[0001] This in\ention relotes to on air breuk switch, and to a method of reducing shock
wave generation in operation of such switch.
[0002] Previous air break switches have suffered from the disadvantage that when separate
contacts of the switch are opened, an electrical arc con occur within the switch casing,
this arc generating (air) shock fronts within the switch, often causing considerable
damage to the switch.
[0003] Switches have been proposed (GB-A-1,499,486) in which flow of arc current through
conductive parts of the switch provides a blow-out magnetic field which causes the
arc to move with high velocity away from the contacts in order to avoid damage to
the contacts. However, such high velocity movement of the arc tends to maintain or
augment air shock fronts generated by the arc, and such shock fronts may damage the
switch.
[0004] Switches have also been proposed (GB-A-267,515) in which magnetically susceptible
material is positioned in the switch so as to deflect the magnetic field due to flow
of arc current, the deflected field being capable of acting as a blow-out field.
[0005] It is an aim of this invention to provide an air break switch in which such shock
fronts are prevented from attaining sufficient strength to damage the switch.
[0006] According to a first aspect of the invention I provide an air break switch comprising
two electrical contacts which can undergo relative motion between open and closed
positions, and a coil through which at least part of the current undergoing interruption
flows and which, preferably in conjunction with magnetically susceptible material,
provides a magnetic field in the vicinity of at least one of the contacts, characterised
in that the magnetic field is substantially normal to a shock front which tends to
be set up by establishment of an arc between the contacts and has a value such as
to cause the Alfven speed, at least in said vicinity in plasma associated with the
arc, to be significantly in excess of the air speed attainable by such shock front.
[0007] The coil may be connected in series with the contacts.
[0008] Alternatively or additionally the coil may be powered by an energy source other than
the switched current, and derived from or controlled by other contacts of a circuit
and said switch operating in timed relation to those between which it is desired to
reduce shock wave generation.
[0009] Current flow in the electrical arc which occurs between the contacts has a magnetic
effect which tends to aid development of any shock front associated with such an arc.
With the establishment of a field as provided by the invention, a significant fraction
of energy released by any such arc can be dispersed mainly by relatively harmless
oscillations of the plasma rather than mainly (as would occur in prior art switches)
by one or more potentially damaging air shock fronts.
[0010] The switch may have an arc chamber for containing the arc while the energy thereof
is dispersed, and in said vicinity the field may be directed transversely to the length
of the arc (along the direction of relative separating motion of the contacts) between
the contacts and lengthwise of a path of arc travel extending from said vicinity into
the chamber.
[0011] In any such arrangement the field may be directed transversely of the shortest path
between the contacts when they are separated.
[0012] Air-occupied space encompassed by part or all of the coil may provide at least a
part of the arc chamber. This ensures the presence of the field within the arc chamber.
[0013] Alternatively or additionally, at least a part of the coil may lie around at least
one other switch component defining the arc chamber.
[0014] The arc chamber may be provided with chutes and/or runners which help to disperse
the energy of the arc by operating to sub-divide the arc..
[0015] According to a further aspect of the invention, provide a method of at least reducing
the generation of a shock wave at the site of an arc established between separable
contacts of a switch as these contacts open, said method comprising causing the current
feeding the arc to flow in a configuration establishing, preferably in conjunction
with magnetically susceptible material, a magnetic field at the site of the arc, characterised
in that such field is substantially normal to any shock front which would otherwise
tend to be set up by the establishment of the arc and the field is of a form and strength
to cause the Alfven speed, at least in the vicinity of said site and in plasma associated
with the-orc, to be significantly in excess of the air speed attainable by such shock
front.
[0016] Two embodiments of the invention will now be described, by way of example only, with
reference to the accompanying drawings wherein:-
FIGURE I is a diagrammatic side elevation of a first air break switch embodying the
invention;
FIGURE 2 is a diagrammatic enlarged sectional side elevation of a portion of the switch
shown in side elevation in Figure I; and.
FIGURE 3 is a diagrammatic partially sectional side elevation of a portion of a further
air break switch embodying the invention.
[0017] Figure I of the drawings shows an air break switch 10 comprising a pair of electrical
contacts I and 15 and a further pair of electrical contacts 12 and 16. An operating
means for making and breaking on electrical connection between the two contacts of
each pair is indicated at 13.
[0018] In order to permit current flow through the switch, operating means 13 is used to
move an electrically conductive connecting member 14 which carries or incorporates
contacts 15 and 16 so that contacts 15 and 16 conductively abut fixed contacts I and
12 respectively, to permit a current flow through the switch via member 14 and both
pairs of contacts.
[0019] During movement of member 14, at stages when there is only a small air gap between
contact I and contact 15 and/or there is only a small air gap between contact 12 and
contact 16, it is possible that an electrical arc will occur in any such gap, said
arc ionising the air along its path to form a plasma. The arc thus effectively continues
to form a conductive link between the contacts. Such an arc generates intense heat
and tends to generate shock fronts in the surrounding air.
[0020] In order to limit the development of such shock fronts, an electrically conductive
coil 20 which may be of an elongate essentially rectangular form, as viewed in plan,
is provided around the perimeter of an arc chamber 17 and is seen in Figure I from
a direction perpendicular to one of its longer sides. If desired, said coil may surround
more of said switch than is the case in Figures 1 and 2 and said coil may, for example,
extend further in a direction towards the operating means 13 up to or beyond said
contacts so that a part of said coil lies around said contacts.
[0021] One end 20a of said coil is conductively connected to contact 12 by connector 21,
and the other end 20b of said coil is connected to a terminal 22. Contact 11 is conductively
connected to a further terminal 23 via a solenoid 24 and a bi-metallic strip 25. In
use, the air break switch is connected into an external circuit using terminals 22
and 23.
[0022] Coil 20 is thus in series with contacts 11 and 15, member 14, and contacts 16 and
12, and carries all the current which flows through the switch either via only the
contacts and member 14 or via the contacts and member 14 and an arc or arcs between
contacts of either pair. As a result of carrying said current, coil 20 generates a
magnetic field which occupies said chamber 17 and extends into the vicinities of contacts
II, 12, 15, and 16.
[0023] A biasing spring 26 is provided which may be made of a magnetically susceptible material,
such as steel for example, and consequently serves a dual purpose of urging contacts
15 and 16 on member 14 to make good electrical contact with contacts I and 12 respectively,
when required, and of acting as a flux director which causes said field to pass through
a gap between the two contacts of each pair when current flows through the switch
due to the establishment of an arc between those contacts.
[0024] All of the contacts 11, 12, 15 and 16 in the embodiment illustrated in Figures and
2 lie between said biasing spring 26 and said coil 20.
[0025] Additionally, flux directors 27 are provided specifically in order to direct said
flux between said contacts located between flux directors 27 and .coil 20 in the embodiment
illustrated in Figures 1 and 2. Flux directors 27, as illusirated, are each in the
form of a plate, but each may alternatively be in the form of a rod or may have any
other suitable form.
[0026] Figure 2 shows the lines of force of said magnetic field in a part of said arc chamber
and in the vicinities of the contacts, member 14, connector 21 (of negligible magnetic
susceptibility), spring 26 and one of the flux directors 27. Dashed lines 28 and 29
are typical of these field lines, and all of these lines are substantially parallel
until they emerge from chamber 17.
[0027] A possible path along which an arc could occur between contact 12 and contact 16
is indicated at 30.
[0028] Dashed lines 31 and 32 and similar lines represent successive positions which may
be occupied by a shock front (generated initially by an arc along path 30) as it travels,
by reason of the known magnetic blow-out effect, towards and into chamber 17. The
flux directors have sizes, shapes and positions such that said field is approximately
normal to path 30 and subsequent shock front positions, and such that said field is
enhanced in the vicinity of said contacts.
[0029] Energy released by said arc would, in prior art switches, have been carried away
from said arc mainly by (air) shock fronts in the air within the switch. However,
energy can also be carried away from the arc via oscillations of the plasma of ionised
air produced by the arc.
[0030] In the air break switch in accordance with the invention illustrated in Figures and
2, the magnetic flux is so strong in the region of path 30 that the Alfven speed (i.e.
the speed at which plasma oscillations perpendicular to the field propogate along
the field lines) is so much in excess of any speed of travel attainable by an air
shock front, that the effect of the flux is to bring about dispersal of said energy
by way of oscillations rather than by a unidirectionally travelling shock front. Said
energy is thus very rapidly conveyed by waves of plasma oscillations along said field
lines into chamber 17, where the field lines are more widely spaced than in said region,
and very little energy remains in the vicinity of the arc path at 30 for the generation
of any air shock front. Most of an arc's energy is in fact dispersed by waves of plasma
oscillations before enough time has elapsed for such a shock front to be generated.
[0031] Thus the generation of air shock fronts which could damage said switch is severely
hindered or prevented in this air break switch.
[0032] The arc posses down chutes 18 between runners 19 in said arc chamber parallel to
the magnetic field in said arc chamber. Said runners help to conduct away said energy,
and each runner comprises a plate of thermally conductive/absorptive material arranged
so that its plane is approximately parallel to the magnetic field in the arc chamber.
The runners 19 are not shown in Figure 2, but have end portions which are indicated
in Figure 1.
[0033] The magnetic field produced by the flow of said current in coil 20 which, as mentioned,
is substantially normal to the shock front is arranged to be sufficiently strong to
have a greater effect on the plasma than that due to the known blow-out field set
up by the current flowing in the arc itself.
[0034] A bi-metallic strip 25 is arranged for use in conjunction with solenoid 24 to stop
current flow in said switch when the current becomes too high (the current flows through
the bi-metallic strip, which is heated by the current to a temperature - and consequently
to a deflection - dependent upon the magnitude of that current). Solenoid 24 operates
a plunger 33 which in turn acts on operating means 13.
[0035] A manually operable release lever 34 is provided to allow the switch to be switched
off and/or on manually.
[0036] A speed-controlling spring 35 is used to exert, on operating means 13, a force which
ultimately acts on member 14 to cause the connection between contacts 1 and 15 and
the connection between contacts 12 and 16 to be broken rapidly so as to minimise the
duration of any arcs which may occur.
[0037] Figure 3 shows a portion of a further air break switch 110 in accordance with the
invention.
[0038] Switch 110 comprises a fixed contact 108 and a movable contact 106 on a movable conductive
member 101. Contact !08 is conductively connected via a conductive element 140 to
one end 120a of an electrically conductive coil 120, and the other end 120b of coil
120 is conductively connected via a further conductive element 141 to a further fixed
contact 109 and thence to a terminal 122.
[0039] Suitable insulating portions 142, 143 serve to insulate conductive elements 140,
141 and the coil ends 120a, 120b from each other.
[0040] Conductive member 101 is T-shaped, with contact 106 located on its central stem portion
104 (seen from one side in Figure 3) and a further movable contact 107, fixed with
respect to movable contact 106, on its crossmember 105 (seen end-on in Figure 3),
and is conductively connected to another terminal 160. Terminals 100 and 122 are used
for connecting switch 110 into an external circuit, and the switch 110, when thus
connected, is used to control current flow between those terminals.
[0041] Member 101 is mounted, via a spring 103, on a movable arm 102 which is in turn mounted
on a pivot, said pivot being located at an end (not shown) of arm 102 distant from
spring 103. Figure 3 shows the contacts at their open positions.
[0042] In order to move member 101 to its closed position so as to permit current flow between
terminals 100 and 122, arm 102 is lowered so as to lower member 101 in the direction
indicated by arrow A. Member 101 is mounted and/or balanced in such a way that contacts
106 and 108 conductively abut each other and establish current flow before contacts
107 and 109 abut each other. During opening of the switch no arc occurs between contacts
107 and 109 since contacts 106 and 108 are still in abutting relation and provide
a short circuit across contacts 107, 109. When contacts 106 and 108 begin to separate
and are only a short distance apart, an electrical arc will occur through the air
between them. The coil 120 is effectively in series between contacts 109 and 108 and
will carry the arc current thereby generating a magnetic field in the vicinity of
said arc. This magnetic field is sufficiently strong, and suitably directed (i.e.
approximately normal to any shock front that may be generated by said arc) to hinder
or prevent development of potentially damaging air shock fronts by said arc, said
magnetic field having this effect for the same physical reasons as those given in
the description of the switch 10 of Figures I and 2. Any suitably positioned part
of the switch may be made of magnetically susceptible material, if necessary, in order
to cause the magnetic field to have a suitable strength and direction at least in
the vicinity of contact 108.
[0043] Energy released by any arc in switch 110 is dispersed (by plasma oscillations) along
chutes 118 situated between the base portions 119b (seen in cross-section in Figure
3) of runners 119 which are U-shaped as viewed in plan. Each said runner 119 comprises
a base portion 119b and two side limbs 119a connected to opposite ends of base portion
119b.
[0044] Coil 120 lies around runner base portions 119b, said limbs having their lengths extending
longitudinally of the coil axis and hence approximately parallel to said magnetic
field generated by coil 120.
[0045] Central stem portion 104 of member 101 moves within a part of an arc chamber 117
located between the side limbs 119a of runners 119.
[0046] The features disclosed in the foregoing description, or the following claims, or
the accompanying drawings, expressed in their specific forms or in terms of a means
for performing the disclosed function, or a method or process for attaining the disclosed
result, or a class or group of substances or compositions, as appropriate, may, separately
or any combination of such features, be utilised for realising the invention in diverse
forms thereof.
1. An air break switch (10;110) comprising two electrical contacts (11,15 and/or 12,
16; 106,108) which can undergo relative motion between open and closed positions,
and a coil (20;120) through which at least part of the current undergoing interruption
flows, which, preferably in conjunction with magnetically susceptible material (26,27),
provides a magnetic field in the vicinity of at least one of said contacts (11 or
15, 12 or 16; 106 or 108), characterised in that the magnetic field is substantially
normal to a shock front which tends to be set up by establishment of an arc between
the contacts (11, 15 and/or 12,16; 106,108) and has a value such as to cause the Aifven
speed, at least in said vicinity in plasma associated with the arc, to be significantly
in excess of the air speed attainable by such shock front.
2. An air break switch (10;110) according to claim 1 wherein the coil (20;120) is
connected in series with the contacts (11,15 and/or 12,16; 106, 108).
3. An air break switch (10; (10) according to claim I or claim 2 wherein the direction
and strength of the field in said vicinity causes a significant fraction of energy
released by the arc to be dispersed mainly by oscillations of said plasma rather than
mainly by one or more potentially damaging air shock fronts.
4. An air break switch (10;110) according to any one of the preceding claims wherein
the switch has an arc chamber (17; 117) for containing the arc while the energy thereof
is dispersed, and wherein in said vicinity, the field is directed transversely to
the length of the arc between the contacts (11,15 and/or 12,16; 106,108) and lengthwise
of a path of arc travel extending from said vicinity into the chamber (17; 117).
5. An air break switch (10;110) according to claim 4 wherein part or all of the coil
(20; 120) provides at least a part of the arc chamber (17;117).
6. An air break switch (10; 110) according to claim 4 or claim 5 wherein at least
a part of the coil (20;120) lies around at least one other switch component defining
the arc chamber (17; 117).
7. An air break switch (10; 110) according to any one of the preceding claims wherein
the switch includes chutes (18; 118) or runners (19; 119) for sub-dividing the arc
and wherein the magnetic field set up by the coil (20; 120) extends lengthwise of
the chutes (18; 118) or runners (19; 119).
8. An air break switch (10;110) according to claim 7 wherein the coil (20; 120) is
wound around at least portions of the chutes (18; 118) or runners (19; 119) with its
axis parallel, or approximately parallel, to the lengths of the chutes (18; 118) or
runners (19;119).
9. An air break switch (110) according to any one of the preceding claims wherein
the contacts (106 to 109) comprise a first cooperative pair (107,109) connected in
parallel through said coil (120) with a second co-operative pair (106,108), which
latter pair (106, 108) are arranged to open after the first pair (107,109) has opened,
the arc being established between the second pair (106,108).
10. An air break switch (110) according to claim 9 wherein one of the contacts (106)
of the second pair (106,108) is carried on the stem (104) of a T-shaped contact member
(101), the cross piece (105) of which acts as one of the contacts (107) of the first
pair (107,109), the other contact (108) of the second pair (106, 108) and the other
contact (109) of the first pair (107,109) being spaced from each other so that the
pairs of contacts (107,109 and 106,108) open in the required sequence and being electrically
connected to each other through said coil (120).
11. A method of at least reducing the generation of a shock wave at the site of an
arc established between separable contacts (11,15 and/or 12,16; 106,108) of a switch
(10; 110) as these contacts (11, 15 and/or 12,16; 106,108) open, said method comprising
causing the current feeding the arc to flow in a configuration establishing a magnetic
field at the site of the arc, characterised in that such field is substantially normal
to a shock front which tends to be set up by the establishment of the arc and is of
a form and strength to cause the Alfven speed at least in the vicinity of said site
and in plasma associated with the arc to be significantly in excess of the air speed
attainable by such shock front.
12. A method according to claim 11 wherein the field is established by the current
in conjunction with magnetically susceptible material (26,27).