MULTIWAY VALVE

Abstract: A description is given of a multiway valve, comprising a chamber into which at least four feed or discharge ducts (61, 68, 92, 96) open out, the state of being open or closed of at least three of the ducts being affected by the positioning of a member (91) which is, moveable in directions of movement substantially perpendicular with respect to one another, accommodated inside the chamber, and which member can be made to interact in a sealing manner with one or more duct openings, and control means (L1-4) for moving the member inside the housing.

Description: ultiway valve The invention relates to a multiway valve which is suitable for controlling, metering and mixing fluid flows through four or more feed or discharge ducts. Multiway valves with three ducts for the feed and/or discharge of fluids are generally known in the prior art. Three-way shut-off valves of this nature can be designed to dispense a feed of fluid to two fluid discharges in a controlled way or to combine two fluids which are supplied separately, and if appropriate mix them, and discharge them together. Although a four-way shut-off valve or a multiway valve with four or more feed or discharge ducts is currently available at a very high cost, such valves are of complicated design comprising a plurality of three-way shut-off valves which are connected in cascade form or are obtained by connecting a rotating connection duct to a feed duct and a selected discharge duct. It is very difficult to achieve complex proportional and/or fail-safe control of fluids using these shut-off valves . The present invention provides a new type of multiway valve, comprising a chamber into which at least four feed or discharge ducts open out, the state of being open or closed of at least three of the ducts being affected by the positioning of a member which is, moveable in directions of movement substantially perpendicular with respect to one another, accommodated inside the chamber, and which member can be made to interact in a sealing manner with one or more duct openings, and control means for moving the member inside the housing. "Directions of movement perpendicular with respect to one another" are understood to mean all directions of movement which can be put together from two mutually perpendicular movement vectors whose magnitude can be selected as desired. One or more ducts will be closed off as a function of the position of the member. By changing the position of the member, it is possible to close off different or additional ducts; in addition to complete closure, the member may also be positioned so as to partially close off one or more ducts, resulting in an additional metering function. By allowing the ducts to open out into the chamber at suitable positions, it is possible to achieve a large number of possibilities for the controlled closure and opening of specific combinations of ducts in order to control, mix and meter various feed streams. The possible combinations of a specific fluid feed and a large number of different discharges can be increased by, for example, branching a general feed duct or discharge duct and allowing the branched ducts to open out into the chamber at a distance from one another which is such that at least one of the branched feed openings will be open in any position of the member inside the chamber. Likewise, a plurality of discharge ducts may be joined together integrally in a wall and/or outside the valve downstream of the multiway valve, in order to discharge a large number of combinations of fluids, which can be fed through various ducts, to one or more branches of a common discharge without interruption. The chamber may have any possible form, such as for example a round chamber in which a spherical member is enclosed virtually without any free space, which sphere can be rotated inside the chamber through two directions of rotation which are perpendicular to one another. Thus the chamber may also have a flattened form, in which case the member is preferably accommodated inside the chamber in such a manner that it is moveable in two dimensions in a plane which runs substantially parallel to the longitudinal axis of the chamber. The member can thus be moved in the length and width directions inside the chamber. The member may preferably adopt any possible position inside the chamber . Preferably, the chamber is delimited at least by two substantially plane-parallel surfaces, the plane in rrj rrj rrj Cn OJ 4J OJ d ε 44 00 υ - H ε d 4-J 4 xl J ft -H CQ ^ 0 -H CD 4-J o 0 α> 0 Xl rrj d rrj 4-1 d 0 , CU rH CQ -H CQ xl X! -H o 1 0 ) Φ CQ J OJ •H υ CQ Xl 0 XI 0 TJ rrj OJ <: ε rrj CD TJ XI rH d 4J 3 ■ H J 4-1 CJ ε ~. XI rrj rH OJ s TJ rrj 0 OJ 4-> 4J rrj rH CQ CJ CD rrj 4 f . ε rrj ■ H CJ d υ CQ CQ d Cn 4J OJ d 5 4-1 rH OJ -H rrj -H rrj XI «. Xl rrj CQ J rrj CQ rrj J 4-1 J -H OJ CQ d XI rrj 4-1 ft 44 ε H OJ .4 CQ 44 4-1 4-1 ^ CJ XI rrj >. 4-1 4-1 CD d -H Xl 0 > 4-1 D -H rrj d 4-1 υ d d υ -H rrj d ε d Φ 44 X! CD rrj ε X) 44 OJ ε XI rH ε CD CJ OJ ε d CQ αj CQ 4-1 xl CD -H 4-1 xl d 4 -H >ι xl rrj 4-1 44 ■ H CD ε 0 5 X) ι d ε 4-1 d 0 cu -H 0 -H -1 ε > • H 4 rrj 4J -H OJ J rrj CQ XI CJ 0 4-1 CQ -H ft -H d Cn l d CD d 4-1 ε XI -H ε 4-1 d -. 0 Cn >. J 44 • H 4-1 0 CQ -H d OJ > -H CU TJ rrj > J CQ -H >. -H 4J CQ rrj υ Cn OJ CQ d ft CD ■ H CQ d d CD -H OJ r4 44 ft CD 0 ■ H TJ chamber in order to place two or more ducts in communication with one another. By dimensioning the chamber in such a manner that the cavity is in communication with one or more ducts to a certain extent at various positions of the member inside the chamber, it is possible to use the said duct as a central feed or discharge, so that this flow is controlled and/or mixed. The member may then be positioned in such a manner inside the chamber that the said central duct is in communication, via the member cavity, with one or more other ducts, it being possible, by moving the member, to interrupt a connection to a greater or lesser extent and/or to bring about a connection to one or more other ducts to a greater or lesser extent. Obviously, it is also possible to close off the other ducts, whether or not together with the central duct, depending on the position of the duct openings in the chamber, the shape of the member cavity and the position of the member. The member preferably comprises a continuous ring section which interacts in a sealing manner with at least one of the plane-parallel surfaces, the member cavity being delimited in the radial direction by the inner circumference of the ring section. This provides a substantially round cavity, allowing a large number of connection combinations between feed and discharge ducts by means of relatively simple movements of the member. Advantageously, the member cavity is in communication with both the top and bottom sides of the chamber. As a result, it is also possible, via the member cavity, to place ducts which each open out at opposite plane-parallel surfaces of the chamber in communication with one another. This allows the valve to be of compact design and reduces the restriction for the controlled flow. Advantageously, the inner walls of the cavity in the member are designed to be convex, thus reducing turbulence in the fluid flow. Advantageously, cavities are formed on both the bottom and top sides of the member, in which case the two cavities are not in communication with one another, so that the two separate fluid flows can be controlled simultaneously with very reliable control of the two flows ft d D * 0 OJ rd 44 o rd r. CQ 0 OJ XI D (Tj 1 OJ OJ 00 4-J TJ υ 0 4-J . rd CD 4-1 4-1 d υ 44 r. • rH flj flj CJ Xl o rd O ι d d 0 CD -H 0 rd r. d d d rd 4-1 d 4-1 © CD ε CQ CD ~. CD XI XI 0 CD 4-J xl Xl CD d rd 0 44 0 -H © XI ■ ? CQ - CD CD rH Φ J d CJ xl 4-1 Ss CQ CQ X! d rH rH φ CD -H > 4-1 CQ 0 ■ CD rH M XI XI TJ XI -H rd xl 0 CD 4-1 d 4-1 4 ε (Tj ft rH d φ xl υ 4J rd ON -H rH Φ d CD d 4J •H CD ε XI 4-1 ft ft -H Cn CQ o -H u rd CD CQ XI 4-1 rd rd υ c ω t to H H cn o n o CJ1 O n rr OJ cr CQ 0 ) OJ TJ 0 Ω rt O Hi P- ft Ω rt Q ft J P- d P- ft ft d CQ Ω Ω ft 0 Ω Ω Ω rt -3 d 4 P < Φ P - rt 0J O rt d d d oi " P- P- d CQ d d P- P- d d 0 0 P- d P- 0 O P- su Φ Ω Φ OJ d 4 d ^ P Ω Ω < P- rt CQ P 3 CQ CQ 3 d P 3 3 CQ Φ P 3 3 0 rt ΓT rt 0 O d Φ rt Φ rt P rt P- Q d Ω J P cr P- Ω Φ Φ Hi 3 J Ω Ω cr TJ ' Ω d 4 d Ω s; φ P cr d 4 P tr Φ CQ rt J *• 0 φ Φ ft CQ d Ω J 3 P CQ OJ d P- 0 CQ OJ 0 Φ ft O CQ Φ φ Φ 0J ^ ft rt Q CQ P φ CQ Φ Ω d P- d P- d d J 0 rt d d J ft P P CQ P- d Φ Ω Φ OJ ≤ P- CQ Φ d CQ P- 0 rt OJ Φ OJ d d 3 Ω d rt Oi d Φ 3 OJ • Φ d Ω ft 0J ~ P 0 rt P- 0 CQ P- Φ CQ rt CQ rt d Ω Φ Φ Φ P- Φ ≤ π. Ω P- Φ ft ω rt ~ d ft Hi t rt d OJ Ξ Ω CQ M 4 • P- rt Φ φ Ω g P Ω O OJ rt rt 3 P- w rt rt "< rt φ Φ d J CQ P t OJ OJ d φ 0 CQ CQ OJ 0 ) ft rt cr Ω rt CQ d 4 cr OJ < 4 t Ω Hi cr d" ft Ω ^ P- rt J Ω P ro d d CQ d Φ Φ d Φ Ω Φ Φ φ φ Φ OJ OJ 0 Φ Φ 0 Ω OJ P- Ω P- rt Ω OJ ^ CQ OJ 3 0 ΓT Ω ft P P- ft O Φ s; P P d Ω d P OJ d tr d Hi t 0 0 d TJ OJ rt ΓT r 3 d 4 O d Q Ω Ω cr CQ d OJ Ω CQ 0 d 3 O P- ω 0 OJ ^ d 4 OJ rt d rt cr P- Ω Ω TJ P- d p- O cr φ 0 0 Φ 3 0 P- P P- Φ 3 rt rt x-x P P φ 3 0 0 p- O P- CQ Ω 0 ) φ Hi 3 ft 3 φ X d P OJ Ω cr d ft d OJ 0 trs- P- rt cr P CQ OJ P d d d d 4 0 <. d tr φ 3 0 ) d Φ rt φ rt Φ cr rt P- CQ ft Φ P- ft rt - Φ • Φ ^ 0 O OJ P. CQ P- P- rt Φ O J 3 φ 0 P- P p- 0 Φ rt rt OJ P ω P- 0 " Ω d P- ≤ d rt Hi OJ Φ rt d d 4 P ≤ ft J Ω P- d 0 - d rt rt P rt d P- P- H fϊ OJ Φ d 4 Φ P- OJ P ft ^ CQ Φ J 0 ) OJ rt d φ d d 4 4 OJ 0 Φ Φ TJ CQ Hi d d Hi P- ft P- 0 Ω φ Oi 0 rt Ω Φ Φ P- 0 Φ Ω J d ft 3 0 0 rt 0 < 0 ) Ω Ω OJ d Φ O 3 Hi P- φ ft rt ft Ω rt d ft rt Φ cr CQ rt P 0 Φ ft d OJ d 0 d 4 d CQ TJ Hi rt OJ Φ ^ ~. d ft d 1 P- 0 CQ Ω P- CD CQ P 0 CQ d 4 3 P P φ d 0 3 0 Ω • P Hi d 4 3 Ω CQ CQ P- rt Φ 3 3 P- d- CQ P- cr 0 ft P- Φ ft P CQ 0 rt rt 3 ft rt P- Φ Φ cr O — - P- d O Φ cr CQ σ OJ Ω ft 0 rt P- cr rt φ d P- H. OJ d 4 d d d 4 P P CD cr O Φ d O d CO d P- 0 3 CQ P- φ P OJ 3 rt ≤ P TJ P CQ φ d Ω Φ Ω d 4 φ ^ ft s; P d 0 d OJ OJ 0J CQ d TJ P cr rt Φ rt φ Φ s; 0 rt φ 0 ) Φ P P- rt P d Φ d d P- Φ Hi Φ Ω P- P- OJ O Φ Φ rt tr OJ d 0 rt Φ ft 0 • Ω CQ P- rt rt Ω d ft Ω 0 CQ Ω ft 0 rt CQ P 0 OJ s. cr rt rt P- 0 ft CQ d 0 ) rt 3 d 4 rt CQ 0 rt rt 0 3 P- O d P- CQ ø j ». rt tr 0 ft d P- CQ rt Ξ P- CQ d P- Φ CQ Φ P- tr P 3 ft d ft OJ 0 P- d cr Ά P- ^ 0 P- ft ft er rt ft P- d 4 OJ • * d rt CQ O Φ d φ d P- d cr ft cr φ P- Ω Hi Ω CQ Φ P- ^ d 4 Φ ^ 0 P- rt 3 TJ d" d 3 d Φ CQ CQ ^ CQ 0 d- P- 0 Ω J CQ Φ d Ω rt 0 ) P- rt Φ P φ d Ω 0 P- € Ω Ω 3 • φ J OJ P d rt 3 CQ Φ Ω Q s- cr d 4 d 4 £ d 4 3 Φ CQ 0 Ω d" P Ω OJ rt 0 Ω J cr ft TJ tr cr d 0 Ω 0 ) Φ £ Φ Ω OJ φ cr CQ φ rt O 01 φ J Φ < rt Ω P P- s; d rt φ P- CQ ft d P- 0 P- 0J P- > < Φ φ 3 3 rt ft cr Φ 0 0 0 Φ CQ P- rt t d d Φ d ft g h- 1 Ω rt P 3 P CQ P. d ft d cr σ Hi P- - ^ 3 P 3 < Ω rt CQ Φ p- Φ Hi d Φ P- 3 d 4 Φ Φ Ω P- rt d 0J P- Φ Φ 0 ft Φ 0 cr 3 P- rt . 4 d Hi rt Ω d d 0 0 3 d 0 ) ft 0 Ω <; d P Φ d ≤ d P d rt P 0 ft 0 rt Ω < rt P- rt CQ d Hi CQ cr d cr P- φ P P- ft Φ OJ ft P- Ω 0 rt OJ P- ft P- H J t tr φ 4 Ω Ω p- Φ d 4 Φ Φ rt d CQ rt rt rt rt • rt d 0 ) d 3 rt φ OJ d Φ P- 0 Ω rt Ω rT ft φ P- P φ s Ω 0J P- P- O P- 4 OJ OJ CQ rt CQ 0 TJ 3 rt φ d Φ d 4 OJ d 4 rt P- OJ O rt rt d O rt P rt ≤ rt ■ ^i cr P- <; P- 3 cr p- CO d d P Φ rt Φ 0 3 d 4 Ω d rt d t O ^ d tr rt 4 P- 0 OJ d 0 Φ CQ OJ Φ Φ 0 J rt Φ rt P- Hi φ Φ OJ d 4 d Φ CQ P- ft 4 P- d P Φ cr CQ d d 3 P d P- Ω OJ rt 0 3 Hi g P < S Φ Φ cr cr CQ P- rt Φ Ω CQ 0 Φ P- rt φ cr ft ^ rt P- ≤ d φ cr P- d 4 p 0 Ω CQ Φ 0 CQ CQ V trs- rt OJ d P- t Φ OJ P- d O cr Φ Ω rt P- Φ P rt P- P rt TJ Ω Φ P rt tr P rt rt 0 d TJ P d 0 Ω Hi 0 cr c 3r ^ P ^ Ω Hi Φ ft Ω Φ P- O t φ P- t P- P Hi rt CQ J ft d P- OJ d Ω P Φ Φ O d 4 0 P- ft φ O CQ CQ OJ 3 CQ CQ φ CQ OJ OJ P ≤ P Ω φ P P 0 P- rt P rt Ω CQ 0 ) P. d d CQ P Φ d d 0 rt 0 OJ OJ Ω d d £. d 4 J Φ d ft Φ rt d 0 P- Q 3 Q CQ rt 4 < 0 d 0 d CQ Φ r Φ ft ft d rt O 0J φ P cr φ cr rt OJ Φ OJ OJ Φ P- Hi P- <; Φ Φ P- Ω d 4 Ω Φ P- 3 P rt Φ rt rt Φ Ω d Hi rt O OJ rt Φ rt Φ P rt ft Φ CQ OJ ^ rt Q P rt 0 ) ^ Hi Q Φ t d Φ cr i • P- rt Ω Hi ft rt OJ rt p- Φ 0 d 4 rt O rt ^ d d φ interacts in a sealing manner with the transverse wall(s) of the chamber around a duct opening. However, it is also possible for a separate closure body, which is held in the open position by spring pressure, for example, to be positioned in front of the duct opening in question. The member can thus move the said closure body counter to the spring stress until it interacts in a sealing manner with the duct opening. For example, it is conceivable for there to be configurations in which the duct opening is provided with an opening body which, in a similar manner to that described above, closes off the duct opening, for example by means of spring pressure, it being possible for the member to be made to interact with the opening body, with the result that the duct in question is opened. In a preferred embodiment of the multiway shu -off valve according to the present invention, the member may be made to interact in a sealing manner with one or more duct openings . In order to improve the above mentioned interaction between the side walls and the member further, at least one side wall of the member is of convex design and the transverse walls of the chamber are of correspondingly concave design at least in the vicinity of the duct openings which are present therein. In order to ensure correct movement and positioning of the member inside the chamber of the multiway valve, the corners between the transverse walls are preferably rounded with a defined radius and the member is correspondingly rounded, at least locally, with a diameter which is equal to or less than twice the said radius. The control means of the multiway valve according to the invention may be directly connected to the member. For example, the control means may comprise pull and push rods, which rods are each locally guided through a side wall of the chamber. Optionally under the influence of an external impulse, the control means may engage on the said rods and exert a pushing or pulling force thereon, with the result that the member is moved inside the chamber. For example, the member may be connected, via a plurality of ω OJ to to H H cn o n σ ( Jl O cn 3 OJ Ω ft- P- cr OJ 3 ft ft rt 0 CQ 3 cr P 3 OJ 3 ft rt Ω 0J 3 ft CQ d OJ P 3 OJ 3 OJ Φ Ω OJ P- d Φ Ω Φ P- P- d 4 Hi Ω d Φ φ OJ Ω 01 d 4 d 4 O Ω Φ d 4 d d Ω Φ OJ Ω Φ P 3 Ω CQ CQ rt 3 P CQ Φ 0J rt CD CQ rt rt Φ Φ 3 Ω g Φ cr P- Ω Ω d ft 3 φ cr 0 Φ TJ €. D d cr φ J rt P rt s- d d d Φ TJ d cr D rt 0 ft d d cr Φ P d 4 P- OJ Φ Ω < d 4 Ω P- φ Φ 0 ) P 3 rt P P Φ Ω rt CQ P P- Φ OJ Φ ft P ft rt OJ P- rt rt P rt OJ P- P- Φ s; φ rt rt rt P- φ 0 P- OJ P d 4 OJ ft -> P rt P P- P- d 4 Ω Ω d P- P- Ω Ω CD OJ d P- P- Ø 3 TJ CD ft OJ d ≤ P- P- P- CD s, d φ P- d 4 OJ d 3 0 P- P- ^ ; Ω d cr Φ φ r 3 rt d 4 d d ft o P- TJ d 4 CQ H d rt CQ P- d d d d rt rt CQ > Φ CQ H 0 cr P- P- CQ ► 0 Φ d 4 TJ d d 0 P- d 3 CQ Ω φ CQ P- 0 ) CQ <! d 4 d 4 Hi OJ ft P P- OJ d Ω Φ øi Ω P OJ O P • CQ CD Ω rt Φ OJ ft OJ 0 rt rt d 0 ) φ φ P- OJ d < • ft 0 cr P h- 1 d 4 rt φ P rt φ P- Φ C t? 0 OJ 3 rt CQ CQ Hi rt ^ d CQ P Φ CQ ft OJ Φ P OJ d Φ • 0 Hi Hi ft ft cr d 4 Φ P- CQ cr d 4 P Ω <! Ω φ H CQ d 0 d ft ^ ØJ φ 3 P- Φ Φ Ω rt J Φ Φ d Φ Φ 3 Φ 0 Φ Φ Φ 0 ft φ rt rt 0 ft 0 P g ? P tt P 0 rt P P OJ d 4 p P rt 3 0 Hi J d P- 3 d 4 OJ Hi rt 0 0 Φ φ d 4 OJ < CQ OJ ft OJ d Φ Φ 3 d 4 rt cr 3 < 3 3 rt rt CQ s; cr φ CQ ≤ d 4 < X! Φ cr φ cr d 4 ft Hi -S OJ Φ d 4 OJ Φ OJ rt OJ P- d 4 P d 4 Φ ft d 4 Φ • Φ 0J d ft 3 TJ Φ P- C cr P- Φ P- CQ φ ^ ft 3 d 4 ^ cr H- O d P- P- Ω 0 t P- P ft P OJ P- TJ ^ φ 0 ^ OJ ~ Φ d P d 3 • φ Φ d φ H Ω 0 Ω φ 0 d Φ Ω P CQ P ^ d CQ * Ω < P Φ Φ d Φ φ d 4 d 4 CQ d ω d 4 0 ) < ØJ J Φ rt P- d 4 f 3 Φ φ rt 3 P- X rt rt rt cr Hi g d rt - Ω ft P- d 0 ) 0 CD rt • ft ft 0 ) ; 0 d ft Hi cr Ω 0 0 0 0 rt P- Φ φ OJ P ^ d 4 p- rt 0J CQ d CQ φ d 4 P- d 4 3 < rt 0 Oi Φ p- €, 0 OJ rt P 0 CD OJ φ rt d 4 0 OJ CQ P φ CQ Φ d φ 0 Φ cr ØJ φ P- φ CQ P d Φ Hi Hi Ω rt d ft rt P- 3 OJ d 3 ft ft d Φ P ft 0 3 CQ P- < 0 rt 0 φ <! CD P Ω rt cr CQ Ω d φ Φ Ω 3 P 0 d cr 0 φ Ω rt Φ rt d 3 X φ P- Hi OJ d 4 3 d 4 Φ d ft P- d CD P P- 0 P- φ d P- 0 Ξ 3 OJ ^< P d 4 OJ OJ ø ) P Oi 0 Ω Φ Φ P P- P- Hi ft 0J d d CD 3 cr d d ft cr d ~ 0 φ rt 0 3 P rt d P rt 0 ) ØJ ft < 0 ft <. rt cr *< ft J P- rt 0 $. P- P TJ • d ft CD P d 3 0J φ Φ P 0 P- P- φ P Ω Φ Ø rt rt 3 d 4 *< cr Hi rt 3 d ØJ ØJ Φ CQ φ d ft 3 Hi rt 0 ) d 0 d 4 P 3 rt d 4 φ Φ Φ d 4 rt Φ CQ rt Φ > rt d 0 3 ft Φ d 4 ft 0J Φ d 4 Φ d OJ OJ φ d 4 3 O ~ d 4 ^ P ft Ω cr rt 3 rt ft P- d P- 0 ) Φ f Φ rt 3 P 3 Φ cr J TJ 3 ^ Φ Φ 0 Φ Φ d 4 cr P d 4 P < < 0 3 CQ co d OJ OJ 0 0 CQ 3 Φ CQ cr OJ 3 P CQ 3 P d P 0 ØJ P- Φ d Φ φ CQ Ω φ CQ 0 CQ d < P- OJ 3 P CQ CQ Φ CQ 3 g φ Φ P- TJ CQ 0 ft d CQ CQ OJ ØJ ft Ω d 4 d rt Hi d d φ ft CQ 0 φ P- d 0J Φ Ω TJ CQ P Ω 0J d P- CQ TJ P Ω d 0 0 OJ Q Φ ft ft Φ d < P- 3 ft 3 Φ P- 3 d 4 Φ d P- 0 C CQ 3 3 d Φ 0 0 CD <! d Hi 3 rt rt rt rt Φ Φ d cr Φ 0 rt d cr OJ φ CQ 3 Φ d 4 Φ P- 0J Ω d 3 P- rt cr d 4 d 4 d 4 rt P- • s rt 3 CD CQ < rt Φ d CD ft Φ TJ CD d CQ rt rt d TJ 0 0 ) P Ω Φ OJ φ OJ d 4 d OJ Φ P- ^ φ OJ Φ P P- P OJ rt CQ d ft P Hi 0 0 P OJ rt Ω φ h-> OJ d ft 0 OJ Ω d Ω rt rt 0 P- 0 ^ P- P ft P- OJ H 0 r d 3 rt rt H- 1 CD rt φ TJ Hi cr rt OJ OJ d 4 O d CQ d Q 0 Φ 0 rt CD ft P OJ ft TJ d d Ω d 4 CD OJ d d TJ - ' Φ Φ φ d rt d d 4 φ rf CQ Φ ft d OJ OJ d 4 Φ 0 φ 0 rt P rt ^ ø j Ω P CQ CQ rt P d 4 0 ) ft Φ Φ d ft P- ft P rt rt OJ Hi 3 Hi d 4 OJ d 4 rt Φ 0 Ω 3 Φ 0 d 4 Hi φ 0 h- 1 d 4 OJ cr d P- rt P- P- 3 Ω cr Φ h- 1 Φ ft P- 1 < 0 Φ d P 0J Φ OJ Hi Φ Ω 3 CQ P- OJ 3 ft d cr d 4 ft rt P- d Hi P- d 3 Φ Ω Ω o d 4 TJ d rt d ft 0 rt 0 0 ) CQ Φ J d 4 ^ d 4 Ω φ Ω CQ CQ P ft d cr P 3 3 rt Φ 0 Hi Ω OJ OJ φ <! d 4 Hi P 3 Φ Φ d 4 h- 1 d 4 J Φ P- Φ Φ OJ 0 OJ 0 d 0 CQ φ 3 d ft d CQ ft Φ r OJ cr 3 0 ) OJ 0 OJ Φ d Ω P rt P CQ TJ ft ft P d σ P P- rt d C ft rt CD Φ Ω OJ 3 3 rt 3 CQ CQ CQ rt • Φ φ d Φ P Ω ft ft Φ OJ ≤ P- Ω rt P- d 4 OJ CD P- P d 4 ^ J cr 0 cr Φ CO 0J P- Φ CD 0 Φ d 4 P P OJ 0 ) d 4 d 4 P Φ Φ d OJ CQ Φ Φ ft φ d OJ 0 > OJ 3 rt P- P- Φ φ P- • <: Φ φ 3 cr 3 OJ d P rt P 3 ft d CQ OJ P- ft 3 OJ OJ ft 0 ) Ω φ cr s; ^ cr γ- χ Φ - d 4 . P- cr CQ N Φ P- 3 d 0 d ; ; h-> d 4 Φ CD rt Φ d P- 01 d OJ rt φ ft Hi ft OJ ^ P- P 0 rt ^ CD Φ cr 0 P- OJ 0 Ω d 4 rt Hi d d OJ H, d 4 Φ φ CQ CQ rt Φ O O to to H H n o cn o υ. o cn PJ 3 P p P OJ ft Φ o O CQ < d d d OJ 0 ) d φ d ft Ω ft ft ft < O I OJ OJ P rt d φ d 4 Ω Φ ft Φ ft O 0J d d CQ Pi Ω ØJ co Φ tr tr rt C O Φ ØJ p- P- d 3 d Hi O 3 cr CQ Φ rt P; p OJ tr d CQ Φ ft φ CQ p- rt d Φ P p- ft 3 d φ Ω cr Ω Ω rt ft Hi O P- p- Φ P- 3 φ $. ft Φ TJ CQ ØJ f H- P CQ ft P- 3 > d CQ tr cr Φ p- OJ C CD P- Ω ft d φ tr < OJ Φ φ f d CQ φ PJ rt Ω P Ω P- O rt φ O 0J Hi p 3 p O ft TJ P rt 3 P- P P. tr p CQ Φ CQ TJ p- d O d TJ Φ CQ CQ Φ rt Φ tt P CD ft PJ C tr 3 T Φ co TJ d P- ft CQ φ (t 0J d OJ d tr ft P O g ft P- 0 ) Φ O 3 d P- P ØJ CQ OJ ft Q O P p. d Hi P- Φ rt O tt Hi In an attractive embodiment of the multiway valve according to the invention, the field lines of the permanent magnet of the member run radially with respect to the member and the magnet-actuating assemblies are designed to generate a magnetic field whose field lines run substantially parallel through the plane of movement of the member. A magnetic field of this nature will be referred to below as a "parallel magnetic field". In this arrangement, a maximum possible force transmission from the magnet- actuating assemblies to the member becomes possible. This method is illustrated diagrammatically in Figure 7b. The member of the multiway valve may also comprise a permanent magnet whose field lines run axially with respect to the member, in which case the magnet-actuating assemblies are designed to generate a magnetic field whose field lines are transverse with respect to the plane of movement of the member. A magnetic field of this nature will be referred to in this application as a "transverse magnetic field" . This method is illustrated diagrammatically in Figure 7a. If desired, the transverse magnetic field may run through a selective area of the chamber, under the influence of which the member can be attracted and consequently can adopt a position inside the chamber which is such that it closes off or opens one or more channel openings. By displacing the transverse magnetic field, the position of the member inside the chamber will be changed accordingly, with the result that, for example, a different duct opening is closed off or opened. Although the force resultant in the direction of movement of the member will be considerably lower in the case of a transversely applied magnetic field compared to a parallel magnetic field, the member can be positioned very accurately within the chamber using the arrangement in which transverse magnetic fields can be generated. In order to generate a transverse magnetic field so as to influence the movement of the member inside the chamber, the magnet- actuating assembly is preferably disposed in such a manner that the centre axis of the pole shoes thereof is at right angles to the centre longitudinal plane of the chamber, the co co to to H P 1 cn o cn O cn O cn P- 3 ft rt 0 ) 0 P- ft 3 CQ to 3 rt rt TJ N ft 3 CD 3 rt p] P 01 rt tt rt CO d 3 ft 0 Ω P d d φ tr tr ft J CO 0 OJ P- P: OJ φ tr Z 0 Φ tr øi 0 O tr tr PJ d 4 tr tr i Φ φ P- d tr Φ Oi 0 3 Oi Φ < φ Z CQ <; CQ CO Φ 0 CQ P Φ rt 0 < φ Φ ft Φ Φ φ g 3 P PJ CD rt d tr d PJ d ft OJ d φ CO d CQ P P- 0 Φ d φ P- P CO 3 P- cr Φ rt 3 TJ d CQ tr Φ Ω d CO Φ P Φ d d Φ Φ TJ . TJ P 3 PJ J ft Φ ft Φ Ω Φ Ω d 4 σ Φ P P- Φ P rt ft CO ft rt Ω rt ft 0 P- 0 P- OJ φ 0 Ω Z P- rt OJ P ft Φ Φ Ω Φ rt tr 0 ØJ ØJ P- CO P- OJ tr P- tr P 0 h- 1 0J CD 0 3 P ft 0 P P • Φ P ft d ft rt φ O CQ C Ω Ω OJ 0 φ d Φ z cr Ω P- 0 φ P- ft 3 z ft p- 0 Φ Φ ft d rt 3 Oi d 3 Φ TJ rt OJ Φ Φ 0 TJ P Ω Ω p^ ► xl Φ OJ ft P- P- P CQ CD 0 d Φ tr OJ Ω CQ ft P CQ ft tr P P z d 0 Ω ft OJ 0 ft 3 d 0 d Φ rt tr ft d Ω ft Φ 0 CQ J Φ 0 ft tr Φ tr tr Φ ft • P P- φ P- Ω P 0 cr ft PJ Ω tr 0 CD ft P d 0 d P o o P- 0 Φ CO Φ φ CQ 0 0 Φ ft ft Φ P ft P- Ω Ω Φ CO rt φ d Φ Φ P 3 o CO tr 0 » d p. d ft ft P ft z tr Ω P- P 0 d Φ tt P- P Φ ft CQ P Q Φ φ ft d d P CO ft tr tr P- Φ OJ TJ 0 D φ OJ 0 TJ 0 P- rt Φ XI tr CQ 0J - 0 3 tr Φ H P Ω tr Oi 0 P- d p- Φ rt d d ØJ CD d P φ CO CQ P- Ω p- d Φ P d cr cr Φ ft Φ Φ 0 X d Ω CQ 0 - 1 TJ CO J P- ft CD d d φ CO 0 0 OJ d Ω rt - Φ rt 0J CO Φ P- ft φ d 0 ft < ft P- Ω CQ d Ω d tr . tr P Ω O d TJ 0 CD OJ 3 ft P- TJ 0 cr Ω OJ φ ft Φ tr d tr ft Φ P- P- CO Φ P- «• Φ rt Φ d - 0 d 4 < d P Φ PJ d ft rt P- P Φ CQ X Φ d ft rt 0 0J CD d tt Ω < Φ Φ P Ω d Φ tr cr ft P co CD 0J ft φ CQ d 0 CQ P- (t P 0 rt tr rt ft ft P- p. Φ J Φ 0 O Φ Φ tr OJ Φ CD P- P P ft π. Φ d 3 tr PJ Ω P P P- tr tr CQ 3 3 3 0 φ 0 P- φ d OJ ØJ d 3 ØJ ft 0 rt O CQ OJ Φ ft Φ Φ CQ d rt Φ z Φ Φ OJ CQ Φ 3 d f CD d Z P- OJ d φ tQ 3 tr ft P- d P- d PJ CO 0 tsi P- d 3 rt φ X ft OJ CQ t Ω <! Ω Oi ft ft d CQ ft Φ Φ Φ ft d 3 0J rt ft 01 3 φ (t rt ø 4 Φ - φ tr tr 3 CQ Φ φ tr d <! d rt 3 ft Φ Φ ØJ P X O ' M rt Φ P d 4 Φ P P Φ Φ 0 d Φ 0 P ft Φ φ φ 0 Φ tr tr CQ P P CQ Φ h- 1 P- P P- tr 3 0 0 P P- P- ft < φ XI r CD O P- P P d P Φ Φ tr 0J (t d ft φ CQ Ω Φ φ cr - P PJ rt φ O Φ rt d Φ φ P 0 co O CQ 0 ) P 0 d tr ft Φ 0 OJ Φ CO Φ Φ ft z ft ØJ 0 3 P- OJ CD 0 ØJ ft Φ ft rt 3 P CD Φ tr rt P OJ CQ 0 Ω P 0! CO ft P- P- 3 P φ Ω z 3 ØJ P- tr tr Φ OJ rt rt < OJ 1 Ω P ft P P- φ d TJ tr rt rt CQ cr Φ Ω d • T øJ ft d ft OJ Z Φ ft CQ 0 φ Φ Ω rt OJ Φ O Φ d d P- ft Φ Φ d 4 0 Φ rt Z -> rt tr Ω rt 01 d CD P tr - Ω d (t rt CD rt co Ω d 3 P- OJ tr Φ Φ TJ 3 cr φ rt rt CD PJ rt P d tr tr d ft P (t rt P σ φ rt OJ Φ 0 φ $ ~. Φ o rt φ ^ rt tr Φ 3 P- d Φ ft Φ Φ tr φ ft tr ØJ φ Φ Ω tr CQ X Ω CQ tr • 3 1 Φ ft cr 0J CO rt Φ P- Φ rt CQ Φ Φ d φ ft 0J C 0J 3 tr P P- Φ cr OJ P- Z Φ rt d (t 3 CO PJ ØJ P 0 rt TJ PJ CQ P- P ft P t P- OJ 0 ) 0 rt H Φ tr Ω CO CO PJ P rt P- tr 0J ø ) d TJ X φ P Φ φ P CQ 0 rt tr rt P CD Ω CQ 3 3 P- 3 P Φ rt OJ rt •> tr d ft Φ CQ P- rt P- Ω Φ ft P Ω P OJ tt d φ Φ 0 OJ 0 d cr 0 φ d P- OJ Φ CQ PJ d ft > OJ CD ft Q tr • rt OJ P tr ft ft d C Φ d Φ Φ rt d 3 rt Z Q OJ ft d tt d Ω φ d Φ d Φ d p. Φ φ 3 cr CQ X CD ft P tr cr tr tr OJ rt Ω 0 tr Ω OJ ft Φ TJ φ 0 ft P] rt CQ P cr φ Φ φ r Φ P- Φ Φ φ P- P- P- rt φ Φ Φ CO d P- 0 tr rt Ω tr 0 φ PJ *< 3 3 P OJ Ω rt P- P Ω ft d P d CQ z rt Ω Φ 0 ft OJ Φ d ft 0 TJ O cr rt Φ rt d 0 Ω rt 3 tr CQ OJ ft ft rt Φ P- P OJ Φ ft 0 d d O rt P 0 0 Φ P d r Φ Ω Φ Ω d 0J d P tr P- P 3 Φ P-" 3 tr z rt rt tr 3 cr d P OJ rt t ft Φ cr d P- P- CO OJ CO 0 Φ CQ φ cr y-> CQ φ 3 Φ OJ P rt φ P- ft Φ d Φ d P d Φ rt co 0 ft CD CQ CO < 3 ft ØJ p; tr 3 0 P 0 φ tr P tr rt P- CQ 0 0 01 ft P CQ P- φ CO φ Ω 0J OJ p; 0J X 0 cr TJ ft Φ TJ P Φ 0 TJ d <! d ft P D Φ Φ Z ft 3 φ P rt tr d X P- Ω Φ Φ Φ o O PJ 0 d 0 0 CO Φ P P- Φ tr CQ Oi P- cr 3 CO tr PJ Ω P- P- CQ CD O CQ P 3 ft X CD 01 P 3 TJ P- P ft rt OJ 0 0J ^ P tr φ Φ 3 Φ CQ CQ O d • Φ Φ OJ tr P- d d 1 OJ TJ Φ ft CO d 4 tr 0 P X O φ P. cr σ ft z d d Φ co 3 Φ CQ tr 0 φ φ P- Φ rt P- < Ω z Φ o cr Φ d P- rt CD ft 1 Φ CD CD CQ Φ CQ 0 ) ft Oi P Φ rt Ω CQ tr 0 0 0 P- tr ft Z 0 P Φ Oi H Z ft 0 0 rt 0 tr P- P tr ft 0 <! ft P- ft φ P- Φ Φ Φ φ (t f Ω Φ 0 P φ . CQ tr φ < CD tr Φ Φ d Φ • p; member for as long as the member is to remain in the said position, thus ensuring the correct position of the member and the correct function of the multiway valve. If the said distances are equal, the assembly will not exert a radial force on the member and the member will only be held passively in this position. In the case in which the member closes off a duct opening by direct interaction with a transverse wall of the chamber, in the above-mentioned case the shortest distance from the magnetic centre of the member to the transverse wall will be determined by the diameter and the shape of the member and the position of the magnetic centre therein; however, if the member interacts with a closure body or opening body as described above, the distance is partly determined by the shape and the configuration of this body. Magnetic centre is intended to mean the centre point of the magnetizable material of the member. If one or more duct openings are incorporated in the transverse walls, it is highly advantageous, in order to achieve optimum immediate closure, if the centre axis through the pole shoes of the magnet-actuating assembly intersects a radial axis of the chamber through the duct opening. In this way, the magnetic force resultant will be directed directly onto the duct opening in question, ensuring successful closure, which is especially advantageous if the multiway valve comprises a plurality of magnet-actuating assemblies which comprise electromagnets with a soft-iron core. The invention furthermore relates to a method for actuating a multiway valve according to the invention with the aid of one or more magnetic fields, wherein one generates a magnetic field with at least one magnet- actuating assembly, in order to move the member, under the influence of the magnetic field into a position inside the chamber which opens or closes at least one duct opening. It is thus possible to generate a transverse or parallel magnetic field, so that the member is moved, under the influence of the magnetic field, into a position inside the chamber which allows at least one duct opening to be opened CO ω to to H H cn o cn o cn O cn φ 3 d OJ O φ Ω J 0J P- cr OJ d 4 CQ Φ φ cr Φ P- rt d Φ P- CQ ft Ω Φ 3 3 3 Φ 0 ) < Φ Φ CO P OJ t-x 0 CQ d Φ d PJ z d Φ d CQ tr Φ rt tr tr tr 01 0 ) Φ OJ d φ 3 0 CQ P- ft φ 0 CQ CQ P- O CD P- Φ Φ rt Φ OJ Φ Φ CO 0 Φ OJ Φ ft CQ 3 d Φ ft d cr d Φ CQ rt Ω CQ 0J Φ P- d ft rt P Ω z P rt ft Ω Φ 3 Ω ft d cr d Ω ft Φ CD 3 P- Φ ft d P 3 ft CQ tr tr Ω CQ rt Φ CQ O ft J CD PJ cr ft Φ Φ Φ Φ ft rt P cr d P P P P- cr Φ Φ Φ tr P- P Φ P- P P- P φ rt Φ P P rt P P P tr 0 p. OJ 0 Φ ft φ P Φ φ t i O d N CQ 0 O P 0 rt P O •« O Φ OJ P- - P- 3 p. P. ft d d ft φ g Φ 0J P g g P 3 O Ω rt 3 d φ t- h- ' co ØJ 0 tr M φ Φ ft PJ tt ft d P 0 ) PJ PJ z PJ O J tr OJ 3 TJ PJ ft P- CQ P- p; CQ P- Φ P 3 0 CQ tr 0 Φ ØJ CQ d ft Ω tr C d P 0 OJ CQ ØJ P d d CQ ft d CQ CQ CQ Φ 0 φ d Φ CQ ft XI d d Φ tr ft Φ d Ω ft Φ O It d CQ φ rt 0 tr TJ P Φ ft O Ω P- P- Ω < Φ d tr d Φ d Φ P- d Φ Φ tr P- Φ d J tr CD - 1 o P- rt tr OJ d 4 tt N ft Φ •» Φ rt 3 Hi Φ H- φ rt rt 0 rt Φ Φ d P- ft Φ Φ Ω Φ d CQ < Φ rt ft OJ Φ P ft Ω . Φ Hi P P H D d rt - P- P CQ rt » it P • ft Ω OJ P- φ Z tr < 3 P- ft 0 PJ ft 3 P- Φ φ z 3 Z tr ft 3 0J 0J d 0 tr PJ tt d P- ft OJ OJ cr CD • 3 cr CQ P P3 cr Ω 3 ft Ω tr PJ P- cr Φ 3 Φ cr O 0J OJ PJ tr PJ rt 3 ft P- d rt d Φ OJ p. 0J 0 tr Φ P- 0i ft P- CQ ft Φ PJ tr 3 Hi it d Ω rt tr ØJ C 0 0 Ω ft P ft CQ P- g Φ P Φ CQ ft P Ω d Ω rt Φ P- 0J cr . Hi rt ft ft . P- Φ -> PJ d d rt ft 01 Φ d rt d PJ d d 0 0 tr Φ tr z d O Φ P d 0 P 3 rt d φ rt cr tr CQ rt O Φ tr CQ 3 0J ft Φ 3 rt Φ Φ Φ rt P 0 OJ (t ØJ d 0J P- ft ft Φ 0 Φ Φ 0 P- rt Φ 3 d Φ d rt ft OJ P- ft Φ Ω PJ tr ft P Ω tr rt rt OJ d Z 0J 0 TJ O P ØJ φ 3 ft p. P- CQ CQ ft P- Φ P- tr It Φ P- tr 0 CD d OJ CQ cr 3 Φ 3 d cr ØJ ø ) CO P- rt cr 0J CQ d Z O P d Φ co Φ 0 CD d Φ CD Φ p. Φ p; OJ d φ CD Φ cr tt PJ d Φ rt rt Ω TJ Φ CQ P- rt 0 CO d TJ Φ Q φ P 0 P- ft P- 3 ft P- rt PJ P d 4 O ft ft Z tr 3 CO 3 φ O 3 ft 3 <! d tt ft Φ d σ P. Ω Φ P ft 0 ) d Φ d 0J P- Φ OJ tt 0J φ OJ d P Φ OJ Φ d 4 cr rt OJ CO tr CQ CQ Φ tr OJ P- ft P- O ØJ Ω ft rt 3 CQ tr rt CQ P- Ω CQ 3 P- tr Φ rt • P Φ 0J Ω Φ d CD < tt Φ O Ω ø ) 0 ) TJ d Φ rt φ d d P tt CQ cr CQ P- OJ < P 4 TJ o d d 0 rt d CD P- Φ P- tr rt CQ Φ Φ P Ω Φ CQ φ P Φ Φ Φ rt φ OJ 0 rj P Φ CQ P CD Φ PJ rt P P d ft cr Φ rt d P rt P 01 ft rt TJ 0 3 P d CD rt CQ P * Φ P Φ P P- tr CD Ω CQ tr Φ ft P φ 3 φ Ω Φ P- 0J φ 3 cr OJ 0 OJ <! rt P- φ < CQ ft ft rt CQ rt ft Φ ft O Φ ø ) rt Oi tr CO rt ft Ω it PJ Ω ft P d P Oi P ft TJ P Φ P- tr tr P- CO Φ d 3 01 TJ 0 Ω • d OJ d Φ CQ CQ p. o d Φ Φ φ P ØJ P- φ Φ p N Φ φ N P CQ Φ CO 3 Φ ft Φ D ft P- CQ d 3 P TJ P- Ω 0 <! CD Φ tt φ TJ 3 z CQ φ P p] d ft d ft Φ It Φ Ω TJ Φ Φ ØJ φ 0 ft d Φ φ ft tr TJ 3 ft 0 rt 0 H- tt φ 3 3 - ft tr rt cr 01 cr P PJ tr it O P » D d d P- ft P CQ Φ 0 Φ CD tr < rt tr 3 cr OJ tr Φ Φ d : CQ φ CD φ 3 P- CO φ CO d P- d 4 CD CD 3 φ P- Φ Φ Ω Φ cr Φ d CQ Φ 3 Φ rt d d rt P- TJ CD rt ft Φ P CQ d Φ P- ft z P- 3 P- cr -x rt ft tr P φ O 3 ØJ d PJ Ω CQ TJ CD P Φ tr tr 3 CQ 3 d tr rt ØJ ft Φ φ P- Φ Φ ØJ 4 d TJ Φ CQ TJ d tr rt O Φ P- CQ Φ Φ cr P- ØJ Φ Z 3 CQ Φ tr CQ P- P Ω 0 rt ft rt P- ft ft O 3 d CD O tr d P φ CD tsi CQ d tr Φ d 0 ft d Φ 0 tt ft d tr cr Φ z CQ Φ OJ Φ 3 d Φ 0J 3 3 * φ d Φ P- 3 rt o P φ d pi P Ω Z O P 0 CQ 4 PJ Φ Φ tt P- P- d 0 ØJ φ CD φ φ ft Φ P Ω cr tr J φ rt O 0 P- rt PJ ØJ P- rt P ft rt Φ 3 ft d P TJ 3 3 01 rt CQ tr Φ φ Φ < 0 g d P P Ω cr ft Φ O OJ Ω P- P ØJ d φ CQ 0 ) Φ cr cr rt CO P- P d φ OJ PJ PJ rt 0 ft rt Φ Φ d rt tr d tr O CQ d It Ω d P- d P Φ Φ rt P- OJ N P- - TJ P- P Ω CQ 0 g CQ P- Φ tr 0 cr ft Φ d P- d tr rt rt N 3 P P P 3 Ω OJ rt 0 d CQ ft ft P d PJ O cr ft P Φ Φ p. ft N φ Φ φ 01 . OJ d ft ft CQ CQ Φ d tr Φ φ CQ P CQ rt P- Φ P O 3 ft d P- z CQ ft d P tr Ω d P- Z 0 ØJ ft 0J Φ CD ft tr d tr P- Φ P- Φ 3 tr 0 d ft TJ TJ 0J Φ CQ tt ft OJ 0 ØJ P 0 rt d P- φ Φ Φ N o Φ Φ O ft Φ Φ CQ P- d d CQ PJ ft d CO rt P- P P- 3 - 1 d Ω ft O Ω Φ P- OJ P- tr P d d d rt Q P- tr rt d Φ ft d tr P tr ft CD d TJ ft ØJ 3 P- Φ d ft ft d OJ P. CQ 3 ft P- Ω p; ØJ • OJ O o ft φ rt ø ) d ft CQ 3 P- tr tr CQ rt cr 0 P- P- CD Φ 3 d d d d CQ d ØJ ft Φ Φ Φ h- 1 rt cr > O 0 φ Φ ft rt Φ . Ω CQ φ rt ft p Φ tr tr d It tr d ft tr tr P ft Φ Φ It tr Φ Φ Φ O Φ ØJ rt inside the chamber, as it were towards the desired position, due to the fact that the resultant force for displacing the member is intensified by the repelling magnetic fields. Furthermore, relatively weak energizing pulses are sufficient to displace the member from a certain position to another position inside the chamber of the multiway valve. In order to achieve accurate actuation, it is advantageously possible to dispose a plurality of magnet- actuating assemblies in the multiway valve and to energize them in such a manner that they repel the permanent magnet, the positioning of the member being influenced by varying the magnetic field strength of one or more magnet-actuating assemblies. Due to the fact that all the magnet-actuating assemblies repel the member, the member will be moved towards the magnet-actuating assembly which is repelling the member the least. By changing the magnetic field strength of one or more of the magnet-actuating assemblies, the position of the member will be changed accordingly. However, in this embodiment it is necessary for the magnet- actuating assemblies in question to be energized continuously . The present invention will now be explained in more detail with reference to the drawings, in which: - Figure 1 shows a simplified, diagrammatic plan view of a chamber of an embodiment of the multiway shut-off valve according to the present invention, in which the member is designed as a hollow disc and in which five ducts open out into a bottom surface of the chamber, Figures 1A, B, C and D each showing different closure positions of the member. - Figure 2 shows a perspective view of a multiway valve according to the present invention, in which the member is connected to control means by direct coupling. - Figure 3 shows simplified cross sections through various embodiments of the member and the relative position thereof inside the chamber. - Figure 4 shows an embodiment of the multiway valve according to the present invention in which the valve comprises magnet-actuating assemblies for generating a transverse magnetic field. - Figure 5 shows a simplified view of the cross section in accordance with Figure 4, in which the forces are illustrated as vectors. - Figure 6 shows a possible circuit diagram for actuating the multiway valve in accordance with Figure 4. - Figure 7 shows possible magnet assemblies for generating a transverse magnetic field and a parallel magnetic field. - Figure 8 shows various embodiments of the member, each part of the figure showing half a plan view, a cross section and half a bottom view. That half of the views which is not shown is in each case identical to the half which is shown. - Figure 9 shows a possible combination of the axial ducts from Fig. 1 and the radial ducts for Figure 4. - Figures 10 and 11 show simplified, diagrammatic plan views of two further embodiments of the multiway valve according to the present invention. - Figure 12 diagrammatically depicts an application of an embodiment of the shut-off valve according to the present invention. - Figure 13 shows a plan view, two cross sections and a bottom view of an embodiment of the multiway valve according to the invention in which the member and the chamber are of convex design. Figure 1 shows a highly simplified, diagrammatic illustration of a plan view of a chamber 90 in which a member 91, which is designed as an annular disc, is accommodated. A member cavity which is enclosed by the ring shape is denoted by 97. The parallel surface of the chamber which is situated beneath the disc includes four peripheral duct openings (93, 94, 95, 96) and a central duct opening (92), the central duct opening being in communication with one peripheral duct opening in every position of the member 91 while the other peripheral duct openings are closed off, (cf . Figures 1A, B, C and D; the duct openings which are closed off are illustrated as broken circles) . The dead volume of the valve according to this embodiment is determined by cavity 97 which is delimited by the disc-like member 91. In this embodiment, the dead volume does not vary during operation of the multiway valve. For this reason, and due to the fact that the direction of movement of the member is at right angles to the ducts 92-96, the operation of this multiway valve is insensitive to any feed pressures through the ducts. This embodiment is therefore eminently suitable for use at high pressures, such as in the case of HPLC. It is possible to connect the chamber 90 to ducts which open out into its side walls. Member 91 may, if desired, also close off or open the latter ducts. In principle, the number of central and peripheral duct openings in this embodiment is unlimited. The number of corners of the chamber may also be adapted as desired: the chamber may also be of round design. For considerations of clarity, the control means are not shown in this figure. In Figure 2, the multiway valve comprises, in addition to central duct opening 92 and the peripheral duct openings (93-96) , duct openings 61-68 which likewise open out on the underside of the chamber, but which are situated in the vicinity of the side wall. Owing to the shape of the chamber and the member, these ducts cannot be placed in communication with the member cavity. Consequently, two closure circuits are defined, namely the central circuit, comprising the duct openings 92/96, and the peripheral circuit, comprising the duct openings 61-68. Obviously, it is also possible for the position of the duct openings 93- 96 to be selected in such a manner that they may form part of both the peripheral circuit and the central circuit. Hollow disc 91 is connected, via push and pull rods 71-74, to control means LI, L2 , L3 and L4 , respectively, which each contain a magnet 81, 82, 83 and 84, respectively. Depending on the direction of the current passing through a coil situated in LI, L2 , L3 and L4 , respectively, the magnet in question is moved either towards the chamber or away from the chamber. In Figure 3A1, a member 31, which is designed as a continuous disc, is situated in the vicinity of the centre of chamber 30. The control means are not shown in this cross-sectional view. A feed duct 32 opens out into chamber 30 via duct branches 32A and 32B. Via chamber 30, duct 32 is in communication with discharge duct 33. Duct 34 is closed off by member 31. In Figure 3A2 , member 31 is situated in the far left of chamber 30, closing off feed duct branch 32A and discharge 34. Feed duct 32 is in communication with discharge duct 33 via duct branch 32B. Figure 3B shows an embodiment of a member 310 in which a groove 311 is arranged tangentially in the outer circumference. A central feed 312, which via groove 311 is in communication with that part of the chamber which is not closed off by member 310, opens out in the side wall of chamber 313. In Figure 3A3 , member 31 is situated in the far right of the chamber, with the result that feed branch 32B and discharge duct 33 are closed off. Via duct branch 32A, the central feed 32 is in communication with discharge 34, the opening of which is situated in the opposite plane- parallel surface with respect to duct branch 32A. In order for the member to be correctly guided inside the walls, the side walls of the member may be of convex design and those of the chamber may be correspondingly concave. Through groove 311, duct 312 is in communication with discharge duct 314. If member 310 is moved to the right, duct 314 will be closed off, so that the central feed duct will be placed in communication with duct 315. In Figure 3C, the member 316 comprises a cavity 317. Via cavity 317, feed duct 318 is in communication with discharge duct 319. By displacing member 316, discharge duct 319 can be closed off and duct 320 can be connected to duct 318. In Figure 3D, member 321 is designed as a hollow disc. In the position of the member which is illustrated, feed duct 322 is connected to discharge ducts 323 and 324. Duct 325 is closed off. By moving the member to the right, discharge duct 324 will also be closed off. When the member is moved to the left, discharge duct 323 will be closed off co t to H n o cn o cn o cn TJ OJ Ω PJ p Ω O o ft ØJ Ω ft Ω Ω O co ft μ- ft z ft TJ 3 ccrr ft Ω Ω P Ω PJ P Φ 01 Hi μ- μ- d O d o - OJ φ Hi CO Φ d Φ OJ P- co PJ Φ Φφ μ- o M t- χ to μ- to t Φ ft Ω < Φ CD < Hi rt CQ ft d Ω d d d ιl co rt o - χ co --» P 3 co d to O oo p. -J Φ O P- d P- d Ω d it ft CQ CQ μ- Φ Ω co PJ cr 0 Ω d CQ Φ P rt Ω h- 1 (t OJ ØJ LO Φ μ- O rt d p- CQ P CQ Φ 3 tr Φ Φ μ- co ε d 0 ft O rt 4 d rt co Ω LO d d tr P d d OJ d O P P- OJ Ω ft ft CQ tr P Hi P- d ft p- it CO d Hi It p] Ω o d Φ rt p rt d O p- Φ d o d ft o Φ 00 o p; PJ 01 φ tr rt PJ Hi CO tt Q Φ Ω O Ω Hi Ω ft CQ TJ Φ d 4 O ft d ft d d Ω P Φ OJ o d z t Φ Φ ft ft Hi O tr M o tr p- cn Ω PJ μ- d tr o OJ CD σ ft Φ OJ ft rt tr ft cn ft CQ Hi d ft d r Hi Φ ft CQ ft rt O Ω d it P Φ I Ω rt Z tr p- o ft rt d tr μ- O d Φ Ω it tr Ω O P cr z It ft Φ tr p- rt Φ Ω TJ TJ μ- d O CO φ Φ co o TJ P ft ft o ft OJ o p μ- O 3 o rt tr tr p- d J Ω to td Ω μ- t d rt φ d ε cr rt d p o ft ε cr d tr OJ p CQ PJ rt P tt ft CD p; ft Ω μ- CQ c OJ tr rt Ω co d φ tr CQ Φ It rt μ- φ CQ It o d d Φ O co d φ tr d d d Φ co O ft co φ Φ Φ OJ tr d rt P tr it rt P ft P < Ω OJ g ft ØJ P 0 φ Q P- d ft co rt p tr tr o OJ P φ ØJ μ- rt d O 3 Ω Φ P p- O co P- P- d to 3 co Φ ft Hi Ω rt Φ Hi tt o cr Ω ft rt ft < ft cr O 0 d CQ d co Cfl P Φ μ- σ. ft μ- OJ o O tr OJ rt o rt φ tr μ- O Φ 3 co Hi < tr Φ H TJ o ø j 3 d P Ω d 3 μ- ft ft cr OJ TJ rt ft Φ co ω p p 3 TJ o φ o d p- μ- ft d cr OJ μ- φ Φ φ TJ D μ- tr It rt μ- H co IQ ft d c P d Z PJ P- o d CQ OJ ft Φ rt d d Ω P co Φ φ PJ o d rt CQ o d co d φ o rt CQ d CD z d ft p tr ft ft Ω μ- ft Ω cr it 3 tr μ- g Ω μ- 3 < μ- O Ω P φ co Φ rt μ- 0 d co o Ω ft tr ØJ ft OJ φ ft co Ω Φ o φ 0 rt O φ ft Ω tr o d o φ φ μ tr μ- Φ Φ ε rt Φ Hi P CQ OJ Hi d tr co ØJ CD co Φ d rt It o co co OJ D OJ co φ cr rt Cr φ Ω Φ O co I ΓtT < μ- -J OJ tr 3 Ω ft 3 φ rt ε ft φ O μ- Φ ft d P p CQ rt I d ttrr ØJ μ- ft Ω Ω Φ 3 d O cr p- Φ tr 01 d Ω P to O P tr rt Z O Φ tr d P P P rt φ tr μ- ft p Φ O Hi Φ CD Φ Ω d Φ p- 0 ) ft φ p- O 0 Φ μ- ØJ d it 3 CO p P Ω cr μ- ft O ) ft o rt d Ω d >-• φ Z d μ- Ω φ Φ d rt CQ to tr to ft Hi tr ft O 0J CQQ Ω D OJ tr rt σ d Φ d O OJ p LO CQ O Φ σ. d φ σ. d φ ft o ttrr ft Φ tr p φ P rt Hi it-, J co ft ft it Ω Ω rt ft Φ rt Hi Hi μ- 0 ØJ tr p φ CQ Ω P o μ- cn 3 --» to TJ tr Ω rftt tr d Ω O ft o It H H CQ d φ Ω Ω φ Φ rt P CQ OJ tt-. CD O OJ o O C COQ Φ Ω It OJ I d tr oooo Φ ft O Ω ØJ CQ CO tr d d Hi D CO cr 3 rt P- ft d tr 0J oo ft Hi Ω α tr <1 CQ TJ Φ ft Ω d ft O OJ Hi o P- O TJ 3 co o d ft OJ z rt rt μ- ØJ μ- ØJ O tr O φ Hi d μ- - ft rt P r rtt Φ d Ω d μ- 0 tr ft CQ CQ d Φ J P tr ft OJ P- tr μ- dd 44 3 TJ ft ft ft rt ft Z Hi Φ tr φ o σ μ- p; ft o μ- O T o It d Oi o CQ Φ Φ tr O ft d d 4 d μ- Hi P Φ Φ Ω d μ- Ω p O rt tr co ft d d d rt Φ Φ CO d 4 LO Ω TJ Ω rt . Φ co p ØJ CQ co p; ε d OJ o P- rt Φ co ft tr co 3 P P- P It o it rt Hi Ω l d CQ rt TJ Φ Hi (t o H ft It Φ Φ • (t 0 o ω tr O tr cn tr μ- ft tr Ω d P ft 3 P- d p- Φ co P d P OJ d z cr ØJ ØJ P; O P O ft tr Oi Ω OJ d rt cr tfl 0 CQ < co rt φ φ 3 o Ω tr Φ d < d rt d O tr rt co PJ P It rt Ω d o 3 Φ p; d d- P- .t- p- oo TJ cr rt O μ- d O Φ Ω φ Hi φ tr μ- Φ Φ ft TJ Φ P 11 0J t O TJ μ- ft Φ P d 3 Φ μ- O Z o ft φ ft cr CO ft ft 3 < ft ø j d μ- Φ CQ o p OJ rt o Q it d tr Hi PJ Ω Φ Φ ft to P OJ cr w 0 ) tt ØJ tr CQ Ω d It OJ < Ω O Ω Φ d tr TJ CQ p Φ oo μ- Oi d Φ cn P o tr d Φ rt P ft co φ μ- ft φ cr CO OJ p Ω P3 OJ d ft ft p o p. d PJ Φ ft Z p Ω φ d it-. ft d μ- ft p. cr < Φ O tr PJ 3 co μ- Φ P- p- rt Ω o CD co co Φ Φ d Φ d cr d --» CQ TJ μ- ft cr Ω Ω d φ rt o O co ft Ω co p- < d Φ co P μ- D O OJ OJ CQ μ- φ co tr TJ OJ PJ Φ co It rt Φ d p I ft φ CQ rt < it φ rt to PJ tr X tr Ω ft d ft it μ- It tr cr rt ft tr (t d OJ Φ ft PJ φ OJ p d O ιt cr tr Φ Φ d 4 Φ tr d φ p d ØJ Φ Ω 3 p; Φ Φ p p Φ Φ ft ft pressed against the top or bottom wall (356 and 357, respectively) of the chamber 355, thus ensuring the correct positioning of the member. In Figure 3G1, the member 350 is pressed against the top wall 356, duct 351 which has a cross-sectional area A2 and a pressure P2 being closed off. Ducts 352, 353 and 354, in which pressures Pla, Plb and Pic respectively prevail and which ducts respectively have a cross-sectional area Ala, Alb and Ale, are arranged on the opposite side with respect to the plane of movement of the member 350. In the case illustrated, the sum of the pressure exerted by the ducts 352, 353 and 354, each multiplied by the cross-sectional area thereof, Σ(P1*A1) is greater than feed pressure P2 multiplied by A2 (P2*A2) . As a result, a force will be exerted on member 350 in the direction towards top wall 356, with the result that the member will be prevented from moving within the chamber. Duct 352 is also closed off, while ducts 353 and 354 are connected to one another. If Σ(P1*A1) is equal to P2 multiplied by A2 , member 352 is not pressed against either the top wall 356 or the bottom wall 357 of chamber 355, so that movement of the member is not impeded, cf. Fig. 3H. Movement of the member may also be impeded if P2 multiplied by A2 is greater than Σ(P1*A1), with the result that member 350 is pressed against the bottom wall 357 of chamber 355, cf. Figure 31. In Figures 3G, 3H and 31, the cross-sectional area of duct 351 is varied; however, it will be clear to the person skilled in the art that it is also possible to change the cross-sectional area of one or more other ducts and/or the feed pressure in one or more ducts. With this embodiment, it is possible to improve control of the lateral movement of member 350 in chamber 355 by varying feed pressures. Figure 4 illustrates the method for positioning a member by means of magnet-actuating assemblies with the aid of a transverse magnetic field. Although the method can be carried out for, for example, eight magnet -actuating assemblies, it has been decided here, for the sake of clarity, to explain this method with reference to a radial three-way valve. In the plan view of Figure 4A, the multiway valve comprises a housing 1 made of a non- magnetizable material, such as stainless steel or plastic. A cover 2, which is likewise made from a non-magnetizable material, is mounted on the housing by means of screws 14. The multiway valve is connected to ducts 12, 12', 12'' for feeding and discharging a medium. Three magnet-actuating assemblies 5, 5', 5'' are disposed around the housing, a pole shoe 6, 6', 6'', respectively, of each of these assemblies extending above the housing as far as close to the centre thereof. The multiway valve is illustrated further in the longitudinal section shown in Figure 5, in which a chamber 10 is situated in the centre of the housing 1. An annular member 4, in which a permanent magnet 3 is concentrically accommodated, is situated in the chamber. The shape of the chamber 10 substantially corresponds to a triangle, the corners being rounded with a radius which is equal to half the diameter of the member 4. Via narrowed section 13, 13' and 13'', ducts 12, 12', 12'', respectively, open out into chamber 10. The ducts which open out into the plane-parallel surfaces are not shown for the sake of clarity. The magnet assemblies 5, 5' and 5'' comprise windings 9, 9', 9'', respectively. The ends of the pole shoes of the electromagnet assemblies 5, 5' and 5'' are indicated by broken circles, but they are situated above and below the plane illustrated; they are shown more clearly below in the cross sections shown in Figures 4B and 4C. In the position shown, the member 4 closes off the opening of duct 12. The openings of ducts 12' and 12'' are in communication with one another via chamber 10. The volume inside the chamber which is not taken up by the member (the so-called dead volume) is very low in the case illustrated. If desired, the dimensions of the chamber may be selected to be larger. Figure 4C shows a cross-sectional view through magnet-actuating assembly 5'', pole shoes 6'' and 7'' being respectively mounted above and below the chamber, the centre axis of both pole shoes running just next to the ω CO to to H t- χ cn o cn o cn CD cπ 3 CO Hi Hi rt »t- 3 ft TJ Hi rt 0 φ CQ OJ 3 Z _ OJ 0J Φ OJ μ- 0 tr - Φ P- φ P- tr P d φ CO ØJ OJ TJ It X 3 3 φ P φ 3 P P Φ Φ φ d CQ CQ y- χ It μ- cr Φ Z σ Φ 3 y- χ rt P φ φ d -x tr CQ P 3 Φ OJ P ø> Φ ft φ TJ P- Φ Ω PJ ft 3 OJ y- χ P ft X o rt P rt d oi Φ μ- 0J cr ft O d Ω μ- ØJ CD tr Φ φ y- χ CQ N rt Hi ft ft Hi j-. P μ- 3 μ- *> ft d μ- d TJ Φ Φ P 4 co μ- TJ O Φ d TJ rt rt ft d Φ Φ ft ft ft t O P μ- Ω φ t-x μ- tr ε rt φ tt P μ- O tr d Ω CD tt CQ Φ 0 Φ μ- 0 3 CD 1 3 Φ CQ d Φ Φ μ- * d y- χ ε OJ OJ 0J y- χ OJ p Hi O PJ 0 cr P H OJ CQ P Ω d φ y- χ Φ TJ " Ω Φ O rt d Φ μ- μ- Φ P d d ft Φ Ω cr d O tr O P TJ it rt co CD cr ft Φ d d d rt φ Φ ØJ J Ω Ω P ØJ z d Φ co tt ØJ rt P μ- P φ 3 Φ Φ OJ CO φ d d y- χ μ- rt 0 ιt CQ cr Ω φ 0 CO rt P It co n d μ- 3 3 μ- CO Φ rt O 0 ) It It d ε It Φ tr - d ØJ OJ OJ N tr P P- Hi d Φ tr P rt TJ Φ rt CQ CQ C Q φ 0 • ft ft 0 It Φ OJ tr Φ Hi tr d d ft Φ φ rt TJ D tr d rt ØJ y- χ μ- O Φ OJ Φ. Φ OJ CD μj tr cr φ φ Φ Φ rt y- χ d P O It rt tr Ω *< Φ t p . P ft φ It Ω O CD P Ω cn φ 0 TJ CQ rt ft φ Φ J φ co OJ φ O 3 μ- ØJ Hi 0 μ- tr P CD J 3 Ω CQ 3 Oi ft μ- ØJ co CD y- χ N H Φ Hi μ- 0 cr O ft d TJ d d CD CQ CD It φ Φ Hi P 0 TJ CD Hi μ- H" ø ) ft Ω d o φ tr ft 3 0 P μ- ; d It P ft p Φ 3 Φ CO 3 φ 3 tt ft CQ øi 1 0J rt PJ cr tr μ- ØJ 3 o TJ d φ n tr 0 cr . H ft P 0 d CQ cr rt Hi d Φ tr ft Φ O Hi y- χ to μ- co ft p. Φ φ ft μ- d φ -3 øJ P D O Φ P Φ ft μ- TJ d 3 It tr μ- y- χ O it cn 3 d rt tr P φ rt d 4 Hi Φ D d tr ~ PJ cn Ω 1 z TJ Φ φ CO 3 tr Φ O d μ- φ d - tr OJ μ- 0 z Ω d cr Φ P Ω P It OJ Φ Ω y- CQ Ω P- ft Ω Φ 3 Ω It y- χ tr p d d OJ It y- χ μ- tr y- χ P- tr P 3 OJ φ tr O rt Φ Φ ft rt PJ d rt OJ O ØJ CQ CQ Φ CO tr CQ d 3 OJ tr μ- 3 d ØJ CQ d φ Φ TJ c 0 ) 3 ft OJ rt φ 0 cr tr rj d Φ ε 3 ft 0 y- χ ft PJ d μ- d Φ ØJ ft 3 p; Φ It μ- OJ ft y- χ rt 0 CQ o d d ft P 0 ØJ ft μ- CQ cr μ- φ PJ TJ d Φ CQ P CQ • φ d rt μ- Ω y- 1 d p. p P ft Φ - P μ- tr rt d tr N Φ φ O rt CD rt ØJ o > ØJ tr φ Φ ø ) Hi rt rt Ω tr P rt CO φ Z O 0 P d cr μ- μ- 1 tr rt 0 J OJ CO d tr CO d d p CD φ rV 0J Φ P- Φ Ω ^ d ØJ Φ ØJ φ φ rt Φ Φ y- χ φ Ω O O w TJ rt 3 0 μ- CD tr d ft z It 0J P 0 tt μ- cr d d P 0 ØJ Φ 3 μ- d Ω cn O CD tr d rt It φ Hi rt P 0J O CQ OJ rt 0 Hi P- Φ tr p; TJ CD rt CQ ft Hi φ rt μ- Hi ØJ ft rt Φ 0 μ- d μ- φ ft OJ ft tt μ- O d μ- tr n Hi Q P tr tr N P ft cr d d ft ft tr 0 Φ ~ d ft rt Φ φ μ- μ- tr Φ CQ tr Φ d P d øi Φ 0 Φ -j Φ iQ Hi inside chamber 10 closing off duct 12'. This situation is comparable to that which is illustrated in Figure 4 for duct 12. The energizing provided by magnet assembly 5 (and if appropriate also by assembly 5'') repelling the member and the energizing of magnet assembly 5' which attracts the member can be turned off as soon as the member is situated in the position in which it closes off the duct 12'' . After the energizing of the magnet assemblies 5, 5' and, if appropriate, 5'' has been switched off, member 4 maintains its adopted position owing to the force attracting magnet 3 to the two pole shoes 6' and 7'. If member 4 comprises magnetizable material instead of a permanent magnet, at least the magnet assembly which in the case shown, holds the member in a duct-closing position (for example magnet- actuating assembly 5 with pole shoes 6 and 7 for closing off duct 12, as shown in Figure 4) must remain in the energized state for as long as closure of the duct in question is desired. Figure 6 shows a circuit diagram for actuating the multiway valve shown in the preceding figures, and it should be noted that LI, L2 and L3 refer to magnet assemblies 5, 5' and 5'', respectively, and that the windings 9, 9' and 9'' are wound in identical directions. If none of the magnet assemblies is energized, as shown in Figure 6A, the multiway valve is situated in an at-rest position in which the member is not being attracted by any of the electromagnets. If the member comprises a permanent magnet, the member will retain the position brought about by the most recent energizing of one of the electromagnets. By means of the circuit shown in Figure 6B, the electromagnets of the magnet-actuating assemblies are energized in such a manner that assembly 5 attracts the member 4 and the assemblies 5' and 5'' repel the member. Figure 6C shows a circuit in which the electromagnets of the magnet-actuating assemblies are energized in such a manner that assemblies 5 and 5'' repel the member 4 and assembly 5' attracts the member. Similarly, magnet assemblies 5 and 5' will repel the member and assembly 5'' will attract the member if the electromagnets are energized co co t to μ> H cn o σι O cn o cn Ω 0 sϊ 3 tt Ω 0 PJ S μ- TJ oo 0 3 ft H tr TJ TJ PJ 0J _ 3 -j rt CQ TJ ft TJ μ- it CQ Z O μ- d tr Φ tr O d P Φ co P- o TJ φ μ- d OJ 0 P t PJ H 0 Φ d t-x Φ Φ d P Φ cr t P g Φ d φ 3 CQ cπ φ 3 o <-. CQ Φ ft 3 CQ co d 0 ) d P OJ d rt < Ω It Ω cr ft Φ cr ft d d cr Ω TJ Φ CQ CD μ- Φ d • rt Φ J d 0 3 Ω d Φ tr μ- Ø d tr tr Φ 3 J μ- d Φ φ P ε μ- Φ ^ P- P- Φ CD 3 OJ Φ tr P μ- φ ft 0 ) tr CQ P 0 t- χ Φ P φ μ- rt 0 P CQ Φ tr d P CQ 0 cr d Ω cr d rt S Φ OJ CQ φ d OJ < OJ >t- d PJ OJ 3 d tr It μ- μ- CQ ε d d rt Φ ft ^ Φ ft d 0 ft Φ 3 Φ rt CQ P 3 P 00 cr CO Φ oo Q oo Ω • Ω tr P Φ Φ t-x P 3 ft φ P Hi d cr P Φ 0 t-x φ Φ t- χ Φ P μ- o d α tr 0J μ- φ μ- J = rt cr μ- CO Φ TJ cr rt Φ CQ CO TJ P . 3 3 ■ £> P 3 d oo Φ H < t- 1 0 Ω d - μ- Ω N tr Φ P μ- It p; P Φ μ- 0 Φ cr ØJ φ CO ft CQ μ- d φ oo P 0 < φ CQ OJ = Φ P Φ OJ I CQ tr 3 t- χ OJ CQ 3 3 Φ P z Ω 3 μ- Ω Ω tr CO rt > d φ d < • Ω J d Φ ØJ -j p; d 0 ft cr P P OJ cr ft 0 0 øJ 0 TJ 4 μ- 3 d d 3 P P- d ι ft 3 ^. P -3 CQ o 3 P P tr Φ . PJ rt < Φ φ 3 d CQ Z ft μ- d 0 Φ It φ Φ (t H 0 o μ- OJ Φ Ω d co rt OJ Φ φ μ- P d tr μ- P 3 rt CO φ iQ co OJ P Ω μ- 3 p. d P to 0 CQ μ- tr Φ • 0 CQ CO s CQ It 0 d OJ PJ CQ d o TJ φ ft 0 cr oo it d d d l ØJ OJ rt d ι 3 Ω Φ φ rt μ- Ω Hi d μ- 01 μ- P ω μ- 3 μ- d Φ 1 ft d 4 Ω Φ cr 3 d ^ 3 It Φ OJ øi Ω I PJ 3 ft Z φ OJ μ- d Ω CQ Φ CQ Φ Ω 0 • P CD H tr 0 0 rt rt tr ft Φ tr tt CQ μ- t < cr 0 CO < It Ω CQ μ- 3 d Z d 3 0 ) d tr H Φ 01 g Hi μ- tr CO Φ rt 3 Φ μ- CD d P Φ 0 tr PJ P Φ φ oo tr P cr < CQ α Hi 0 • d TJ Ω μ- tr P tr cr Ω tr Φ Ω It P d Ω CO rt Φ rt ft Ω 3 ft n μ- Φ Φ μ- Φ 0 ε Ω ft P 3 co 0 • N Φ Φ ft 0 it d t μ- μ- tr μ- μ- ε d cr Ω P rt Hi TJ P CQ PJ μ- 0 Hi ε - P p- Hi z μ- Φ oo φ P 0 Φ 3 0 0 H Φ OJ tr 00 μ- 0 Φ CQ CO co <5 μ- Ω CQ • d P μ- CD OJ rt O t- χ μ- Ω Z O φ d PJ P CD 3 u oo φ P d 0J 0J φ 0 Φ Φ Φ PJ 0 ι φ φ CD ι rt d d 3 3 P Φ μ- o O ft d CD 3 t- χ O rt 3 P o Ω t- χ OJ CO Ω oo tr t- χ oo cr ε Φ oo OJ 3 co ØJ t-x ft μ- 3 d μ- rt φ Q- φ tr tt t ft ft Φ ØJ μ> φ O μ- H Φ μ- 3 tr o cr 0 tr d d d t- χ tr OJ d ~ φ μ- tr μ- 3 3 d CO d P P d to P rt cr 0 cn tr Φ ft ft Hi Φ CQ H 3 t- χ rt Z d Ω 0 ε OJ cr tr Φ t-> 0 P φ P- CQ It cr d TJ J tr ØJ TJ ft PJ 0 d tr CQ t- χ φ Oi TJ CD g oo ØJ oo P t- χ Z t- χ CD CQ μ- 3 0 μ- Φ O 0 φ 0 0 ØJ μ- d 3 0 d 0 ) r d μ- P- Φ O d o 0 0 t- χ oo μ- Ω ft ft d d ε P rt t- χ P Hi CO 3 It Ω ft TJ 0 CO Φ φ CO ft CQ ft 3 ft d Ω ε rt 0 o Q 1 φ φ OJ P φ 3 φ ØJ tr OJ P Hi φ rt CO μ- C d φ cr OJ . Φ OJ tr Z --» d t- χ CQ d ft It p; 0 PJ CO ØJ 0J CQ rt CO μ- • t- χ t 00 P Φ d oo <j PJ φ μ- ft P- tr Hi ft d Hi d o φ 0 CD 3 Hi OJ ; H φ ØJ P ft t-x H J μ- P ØJ Z Ω ft rV CQ μ- ε Φ < φ 0 φ 3 μ- Φ Hi CD d φ 0 μ- CD UD d CO d d ft P tr 0 Φ d Ω OJ 0 ) TJ ft Hi d Φ φ ft rt CD < φ CD cr 00 ft Ω oo - o μ- PJ 3 d øi Φ OJ p; ft t- χ 0 ft 3 y- χ 3 rt tr Φ Φ φ 0 X OJ α TJ rt φ d Φ Ω ft CD 3 ft y- χ φ < CQ ε cr ft 0J ØJ tr 0 ) 3 ft 3 μ Hi 0 < . μ- μ- tr CD CQ 3 tr OJ φ < CD Φ CQ 3 tr P Φ Ω CQ Φ J d Φ cr øi d Ω TJ • CQ Φ Φ cr P- OJ 3 OJ 0 ØJ μ- μ- φ μ- ØJ P t- χ ft d o d y- χ ft ft 0 TJ rt TJ Φ d P oo ft Φ d cr CQ P t-x P OJ cr 3 Ω ft d Φ Ω t- χ PJ rt μ- • p; OJ μ- d 0 μ- P o P CD CO Ω Φ < Φ Ω y- χ cr tr μ- -j d OJ It Φ φ X d TJ μ Hi ft CO Φ CQ φ PJ O 0 0 P OJ ft φ ft Ω φ Φ ØJ H φ rt P- d CO μ- 0 φ -J ft CQ Hi OJ μ- CQ d ØJ d d Ω d OJ d μ- - 0 P OJ t- χ to CQ μ- Ω It 01 Hi CD o φ d φ μ- rt P oo ft ø) 0J 0 ft oo Ω Hi d P φ P t- χ d P o t- χ t-x ft P P d φ oo Φ Ω TJ d 0 < ft 3 μ- o 0 Hi ft d ft 3 -j Φ P 4 μ- P CQ Hi Φ Hi t- χ 0J P Φ φ CD t- χ 0 øj ft d P- φ d t d φ tr 3 P- cr μ> d d μ- p. d Z Hi d 0 cn 00 3 P φ ft Ω 3 d ft P Φ cr d 0 to ft TJ d OJ φ ε 3 d tr 0 c ft It d Q cr 3 Φ co p; 0 cr 0 Ω μ- φ Φ CQ ft Φ 0 Ω CO 0 tr TJ φ μ- P ε φ OJ μ- Φ H CQ d φ d 0 d d 3 P μ- Ω d t- 1 tr TJ CO ft d P- 0 3 Ω • ft 0 d CO d 3 OJ O P- oo ft P CD d d ft φ rt 3 0 0 OJ 0J 0J φ CQ Ω t- χ cr tr Ω P- 0 ) ft tr PJ cr P ft o μ- ft 0 3 0 0 Φ 3 rt P 3 P 3 t-x μ- tr 01 Φ 0 OJ d 0 rt Φ p ε Φ -J d Ω OJ d Hi tr Hi d TJ Φ μ- tr PJ tr μ- rt P P d 3 0 00 Z μ- P 0J tr . d ØJ P- CO 0 Φ tt ft P ft N Φ t- χ t- χ d d ØJ μ- ft Φ rt t-x CQ 0 d ε 0 < d P P tr CO P- φ P t- χ p; φ ft P N o P It tr cn d oo CQ Ω tr d CQ 3 Φ o cr ft φ O μ- Φ Φ o 0 φ Φ » PJ t- χ Φ tr CO rt CO 3 0 φ p. t-x -J d ft t t-x P P 0 H ft Ω • p 4 01 • OJ Hi CO t- χ ØJ OJ CD Hi tr p; o CD t- χ co o to to H cπ o cn o cπ o cn TJ r o ε o P TJ ft P VO P VO vo O P VO TJ ft ε TJ P Ω 3 tr rt P o TJ tr o d 0 o Φ CD O d cr o d O o φ Hi P μ- o μ- φ μ- P d O φ o tr t Φ ft ft 3 tt P rt O co Ω cπ ft ] 3 P d -J CQ CQ rt 0 ft d t- 1 Φ Hi P μ- P- Ω TJ d Z Φ rt o It tr It P φ d μ- tr <! d t- χ P Φ d φ 3 rt tr P μ- Φ tr p TJ CD μ- Φ tr d P P ft μ- oo φ Φ o Φ t P tr co d μ- p- d P μ- O ft cr rt μ> co Ω p Φ d Φ d TJ ft to Ω P z 0J cr Ω P co rt co Ω d μ- o lt- t- χ Φ ft φ ft μ- φ o ft μ- cr Φ P P φ 0 tr CQ o φ d μ- O Φ ft H H ft tr CQ ft Φ Ω o t-x p ft o Ω Φ o ft d Ω TJ P d CD t- χ to TJ • p d TJ ft P < φ o Φ Hi P tr P Hi rt o μ- P μ- cn φ P- Φ P o P ε μ- P <! P o P P d Ω P P d t- 1 O ε d Q φ Ω d Ω d P d φ μ- CQ φ rt μ- Ω p d d o Ω It TJ ft t-x P o ft d O CQ μ- ft μ- d CQ it d CD 0 rt TJ Ω o rt μ- φ d ft tr tr o μ- p. P p μ- 3 co P ft cn TJ P tr ι P TJ μ- μ- p P H P d Ω d μ- Φ Hi CQ O d it o Φ d 3 o o tr tr f Itt d P φ Φ Φ CQ <! P Φ rt φ Ω P P ft tr Φ d Hi o 3 Φ ε φ ttrr P Hi Ω Φ d μ- φ Hi Φ μ- Ω o o o p It P Φ TJ S Ω d Hi μ- P tr P ΦΦ o vo ft 3 P ft O TJ O ft I p μ- d Φ Ω d TJ P P O μ- tt CQ co P Ω Φ d μ- cr oo φ P 4 TJ o d d d Φ d ft cr O P φ ft P ft Ω ft d d μ- Ω tr P p co < Φ to o d CQ P ft μ- Φ Φ o H 3 φ P d P Ω μ- P d P Φ ft tr P P Ω tr Φ p to oo oo d TJ V p tt O cr μ- Ω ft O P I d rt Ω rt rt Φ ft CO 3 tr Φ O t- χ n to o ft p; o ] tt Φφ ε P μ- cr d rt φ CQ d μ- ft Φ o Ω d ft cr t- χ sS p; Ω P o a CD ØJ co ] 0 o P d d . CQ cr P μ- O ft P Ω μ- Φ Hi Φ CD P d d Ω φ cr Hi rt P φ O Ω H- p Ω d P d ft p o Ω ft 3 sS Φ ft ft o μ- ft 0 μ- ft rt CO TJ P- dd 3 P μ- o CD tr Ω P ft < P Φ tr μ 0 3 co μ- ft ft CD P tr Φ P P P 3 rt Z d cr o P rt oo 3 t- χ - r rt TJ CQ 4 tr o Φ O d Ω rrtt P μ- Φ P ε O CQ o g P. t cr Ω t ft tr P ft P Ω Φ P t- χ TJ rt μ- d μμ-- tt O rt rt P d cn φ 3 d LO Φ tr Φ tr Φ μ- tr P ■ 4, rt φ 3 d μ- O 0 μ- d tr tr o o Ω φ CD d P t- χ co p p Φ Φ oo Ω φ d φ CQ rt dd Ω Φ Hi t-x μ- Φ CQ tt to Z μ- p φ tr co Z μ- 3 co co P ε ft O ft P P P d μ- cn tr o p P P P P XI P d tr 0 t- χ μ- d CD Φ Ω P Φ μ- to μ ft d φ d 3 o d p. Q Φ O rt Hi t- χ rt < ft Ω tr Φ d Ω Ω ε ft ft ε P P Ω ft ft μ- P p O ft cr d P co p 0 ≥ 4 p. tr ft Ω d Φ ft o Φ O tr μ- p; d tr φ φ μ- d d Hi ft cr Φ d P < ft P P μ- ft d μ- d ft Ω o d P P o Hi p ft Φ P P tr cr rt P ft 0 CD d ft Ω O φ It 3 vo • P 0 μ- 0 φ Ω rt ft O Φ t-x P Φ d ft Φ d t- χ tr tr Hi ft P O tr o p co p d H o Φ Φ P 4 d ft ft < t- χ rt p P- TJ φ t- χ rt Φ P Hi P ft P to φ ft d o P ft p > Φ Φ o ft P P μ- P P. 3 tr P p I < cn P φ ft Hi CD O TJ φ t- χ Ω P P d Ω tr cr tt rt vo Φ P μ- ft t ft ft Hi μ- oo α μ- Ω z P rt d d ft o P Φ p; ft φ 3 p o Φ d Φ ft tr μ- d P d CQ O p p; ft CQ o ft Hi CD p d ft Φ P <! co P tr Φ Ω ft cr rt Ω d <! It d ft Φ rt o Ω d μ- TJ Φ tr rt p; Φ CT rt TJ φ μ- d Ω P tr ft tr co ft - 3 cr μ- p Φ rt co 3 φ tr Φ CD p P P P φ ft Φ d cn μ- p- Φ P Φ <! d Ω ε p P P Φ P d μ- p; ft < p Ω Φ d vo μ- p φ sS TJ ft o o It ft Φ μ- ft CO P ft Ω 3 H co P P tr P μ- Ω Φ d Φ φ P Ω P rt φ P co P t- x <; O ft d rt φ H ft vo O Ω o < Ω φ p d P ft tr d φ cn Ω φ Hi CQ d < μ- Φ P co tr 3 ft Φ o φ Ω Ω CD Φ μ- d ft φ p I Ω P 0 ft Φ P d O rt φ cr Φ cn O tr P P It Φ cr z d P P it 3 P Φ 3 d Ω 3 P CQ Ω P 3 ft rt cr o o tr Z P μ- t- χ P Z Ω to P P P < p 0 o P P ft φ d P 0 Φ μ- φ Hi ft tr Ω P d φ CQ X tr tr P CQ it P ft μ- ε CQ P CO t- χ P Ω rt μ- Ω μ- tr ft CQ X 0 μ- P d Φ Ω vo φ φ tr d d d P φ o cr co Φ φ tr O Ω P φ P P Ω Φ ft μ- o o ft Φ μ Φ Ω 00 P o p o d co TJ tr 3 o tr ft it d cn <1 ft Ω rt Φ to < d ft Ω TJ Φ tr Hi TJ φ co d μ- Φ cr P- oo φ Φ d 4 O d Φ p Ω rt P p p. μ- Ω P p P cn tr p p Φ co It P. P d μ- Φ Φ co of the side walls of the chamber. Positioning the member as shown in Fig. 10A opens ducts 71 and 72 and closes off ducts 73 and 74. Figures 10B and D show other positions of the member 75 inside the chamber 70. In Fig. 11, the member 85 comprises four disc-like closure bodies 85A-D which are coupled via elastic connections 87, and ducts 81-84. In Fig. 11A, ducts 81 and 82 are closed off by closure bodies 85A and 85B, respectively. Figs. 11B and 11C show other possible positions of the member 85 inside the chamber. The closure bodies may each comprise a magnetizable or magnetic material which can be controlled using magnet-actuating assemblies (not shown) as shown, for example, in Fig. 7. Figure 12 shows an application of an embodiment of the present invention. Figure 12.1 shows a rudimentary circuit diagram for the bidirectional control of two cylinders X and Y in which A is the feed of the medium (oil or air) and B is the discharge. The switches I and II are both bipolar and have three positions. The points 1, 2, 3 and 4 are connected to the cylinders. Figure 12.2 shows the equivalent of the switches in Figure 12.1, while Figure 12.3 shows the equivalent of Figure 12.1 with switch II in the centre position. Similarly, it is possible to position the member in the chamber for any combination of the switches I and II from Figure 12.1, with the exception of total closure of duct B. Figure 13a shows a plan view of a multiway valve according to the present invention which comprises a round chamber 1301 in which a member 1313 is accommodated. Member 1313 is connected to a joystick-like component 1310, it being possible for the member 1313, in the case illustrated, to be tilted inside the chamber through plane II -II and to be rotated. The joystick- like component 1310 may be connected to a control device, but may be also designed for manual operation. Member 1313 is provided with member cavities 1315 and 1314, member cavity 1314 being designed as an annular recess running over the circumference of member 1313. Thirteen ducts, ducts 1361- 1368 of which are shown in Figure 13a and ducts 1392-1394 of which are shown in the bottom view shown in Figure 13d, open out into the chamber. In the position of the multiway valve which is illustrated in Figure 13b, which is a cross section on line I-I from Figure 13a, ducts 1361-1368 are connected to one another via the annular member cavity 1314. Ducts 1393 and 1395 are closed off. In the cross section on line II-II in Figure 13a, which is shown in Figure 13c, it can be seen that duct 1392 is connected to duct 1394 and that duct 1367 is in communication with member cavity 1314, i.e. duct 1367 is in communication with the ducts 1361 and 1365 of Figure 13b. In this position, ducts 1368 and 1366 are likewise connected to ducts 1367, 1361 and 1365 via member cavity 1314. In this position, duct 1363 is closed off, as is 1396. The member can be moved in two directions of movement which are perpendicular to one another, i.e. it can be tilted in the plane of cross section II-II and can be rotated about the axis of the joystick-like member 1310. It is also possible for the member 1313 to be designed so that it can be tilted in the common plane of the axes of ducts 1361-1365. The member can then be moved in three dimensions inside the chamber, resulting in even more possible combinations with regard to closing off and opening various ducts. Obviously, the valve may be designed in such a manner that the member can be moved in two of the three dimensions mentioned above. The multiway Valve has a very large number of conceivable applications in measurement and control engineering for hydraulics and pneumatics, but also as a flow regulator, such as for regulating, mixing and metering pigments and solvents in the paints industry, addressing valve in analytical chemistry, such as for HPLC, or for regulating and/or mixing bulk materials, such as compound feed. Since the valve can be of completely closed design, there are also numerous possible applications for hazardous substances such as the petrol/air mixture in internal - combustion engines, natural gas or nuclear reactor coolant. Due to the possibility of simultaneous proportional regulation of various streams, this valve may, for example, be directly coupled at the position of a joystick at the position of a manipulator.

Claims: CLAIMS 1. Multiway valve, comprising a chamber into which at least four feed or discharge ducts open out, the state of being open or closed of at least three of the ducts being affected by the positioning of a member which is, moveable in directions of movement substantially perpendicular with respect to one another, accommodated inside the chamber, and which member can be made to interact in a sealing manner with one or more duct openings, and control means for moving the member inside the housing. 2. Multiway valve according to claim 1, characterized in that the member is accommodated inside the chamber in such a manner that it is moveable in two dimensions in a plane which runs substantially parallel to the longitudinal axis of the chamber. 3. Multiway valve according to claim 2, characterized in that the chamber is delimited by at least two substantially plane-parallel surfaces, the plane in which the member can move being parallel to the plane-parallel surfaces . 4. Multiway valve according to claim 3, characterized in that the member is flattened on two sides, the said flat sides of the member interacting in a sealing manner with the plane-parallel surfaces by means of surface contact. 5. Multiway valve according to one of claims 1-4, characterized in that the member comprises a cavity which is delimited by at least one wall of the housing, into which wall at least one central duct opens out, the opening of which duct is in communication with the member cavity irrespective of the position of the member in the chamber. 6. Multiway valve according to claim 5, characterized in that the member comprises a continuous ring section which interacts in a sealing manner with at least one of the walls of the chamber, the member cavity being delimited in the radial direction by the inner circumference of the ring section. 7. Multiway valve according to one of claims 1-6, characterized in that the member cavity is delimited by two walls of the chamber which are situated on either side of the plane of movement . 8. Multiway valve according to one of claims 5-7, characterized in that the central duct can be placed in communication, via the member cavity, with at least one of the other ducts which open out into the chamber. 9. Multiway valve according to one or more of claims 2-8, characterized in that the chamber comprises at least one transverse wall which is positioned substantially transversely with respect to the plane of movement of the member, into which transverse wall at least one feed or discharge duct opens out . 10. Multiway valve according to one of claims 1-9, characterized in that the member comprises a magnetizable material and the control means comprise one or more magnet- actuating assemblies which are designed to generate a magnetic field which attracts or repels the member. 11. Multiway valve according to claim 10, characterized in that the member comprises a permanent magnet. 12. Multiway valve according to claim 11, characterized in that the field lines of the said permanent magnet run substantially radially with respect to the plane of movement of the member, and the magnet -actuating assemblies are designed to generate a magnetic field whose field lines run substantially parallel with respect to the said plane of movement . 13. Multiway valve according to claim 11, characterized in that the field lines of the said permanent magnet run substantially axially with respect to the plane of movement of the member, and the magnet-actuating assemblies are designed to generate a magnetic field whose field lines are substantially transverse with respect to the said plane of movement . 14. Multiway valve according to claims 2 and 10 or 2 and 13, characterized in that at least one magnet-actuating assembly is disposed in such a manner that the centre axis of the pole shoes thereof is positioned at right angles with respect to the centre longitudinal plane (M) of the chamber, the distance between each of the two pole shoes and the said centre longitudinal plane (M) being equal . 15. Multiway valve according to claim 14, characterized in that, if the centre axis of the two pole shoes of the said magnet-actuating assembly runs inside the chamber, the distance therefrom to the closest transverse wall of the chamber is at maximum equal to the shortest distance from the magnetic centre of the member to the said transverse wall . 16. Method for actuating a multiway valve according to one or more of claims 10-15 with the aid of one or more magnetic fields, characterized in that one generates with at least one magnet-actuating assembly a magnetic field whose field lines run parallel to the field lines of the member, in order to move the member, under the influence of the magnetic field, into a position inside the chamber, resulting in opening or closure of at least one duct opening . 17. Method according to claim 16, characterized in that the member is designed as a permanent magnet and an electromagnet is accommodated in the magnet-actuating assembly and is energized in such a manner that it attracts or repels the permanent magnet of the member, the member closing or opening at least one of the ducts which open out into the chamber. 18. Method according to claim 17, characterized in that the magnetic strength of the permanent magnet of the member is selected in such a manner that the latter, once it has been attracted by an energized electromagnet, maintains the resultant position inside the chamber when the electromagnet has been switched off due to the attraction between the permanent magnet and one or both pole shoes of the switched-off magnet. 19. Method according to claim 17 or 18, characterized in that the magnet-actuating assembly is energized with reversed polarity, so that the member reverses the opening or closure of the duct opening. 20. Method according to one or more of claims 17-19, characterized in that various magnet -actuating assemblies of a multiway valve are energized simultaneously, in such a manner that one assembly attracts the member and the other assemblies repel the member. 21. Method according to one or more of claims 16-20, characterized in that the member is designed as a permanent magnet and a plurality of electromagnets are accommodated in the magnet-actuating assembly and these electromagnets are energized in such a manner that they repel the permanent magnet, the positioning of the member being influenced by varying the magnetic field strength of one or more magnet-actuating assemblies.

Inventors: FONDSE JAN HENDRIK, FONDSE, JAN, HENDRIK
Applicants: FONDSE JAN HENDRIK, FONDSE, JAN, HENDRIK
Application year: 1999
Main classification: F16K31
IPC codes: F16K11, F16K31