electrode 5, moving magnetic body 11, and fixed magnetic body 10. Further, when a current is carried between the fixed stem and the moving stem with the vacuum interrupter being in a closed state, a repulsive force to put the vacuum interrupter toward an open state can be reduced.

The mechanism of the generation of repulsive force has been mentioned above by taking a conventional vacuum interrupter as an example. As mentioned before, the repulsive force is caused by Lorentz forces Fu and Fd due to current components Icu and Icd flowing in the vacuum interrupter in a closed state. If the contact part is limited to protrusion 8x of central portion 8c, the current does not flow through the wings, resulting in reduction in repulsive force.

Further, when a current is carried between the fixed stem and the moving stem with the vacuum interrupter being in a closed state, the generation of Joule loss can be reduced. Fixed electrode 5 and moving electrode 8, which are made of an alloy mainly composed of a conductive material (e.g., copper or silver), have a lower conductivity than, for example, pure copper. In order to reduce the Joule loss, it is preferred that the current-carrying path through fixed electrode 5 and moving electrode 8 be made shortest. A conventional vacuum interrupter, in which a current flows along the wings, has a long current-carrying path. By contrast, in embodiment 2, in which the contact portion is limited to central portion 8c, a current does not flow through the wings, thus allowing a shorter current path length.

The above describes a mode in which protrusion 8x is located at central portion 8c of contact surface 8f of moving electrode 8A. Alternatively, however, the protrusion may be located on the fixed electrode, or may be located on both moving electrode 8A and the fixed electrode.

Further, while protrusion 8x is located at central portion 8c in the above-described mode, protrusion 8x may be located at any position other than central portions 8c and 5c that can limit the position of initial arc discharge occurrence to protrusion 8x.

Embodiment 2 can provide the same advantageous effects as those of vacuum interrupter 100 in embodiment 1. Additionally, embodiment 2 can simplify the design of moving electrode (8, 8A), fixed electrode 5, moving magnetic body 11, and fixed magnetic body 10, resulting in reduction in product cost. Also, a small-sized, reliable vacuum interrupter can be provided.

Further, embodiment 2 can provide a small-sized, reliable vacuum interrupter with a reduced magnitude of electromagnetic repulsive force, without upsizing and complication of the reduction load application mechanism. Still further, embodiment 2 can provide an efficient vacuum interrupter having a reduced Joule loss.

Embodiment 3

Embodiment 1 describes a mode in which notch 11n of moving magnetic body 11 is 180 degrees rotationally displaced from notch 10n of fixed magnetic body 10 around a Z-direction axis.

Embodiment 3 describes a mode in which notch 11n is rotationally displaced from notch 10n by an angle other than 180 degrees around the Z direction, so that the two regions where the solid part of moving magnetic body 11 overlaps with the solid part of fixed magnetic body 10 (i.e., regions v1 and v2 in embodiment 1) have different areas.

FIG. 14(a) shows a layout of moving magnetic body 11 and fixed magnetic body 10 as seen from front in the Z direction, with the directions of leakage fluxes Mv, Mvr, and Mp added therein. Regions v1w and v2n are the region where the solid part of moving magnetic body 11 overlaps with the solid part of fixed magnetic body 10.

FIG. 14(b) is a front view illustrating the state of arc discharges (a1, a3) on contact surface 5f of fixed electrode 5.

In FIG. 14, the same reference numbers or signs as those of FIGS. 1 to 13 designate the same or equivalent elements as those described in embodiments 1 and 2, and thus the detailed description of such elements is omitted.

With reference to FIG. 14(a), notch 11n of moving magnetic body 11 is displaced from notch 10n of fixed magnetic body 10 around the Z direction by an angle θm other than 180 degrees.

Accordingly, region v1w and region v2n are not equal in area. Here, region v2n has a smaller area than region v1w.

Leakage flux Mvn mainly passes through region v2n, whereas leakage flux Mvr mainly passes through region v1w. By the nature of magnetic field, leakage fluxes Mvn and Mvr equally contribute to the parallel magnetic field intensity. Accordingly, region v2n has a higher magnetic flux density than region v1w.

With reference to FIG. 14(b), an arc discharge typically has the property of moving to a place having a higher intensity of magnetic field parallel to the discharge current (parallel magnetic field), as described above. Accordingly, arc discharge a1 from central portion 8c to central portion 5c moves in the direction di to region v2n (to the position of arc discharge a3).

Then, with Lorentz force Fa, arc discharge a3 circulates on contact surface 8f of moving electrode 8 and on contact surface 5f of fixed electrode 5, thereby being cooled and extinguished, as in embodiment 1.

That is, an initial arc discharge can be guided to move in direction di. This allows a simplified design of the moving electrode, the fixed electrode, the fixed magnetic body, and the moving magnetic body, as in embodiment 2.

Embodiment 3 can provide the same advantageous effects as those of vacuum interrupter 100 in embodiment 1. Additionally, embodiment 3 can simplify the design of the moving electrode, the fixed electrode, the fixed magnetic body, and the moving magnetic body, resulting in reduction in product cost. Also, a small-sized, reliable vacuum interrupter can be provided.

Embodiment 4

Embodiment 4 describes a mode in which a gap 13 is provided between moving electrode 8 and moving magnetic body 11, and by fixed electrode 5 and fixed magnetic body 10.

FIG. 15 is a cross-sectional view illustrating a part including fixed electrode 5, moving electrode 8, and their surrounding area of a vacuum interrupter.

In FIG. 15, the same reference numbers or signs as those of FIGS. 1 to 13 designate the same or equivalent elements as those described in embodiments 1 and 2, and thus the detailed description of such elements is omitted.

With reference to FIG. 15, gap 13 is provided between moving electrode 8 and moving magnetic body 11, and by fixed electrode 5 and fixed magnetic body 10.

Embodiment 1 describes a mode with no gap 13, where an arc discharge occurring at the time of interruption operation causes current Ia to flow through wings 8w of moving electrode 8 in the Y direction and through wings 5w of fixed electrode 5 in the direction opposite to the Y direction.

Specifically, with no gap 13, current Ia branches into a current component Iam flowing from moving current-carrying stem 7 to wings 8w, and a current component Ias flowing from moving current-carrying stem 7 to wings 8w via moving magnetic body 11.

Current component Iam contributes to Lorentz force Fa that drives an arc discharge, whereas current component Ias does not contribute to Lorentz force Fa.

Gap 13 can decrease current component Ias and increase current component Iam, thus strengthening Lorentz force Fa. That is, Lorentz force Fa can improve the effectiveness of driving an arc discharge to extinguish it.

Embodiment 4 can provide the same advantageous effects as those of vacuum interrupter 100 in embodiment 1. Additionally, embodiment 4 can provide a small-sized, reliable vacuum interrupter that can improve the effectiveness of driving an arc discharge to extinguish it.

Next, examples according to embodiment 4 are shown. The examples have different widths ds of gap 13 (see FIG. 15), and their effects are compared.

Comparison Examples

FIG. 16 is a graph comparing the arc-driving forces among three types of vacuum interrupters: with no gap 13, “no”; with gap 13 having a relatively narrow width ds, “narrow”; and with gap 13 having a relatively wide width ds, “wide”. The arc-driving force is a value obtained by calculating a Lorentz force on an arc discharge by electromagnetic field calculation. The vertical axis shows the relative value of arc-driving force.

FIG. 16 shows that gap 13 having a wider width ds produces a stronger arc-driving force. This results in an efficient decrease in current component Ias and increase in current component Iam, thus strengthening Lorentz force Fa.

Embodiment 5

Embodiment 5 describes a vacuum interrupter 110 in which a moving magnetic body 11B has inclined portions 11s in the vicinity of notch 11n, and a fixed magnetic body 10B has inclined portions 10s in the vicinity of notch 10n.

Further, as a variation of embodiment 5, a vacuum interrupter 120 is also described in which a moving magnetic body 11C has step portions 11e in the vicinity of notch 11n, and a fixed magnetic body 10C has step portions 10e in the vicinity of notch 10n.

These structures can improve the intensities of leakage fluxes Mv and Mvr and quickly extinguish an arc discharge.

With reference to FIGS. 18 to 23, description will now be given to the differences of vacuum interrupter 110 in embodiment 5 from vacuum interrupter 100 in embodiment 1, and to the features of vacuum interrupter 110.

FIG. 18 is a perspective view illustrating a part including moving magnetic body 11B, fixed magnetic body 10B, and their surrounding area of vacuum interrupter 110 in embodiment 5, with the directions of magnetic flux Mr and leakage fluxes Mv, Mvr, and Mp added therein.

FIG. 19 is a side view illustrating, on the upper half of the drawing sheet, a lateral side of moving magnetic body 11B as seen from direction N1 in FIG. 18; and illustrating, on the lower half of the drawing sheet, a lateral side of fixed magnetic body 10B as seen from direction N2 in FIG. 18, with the directions of magnetic flux Mr and leakage fluxes Mv, Mvr, and Mp added therein. Moving electrode 8 and fixed electrode 5 are not shown. Direction N1 coincides with the direction opposite to the Y direction, and direction N2 coincides with the Y direction.

FIG. 20 is a perspective view illustrating a part including moving magnetic body 11, fixed magnetic body 10, and their surrounding area of vacuum interrupter 100 in embodiment 1, with the directions of magnetic flux Mr and leakage fluxes Mv, Mvr, and Mp added therein. Moving electrode 8 and fixed electrode 5 are not shown.

FIG. 21 is a side view illustrating, on the upper half of the drawing sheet, a lateral side of moving magnetic body 11 as seen from direction N1 in FIG. 20; and illustrating, on the lower half of the drawing sheet, a lateral side of fixed magnetic body 10 as seen from direction N2 in FIG. 20, with the directions of magnetic flux Mr and leakage fluxes Mv, Mvr, and Mp added therein. Moving electrode 8 and fixed electrode 5 are not shown. Direction N1 coincides with the direction opposite to the Y direction, and direction N2 coincides with the Y direction.

Further, FIG. 22 is a magnetic circuit diagram illustrating a magnetic circuit of vacuum interrupter 100, and FIG. 23 is a magnetic circuit diagram simplifying the circuit diagram of FIG. 22.

In FIGS. 18 to 23, the same reference numbers or signs as those of FIGS. 1 to 12 designate the same or equivalent elements as those described in embodiment 1, and thus the detailed description of such elements is omitted.

Also, vacuum interrupter 110 in embodiment 5 is similar to vacuum interrupter 100 in embodiment 1 in the regions other than moving magnetic body 11B and fixed magnetic body 10B, and thus the detailed description of the general configuration of vacuum interrupter 110 is also omitted.

Region v1 and region v2 have the same area, denoted by area Sg; and moving magnetic body 11 and fixed magnetic body 10 have the same thickness in the Z direction, denoted by thickness Lc. An end face 11f of moving magnetic body 11 adjoining notch 11n and an end face 10f of fixed magnetic body 10 adjoining notch 10n have the same area, denoted by area Sb.

First, with reference to FIGS. 20 to 23, description will now be given to the shapes of moving magnetic body 11 and fixed magnetic body 10 of vacuum interrupter 100 and the magnetic fluxes generated in embodiment 1, and further given to a magnetic circuit formed by vacuum interrupter 100.

Notches 11n and 10n, which have a low magnetic permeance, cause magnetic flux Mr to branch into leakage flux Mp and leakage flux Mv. That is, the relation of (the total quantity of magnetic flux Mr)=(the total quantity of leakage flux Mp)+(the total quantity of leakage flux Mv) is satisfied. Similarly, magnetic flux Mr branches into leakage flux Mp and leakage flux Mvr, and thus the relation of (the total quantity of magnetic flux Mr)=(the total quantity of leakage flux Mp)+(the total quantity of leakage flux Mvr) is satisfied.

Further, with reference to FIG. 22, description will now be given to a magnetic circuit related to magnetic flux Mr and leakage fluxes Mv, Mvr, and Mp.

As to moving magnetic body 11, the magnetic reluctance of notch 11n through which leakage flux Mp transmits is Db/(μ·Sb), where Sb denotes the area of end face 11f of moving magnetic body 11, Db denotes the distance between the edges of end face 11f, and μ denotes the magnetic permeability.

Similarly, as to fixed magnetic body 10, the magnetic reluctance of notch 10n through which leakage flux Mp transmits is Db/(μ·Sb), where Sb denotes the area of end face 10f of fixed magnetic body 10, and Db denotes the distance between the edges of end face 10f.

The magnetic reluctance between moving magnetic body 11 and fixed magnetic body 10 through which leakage flux Mv transmits is Dg/(μ·Sg), where Sg denotes the area of region v2, and Dg denotes the distance between moving magnetic body 11 and fixed magnetic body 10.

Similarly, the magnetic reluctance between moving magnetic body 11 and fixed magnetic body 10 through which leakage flux Mvr transmits is Dg/(μ·Sg), where Sg denotes the area of region v1, and Dg denotes the distance between moving magnetic body 11 and fixed magnetic body 10.

Leakage fluxes Mv and Mvr are opposite in direction but equal in absolute value. Accordingly, the magnetic circuit shown in FIG. 22 can be replaced by a simplified magnetic circuit shown in FIG. 23 because of the symmetry. Further, formula 1 below can be derived from the magnetic circuit of FIG. 23.

$\begin{matrix} M v = M r \times \frac{\frac{D b}{μ \cdot Sb}}{\frac{D g}{μ \cdot Sg} + \frac{D b}{μ \cdot Sb}} = M r \times \frac{1}{1 + \frac{D g}{D b} \times \frac{S b}{S g}} & [Formula 1] \end{matrix}$

Formula 1 shows that leakage fluxes Mv and Mvr can be increased by increasing distance Db between the edges and by decreasing area Sb.

Next, with reference to FIGS. 18 and 19, vacuum interrupter 110 in embodiment 5 will now be described.

Vacuum interrupter 100 in embodiment 1 described above has moving magnetic body 11 and fixed magnetic body 10. However, vacuum interrupter 110 has moving magnetic body 11B, instead of moving magnetic body 11, and fixed magnetic body 10B, instead of fixed magnetic body 10.

Moving magnetic body 11B includes inclined portions 11s at its both ends adjoining notch 11n, each inclined portion 11s having an inclined surface R. Similarly, fixed magnetic body 10B includes inclined portions 10s at its both ends adjoining notch 10n, each inclined portion 10s having inclined surface R. Moving magnetic body 11B and fixed magnetic body 10B have the same shape. Specifically, inclined portions 11s and inclined portions 10s have the same shape.

Regions v1 and v2 each have area Sg, the same as that of vacuum interrupter 100; and moving magnetic body 11B and fixed magnetic body 10B each have thickness Lc in the Z direction, the same as that of vacuum interrupter 100.

Further, the area of an end face 11Bf of moving magnetic body 11B adjoining notch 11n, and the area of an end face 10Bf of fixed magnetic body 10B adjoining notch 10n are each denoted by area Sc.

The advantageous effects of inclined portions 11s and 10s will now be described.

As to moving magnetic body 11B, its end face 11Bf adjoining notch 11n has area Sc satisfying area Sc<area Sb. This is because, due to moving magnetic body 11B having inclined surfaces R, the length component of end face 11Bf in the Z direction satisfies (Lc−Rz), where Rz denotes the length component of inclined surfaces R in the Z direction.

The distance between one end face 11Bf and the other end face 11Bf is set to Db. Further, average distance Ds between the inclined portions, i.e., the average distance between one inclined portion 11s and the other inclined portion 11s, satisfies Ds=((Rx·Rz)/Lc+Db), where Rx denotes the length component of inclined surfaces R in the X direction, and Rz denotes the length component of inclined surfaces R in the Z direction. Since Rx>0 and Rz>0 are satisfied, Ds>Db is always satisfied. In other words, inclined portions 11s of moving magnetic body 11B allow the effective distance between the inclined portions to be longer than Db.

In view of formula 1, providing inclined portions 11s and 10s and setting average distance Ds between the inclined portions and area Sc is equivalent to increasing distance Db between the edges and decreasing area Sb as described above. Thus, the intensities of leakage fluxes Mv and Mvr can be strengthened.

The description of moving magnetic body 11B also applies to fixed magnetic body 10B, which has the same shape as moving magnetic body 11B. Thus, fixed magnetic body 10B can also strengthen the intensities of leakage fluxes Mv and Mvr.

Providing inclined portions 11s and 10s can thus strengthen the parallel magnetic field intensity. This allows an arc discharge to move to region v1 or v2, thereby improving the effectiveness of extinguishing the arc discharge.

With reference to FIGS. 24 and 25, the features of vacuum interrupter 120 in a variation of embodiment 5 will now be described.

FIG. 24 is a perspective view illustrating a part including moving magnetic body 11C, fixed magnetic body 10C, and their surrounding area of vacuum interrupter 120 in the variation of embodiment 5, with the directions of magnetic flux Mr and leakage fluxes Mv, Mvr, and Mp added therein.

FIG. 25 is a side view illustrating, on the upper half of the drawing sheet, a lateral side of moving magnetic body 11C as seen from direction N1 in FIG. 24; and illustrating, on the lower half of the drawing sheet, a lateral side of fixed magnetic body 10C as seen from direction N2 in FIG. 24, with the directions of magnetic flux Mr and leakage fluxes Mv, Mvr, and Mp added therein. Moving electrode 8 and fixed electrode 5 are not shown. Direction N1 coincides with the direction opposite to the Y direction, and direction N2 coincides with the Y direction.

In FIGS. 24 and 25, the same reference numbers or signs as those of FIGS. 1 to 12 and 18 to 23 designate the same or equivalent elements as those described in embodiment 1, and thus the detailed description of such elements is omitted.

Also, vacuum interrupter 120 is similar to vacuum interrupter 100 in embodiment 1 in the regions other than moving magnetic body 11C and fixed magnetic body 10C, and thus the detailed description of the general configuration of vacuum interrupter 120 is also omitted.

Vacuum interrupter 100 in embodiment 1 described above has moving magnetic body 11 and fixed magnetic body 10. However, vacuum interrupter 120 has moving magnetic body 11C, instead of moving magnetic body 11, and fixed magnetic body 10C, instead of fixed magnetic body 10.

Moving magnetic body 11C includes step portions 11e at its both ends adjoining notch 11n, each step portion 11e having a stepped surface E. Similarly, fixed magnetic body 10C includes step portions 10e at its both ends adjoining notch 10n, each step portion 10e having stepped surface E. Moving magnetic body 11C and fixed magnetic body 10C have the same shape. Specifically, step portions 11e and step portions 10e have the same shape.

Moving magnetic body 11C includes plate magnetic members 11c1 and 11c2 one on top of the other. Similarly, fixed magnetic body 10C includes plate magnetic members 10c1 and 10c2 one on top of the other. Magnetic members 11c1 and 10c1 have the same shape, and their thickness in the Z direction is a length component Ez.

Magnetic members 11c2 and 10c2 have the same shape, and their thickness in the Z direction is a thickness (Lc−Ez).

Plate magnetic members 11c1 and 10c1 are an example of the first plate magnetic body in the claims, and plate magnetic members 11c2 and 10c2 are an example of the second plate magnetic body in the claims.

Further, the area of an end face 11Cf of moving magnetic body 11C adjoining notch 11n, and the area of an end face 10Cf of fixed magnetic body 10C adjoining notch 10n are each denoted by area Sd.

The advantageous effects of step portions 11e and 10e will now be described.

As to moving magnetic body 11C, its end face 11Cf adjoining notch 11n has area Sd satisfying area Sd<area Sb. This is because, due to moving magnetic body 11C having stepped surfaces E, length component Rz of stepped surfaces E in the Z direction satisfies Rz=(Lc−Ez)<Lc.

The distance between one end face 11Cf and the other end face 11Cf is set to Db. Further, average distance De between the step portions, i.e., the average distance between one step portion 11e and the other step portion 11e, satisfies De=((2·Ex·Ez)/Lc+Db), where Ex denotes the length component of stepped surfaces E in the X direction, and Ez denotes the length component of stepped surfaces E in the Z direction. Since Ex>0 and Ez>0 are satisfied, De>Db is always satisfied. In other words, step portions 11e of moving magnetic body 11C allow the effective distance between the inclined portions to be longer than Db.

In view of formula 1, providing step portions 11e and 10e and setting average distance De between the step portions and area Sd is equivalent to increasing distance Db between the edges and decreasing area Sb as described above. Thus, the intensities of leakage fluxes Mv and Mvr can be strengthened.

The description of moving magnetic body 11C also applies to fixed magnetic body 10C, which has the same shape as moving magnetic body 11C. Thus, fixed magnetic body 10C can also strengthen the intensities of leakage fluxes Mv and Mvr.

Providing step portions 11e and 10e can thus strengthen the parallel magnetic field intensity. This allows an arc discharge to move to region v1 or v2, thereby improving the effectiveness of extinguishing the arc discharge.

In the above description, two plate magnetic members, 11c1 and 11c2, are placed one on top of the other to form stepped surfaces E of the step of step portions 11e. However, three or more plate magnetic members may be placed one on top of another to form a plurality of stepped surfaces. Similarly, as to step portions 10e, a plurality of stepped surfaces may be formed.

Embodiment 5 can provide the same advantageous effects as those of vacuum interrupter 100 in embodiment 1. Additionally, embodiment 5 can strengthen the parallel magnetic field intensity, thereby improving the effectiveness of extinguishing an arc discharge. In other words, a small-sized, reliable vacuum interrupter can be provided that can improve the effectiveness of extinguishing an arc discharge.

Embodiment 6

Embodiment 6 describes a vacuum interrupter 130 in which a moving magnetic body 11D has a magnetic deterioration portion 11r, instead of notch 11n, and a fixed magnetic body 10D has a magnetic deterioration portion 10r, instead of notch 10n.

Such a structure can improve the effectiveness of protecting parts from the metal vapor and metal particles scattering from moving electrode 8 and fixed electrode 5 due to the heat from arc discharge.

FIG. 26 is a perspective view illustrating a part including moving magnetic body 11D, fixed magnetic body 10D, and their surrounding area of vacuum interrupter 130 in embodiment 6, with the directions of magnetic flux Mr and leakage fluxes Mv, Mvr, and Mp added therein.

In FIG. 26, the same reference numbers or signs as those of FIG. 24 designate the same or equivalent elements as those described in the variation of embodiment 5, and thus the detailed description of such elements is omitted.

Also, vacuum interrupter 130 in embodiment 6 is similar to vacuum interrupter 120 in the variation of embodiment 5 in the regions other than moving magnetic body 11D and fixed magnetic body 10D, and thus the detailed description of the general configuration of vacuum interrupter 130 is also omitted.

The lateral side of vacuum interrupter 130 is similar to FIG. 25 except that notch 11n is replaced with magnetic deterioration portion 11r and that notch 10n is replaced with magnetic deterioration portion 10r. Thus, the lateral side of vacuum interrupter 130 is not shown here. Further, the directions of magnetic flux Mr and leakage fluxes Mv, Mvr, and Mp are the same as those of FIG. 25, and thus they are not shown here.

With reference to FIG. 26, the structure of moving magnetic body 11D and fixed magnetic body 10D will now be described.

Moving magnetic body 11D includes plate magnetic members 11c1 and 11d2 one on top of the other. Magnetic member 11c1 is similar to that of the variation of embodiment 5. Magnetic member 11d2 has magnetic deterioration portion 11r, instead of notch 11n.

Magnetic deterioration portion 11r is formed by magnetically deteriorating a part of magnetic member 11d2 by, for example, applying a pressure. In other words, magnetic deterioration portion 11r has a lower magnetic permeance than the other part of magnetic member 11d2.

Similarly, fixed magnetic body 10D includes plate magnetic members 10c1 and 10d2 one on top of the other. Magnetic member 10c1 is similar to that of the variation of embodiment 5. Magnetic member 10d2 has magnetic deterioration portion 10r (not shown), instead of notch 10n.

Magnetic deterioration portion 10r is formed by magnetically deteriorating a part of magnetic member 10d2 by, for example, applying a pressure. In other words, magnetic deterioration portion 10r has a lower magnetic permeance than the other part of magnetic member 10d2.

Magnetic deterioration portions 10r and 11r are an example of the first magnetic deterioration portion in the claims, and plate magnetic members 11d2 and 10d2 are an example of the second plate magnetic body in the claims.

The magnetic permeance of magnetic deterioration portions 11r and 10r is set to equal to the magnetic permeance of notches 11n and 10n. Thus, the magnetic flux flowing through magnetic deterioration portions 11r and 10r is equal to the total quantity of leakage flux Mp. Accordingly, vacuum interrupter 130 in embodiment 6 can strengthen the parallel magnetic field intensity, thereby improving the effectiveness of extinguishing an arc discharge, as with vacuum interrupter 120 in embodiment 5.

As mentioned above, the heat from arc discharge causes metal vapor and metal particles to scatter from moving electrode 8 and fixed electrode 5. With a vacuum interrupter (100, 110, 120) having an open notch (10n, 11n), the metal vapor and metal particles might scatter through the notch (10n, 11n).

By contrast, vacuum interrupter 130 in embodiment 6 has a non-open magnetic deterioration portion (10r, 11r) through which the metal vapor and metal particles cannot scatter, instead of the open notch (10n, 11n). That is, the magnetic deterioration portion (10r, 11r) can prevent the metal vapor and metal particles from scattering.

Embodiment 6 can provide the same advantageous effects as those of vacuum interrupter 120 in embodiment 5. Additionally, embodiment 6 has the effect of preventing scattering of metal vapor and metal particles caused by the heat from arc discharge. In other words, a small-sized, reliable vacuum interrupter can be provided that can improve the effectiveness of extinguishing an arc discharge.

In embodiments 1 to 5, the magnetic body (10, 10A, 10B, 10C, 11, 11A, 11B, 11C) strengthens the parallel magnetic field intensity by including the notch (10n, 11n) having a lower magnetic permeance than the solid part. Similarly, in embodiment 6, the magnetic body (10D, 11D) strengthens the parallel magnetic field intensity by including the magnetic deterioration portion (10r, 11r) having a lower magnetic permeance which is formed by deteriorating a part of the magnetic body (10D, 11D).

That is, it is simply required that the magnetic body (10, 10A, 10B, 10C, 10D, 11, 11A, 11B, 11C, 11D) include a lower magnetic permeance portion, which is a portion having a lower magnetic permeance. The lower magnetic permeance portion may be a groove formed in a part of the magnetic body, instead of the notch (10n, 11n) or magnetic deterioration portion (10r, 11r).

For example, the groove may be formed by cutting the magnetic body in the thickness direction from its surface to an appropriate depth by machining.

In embodiments 5 and 6, the magnetic body (10B, 10C, 10D, 11B, 11C, 11D) include the inclined portions (10s, 11s) or step portions (10e, 11e) disposed at its both ends adjoining the notch (10n, 11n) or magnetic deterioration portion (10r, 11r). The inclined portions (10s, 11s) or step portions (10e, 11e) have a reduced magnetic permeance as compared to the other portion except the notch (10n, 11n), thus strengthening the parallel magnetic field intensity.

That is, it is simply required that the magnetic body (10B, 10C, 11B, 11C) include a magnetic permeance reduction portion at its both ends adjoining the notch (10n, 11n), the magnetic permeance reduction portion having a reduced magnetic permeance. The magnetic permeance reduction portion may be a second magnetic deterioration portion having a lower degree of magnetic deterioration than the first magnetic deterioration portion.

In the above description, step portions 11e include magnetic members 11c1 and 11c2 one on top of the other. However, step portions 11e may be made of a single magnetic member. Specifically, the magnetic permeance reduction portion may be formed by machining.

In the above description, the magnetic permeance reduction portion is disposed at both ends of the lower magnetic permeance portion. However, the magnetic permeance reduction portion may be disposed at only one end of the lower magnetic permeance portion, in which case the effect of strengthening the parallel magnetic field intensity can still be obtained.

Embodiments 1 to 6 describe examples in which the notch (10n, 11n) or magnetic deterioration portion (10r, 11r) is disposed on both fixed current-carrying stem 4 and moving current-carrying stem 7. However, the notch (10n, 11n) or magnetic deterioration portion (10r, 11r) may be disposed on only one of fixed current-carrying stem 4 and moving current-carrying stem 7, in which case an arc discharge can still be driven and extinguished by forming a parallel magnetic field.

Embodiments 1 to 4 describe examples in which the region on the edge portion (5e, 8e) side relative to the central portion (5c, 8c) has wings (5w, 8w). However, the region on the edge portion (5e, 8e) side relative to the central portion (5c, 8c) may have other configurations that have the effect of driving and extinguishing arc discharge.

In embodiments 1 to 4, an electrode (5, 8) has three slits (5s, 8s) dividing the outer periphery of the electrode (5, 8) into three parts, thus creating three circular segment portions (5a, 8a) and three wings (5w, 8w). Although the slits (5s, 8s) create three divisions herein, two or four or more divisions can still provide the advantageous effects. In other words, the present invention does not depend on the number of divisions.

In the present invention, the embodiments may be combined in any manner or modified or omitted as appropriate within the scope of the present invention. For example, embodiments 2 and 4 may be combined so that a moving electrode has a contact surface with a protrusion and also has a gap provided between the moving electrode and the moving magnetic body. Alternatively, embodiments 2 to 4 and 5 may be combined so that each magnetic body (10, 10A, 11, 11A) has a magnetic permeance reduction portion.

REFERENCE SIGNS LIST

- 4: fixed current-carrying stem; 4f: stem surface; 5: fixed electrode; 5a: circular segment portion; 5c: central portion; 5e: edge portion; 5f: contact surface; 5s: slit; 5t: tip; 5w: wing; 7: moving current-carrying stem; 7f: stem surface; 8, 8A: moving electrode; 8a: circular segment portion; 8c: central portion; 8e: edge portion; 8f: contact surface; 8s: slit; 8w: wing; 8x: protrusion; 10, 10A, 10B, 10C: fixed magnetic body; 10n: notch; 10r: magnetic deterioration portion; 10s: inclined portion; 10e: step portion; 11, 11A, 11B, 11C: moving magnetic body; 11c1: magnetic member; 11c2, 11d2: magnetic member; 11n: notch; 11r: magnetic deterioration portion; 13: gap; 100, 110, 120, 130: vacuum interrupter

VACUUM INTERRUPTER

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