US3166727A - Magnetic coil and core structure - Google Patents
Magnetic coil and core structure Download PDFInfo
- Publication number
- US3166727A US3166727A US243147A US24314762A US3166727A US 3166727 A US3166727 A US 3166727A US 243147 A US243147 A US 243147A US 24314762 A US24314762 A US 24314762A US 3166727 A US3166727 A US 3166727A
- Authority
- US
- United States
- Prior art keywords
- magnetic
- enclosure
- particles
- members
- wall
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/0302—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity characterised by unspecified or heterogeneous hardness or specially adapted for magnetic hardness transitions
- H01F1/0311—Compounds
- H01F1/0313—Oxidic compounds
- H01F1/0315—Ferrites
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F21/00—Variable inductances or transformers of the signal type
- H01F21/02—Variable inductances or transformers of the signal type continuously variable, e.g. variometers
- H01F21/06—Variable inductances or transformers of the signal type continuously variable, e.g. variometers by movement of core or part of core relative to the windings as a whole
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F29/00—Variable transformers or inductances not covered by group H01F21/00
- H01F29/08—Variable transformers or inductances not covered by group H01F21/00 with core, coil, winding, or shield movable to offset variation of voltage or phase shift, e.g. induction regulators
- H01F29/10—Variable transformers or inductances not covered by group H01F21/00 with core, coil, winding, or shield movable to offset variation of voltage or phase shift, e.g. induction regulators having movable part of magnetic circuit
Definitions
- This invention relates to magnetic circuit structures and isl especially though not exclusively concerned with magnetic circuits for electromagnetic apparatus'units of large power ratings, e.g. of the order of several thousand kilovoltamperes, operating at intermediate to high (and ultra-high) frequencies.
- Magnetic circuits are utilized in a great variety of equipment in electrical engineering and related fields, and can assume widely differing forms depending on their particular use. Thus they may constitute closed circuits or may include airgaps; they may consist of essentially stationary components or may involve relatively displaceable parts such as adjustable cores; they may be associated with various kinds of electrical winding.
- the actual magnetic structure comprising it has generally been of one of two types, the type selected depending primarily on the ⁇ frequency ofthe electromagnetic energyinvolved in the 4operation of the circuit, For low frequencies, the magnetic structure has usually consisted of stacks of thin, mutually insulated laminations of various magnetic alloys, while for higher frequencies it is now usual to use sintered blocks of so-called ferrimagnetic compounds.
- ferrimagnetic has in recent years acquired a precise and well-defined meaning in physical science and electromagnetic engineering.y A definition of ferrimagnetism may be found eg. in Solid-state Physics by Charles Kittel, 2nd Edition, New York, 1960, page 445 and is based on a relationship between lthe constituent atoms of the molecules of the substances involved, Vsuch that the atomic spins arein part parallel and in part antiparallel in the saturated condition. While the significance of this definition depends on rather complex theory, it is for practical purposes sufiicient to understand that ⁇ all ferrimagnetic substances are characterized by a high magnetic permeability coupled with high electric resistivity, a combination of properties not to be found in the usual ferromagnetic materials such as ferrous alloys. Ferrimagnetic materials' include thenaturally occurring ferrites, which are complex oxides deriving from magnetite (lFe++O, Fe2+t+03) through replacement of the divalent iron atom therein with anatomlof some other metal.
- ferrimagnetic is used in its accepted sense as just explained. These materials are generally moulded prior to firing. Their fabrication to requisite shapes presents difficult problems especially in the case of large vand more or less intricately formed magnetic circuitv components. Usually they are moulded to simple parallelopipedic bar shape and these basic elements are lthen assembled by means of adhesive to the shape of the final magnetic circuit. This procedure is longand tedious, and the brittleness of the materials concerned leads to considerable reby further increasing manufacturing costs; Y.
- a magnetic structure or component comprises wall means providing a ⁇ casing conforming externally to the desired shape of the magnetic structure or component and internally defining an enclosure, and a body of loose particles of ferrimagnetic material substantially filling said enclosure.
- the particles may vary widely in size and shape, and may include particles differing ⁇ considerably from one another as to each of these characteristics. However, according to the invention it is preferred so to select the range of size and shapes of the particles used as to .pro-y vide a packing coefficient within the enclosure of approximately from :to 90%, 80% being a preferred average value. In other words, it is preferred that the weight of the :body of particles filling the enclosure shall be about from 70% to 90% of the weight of a Ibody ofthe same dimensions made of compact material of similar composition to that of the particles used, and preferably about of such weight. y y
- the loose character of ⁇ the filler mass of ferrimagnetic material used according to the invention and its non-compact condition is in complete contrast with the bound and compact state of the powder particles of ferrimagnetic material as heretofore produced by sintering and the like techniques.
- the method of the invention not only affords a very great simplification in manufacturing procedure and a corresponding reduction in cost, but it has been found to lead to considerably improved operation, owing primarily to the presence of the interstitial gaps between the individual particles, and tothe possibility of providing effective cooling thereof by the presence of a body of cooling fluid filling said interstitial gaps.
- fluid inlet and outlet means are provided in the ⁇ walls defining the enclosure, and an electrically in ⁇ sulating cooling fluid is circulated therethrough so as to pervade the interstitial gaps in the ferrimagnetic filler body and Vremove the heat therefrom in operation.
- the walls of the casing defining the enclosure filled with loose ferrimagnetic particles comprise, at least in the parts thereof lying withinthe magnetic field in the operation of the circuit, a material which is inactive both electrically yand magnetically, that is non-magnetic and has low electric conductivity,osuch as a suitable plastic-base composition.
- the over-all design of the inductor shown is broadly conventional, comprising a vertical solenoid 1 made of copper tubing supported as presently described and provided with means, not shown, 'for circulating cooling Water through'it in use.
- the magnetic circuit structure of the variable inductor is in two parts, and includes a fixed outervpart 3 and a verticallyv displaceable inner part or core 2.
- Each of the parts 2 and 3 is constructed in accordance with the invention in the form of a casing filled with loose particles or granules of ferrite. 4
- the stationary outer part 3 of the magnetic circuit V comprises an inner WallS and an outer Wall '7 in spaced relationship defining a generally lbell-shaped casing having a vertical cylindrical portion and an inturned flange portion at its top.
- the displaceable core 2 comprises an inner wall 6 and an outer Wall t assem-.
- the casing 2 is provided with a bottom inlet-10 and a top outlet v12 for the circulation of coolant fluid, c g. water, and similarly the casing 3 is provided with a bottom inlet 11 and a top outlet 13.
- the wall portions ofthe casing that are exposed to be traversed by magnetic ⁇ flux in the operation of the apparatus are made of non-magnetic, electrically insulating material.
- Various materials may be used for this purpose having ⁇ the requisite magnetic and electrical properties as lwell as mechanical strength, including various synthetic resin compositions such as ⁇ polyvinyl chloride, fiber-reinforced resin laminates, and the like.
- the outer wall 7 of the outer magnetic component and the ,inner wall 6of the inner component which are not substantially exposed to the magnetic field in use, these may be made from similar materials as those mentioned above, but may preferably comprise metal of non-ferromagnetic character having good electrical conductivity, e.g. copper and/or aluminium alloys, thereby to serve as shielding forthe magnetic structure while imparting improved mechanical strength to it.
- Y f A plurality of vertical racks such as-17 secured to the inner Wall 5 of'the outer magnetic member 3 serve to support the solenoid las shown.
- the innermagnetic component Z is shown as 'being suspended from a cable 14 attached to the ⁇ top centre of said vcomponent as at 15 and wound around -an overhead sheave 16 actuated by a Winch not shown.
- Suitable guiding means are provided for vertically guiding the displaceable ⁇ lmagnetic core 2 in its vertical movements.
- cooling fluid eg. liq-v uid
- casing 2 is circulated through casing 2 from inlet 9 to outlet 1,2, andthrough casing 3 from inlet 11 to outlet 13.
- the orifices of outlets 12 and 13 are positioned rather close to the top of the casings 2 and 3 respectively, so that thev egress of the granular iilling material f18 through said outlets is prevented.
- screens of suitable mesh size may if desired be provided across the fluid outlets to assist in lpreventingA such outflow of the 'granular material with the fluid.
- the circuit inductance can thus be varied over a total range corresponding to a lfactor of about 4:1. lf such a wide range of variation is not needed, the parts 2 and 3 may be shaped as simple cylindrical members. With such an :arrangement ⁇ the 1n- Vductance can still :be varied by a factor of about 3:1 over l' chosen for providing a packing coeliicient of 80%.
- thel production of the large-size magnetic components 2 and 3 posed no special engineering problem, since it was simply required to press-mould, or otherwise form the plastic and d g metallic wall members by well-knownvtechniques, fill the resulting casings With the loose ⁇ ferrite material and f finally assemble the casing parts.
- This relatively simple procedure contrasts extremely favourably with the drfculties that would b e normally encountered in moulding and sintering. large bodies of ferrite powder material as would be necessary in constructing the magnetic parts Z and 3 by present-day techniques.
- theinductor described hereabove may be operated at several thousand kilovolt-amperes, due tothe fact that the liquid filling all the gaps between the particles of ferrite acbievesa fully eliicient cooling, and the loss coefficient is only 1%. lt is clear that a comparable cooling effect cannot possibly be achieved in conventional apparatus where thermagnetic parts are solid, compact bodies. l
- the invention as earlier stated is broadly applicable to all apparatus embodying the use of magnetic circuits, including fixed and variable inductors, transformers, fields, and the like, both in the fields of powerand communications engineering.
- a magnetic structure which comprises wall means providing at least one casing internally defining a sealed enclosure, a body of loose particles of ferrimagnetio material substantially filling said enclosure and providing interstitial gaps between the particles, and inlet and outlet means connected to said wall means for circulating a cooling fluid through said enclosure to'lill said interstitial gaps between thev particles therein and remove theV heat l generated in said particles in thel operation of apparatus of which said structure forms part.
- the two parts of the magnetic circuit structure# f are so sha-pedowing to the provision of the top and base lianges of the outer and inner'parts 3 and 2 respectively,
- Electromagnetic apparatus comprising in combination electromagnetic means of creating a magnetic eld, magnetic circuit structure comprising rigid wall members, means for interassembling the wall members, the outer surfaces or" the wall members when assembled defining a structure so shaped and positioned relative tosaid electromagnetic means as to Vbe substantially traversed by said field and the inner surfaces of the wall members when assembled defining an enclosure therebetween, and a body of loose ferrimagneticparticles substantially filling said enclosure'with interstitial gaps between the particles.
- iluid inlet and outlet means associated with at least one of said wall members and connectable to a source of cooling lluid and means for circulating said i'luid through said enclosure and in the interstitial gaps between said loose particles.
- Electromagnetic apparatus comprisingin combination electromagnetic winding means for creating a magnetic field, magnetic circuit structure comprising rigid wall members, means for interassembling said members, the outer surfaces of said members whenassembled dening at least one generally cylindrical structure coaxial with said winding means and the inner surfaces of said members when assembled deiining an enclosure therebetween, and a body of loose errimagnetic particles tilling the enclosure with interstitial gaps between the particles.
- Electromagnetic apparatus comprising in combination electromagnetic winding means for creating a magnetic iield, atleast one pair of rigid wall members interconnectable to deline therebetween a sealed enclosure of generally 'annular cylindrical shape coaxial with said winding means, a body or loose ferrimagnetic particles substantially filling said enclosure with intenstitial gaps between the particles, and iluid inlet and outlet means associated with at least one of said members and connectable to a fluid circuit for circulating cooling fluid through the enclosure and in the gaps between the particles.
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Soft Magnetic Materials (AREA)
- Hard Magnetic Materials (AREA)
Description
, Jan. 19, 1965 c. A. E. BEURTHERET 3,156,727
' MAGNETIC con. AND com: STRUCTURE Filed Dec. 7, 1962 Inve rH-or C.\.E. BEUR-rHERE-r Mlwrneq s United States Patent Mlee 3,166,727 MAGNETIC COIL AND CORE STRUCTURE Charles Alphonse Emile Beurtheret, Seine-et-Oise, France,
assignor to Compagnie Francaise Thomson-Houston, Paris, France, a French body corporate Filed Dec. 7, 1962, Ser. No. 243,147 Claims priority, application France, Dec. 18, 1961,
882,233, Patent 1,316,558 13 Claims. (Cl. 336-57) This invention relates to magnetic circuit structures and isl especially though not exclusively concerned with magnetic circuits for electromagnetic apparatus'units of large power ratings, e.g. of the order of several thousand kilovoltamperes, operating at intermediate to high (and ultra-high) frequencies.
Magnetic circuits are utilized in a great variety of equipment in electrical engineering and related fields, and can assume widely differing forms depending on their particular use. Thus they may constitute closed circuits or may include airgaps; they may consist of essentially stationary components or may involve relatively displaceable parts such as adjustable cores; they may be associated with various kinds of electrical winding. However, regardless of the particular design of the circuit, the actual magnetic structure comprising it has generally been of one of two types, the type selected depending primarily on the `frequency ofthe electromagnetic energyinvolved in the 4operation of the circuit, For low frequencies, the magnetic structure has usually consisted of stacks of thin, mutually insulated laminations of various magnetic alloys, while for higher frequencies it is now usual to use sintered blocks of so-called ferrimagnetic compounds.
'Ihe term ferrimagnetic has in recent years acquired a precise and well-defined meaning in physical science and electromagnetic engineering.y A definition of ferrimagnetism may be found eg. in Solid-state Physics by Charles Kittel, 2nd Edition, New York, 1960, page 445 and is based on a relationship between lthe constituent atoms of the molecules of the substances involved, Vsuch that the atomic spins arein part parallel and in part antiparallel in the saturated condition. While the significance of this definition depends on rather complex theory, it is for practical purposes sufiicient to understand that `all ferrimagnetic substances are characterized by a high magnetic permeability coupled with high electric resistivity, a combination of properties not to be found in the usual ferromagnetic materials such as ferrous alloys. Ferrimagnetic materials' include thenaturally occurring ferrites, which are complex oxides deriving from magnetite (lFe++O, Fe2+t+03) through replacement of the divalent iron atom therein with anatomlof some other metal.
In the present .specification and claims, the term ferrimagnetic is used in its accepted sense as just explained. These materials are generally moulded prior to firing. Their fabrication to requisite shapes presents difficult problems especially in the case of large vand more or less intricately formed magnetic circuitv components. Usually they are moulded to simple parallelopipedic bar shape and these basic elements are lthen assembled by means of adhesive to the shape of the final magnetic circuit. This procedure is longand tedious, and the brittleness of the materials concerned leads to considerable reby further increasing manufacturing costs; Y.
one of the main advantages of these Vsubstances in electromagnetic engineering-they are correspondingly poor conductorsv of heat. Because of y'this the considerable amounts of heat evolved inservice due primarily toghysA 3,166,727 Patented Jan. 19, 1965 teresis losses are unable to be dissipated at a satisfactorily high rate out of the magnetic structure and objectionably high temperatures result.
It is an object of this invention to provide a novel form of manufacturing technique for magnetic circuit structures which will be especially useful in the construction of electromagnetic apparatus of various types of large powerratings andoperating e.g. at high frequencies, and which will combine the well-known benefits of ferrimagnetic materials such as ferrites while being completely free from the manufacturing difficulties and other drawbacks of the same.
It is an object to provide a magnetic structure comprising ferrimagnetic material, which will be considerably easier and cheaper to produce lthan was heretofore possible, can :readily be shaped to any required configuration, and will be easy to cool effectively in service.
In accordance with a basic aspect of the invention, a magnetic structure or component comprises wall means providing a `casing conforming externally to the desired shape of the magnetic structure or component and internally defining an enclosure, and a body of loose particles of ferrimagnetic material substantially filling said enclosure. l
The particles may vary widely in size and shape, and may include particles differing `considerably from one another as to each of these characteristics. However, according to the invention it is preferred so to select the range of size and shapes of the particles used as to .pro-y vide a packing coefficient within the enclosure of approximately from :to 90%, 80% being a preferred average value. In other words, it is preferred that the weight of the :body of particles filling the enclosure shall be about from 70% to 90% of the weight of a Ibody ofthe same dimensions made of compact material of similar composition to that of the particles used, and preferably about of such weight. y y
It will be understood that the loose character of `the filler mass of ferrimagnetic material used according to the invention and its non-compact condition is in complete contrast with the bound and compact state of the powder particles of ferrimagnetic material as heretofore produced by sintering and the like techniques. The method of the invention not only affords a very great simplification in manufacturing procedure and a corresponding reduction in cost, but it has been found to lead to considerably improved operation, owing primarily to the presence of the interstitial gaps between the individual particles, and tothe possibility of providing effective cooling thereof by the presence of a body of cooling fluid filling said interstitial gaps. In accordance with a preferred aspect of the invention, fluid inlet and outlet means are provided in the `walls defining the enclosure, and an electrically in` sulating cooling fluid is circulated therethrough so as to pervade the interstitial gaps in the ferrimagnetic filler body and Vremove the heat therefrom in operation. Air, water, or oil may be used as the cooling agent as may be dictated by circumstances.l v l j According to an important feature of the invention, the walls of the casing defining the enclosure filled with loose ferrimagnetic particles comprise, at least in the parts thereof lying withinthe magnetic field in the operation of the circuit, a material which is inactive both electrically yand magnetically, that is non-magnetic and has low electric conductivity,osuch as a suitable plastic-base composition. t Y
An exemplary embodiment ofthe invention willnow "be describedffor purposes of illustrationbutnot of limin tation with reference to theaccompanying drawing, whichis a yiewin elevation, withoue half in section, ofa highpower, low-loss vvariable vinductor constructed in accord-V' ance with the invention, and especially ywell-suited for intermediate frequencies.
`The over-all design of the inductor shown is broadly conventional, comprising a vertical solenoid 1 made of copper tubing supported as presently described and provided with means, not shown, 'for circulating cooling Water through'it in use. The magnetic circuit structure of the variable inductor is in two parts, and includes a fixed outervpart 3 and a verticallyv displaceable inner part or core 2. Each of the parts 2 and 3 is constructed in accordance With the invention in the form of a casing filled with loose particles or granules of ferrite. 4
Specifically, the stationary outer part 3 of the magnetic circuit Vcomprises an inner WallS and an outer Wall '7 in spaced relationship defining a generally lbell-shaped casing having a vertical cylindrical portion and an inturned flange portion at its top. The inner and outerwalls 5 and 7 are assembled together =by bolts 8 with interposed sealing rings as at 9 so as to provide a tightly sealed enclosure within the casing'. Similarly the displaceable core 2 comprises an inner wall 6 and an outer Wall t assem-.
bledV together with :bolts -8 by way of seal rings 9 and definingbetween them a fluid-tight enclosure of a shape generally similar to the outer component 3 but inverted with respect thereto. `Each of the fluid-tight enclosures thus defined by the parts 2 and 3 is filled with granulated ferrite material `18. The casing 2 is provided with a bottom inlet-10 and a top outlet v12 for the circulation of coolant fluid, c g. water, and similarly the casing 3 is provided with a bottom inlet 11 and a top outlet 13.
As earlier stated, the wall portions ofthe casing that are exposed to be traversed by magnetic `flux in the operation of the apparatus, herein the inner Wall 5 of the outer magnetic part 3 and the outer wall 4 of the inner magnetic part 2, are made of non-magnetic, electrically insulating material. Various materials may be used for this purpose having `the requisite magnetic and electrical properties as lwell as mechanical strength, including various synthetic resin compositions such as `polyvinyl chloride, fiber-reinforced resin laminates, and the like. As concerns V.the remaining ywall elements, lherein the outer wall 7 of the outer magnetic component and the ,inner wall 6of the inner component, which are not substantially exposed to the magnetic field in use, these may be made from similar materials as those mentioned above, but may preferably comprise metal of non-ferromagnetic character having good electrical conductivity, e.g. copper and/or aluminium alloys, thereby to serve as shielding forthe magnetic structure while imparting improved mechanical strength to it. Y f A plurality of vertical racks such as-17 secured to the inner Wall 5 of'the outer magnetic member 3 serve to support the solenoid las shown. The innermagnetic component Z is shown as 'being suspended from a cable 14 attached to the` top centre of said vcomponent as at 15 and wound around -an overhead sheave 16 actuated by a Winch not shown. Suitable guiding means, not shown, are provided for vertically guiding the displaceable` lmagnetic core 2 in its vertical movements.
In use it will be understood that cooling fluid, eg. liq-v uid, is circulated through casing 2 from inlet 9 to outlet 1,2, andthrough casing 3 from inlet 11 to outlet 13. As shown the orifices of outlets 12 and 13 .are positioned rather close to the top of the casings 2 and 3 respectively, so that thev egress of the granular iilling material f18 through said outlets is prevented. As will :be evident, screens of suitable mesh size may if desired be provided across the fluid outlets to assist in lpreventingA such outflow of the 'granular material with the fluid.
It`will -be noted that' in the exemplary variable inducor nearly completely closed. The circuit inductance can thus be varied over a total range corresponding to a lfactor of about 4:1. lf such a wide range of variation is not needed, the parts 2 and 3 may be shaped as simple cylindrical members. With such an :arrangement `the 1n- Vductance can still :be varied by a factor of about 3:1 over l' chosen for providing a packing coeliicient of 80%.
It will be appreciated that the exemplary apparatus`r described above is purely illustrative of the wide range of possibilities of the invention and was selected because of the particular diiculties that would be involved in the provision of such a high-power, low-loss electromagnetic apparatus involving variable airgaps and large size magnetic components, by the use of conventional techniques, such as sintered ferrites'. By constructing the apparatus in accordance with the teachings of the invention as above described, on the other hand, thel production of the large-size magnetic components 2 and 3 posed no special engineering problem, since it was simply required to press-mould, or otherwise form the plastic and d g metallic wall members by well-knownvtechniques, fill the resulting casings With the loose `ferrite material and f finally assemble the casing parts. This relatively simple procedure contrasts extremely favourably with the drfculties that would b e normally encountered in moulding and sintering. large bodies of ferrite powder material as would be necessary in constructing the magnetic parts Z and 3 by present-day techniques. Moreover, theinductor described hereabove may be operated at several thousand kilovolt-amperes, due tothe fact that the liquid filling all the gaps between the particles of ferrite acbievesa fully eliicient cooling, and the loss coefficient is only 1%. lt is clear that a comparable cooling effect cannot possibly be achieved in conventional apparatus where thermagnetic parts are solid, compact bodies. l
The invention as earlier stated is broadly applicable to all apparatus embodying the use of magnetic circuits, including fixed and variable inductors, transformers, fields, and the like, both in the fields of powerand communications engineering.
Iclaim: d n Y l. A magnetic structure which comprises wall means providing at least one casing internally defining a sealed enclosure, a body of loose particles of ferrimagnetio material substantially filling said enclosure and providing interstitial gaps between the particles, and inlet and outlet means connected to said wall means for circulating a cooling fluid through said enclosure to'lill said interstitial gaps between thev particles therein and remove theV heat l generated in said particles in thel operation of apparatus of which said structure forms part.
enclosure, a'body of loose particles of ferrirnagnetic material substantially Vfilling said enclosure and providingk Y interstitial gaps between the particles, and means for cirtor shown, the two parts of the magnetic circuit structure# f are so sha-pedowing to the provision of the top and base lianges of the outer and inner'parts 3 and 2 respectively,
that in the uppermost end position lof the -movable inner culating cooling fluid through the enclosure. Y
3. 'A magnetic structure, as defined in claim 2, wherein said wall means is made of a1 substance having substan-V tially non-magnetic, electrically non-conductive properties at least in a part of said Wall meansexposed to magnetic `flux in the operation of said structure.
v4. Magnetic structure as claimed in claim 3, wherein said substance ycomprises a synthetic resin-basecomposition.. Y l Y .Y
`5. Magnetic structure as `claimed inclaim 3', wherein said wall `means is made of a metallic material' havingV non-ferrolriagnetic, electrically conductive properties in ensayar a part thereof not exposed to magnetic ilux in the operation of the structure. t K
6. Magnetic structure as claimed in claim 1, wherein said material ills the enclosure with a packing coeilicient of approximately from 7() to 90%. i
7. Electromagnetic apparatus comprising in combination electromagnetic means of creating a magnetic eld, magnetic circuit structure comprising rigid wall members, means for interassembling the wall members, the outer surfaces or" the wall members when assembled defining a structure so shaped and positioned relative tosaid electromagnetic means as to Vbe substantially traversed by said field and the inner surfaces of the wall members when assembled defining an enclosure therebetween, and a body of loose ferrimagneticparticles substantially filling said enclosure'with interstitial gaps between the particles.
8. The apparatus delined in claim 7, including iluid inlet and outlet means associated with at least one of said wall members and connectable to a source of cooling lluid and means for circulating said i'luid through said enclosure and in the interstitial gaps between said loose particles.
9. Electromagnetic apparatus comprisingin combination electromagnetic winding means for creating a magnetic field, magnetic circuit structure comprising rigid wall members, means for interassembling said members, the outer surfaces of said members whenassembled dening at least one generally cylindrical structure coaxial with said winding means and the inner surfaces of said members when assembled deiining an enclosure therebetween, and a body of loose errimagnetic particles tilling the enclosure with interstitial gaps between the particles.
10. The apparatus defined in claim 9, including fluid inlet and outlet means associated with at least one of said members and connectable to a cooling fluid circuit and y means for circulating cooling lluid through the enclosure and the interstitial gaps between said loose particles.
1l. The apparatus defined in claim 7, including means for relativelyrdisplacing said magnetic circuit structure and said eld creating means.
l2. Electromagnetic apparatus comprising in combination electromagnetic winding means for creating a magnetic iield, atleast one pair of rigid wall members interconnectable to deline therebetween a sealed enclosure of generally 'annular cylindrical shape coaxial with said winding means, a body or loose ferrimagnetic particles substantially filling said enclosure with intenstitial gaps between the particles, and iluid inlet and outlet means associated with at least one of said members and connectable to a fluid circuit for circulating cooling fluid through the enclosure and in the gaps between the particles.
13. The apparatus defined in claim 12, including two pairs of said wall members respectively deiining two sealed enclosures coaxial 'with said winding means radially inward and radially outward thereof.v
Tmmel May 14, 1957
Claims (1)
- 9. ELECTROMAGNETIC APPARATUS COMPRISING IN COMBINATION ELECTROMAGNETIC WINDING MEANS FOR CREATING A MAGNETIC FIELD, MAGNETIC CIRCUIT STRUCTURE COMPRISING RIGID WALL MEMBERS, MEANS FOR INTERASSEMBLING SAID MEMBERS, THE OUTER SURFACES OF SAID MEMBERS WHEN ASSEMBLED DEFINING AT LEAST ONE GENERALLY CYLINDRICAL STRUCTURE COAXIAL WITH SAID WINDING MEANS AND THE INNER SURFACES OF SAID MEMBERS WHEN ASSEMBLED DEFINING AN ENCLOSURE THEREBETWEEN, AND A BODY OF LOOSE FERRIMAGNETIC PARTICLES FILLING THE ENCLOSURE WITH INTERSTITIAL GAPS BETWEEN THE PARTICLES.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR882233A FR1316558A (en) | 1961-12-18 | 1961-12-18 | Improvements made to the methods of constituting magnetic circuits, in particular for high powers, and to devices comprising such magnetic circuits |
Publications (1)
Publication Number | Publication Date |
---|---|
US3166727A true US3166727A (en) | 1965-01-19 |
Family
ID=8768897
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US243147A Expired - Lifetime US3166727A (en) | 1961-12-18 | 1962-12-07 | Magnetic coil and core structure |
Country Status (3)
Country | Link |
---|---|
US (1) | US3166727A (en) |
CH (1) | CH388445A (en) |
FR (1) | FR1316558A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3423670A (en) * | 1964-08-07 | 1969-01-21 | Perkin Elmer Ltd | Magnetic shield arrangement for a high flux homogeneous field-producing magnet |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US1809042A (en) * | 1926-11-30 | 1931-06-09 | Bell Telephone Labor Inc | Magnet core |
US2168351A (en) * | 1936-08-31 | 1939-08-08 | Rca Corp | Adjustable magnetic-core inductor |
US2407916A (en) * | 1943-04-10 | 1946-09-17 | Stewart Warner Corp | Shielded coil |
US2605311A (en) * | 1950-12-20 | 1952-07-29 | Westinghouse Electric Corp | Reactor |
US2792536A (en) * | 1953-10-30 | 1957-05-14 | Westinghouse Electric Corp | Electro-magnetic solenoids and actuators |
-
1961
- 1961-12-18 FR FR882233A patent/FR1316558A/en not_active Expired
-
1962
- 1962-12-07 US US243147A patent/US3166727A/en not_active Expired - Lifetime
- 1962-12-18 CH CH1488762A patent/CH388445A/en unknown
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US1809042A (en) * | 1926-11-30 | 1931-06-09 | Bell Telephone Labor Inc | Magnet core |
US2168351A (en) * | 1936-08-31 | 1939-08-08 | Rca Corp | Adjustable magnetic-core inductor |
US2407916A (en) * | 1943-04-10 | 1946-09-17 | Stewart Warner Corp | Shielded coil |
US2605311A (en) * | 1950-12-20 | 1952-07-29 | Westinghouse Electric Corp | Reactor |
US2792536A (en) * | 1953-10-30 | 1957-05-14 | Westinghouse Electric Corp | Electro-magnetic solenoids and actuators |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3423670A (en) * | 1964-08-07 | 1969-01-21 | Perkin Elmer Ltd | Magnetic shield arrangement for a high flux homogeneous field-producing magnet |
Also Published As
Publication number | Publication date |
---|---|
CH388445A (en) | 1965-02-28 |
FR1316558A (en) | 1963-02-01 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US4543208A (en) | Magnetic core and method of producing the same | |
US2966704A (en) | Process of making a ferrite magnetic device | |
US2903329A (en) | Device for molding anisotropic permanent magnets | |
KR102627781B1 (en) | An inductive device | |
EP0087781B2 (en) | Core material | |
US3287677A (en) | High frequency transformer core comprised of magnetic fluid | |
US3354417A (en) | Coil bobbin having projections extending beyond magnetic core | |
BRPI0014061B1 (en) | Transformer and inductor for low frequency applications using isotropic composite magnetic materials | |
KR101573729B1 (en) | Varialble inductor and mehtod for manufacturing thereof | |
US3028570A (en) | Ferrite inductance cores | |
US3166727A (en) | Magnetic coil and core structure | |
US3611225A (en) | Electrical inductive apparatus having liquid and solid dielectric means | |
GB829856A (en) | Improvements relating to reactors for high-frequency current | |
ES548860A0 (en) | METHOD OF MANUFACTURING DISTRIBUTION TRANSFORMERS | |
US3210610A (en) | Apparatus for electrically insulating the turns of superconducting coils | |
US3396355A (en) | Cooled hydrogen or neon used as transformer dielectric | |
KR102601127B1 (en) | Inductor core exhibits low magnetic losses | |
RU2225051C2 (en) | Method and device for manufacturing anisotropic polycrystalline ferrite material | |
CN202384154U (en) | Low-loss power transformer | |
JPH0227547Y2 (en) | ||
FR2056159A5 (en) | ||
Brockman | Magnetic ferrites for high-frequency uses | |
US890638A (en) | Variable-voltage transformer. | |
US9607755B2 (en) | Inductor and inductor core | |
Summers et al. | Acceleration for the/spl mu//sup+//spl mu//sup-/collider |