GB2312861A - Valves in continuous casting - Google Patents

Abstract

In the continuous casting of steel the liquid, molten, metal is poured under gravity from a reservoir container known as a tundish through a tube into an open-bottomed, water-cooled mould from which a solidifying strand of steel is withdrawn continuously. Accurate control of the pouring is traditionally accomplished by hydraulic manipulation either of a slide gate fitting across the pouring tube or of a conical ceramic stopper in the tundish outlet, but these devices are subject to blockage and erosion, to freezing up of the apertures through which the melt passes, to leakage, and to wear, all of which make accurate control difficult and necessitate frequent replacement of the moving parts. Ideally, a control valve for this sort of use should have no moving parts, be capable of rapid and continuously variable flow rate adjustment, be usable with standard pouring tubes, and should be small and light. The present invention proposes a form of electromagnetic valve which substantially or wholly meets the desired criteria. More specifically there is to be created across or around the outlet/pouring tube (channel) of the molten metal reservoir ( the tundish, for example) an alternating electromagnetic field, that there be induced electrical currents - eddy currents - in the molten metal as it passes through this field, which eddy currents interact, directly or indirectly, with the applied magnetic field, and that the directions and magnitudes of the field and of the induced eddy currents are arranged such that forces are generated in the molten metal which oppose the downward flow of the liquid and so provide the desired controllability of the passage of the metal through the outlet. The channel may have a reducing cross-section or alternatively there may be two magnetic field generators.

Description

Valves This invention relates to valves, and concerns in particular valves for controlling the flow of elecrically-conductive fluids, for example molten metals from a reservoir thereof.

In the continuous casting of steel the liquid, molten, metal is poured under gravity from a reservoir container known as a tundish into an open-bottomed, water-cooled mould from which a solidifying strand of steel is withdrawn continuously; the tundish may have either an open nozzle or an elongate pouring tube the free end of which is actually submerged in the mould contents. In many applications there are used pouring tubes which have internal diameters ranging from 12mm to 25mm. Similar processes are in use in the casting of other metals and alloys.

The trend in the primary metals industries is towards higher product quality and faster casting speeds. Both requirements necessitate accurate control of pouring, determined by factors such as the cooling rate, the reciprocation rate of the mould, and the withdrawal speed of the solidifying metal strand. Most preferably the pouring rate should be decoupled from, and independent of, the head of liquid metal in the tundish, and ideally the pouring should be amenable to continuous, rapid, automatic modulation under computer control.

The traditional control of the pouring rate is by hydraulic manipulation of a slide gate fitting across the nozzle or pouring tube, or of a conical ceramic stopper which is inside the tundish and in operation is raised from or lowered into the tundish outlet.

However, these devices are subject to blockage and erosion, to freezing up of the apertures through which the melt passes, to leakage, and to wear, all of which make accurate control difficult and necessitate frequent replacement of the moving parts. A slide gate may also suck in air through the clearances between the sliding surfaces, and the air thus sucked in causes oxidation of the molten steel and increases the impurity content of the casting.

Ideally, a control valve for use in an application such as a continuous casting process should have no moving parts, should be capable of rapid and continuously variable flow rate adjustment (preferably from full flow to zero flow) under computer control, should be usable with standard pouring tubes, and should be small and light enough that it is capable of being fitted into position with minimum difficulty by one or two men. Such a desideratum might be met by an electromagnetic valve rather than a mechanical one, and the present invention proposes a novel form of electromagnetic valve which substantially or wholly meets the desired criteria.

Various attempts have been made since the late 1970s to develop an effective electromagnetic valve for flow control of liquid metals, of which perhaps the best-known is the simple electromagnetic pinch valve.

This comprises a solenoid surrounding the pouring tube; a high-frequency current through the solenoid generates magnetic fields which exert a radial force on the liquid metal and so "squeeze" the stream to a smaller diameter, throttling its flow. Unfortunately, this type of valve suffers from several disadvantages; since it relies on physically reducing the stream diameter, it must be positioned at the nozzle outlet, and cannot work with a submerged pouring tube, which is preferred for many casting operations; the control of the separation point of the metal from the walls of the tube is problematical; and the power -requirements are usually extremely high, leading to difficult cooling problems.

To date there has been no truly successful commercial development of this concept.

A variation on this technique employs a relatively complex structure of baffles in the pouring tube, which baffles distort the magnetic field, resulting in a net upward force on the liquid metal. Though finding some use in the non-ferrous metals industries, where temperatures are lower and the environment less aggressive, this has not been found suitable for steel casting, where, because of the valve's complex structure, it is likely to suffer from erosion and blockage. It also requires very high power levels.

It has also been known for many years to control the flow of liquid metal using electromagnetic pumps, sometimes known as Faraday pumps. These pumps work on the principle that an electrical conductor through which a current is passed will, if subjected to a magnetic field, experience a force (the Lorenz force) in a direction mutually orthogonal to the directions of the field and the current; where the electrical conductor is a liquid, such as a molten metal, the liquid will tend to flow in the direction of the force. This principle has been used for many years in the design of electromagnetic liquid sodium pumps for use in the nuclear industry. Many versions have been described.

Most commonly, these pumps require an electrical contact to be made with the liquid metal, and in all cases the channel through which the liquid metal flows is configured to optimize the performance of the pump; it may, for example be a wide, narrow slot or may have side branches to allow return current flows through the liquid metal.

The invention proposes a simple but significant and surprising variation of the various techniques suggested hitherto. More specifically, the invention suggests that there be created across or around the outlet/pouring tube of the molten metal reservoir (the tundish, for example) an alternating electromagnetic field, that there be induced electrical currents - eddy currents - in the molten metal as it passes through this field, which eddy currents interact, directly or indirectly, with the applied magnetic field, and that the directions and magnitudes of the field and of the induced eddy currents are arranged such that forces are generated in the molten metal which oppose the downward flow of the liquid and so provide the desired controllability of the passage of the metal through the outlet.

The invention proffers a number of different ways in which the concept described above could be realised.

For example, in one of these the reservoir/tundish would be fitted with an output tube/channel with a reducing section - that is, smaller below, larger above - across which the alternating magnetic field is formed with a component in a direction orthogonal to that of the liquid flow so that the eddy-currents caused by that field itself are orthogonal to both field and flow direction such that the magnetic fields that those currents themselves generate interact with and in opposition to the applied field to provide the desired net contra-flow force, and so usable to impede/control that flow. In such a realisation of the invention the eddy currents interact indirectly (by way of the magnetic field they generate) with the applied magnetic field.

In a second realisation, which can be used with a uniform-section output tube/channel, there are employed two adjacent out-of-phase magnetic fields which each cause eddy currents in the field space of the other that are in phase with that field and so create Lorenz forces the effects of which in that field are directed to impede/control liquid flow. In this type of embodiment the eddy currents interact directly with the applied magnetic field.

In one aspect, therefore, the invention provides valve apparatus for controlling the flow of an electrically-conductive liquid along a channel, which valve apparatus comprises: means for creating across or around the channel an alternating magnetic field or fields; means for inducing electrical eddy currents in the liquid as it passes through this field, which eddy currents interact directly or indirectly with the applied field thereby to generate forces acting on the flowing liquid; and means for arranging the directions and magnitudes of the field and of the forces generated by the induced eddy currents such that the generated forces have a component against the liquid flow direction which has a value sufficient to provide the desired controllability of the passage of the liquid along the channel.

In a first generally-preferred form of the invention: the valve apparatus includes a portion of the channel along which the liquid flows, and this portion is of a reducing cross-section, being of greater area on the inlet side than on the outlet side; the magnetic-field-creating means is a single-phase alternating-current electromagnetic field generator, for creating across the liquid flowing in the channel portion an alternating magnetic field; the poles of the generator are positioned so that the change in cross-section of the channel portion occurs within the influence of the magnetic field; and the generator is so shaped and disposed adjacent the channel portion that it creates in the liquid a magnetic field some part of which is substantially orthogonal to the liquid flow direction; whereby in operation the magnetic field generated by the induced eddy currents interacts with the applied magnetic field to create within the liquid forces acting to impede the flow of the liquid.

In a second generally-preferred form of the invention the valve apparatus comprises: a first magnetic field generator, for creating across the flowing liquid a first alternating magnetic field, this first generator being shaped and disposed adjacent the channel to create that first field in a direction substantially orthogonal to the liquid flow direction; a second magnetic field generator, also for creating across the flowing liquid an alternating magnetic field, this second field being of the same frequency as the first magnetic field but having a substantial component 90" out of phase with it, this second generator being shaped and disposed adjacent the channel to create that second field in a direction substantially orthogonal to the liquid flow direction and substantially parallel to the first field; the two generators being so disposed that the path of the eddy currents induced in the flowing liquid by each generator lies at least partially in the field of the other generator; whereby in operation the eddy currents induced in the liquid by each magnetic field in the field space of the other magnetic field interact with that other magnetic field to create within the liquid Lorenz forces acting to impede the flow of the liquid.

The invention provides valve apparatus for controlling the flow of an electrically-conductive liquid along a channel. Although notionally the liquid could be any electrically-conductive liquid - an ionic aqueous liquid, for example, or mercury - and the channel be any channel, tube, passageway or duct along which the liquid is required to flow in a controlled manner, the primary purpose of the invention is to control the flow of liquids which are molten metals, and in particular steel which, as noted above, is being poured out of a tundish into an open-bottomed mould from which it will then be drawn in a continuous-casting process.

The first version of the valve apparatus of the invention includes a portion of the channel along which the liquid flows, and this portion is of a reducing cross-section, being of greater area on the inlet side than on the outlet side. As is explained hereinafter, the reducing nature of this channel portion is required to cause there to be a net imbalance in the "levitational" forces acting on the liquid. Here, though, it is worth noting that it is convenient if the outlet portion have a cylindrical internal cross-section about 20mm in diameter, this being typical of pouring tube diameters currently used, while the inlet portion have a cross-section that is elliptical (and larger parallel to the magnet's poles than it is between them, the length of its minor axis being equal to or a little greater than the diameter of the outlet portion, and the length of its major axis being three to four times the diameter of the outlet portion; i.e., in this case 60-80mm). Naturally, the transitions between the walls and base of the upper portion, and between the lower portion and the base of the upper portion, should be smooth and rounded to minimise obstructions to the liquid metal flow.

The apparatus of the invention includes means for creating across or around the channel through which the conductive liquid is to flow an alternating magnetic field. Most conveniently this field is formed using an electromagnet suitably fed with an AC electrical supply.

If, as is very much preferred, the apparatus is to be handleable - lifted into position - by one or two men, then it should be as light as possible, and this can be brought about if the electromagnet's windings are of aluminium rather than the more conventional copper. And because of the relatively high-frequency field required it is advantageous to us multi-strand, Litz-wound wire for these windings.

Although it might be thought that almost any frequency might be employed for the alternating magnetic field, this is in fact not the case, or at least not the preferred case. There is a preferred frequency of operation which will maximise the levitational forces on the liquid for a given input power and a given channel (pouring tube) diameter; this is because whereas, for constant values of magnetic field, the eddy current strength, and hence the forces on the liquid, will increase with frequency, by contrast the strength of the magnetic field in the liquid metal will decrease with frequency as a result of skin-depth effects which reduce the penetration of the magnetic field into the liquid metal. There is, then, an optimum value for the excitation frequency; it varies directly with the electrical resistivity of the liquid metal, and inversely with the square of the diameter of the liquid metal stream, and is in general given approximately by the expression f = 1/Xpod2, where p is the magnetic permeability of free space, a is the conductivity of the liquid metal, and d is the diameter of the liquid metal stream. It can be shown both theoretically and experimentally that the optimum excitation frequency for molten steel flowing through a pouring tube of 20mm internal diameter is around 2.0 to 2.5kHz, possibly up to 3kHz.

To attain the desired field frequency it is convenient to employ any of the conventidnal commercially-available generator devices that can output a controlled wattage at a pre-selected and controllable frequency. Such a device is a solid state inverter fed from a single or three-phase mains supply.

Using, as the means for creating the alternating magnetic field, an electromagnet, it is highly desirable appropriately to arrange the position and the dimensions of the magnet's poles. In, for example, the case of the reduced section channel version of the invention it is preferable that the width of the magnet poles be substantially greater than the diameter of the narrower outlet end of the channel portion but less than the length of the major axis of the wider inlet end of the channel portion. A convenient practical width of the poles is about 40-50mm.

It is also preferable that the height of the poles should be greater than the skin depth of the magnetic field in the liquid metal at the frequency selected. A convenient height of the poles is about 40mm.

A brief explanation of how these particular pole piece dimensions are chosen might be helpful. Without the metal between the poles the magnetic field lines will go essentially directly from one pole to the other, but once there is conductive liquid between the poles the field lines are deflected; if the base of the liquid is about level with the bottom of the poles then the field lines pass down under the liquid and then up again, either not penetrating the liquid at all or only do so at the lower part (and not to more than the skin depth), and can be thought of as being rather like rubber bands that have been stretched by the liquid, and so exert a restoring force. If, though, the pole height is less than the skin depth then the deflection achieved is minimal, as are the resulting restoring forces.

As to the pole width, it must be such as to permit a return path for the induced eddy currents flowing in the liquid. Now, if the return path lies within the applied magnetic field then the action of the field will be to oppose the current flow, so reducing the required upwards force; to avoid this the upper (and larger) part of the reduced channel section should be wider than the poles. However, the lower (and smaller) part should be narrower than the poles, so that the return current is hampered by the applied field, and so produces little or no downwards force. In this way there is a net upwards force, and this will effectively be acting on the larger portion of the liquid in the wider section of the channel.

The degree of flow control achieved naturally depends upon the value of the magnetic field and the eddy currents interacting with it. Fields in the region of half a tesla - say, from 0.3 to 0.6T - should provide sufficient control. To apply such fields it is best to utilise an electromagnet with a C-shaped laminated iron core, with an air gap of around 25mm (through which a 20mm pouring tube can comfortably be passed). At a working frequency of around 2.5kHz, the laminations should be not more than about 0.05mm thick. Strip-wound cores are preferred over cores built from stampings because the former result is less stray field. The required field can be generated in this way using roughly 10,000 ampere-turns; the actual number of turns, and hence the actual current therethrough, will naturally depend on the operating frequency and voltage (for a given number of turns the coil impedance - which depends upon the pole area - varies directly as the frequency, and so for a given supply voltage the current varies inversely). One example of a suitable electromagnet is one with two coils per core each of 55 turns connected in parallel with 200 amps through each (the core cross-section is 45x20mm tapering to 25x20mm at the poles); those experienced in this Art will be able to construct electromagnets suitable for their particular requirements.

The invention's apparatus includes means for inducing electrical eddy currents in the liquid as it passes through the applied alternating magnetic field.

In the first of the two main variations of the invention these eddy currents are those arising from the magnetic field itself, which is the means, and it is the reducing section of the channel portion which causes there to be a component of the resulting force acting against the liquid flow, while in the second main variation each set of eddy currents arises from the other of the two magnetic fields, which is the means, and it is the outof-phase nature of the two that causes a resulting Lorenz force component.

The second version of the valve apparatus of the invention includes a first magnetic field generator, for creating across the flowing liquid a first alternating magnetic field, and a second magnetic field generator, also for creating across the flowing liquid an alternating magnetic field, this second field being of the same frequency as the first magnetic field but having a substantial component 90" out of phase with it; the idea is that each field's associated eddy currents are formed at least partly within the other field's space, and because of the substantial component 90" out of phase the generated Lorenz forces in each case act together to oppose liquid flow. While in principle, and by selection of suitable energising current sources, it is possible to provide two alternating fields that are exactly 900 out of phase, in practice it is much more convenient to employ the conventional three-phase mains electricity supply, and simply to utilise two of the available phases to control the means - the inverters, say - energising the two electromagnets. Of course, if this is done then the two alternating fields, like the two energising alternating currents, will be not 90" out of phase but rather 1200 out of phase; that, however, is quite satisfactory, for each resulting field has a component, of around 86t of the whole, which is the desired 90" out of phase.

The second version of the invention's valve apparatus of the invention includes two magnetic field generators so disposed adjacent one another that the path of the eddy currents induced in the flowing liquid by each generator lies at least partially in the field of the other generator. To maximise the interaction between the field from the first electromagnet and the eddy currents induced in the liquid by the second electromagnet, and similarly between the field from the second electromagnet and the eddy currents induced in the liquid by the first electromagnet, the vertical separation between the pole faces is preferably kept small. However, a small separation will result in the magnetic field from each assembly being diverted through the laminations of the other assembly, so reducing the field through the liquid metal, and in order to minimise this effect, it is a much preferred feature of the invention that an electromagnetic shield be fitted between the two electromagnet yokes in the region where they are close to each other. The thickness of the electromagnetic shield, which may be a plate of copper or other high conductivity metal, should be as small as possible, but should be greater than the skin depth of magnetic fields in the shield material at the frequency of operation. For an operating frequency of 2.5kHz, a copper plate of 2-3mm thickness is preferred.

The invention's embodiments include means for arranging the directions and magnitudes of the field and of the induced eddy currents such that the generated forces have a component against the liquid flow direction which has a value sufficient to provide the desired controllability of the passage of the liquid along the channel. As noted immediately above, in the first main variation it is the reducing section of the channel portion which causes there to be a component of the resulting force acting against the liquid flow, while in the second main variation it is the out-ofphase nature of the two fields that achieves this. Of course, the actual magnitude of the forces is determined (as noted above) by the strength of the magnetic fields and the engendered eddy currents; in the reducedchannel-portion version of the invention the desired control is attained simply by appropriately varying the driving current to the magnetic field generator, but in the two-field version other factors, such as the phase of the two alternating magnetic fields, may be used for this purpose. Normally, though, any adjustment of the forces even in the two-field version is attained by current variation.

As noted hereinbefore, the magnetic-coil-driving currents necessary to achieve the necessary magnetic fields using a solenoid-type system are high, and there is inevitably a concomitant, and usually undesirable, heating effect. Moreover, since in operation a stream of molten metal, at several hundred degrees Celsius, may be passing through the centre of the apparatus, and much of that heat will be transferred to the apparatus, that heating will be considerably increased. Accordingly, it is desirable to provide such apparatus with means for cooling, both to deal with its proximity to the molten stream and to enable the windings to be run at a higher current density (so allowing the size and weight of the apparatus to be reduced). It is therefore a preferred feature of the invention that cooling channels or a cooling jacket should be incorporated through which a cooling agent such as transformer oil, Freon or cold air can be circulated (water is not a preferred cooling agent because of safety hazards arising if the water comes into contact with the liquid metal).

Although in operation the Lorenz forces generated in the two-field version by the interacting electric currents and magnetic fields in the flowing liquid could act to retard or to accelerate the flow of the liquid, so that this type of apparatus may be caused to act as a fully proportional control valve for the flowing liquid, in practice retardation will be the norm, the valve therefore acting to reduce the flow to a chosen amount, or even to switch it off entirely, rather than to increase it.

The valve apparatus of the invention is, as noted above, primarily for use for controlling liquid specifically molten - metal flows. It has particular relevance to controlling the flow of molten metal from the tundish to the mould during the continuous casting of steel; in this application it provides a controllable force to counteract the static head of liquid metal, and so to reduce and control the flow rate. The two-field version is particularly advantageous in that is can be retrofitted to an existing caster without modification to the ceramic pouring tube, and without making contact with the liquid metal. The whole assembly may be designed as two fitting halves, into which it may be split for ease of assembly around the pouring tube.

The main features and advantages of the valve apparatus of the invention can perhaps be summarised as fol lo-ws: - 1. It is a fully-proportional flow control valve in which a retarding (or, in the two-field version, an accelerating) force is applied resulting from the interaction of an alternating magnetic field with either an alternating electrical current induced in the liquid metal or the magnetic field produced by such a current.

2. The operating frequency is chosen to maximise the required forces, in accordance with the electrical conductivity of the liquid metal and the diameter of the liquid metal stream.

3. Unlike some previous valves, there is no ohmic electrical contact through the wall of the channel in which the liquid metal is flowing. The alternating current in the liquid metal is induced by a magnetic field generator disposed adjacent the pouring tube. In the two-field version this makes retro-fitting particularly easy, for the channel for the liquid metal is a standard, unmodified pouring tube as conventionally used in the continuous casting of steel.

5. In the preferred two-field version version, two pairs of alternating magnetic fields are produced by two magnetic yokes (with excitation windings) displaced from each other along the longitudinal axis of the pouring tube and electrically excited so that the resulting magnetic fields each have a significant component 90" out of phase with the other. In this version a magnetic shield is preferably positioned between the two magnetic yokes.

6. The whole assembly may be designed as two fitting halves, into which it may be split for ease of assembly around the pouring tube.

7. In use, the flow rate is adjusted simply by controlling the phase or amplitude of the current through one or more of the windings.

Several embodiments of the invention are now described, though by way of illustration only, with reference to the accompanying Drawings in which: Figure 1 shows a diagrammatic perspective view of a first valve apparatus of the invention, being a version having a reduced-section channel; Figure 2 shows a diagrammatic vertical cross section of an alternative configuration of a valve apparatus of the invention similar to that of Figure 1; Figure 3 shows a diagrammatic plan view and vertical cross-section of a preferred embodiment of another similar valve apparatus according to the invention; Figure 4 shows a diagrammatic perspective view of a second valve apparatus of the invention, being a version using two out-of-phase magnetic fields; Figure 5 shows a diagrammatic perspective view of the pouring tube used in the Figure 4 valve, illustrating the direction of the magnetic fields and the flow of electric currents in the liquid; and Figures 6A & B show a preferred embodiment of a valve apparatus of the invention, similar to that of Figures 4 & 5, in elevation and plan views.

The version of valve apparatus shown in Figure 1 is basically a pouring tube (11) for liquid metal, the tube having an inlet portion (12) and an outlet portion (13), and the inlet portion 12 has a greater cross-sectional area than the outlet portion 13. Disposed around the tube 11 is a magnetic yoke (14) for generating an alternating magnetic field across the liquid metal in a direction perpendicular to its direction of flow; the yoke 14 has an excitation winding (15). It will be noted that the poles (16) and (17) of the magnetic yoke 14 straddle tat part of tube 11 where occurs the change in cross-section.

On energising the coil 15, and so applying the magnetic field, eddy currents (not shownl Will be induced in the liquid metal. These eddy currents .ill themselves generate magnetic fields, and the interaction of these latter with the applied magnetic field from the field generator will create replllsive forces between the liquid metal and the poles 16,17. Because the cross-section of the inlet portion 12 of the pouring tube 11 is larger than the cross-section of the outlet portion 13, the liq concentric with the pouring tube 21, and has a laminated core (25) to concentrate and direct the magnetic field, as indicated by the dotted lines (26). On applying the magnetic field, repulsive forces will act on the liquid in directions which are always perpendicular to the magnetic field lines, as indicated by the arrows (27).

These forces will in general have a vertical component and an inward radial component, and because of the shape of the magnetic field and of the pouring tube the vertical components will combine to create a net levitational force on the liquid metal, so retarding its flow.

A particularly preferred embodiment is shown in the plan and vertical cross-section of Figure 3.

The pouring tube (31) has an inlet portion (32) and an outlet portion (33). The outlet portion has a cylindrical internal cross-section about 20mm in diameter, this being typical of pouring tube diameters currently used. The inlet portion has cross-section that is larger parallel to the magnet's poles (36: see below) than it is between them (an elliptical crosssection is shown, the length of its minor axis being equal to or a little greater than the diameter of the outlet portion, and the length of its major axis being three to four times the diameter of the outlet portion; i.e., in this case 60-80mm). The transitions between the walls and base of the upper portion, and between the lower portion and the base of the upper portion, are smooth and rounded to minimise obstructions to the liquid metal flow.

A magnetic yoke (34) is provided for generating an alternating magnetic field across the liquid metal in a direction perpendicular to its direction of flow; the yoke has two excitation windings (35) on its poles 36 of the yoke.

The version of valve apparatus shown in Figure 4 is one wherein there are two fields out of phase with each other.

This version has a pouring tube (41) for liquid metal, magnetic yokes (42,43) for generating an alternating magnetic field across the liquid metal in a direction perpendicular to its direction of flow, and excitation windings (44,45) on the yokes. The alternating electrical current supplied through the first excitation winding 44 is arranged to be 90" out of phase with that through the second excitation winding 45. The first yoke 42 has poles (46, 47) which are positioned adjacent the pouring tube at opposite ends of its diameter; similarly, the second yoke 43 has poles (48,49) positioned adjacent the pouring tube at opposite ends of its diameter, and a little below the first yoke's poles 46,47.

The way the produced magnetic fields are disposed and overlap is shown in Figure 5; the pouring tube (51) is marked with the positions of the poles 46,47 by the dotted rectangles (52,53), and similarly the positions of the other pair of poles 48,49 are indicated by the other dotted rectangles (54,55). The direction of the alternating magnetic fields is indicated by the two sets of arrows (56,57).

In operation, the magnetic field 56 generated by the first coil and yoke assembly 42,44,46,47 will induce in the liquid metal an alternating electrical current flow as indicated by the dotted lines (58), which will be in phase with the alternating magnetic field 57. A part of this electrical current flow will interact with a part of the magnetic field 57 generated by the second coil and yoke assembly 43,45,48,49 to generate Lorenz forces in the liquid metal. Similarly, the magnetic field 57 generated by the second coil and yoke assembly 43,45,48,49 will induce in the liquid metal an alternating electrical current flow as indicated by the dotted lines (59), and a part of this electrical current flow will interact with a part of the magnetic field 56 generated by the first coil and yoke assembly 42,44,46,47 to generate Lorenz forces in the liquid metal, both sets of Lorenz O cues acting in the same direction.

Because the Lorenz forces generated are proportional to the vector product of the magnetic field and the current flowing In the liquid metal, the force and hence the flow rate of the liquid metal can be controlled by controlling either the amplitude or phase of the currents in the coils 44, 45.

A preferred embodiment of this versIon Is now more particularly described with reference to Figure 5.

This Figure shows elevation and plan views of a valve configured substantially as in Figure 4. The valve is built around a ceramic pouring tube (61), around which the valve assembly is fitted.

Electromagnet assemblies (62,53) are wound on stripwound laminated yokes whose pole faces are fitted closely to the pouring tube. The laminations may be silicon iron, or for higher frequency applications, may be of other suitable material such as mumetal or radiometal. The width of the lamination stack is conveniently the same as or slightly less than the diameter of the liquid metal stream, while the height of the stack may be equal to or greater than this.

Twin excitation coils (64,65) are fitted to the side limbs of the yokes as shown, since this arrangement generally results in a more efficient magnetic circuit than does the single coil arrangement shown in Figure 4.

The first electromagnet assembly 62 is supplied from one phase of an alternating electrical supply and the second electromagnet assembly 63 from another phase, the phase difference between the two phases being adjusted (by means not shown) to maximise the Lorenz forces opposing the downward flow of liquid metal through the pouring tube.

To maximise the interact ion between the field from the first electromagnet assembly 62 and the eddy currents induced in the liquid metal by the second electromagnet assembly 63, and between the field from the second electromagnet assembly 63 and the eddy currents induced in the liquid metal by the first electromagnet assembly 62, the vertical separation between the pole faces is kept small. However, a small separation will result in the magnetic field from each assembly being diverted through the laminations of the other assembly so reducing the field through the liquid metal. In order to minimise this effect an electromagnetic shield (66) is fitted between the two laminated yokes in the region where they are close to each other. The thickness of the electromagnetic shield is as small as possible, but greater than the skin depth of magnetic fields in the shield material at the frequency of operation. For an operating frequency of 2.5kHz, a copper plate of 2-3mm thickness is satisfactory.

Claims (9)

1. Valve apparatus for controlling the flow of an electrically-conductive liquid along a channel, which valve apparatus comprises: means for creating across or around the channel an alternating magnetic field or fields; means for inducing electrical eddy currents in the liquid as it passes through this field, which eddy currents interact directly or indirectly with the applied field thereby to generate forces acting on the flowing liquid; and means for arranging the directions and magnitudes of the field and of the forces generated by the induced eddy currents such that the generated forces have a component against the liquid flow direction which has a value sufficient to provide the desired controllability of the passage of the liquid along the channel.

2. Valve apparatus as claimed in Claim 1, wherein: the apparatus includes a portion of the channel along which the liquid flows, and this portion is of a reducing cross-section, being of greater area on the inlet side than on the outlet side; the magnetic-field-creating means is a single-phase alternating-current electromagnetic field generator, for creating across the liquid flowing in the channel portion an alternating magnetic field; the poles of the generator are positioned so that the change in cross-section of the channel portion occurs within the influence of the magnetic field; and the generator is so shaped and disposed adjacent the channel portion that it creates in the liquid a magnetic field some part of which is substantially orthogonal to the liquid flow direction; whereby in operation the magnetic field generated by the induced eddy currents interacts with the applied magnetic field to create within the liquid forces acting to impede the flow of the liquid.

3. Valve apparatus as claimed in Claim 1, wherein the apparatus comprises: a first magnetic field generator, for creating across the flowing liquid a first alternating magnetic field, this first generator being shaped and disposed adjacent the channel to create that first field in a direction substantially orthogonal to the liquid flow direction; and a second magnetic field generator, also for creating across the flowing liquid an alternating magnetic field, this second field being of the same frequency as the first magnetic field but having a substantial component 90" out of phase with it, this second generator being shaped and disposed adjacent the channel to create that second field in a direction substantially orthogonal to the liquid flow direction and substantially parallel to the first field; the two generators being so disposed that the path of the eddy currents induced in the flowing liquid by each generator lies at least partially in the field of the other generator; whereby in operation the eddy currents induced in the liquid by each magnetic field in the field space of the other magnetic field interact with that other magnetic field to create within the liquid Lorenz forces acting to impede the flow of the liquid.

4. Valve apparatus as claimed in Claim 2, wherein, using a channel portion of a reducing cross-section, the outlet portion has a cylindrical internal cross-section matching the pouring tube diameter while the inlet portion has a cross-section that is elliptical (and larger parallel to the magnet's poles than it is between them, the length of its minor axis being equal to or a little greater than the diameter of the outlet portion, and the length of its major axis being three to four times the diameter of the outlet portion.

5. Valve apparatus as claimed in any of the preceding Claims, wherein the means for creating the required alternating magnetic field is an electromagnet suitably fed with an AC electrical supply.

6. Valve apparatus as claimed in any of the preceding Claims, wherein the frequency of the alternating magnetic field is from 2 to 3kHz.

7. Valve apparatus as claimed in any of the preceding Claims, wherein when using an electromagnet in the reduced-channel version the width of the magnet poles is substantially greater than the diameter of the narrower outlet end of the channel portion but less than the length of the major axis of the wider inlet end of the channel portion.

8. Valve apparatus as claimed in any of the preceding Claims, wherein when using an electromagnet the height of the poles is greater than the skin depth of the magnetic field in the liquid metal at the frequency selected.

9. Valve apparatus as claimed in any of the preceding Claims and substantially as hereinbefore described.

9. Valve apparatus as claimed in any of the preceding Claims, wherein the magnetic field is from 0.3 to 0.6T.

10. Valve apparatus as claimed in any of the preceding Claims and as claimed in Claim 3, wherein using first and second electromagnets to create across the flowing liquid first and second alternating magnetic fields the one being of the same frequency as but having a substantial component 90" out of phase with the other, there are employed two of the phases of the conventional three-phase mains electricity supply to control the means energising the two electromagnets.

11. Valve apparatus as claimed in any of the preceding Claims and Claim 3, wherein to maximise the interaction between the field from each electromagnet and the eddy currents induced in the liquid by the other electromagnet the vertical separation between the electromagnets' pole faces is kept small, and to minimise each field's reduction an electromagnetic shield is fitted between the two electromagnet yokes in the region where they are close to each other.

12. Valve apparatus as claimed in any of the preceding Claims, wherein when using electromagnet(s) the actual magnitude of the flow-affecting forces is determined and controlled by appropriately varying the driving current to the electromagnet(s).

13. Valve apparatus as claimed in any of the preceding Claims, wherein there are means for cooling the apparatus.

14. Valve apparatus as claimed in any of the preceding Claims and substantially as hereinbefore described.

Amendments to the claims have been filed as follows CLAIMS 1. Valve apparatus for controlling the flow of an electrically-conductive liquid along a channel, which valve apparatus comprises: a first magnetic field generator, for creating across the flowing liquid a first alternating magnetic field, this first generator being shaped and disposed adjacent the channel to create that first field in a direction substantially orthogonal to the liquid flow direction; and a second magnetic field generator, also for creating across the flowing liquid an alternating magnetic field, this second field being of the same frequency as the first magnetic field but having a substantial component 90" out of phase with it, this second generator being shaped and disposed adjacent the channel to create that second field in a direction substantially orthogonal to the liquid flow direction and substantially parallel to the first field; the two generators being so disposed that the path of the eddy currents induced in the flowing liquid by each generator lies at least partially in the field of the other generator; whereby in operation the eddy currents induced in the liquid by each magnetic field in the field space of the other magnetic field interact with that other magnetic field to create within the liquid Lorenz forces acting to impede the flow of the liquid.

2. Valve apparatus as claimed in Claim 1, wherein the means for creating the required alternating magnetic field is an electromagnet suitably fed with an AC electrical supply.

3. Valve apparatus as claimed in either of the preceding Claims, wherein the frequency of the alternating magnetic field is from 2 to lOkHz.

4. Valve apparatus as claimed in any of the preceding Claims, wherein the magnetic field is from 0.3 to 1 T.

5. Valve apparatus as claimed in any of the preceding Claims, wherein using first and second electromagnets to create across the flowing liquid first and second alternating magnetic fields the one being of the same frequency as but having a substantial component 90C out of phase with the other, there are employed two of the phases of the conventional three-phase mains electricity supply to control the means energising the two electromagnets.

6. Valve apparatus as claimed in any of the preceding Claims, wherein to maximise the interaction between the field from each electromagnet and the eddy currents induced in the liquid by the other electromagnet the vertical separation between the electromagnets' pole faces is kept small, and to minimise each field's reduction an electromagnetic shield is fitted between the two electromagnet yokes in the region where they are close to each other.

7. Valve apparatus as claimed in any of the preceding Claims, wherein when using electromagnet(s) the actual magnitude of the flow-affecting forces is determined and controlled by appropriately varying the driving current to the electromagnet(s).

8. Valve apparatus as claimed in any of the preceding Claims, wherein there are means for cooling the apparatus.