US2329893A - Magnetic device for the purification of fluids - Google Patents

Magnetic device for the purification of fluids Download PDF

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US2329893A
US2329893A US400878A US40087841A US2329893A US 2329893 A US2329893 A US 2329893A US 400878 A US400878 A US 400878A US 40087841 A US40087841 A US 40087841A US 2329893 A US2329893 A US 2329893A
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Girard Georges
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Magnetos Lucifer S A
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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B03SEPARATION OF SOLID MATERIALS USING LIQUIDS OR USING PNEUMATIC TABLES OR JIGS; MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03CMAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03C1/00Magnetic separation
    • B03C1/02Magnetic separation acting directly on the substance being separated
    • B03C1/025High gradient magnetic separators
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B01PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
    • B01DSEPARATION
    • B01D35/00Filtering devices having features not specifically covered by groups B01D24/00 - B01D33/00, or for applications not specifically covered by groups B01D24/00 - B01D33/00; Auxiliary devices for filtration; Filter housing constructions
    • B01D35/06Filters making use of electricity or magnetism

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  • GEOEGESGl/E BY example fluids such as engine oil.
  • the subject of the present invention is a device for the magnetic purification of a fluid and separation of impurities therefrom which obviates the disadvantages above referred to by the fact that the fluid to be purified is caused to circulatein the air gap of a magnet and that the ferromagnetic particles in suspension in the fluid are attracted by means of attraction surfaces subjected to the action of the fiuid in movement, and that the-particles extracted from the fluid are accumulated mechanically and magnetically on accumulating surfaces which bound open spaces in which the intensity of the magnetic field and the intensity of the streams of fluid are weak.
  • the device for the magnetic purification of a fluid is provided with a magnet of which the air gap is traversed by the fluid to be purified, this air gap being provided with ferromagnetic elements having surfaces of attraction subjected to the action of the fluid in movement, and with a plurality of surfaces for accumulating the particles extracted magnetically from the fluid, which bound open spaces in which the intensity of the magnetic field and the intensity of the flow of fluid are weak.
  • Fig. 2 is a partial section to a larger scale of a ferromagnetic element and an accumulating aperture therein, showing the distribution of the magnetic field and illustrating the process of accumulation of the particles.
  • Fig. 3 is a section of a second form of construction.
  • Fig. 4 is a sectional view of a third form of construction.
  • Fig. 5 shows the device mounted in a casing, a portion of the latter being broken away.
  • the device for the magnetic purification of a fluid is formed by a permanent magnet i of horse-shoe form, provided with two pole pieces 2 opposite one another, and field concentrating elements'fl of ferromagnetic material placed between the pole pieces approximately normal to the lines of force of the magnetic field and lying in the direction of the circulation of the fluid (indicated by the arrows B).
  • the elements-,3 are provided with accumulating faces 8 (Fig. 2 which bound open spaces formed by apertures or holes 6 adapted to receive and retain the.,particles extracted magnetically from the fluid.
  • the lines H representapproximately the magnetic lines of force while the lines E indicate approximately the points of equal magnetic potential.
  • the operation of the device may be understood from this figure.
  • the filamentary paths of the circulation of fluid are represented by the lines B.
  • a particle P in suspension in the fluid is carried along by the latter between the pole faces 2 and therefore between the field concentrating ferromagnetic elements 3 (Fig. 1, 3, 4).
  • This particle P reaching the field prevailing in the air gap is attracted by one external attraction face I of the elements '3.
  • This particle P is then held magnetically against this face and cannot detach itself therefrom, but no force opposes the sliding of this particle P along the face 1. It is therefore picked up mechanically by the action of the fluid passing over the external attraction face I and slides along the latter.
  • it When it reaches the edge of an aperture i, bounded by the accumulation surface 8, it is attracted magnetically just into the plane of the attraction surface 1 where this place passes over aperture 6 and then slides on to the accumulation surface 8.
  • This magnetic action acting on the particle is increased by a mechanical action exerted by the fluid.
  • the fluid having the tendency to enter the open space 6 causes the particle to slide on the accumulation surface 8 on the periphery of apertures 6 towards the interior of the latter.
  • This particle, held magnetically to the accumulating surfac 8, is then pushed along the latter towards the interior of the element 3 by the succeeding particles sliding along the attraction surface 1.
  • the particles are thus more or less accumulated in successive layers, and gradually all the free space "in the interior of the hole is filled with particles.
  • the magnetic field present in thi free space bounded by the accumulation surface 8 is weak, as will appear from Fig. 2, as is also the intensity of the circulation of the fluid therein.
  • the particles accumulated on the surface 8 are thus enclosed in apertures 6 and cannot leave these as on the one hand the weak circulation passing through these free spaces only applies a feeble force tending to carry along the particles and, on the other hand, in order to leave these spaces, the particles must pass to outside of a zone of a strong magnetic field located at the edge of the spaces or apertures 6 (see Fig. 2).
  • the permanent magnet is replaced by an electromagnet II, and elements 3, similar to the elements, of Fig. 1, have attraction surfaces 21 provided with projecting attraction points 9 located on the lower edge of the holes 6.
  • These attraction points 9 have the advantage of attracting very violently the particles in suspension in the fluid by reason of the fact of their high degree of magnetic saturation.
  • non-magnetic members l3 For facilitating the manipulation and the cleaning of the ferromagnetic elements, these are assembled together by non-magnetic members l3 into a unit in such a manner as to enable all the elements of a single block to be withdrawn from the magnetic field.
  • the permanent magnet I0 is formed of small parallelopipeds, of a material of high permeability.
  • the field concentrating elements are formed as perforated or 'honeycombed parallelopiped for example of basket or trellis work, filled with ferromagnetic chips, for example, iron or steel wool or iron or steel filings.
  • ferromagnetic chips for example, iron or steel wool or iron or steel filings.
  • this form of construction of the field concentrating elements 30 there is obtained a plurality of accumulation surfaces which define a plurality of free spaces 38 located in the interior. of the element and in which the magnetic field and the velocity of the stream of fluid are low.
  • a plurality of points and attraction surfaces having a very high degree of magnetic saturation. It thus follows that the purification of the fluid by means of elements of this type is effected very rapidly and that the absorption capacity thereof is very great.
  • the device is placed into a casing l5 of rectangular section provided with a supply intake pipe l6 for the fluid and an outflow pipe ll for the fluid.
  • This casing is provided with a cover [8, which can be removed eas y; and provided with a joint 19.
  • this cover I8 is secured by means of a strap 20, pivotally mounted on pivots 2
  • conduit l6 may be secured easily in a wall of the casing I5. For this purpose it is sufilcientto make the latter slightly higher. This latter construction nables the cover to be removed without it being necessary to remove the pipe l6.
  • the ferromagnetic elements 33 may be withdrawn as a block, as they are connected together by means of non-magnetic members 3
  • Ferromagnetic elements according to Fig. 4 have the great advantage of retaining practically all the ferromagnetic particles contained in their free spaces, even when those elements are no longer in a magnetic field, which enables the elements to be removed for cleaning them without the liability of some of these particles falling back into the interior of the casing.
  • the magnet need not be of horseshoe shape and may be shaped according to requirements.
  • the field concentrating elements 3. may for example be formed by simple trellis work of fine mesh, staggered trellis work, split plates, or by assemblies of split or apertured plates which may be or may not be provided with attraction points. It is also possible to provide elements in the form of honeycombs. In this case the attraction surfaces I are formed by the ends of the honeycombs.
  • the attraction points may also be located in a different manner and, for example, the attraction surfaces 1 may be placed on end. i
  • the corners of the pole faces and of the magnet may be rounded as is current practice.
  • the direction of the fluid in the air gap is naturally of no importance from the point of view of the satisfactory operation of the device so. long as the direction is substantially perpendicular to the lines of force H, that is, in Fig. 2 the direction of the current can be from top to bottom, or bottom to top, or perpendicular to the plane of Fig. 2, but not from one side to the other of Fig. 2.
  • the circulation of fluid in the free spaces may be as weak as possible, there is preferably selected a general direction of the fluid which intersects the mag netic lines of force at a right angle. 4
  • the apparatus forming the subject of my invention has a high efficiency of magnetic purification, of which the v locity of purification is within wide limits independent of the concentration of ferromagnetic particles in the fiuid to be purified, and of the velocity of circulation of the latter. Also the efficiency of the device is only slightly infiuenced by the quantity of article already accumulated on the accumulation surfaces.
  • said concentrating members being provided with restricted transverse passages extending therethrough substantially transversely of said channel member transversely between said lateral pole pieces, said members being so arranged that the magnetic field in the interior of 7 said passages toward their respective axes extending through said members is of low intensity as compared with the field strength at the circumferential periphery of said passages, and the velocity of stream flow in said passages is slow.
  • a ferromagnetic channel member adapted for the passage or liquid therethrough, and being constituted of an inverted horseshoe magnet whose pole pieces constitute the respective lateral sides of said channel member, and auxiliary elongated ferromagnetic field concentrating slab-shaped members positioned in said channel member with their length lying in the direction of fiow of liquid therethrough, said concentrating members being provided with restricted transverse passages extending therethrough substantially transversely of said channel member transversely between said lateral pole pieces, said members being so arranged that the magnetic field in the interior of said passages toward their respective-axes extending through said members is of low intensity as compared with the field strength at the cirnel member transversely between said lateral pole pieces, said members being so constructed and arranged that the magnetic fiux path of high reluctance through said transverse apertures therethrough has magnetically in parallel therewith a low reluctance ferro-magnetic path of substantially the same physical length.
  • a channel. member adapted for the passage of liquid therethrough, a magnet having two pole pieces constituting the respective lateral sides of said channel member, and auxiliary elongated ferromagnetic field concentrating slab members positioned insaid channel member with their length lying in the direction of flow of liquid therethrough, said concentrating members being provided with restricted transverse apertures extending therethrough substantially transversely of said channel member transversely between said lateral pole pieces, said concentrating members being further provided with projecting ferromagnetic points formed on their surface adjacent to and immediately below said apertures respectively, said members being so constructed and arranged that the magnetic flux path of high reluctance through said transverse apertures therethrough has magnetically in parallel therewith a low reluctance term-magnetic path of substantially the same physical length.
  • a magnetic liquid clarifier a channel member adapted for the passage of liquid therethrough, a magnet having two pole pieces constituting the respective lateral sides of said channel member, and auxiliary elongated ferromagnetic field concentrating members formed as slab shaped baskets filled with steel wool and positioned in said channel member with their length lying in the direction of flow of liquid therethrough, and being mutually spaced apart torming paths for the flow of liquid therebetween.
  • a channel member adapted for the passage of liquid therethrough a magnet havingtwo pole pieces constituting the respective lateral sides of said channel member, auxiliary elongated ferromagnetic 7.
  • a channel member adapted for the passage oi liquid therethrough a magnet having two pole pieces constituting the respective lateral sides of said chan- 5 nel member, and auxiliary elongated i'erro-magnetic field concentrating members formed as slab shaped baskets filled with an interstitially spaced assembly of discrete small term-magnetic elementary pieces and said baskets being positioned 10 in said channel member with their length lying in the direction of flow of liquid therethrough, and being mutually spaced apart iorming paths for the flow of liquid therebetween.

Description

Sept, 21, 1943. .G. GIRARD 2,329,89
MAGNETIC DEVICE FOR THE PURIFICATION OF FLUIDS Filed July 2, 1941 2 SheesSheet 1 I N VEN TOR 9 kGgeeGEgG/BARD,
ATTORNEYS.
G. GIRARD MAGNETIC DEVICE FOR THE PURIFICATION OF FLUIDS 2 Sheets-Sheet 2 Filed July 2, 1941 I N vEA/Toe HRD',
Arr gA/Ehg.
GEOEGESGl/E BY example fluids such as engine oil.
Patented Sept. 21, 1943 MAGNETIC FOR THE PURIFICATION OF FLUIDS Georges Girard, Geneva, Switzerland, assignor to Magnetos Lucifer S. A., Geneva, Switzerland, a corporation of Switzerland Application July 2, 1941, Serial No. 400,878 In Switzerland September 10, 1940 7 Claims.
There are already known processes and magnetic devices for the purification of fluids, for While the magnetic separation and extraction of ferromagnetic particles in suspension in a fluid at rest is easy, it is, on the contrary, very diificult, when the fluid is in circulation, to retain and accumulate these particles and to prevent them from being detached from the attraction surfaces by the action of the moving fluid.
Various processes and devices have been proposed for separating and accumulating these particles, for exampl by forming impressions or grooves in the attraction surfaces in such a manner as to retain them against the action of the Other devices have been provided with magnets of which the pole pieces are provided with perforations through which the fluid to be purified passes. In these devices the stream of the fluid is therefore parallel to the lines of magnetic force, and the extraction of the particles is effected in a satisfactory manner, but the'surfaces on which the particles accumulate are washed by the fluid, which detaches the particles so that they are again picked up by the fluid.
On the other hand efforts have been made to retain the particles by points of attraction, but without good results, as the particles are always detached by the stream. Efforts have also been made to divide the air gap into a number of small air gaps in which the particles are allowed to accumulate, the fluid circulating outside these air gaps; These latter have given better results; however, their efiiciency is low and the purification slow by reason of the fact that the particles contained in suspension in the fluid are only subjected to a stray field. Further as the particles accumulate in the air gaps, they short-circuit these magnetically so that the stray field, by which the particles are attracted, becomes practically non-existent.
The subject of the present invention is a device for the magnetic purification of a fluid and separation of impurities therefrom which obviates the disadvantages above referred to by the fact that the fluid to be purified is caused to circulatein the air gap of a magnet and that the ferromagnetic particles in suspension in the fluid are attracted by means of attraction surfaces subjected to the action of the fiuid in movement, and that the-particles extracted from the fluid are accumulated mechanically and magnetically on accumulating surfaces which bound open spaces in which the intensity of the magnetic field and the intensity of the streams of fluid are weak.
The device for the magnetic purification of a fluid is provided with a magnet of which the air gap is traversed by the fluid to be purified, this air gap being provided with ferromagnetic elements having surfaces of attraction subjected to the action of the fluid in movement, and with a plurality of surfaces for accumulating the particles extracted magnetically from the fluid, which bound open spaces in which the intensity of the magnetic field and the intensity of the flow of fluid are weak.
The accompanying drawings show diagrammatically and by way of example, a few forms of construction of the subject of the present invention. I
Fig. 1 is a perspective view of a first form of construction, some of the elements being omitted for the sake of clearness.
Fig. 2 is a partial section to a larger scale of a ferromagnetic element and an accumulating aperture therein, showing the distribution of the magnetic field and illustrating the process of accumulation of the particles.
Fig. 3 is a section of a second form of construction. v
Fig. 4 is a sectional view of a third form of construction.
Fig. 5 shows the device mounted in a casing, a portion of the latter being broken away.
The device for the magnetic purification of a fluid is formed by a permanent magnet i of horse-shoe form, provided with two pole pieces 2 opposite one another, and field concentrating elements'fl of ferromagnetic material placed between the pole pieces approximately normal to the lines of force of the magnetic field and lying in the direction of the circulation of the fluid (indicated by the arrows B). The elements-,3 are provided with accumulating faces 8 (Fig. 2 which bound open spaces formed by apertures or holes 6 adapted to receive and retain the.,particles extracted magnetically from the fluid.
The very simple operation of the fluid purifier is shown diagrammatically in Fig. 2. v
In Fig. 2, the lines H representapproximately the magnetic lines of force while the lines E indicate approximately the points of equal magnetic potential. The operation of the device may be understood from this figure.
The filamentary paths of the circulation of fluid are represented by the lines B.
A particle P in suspension in the fluid is carried along by the latter between the pole faces 2 and therefore between the field concentrating ferromagnetic elements 3 (Fig. 1, 3, 4). This particle P reaching the field prevailing in the air gap, is attracted by one external attraction face I of the elements '3. This particle P is then held magnetically against this face and cannot detach itself therefrom, but no force opposes the sliding of this particle P along the face 1. It is therefore picked up mechanically by the action of the fluid passing over the external attraction face I and slides along the latter. When it reaches the edge of an aperture i, bounded by the accumulation surface 8, it is attracted magnetically just into the plane of the attraction surface 1 where this place passes over aperture 6 and then slides on to the accumulation surface 8. This magnetic action acting on the particle is increased by a mechanical action exerted by the fluid. In fact, the fluid having the tendency to enter the open space 6, causes the particle to slide on the accumulation surface 8 on the periphery of apertures 6 towards the interior of the latter. This particle, held magnetically to the accumulating surfac 8, is then pushed along the latter towards the interior of the element 3 by the succeeding particles sliding along the attraction surface 1.
The particles are thus more or less accumulated in successive layers, and gradually all the free space "in the interior of the hole is filled with particles. The magnetic field present in thi free space bounded by the accumulation surface 8 is weak, as will appear from Fig. 2, as is also the intensity of the circulation of the fluid therein. The particles accumulated on the surface 8 are thus enclosed in apertures 6 and cannot leave these as on the one hand the weak circulation passing through these free spaces only applies a feeble force tending to carry along the particles and, on the other hand, in order to leave these spaces, the particles must pass to outside of a zone of a strong magnetic field located at the edge of the spaces or apertures 6 (see Fig. 2). In order that the particles shall pass through this zone or region they must be picked up by a powerful current or eddies of fluid. But the velocity of circulation of the fluid therein is necessarily relatively slow so that the ferromagnetic particles have time to be attracted and to reach the attraction surfaces I. The stream is therefore always laminated and practically no eddy can occur. I
The particles entering the air gap, subjected to a very intense field, reach the attraction surfaces of the field concentrating elements 3 very rapidly. At the commencement of the operation, practically only the portions of the accumulating surfaces 8, which are located near the inlet for the fluid, receive the particles. Then, as the portions of these apertures or spaces, bounded by these surfaces, near the inlet, are filled in the course of time, other portions of the accumulating surfaces 8 in turn receive particles.
According to the modification shown in Fig. 3, the permanent magnet is replaced by an electromagnet II, and elements 3, similar to the elements, of Fig. 1, have attraction surfaces 21 provided with projecting attraction points 9 located on the lower edge of the holes 6. These attraction points 9 have the advantage of attracting very violently the particles in suspension in the fluid by reason of the fact of their high degree of magnetic saturation. These points of attraction being subjected to the action of the fluid, the particles, which are held on their points, slide on the surfaces 21, then on the accumulation surfaces 28, as described above.
For facilitating the manipulation and the cleaning of the ferromagnetic elements, these are assembled together by non-magnetic members l3 into a unit in such a manner as to enable all the elements of a single block to be withdrawn from the magnetic field.
According to the modification shown in Fig. 4, the permanent magnet I0 is formed of small parallelopipeds, of a material of high permeability. The field concentrating elements are formed as perforated or 'honeycombed parallelopiped for example of basket or trellis work, filled with ferromagnetic chips, for example, iron or steel wool or iron or steel filings. In this form of construction of the field concentrating elements 30 there is obtained a plurality of accumulation surfaces which define a plurality of free spaces 38 located in the interior. of the element and in which the magnetic field and the velocity of the stream of fluid are low. By reason of this form of construction of the elements, there is also obtained a plurality of points and attraction surfaces having a very high degree of magnetic saturation. It thus follows that the purification of the fluid by means of elements of this type is effected very rapidly and that the absorption capacity thereof is very great.
According to the modification shown in Fig. 5 the device is placed into a casing l5 of rectangular section provided with a supply intake pipe l6 for the fluid and an outflow pipe ll for the fluid. This casing is provided with a cover [8, which can be removed eas y; and provided with a joint 19. In order to facilitate its removal this cover I8 is secured by means of a strap 20, pivotally mounted on pivots 2|, provided on the casing l5, and provided witha tightening screw 22.
It will be understood that the conduit l6 may be secured easily in a wall of the casing I5. For this purpose it is sufilcientto make the latter slightly higher. This latter construction nables the cover to be removed without it being necessary to remove the pipe l6.
When the cover l8 has been removed, the ferromagnetic elements 33 may be withdrawn as a block, as they are connected together by means of non-magnetic members 3|.
For washing the elements 33 it is sufficient to dip them, for example in gasolene for removing ferromagnetic particles retained in the free spaces thereof.
Ferromagnetic elements according to Fig. 4 have the great advantage of retaining practically all the ferromagnetic particles contained in their free spaces, even when those elements are no longer in a magnetic field, which enables the elements to be removed for cleaning them without the liability of some of these particles falling back into the interior of the casing.
When the apparatus is used for purifying oil, for example, it is of advantage to select a form of construction of the ferromagnetic elements which enables them by film action to retain the major portion of oil contained between them and in their spaces. In this manner oil charged with ferromagnetic particles is not likely to fall back into the casing when the elements are removed from the latter. Elements according to Fig. 4 have given excellent results in this respect.
It will be understood that modifications may be made in the details of the subject of the present invention described as heretofore 'by way of example with reference to the accompanying dhh grammatic drawings. For example the magnet need not be of horseshoe shape and may be shaped according to requirements.
In particular it is possible to employ various modifications of the forms of construction of the field concentrating elements 3.. These may for example be formed by simple trellis work of fine mesh, staggered trellis work, split plates, or by assemblies of split or apertured plates which may be or may not be provided with attraction points. It is also possible to provide elements in the form of honeycombs. In this case the attraction surfaces I are formed by the ends of the honeycombs.
The attraction points may also be located in a different manner and, for example, the attraction surfaces 1 may be placed on end. i
For avoiding too large magnetic leakages, the corners of the pole faces and of the magnet may be rounded as is current practice.
The direction of the fluid in the air gap is naturally of no importance from the point of view of the satisfactory operation of the device so. long as the direction is substantially perpendicular to the lines of force H, that is, in Fig. 2 the direction of the current can be from top to bottom, or bottom to top, or perpendicular to the plane of Fig. 2, but not from one side to the other of Fig. 2. However in order that the circulation of fluid in the free spaces may be as weak as possible, there is preferably selected a general direction of the fluid which intersects the mag netic lines of force at a right angle. 4
It will be understood that it is possible to use in combination with any type of ferromagnetic element, either a permanent magnet or an electromagnet.
From the foregoing it will be seen that the apparatus forming the subject of my invention has a high efficiency of magnetic purification, of which the v locity of purification is within wide limits independent of the concentration of ferromagnetic particles in the fiuid to be purified, and of the velocity of circulation of the latter. Also the efficiency of the device is only slightly infiuenced by the quantity of article already accumulated on the accumulation surfaces. In fact, if after a certain time of operation, a small number of free spaces or apertures are still available for receiving ferromagnetic particles, these particles are in turn attracted more energetically towards attraction surfaces and into the spaces still free, by reason of the fact that the particles accumulated in the elements decrease the reluctance of the magnetic circuit, consequently the greater the quantity of ferromagnetic particles accumulated, the greater will also be the induction in the air gap.
therethrough, said concentrating members being provided with restricted transverse passages extending therethrough substantially transversely of said channel member transversely between said lateral pole pieces, said members being so arranged that the magnetic field in the interior of 7 said passages toward their respective axes extending through said members is of low intensity as compared with the field strength at the circumferential periphery of said passages, and the velocity of stream flow in said passages is slow.
2. In a magnetic liquid clarifier, a ferromagnetic channel member adapted for the passage or liquid therethrough, and being constituted of an inverted horseshoe magnet whose pole pieces constitute the respective lateral sides of said channel member, and auxiliary elongated ferromagnetic field concentrating slab-shaped members positioned in said channel member with their length lying in the direction of fiow of liquid therethrough, said concentrating members being provided with restricted transverse passages extending therethrough substantially transversely of said channel member transversely between said lateral pole pieces, said members being so arranged that the magnetic field in the interior of said passages toward their respective-axes extending through said members is of low intensity as compared with the field strength at the cirnel member transversely between said lateral pole pieces, said members being so constructed and arranged that the magnetic fiux path of high reluctance through said transverse apertures therethrough has magnetically in parallel therewith a low reluctance ferro-magnetic path of substantially the same physical length.
4. In a magnetic liquid clarifier, a channel. member adapted for the passage of liquid therethrough, a magnet having two pole pieces constituting the respective lateral sides of said channel member, and auxiliary elongated ferromagnetic field concentrating slab members positioned insaid channel member with their length lying in the direction of flow of liquid therethrough, said concentrating members being provided with restricted transverse apertures extending therethrough substantially transversely of said channel member transversely between said lateral pole pieces, said concentrating members being further provided with projecting ferromagnetic points formed on their surface adjacent to and immediately below said apertures respectively, said members being so constructed and arranged that the magnetic flux path of high reluctance through said transverse apertures therethrough has magnetically in parallel therewith a low reluctance term-magnetic path of substantially the same physical length.
' 5. In a magnetic liquid clarifier, a channel member adapted for the passage of liquid therethrough, a magnet having two pole pieces constituting the respective lateral sides of said channel member, and auxiliary elongated ferromagnetic field concentrating members formed as slab shaped baskets filled with steel wool and positioned in said channel member with their length lying in the direction of flow of liquid therethrough, and being mutually spaced apart torming paths for the flow of liquid therebetween.
6. In a magnetic liquid clarifler, a channel member adapted for the passage of liquid therethrough, a magnet havingtwo pole pieces constituting the respective lateral sides of said channel member, auxiliary elongated ferromagnetic 7. In a magnetic liquid clariiler, a channel member adapted for the passage oi liquid therethrough, a magnet having two pole pieces constituting the respective lateral sides of said chan- 5 nel member, and auxiliary elongated i'erro-magnetic field concentrating members formed as slab shaped baskets filled with an interstitially spaced assembly of discrete small term-magnetic elementary pieces and said baskets being positioned 10 in said channel member with their length lying in the direction of flow of liquid therethrough, and being mutually spaced apart iorming paths for the flow of liquid therebetween.
GEORGES GIRARD.
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* Cited by examiner, † Cited by third party
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US2452220A (en) * 1942-05-19 1948-10-26 Bower William Leslie Magnetic separator
US2459534A (en) * 1945-03-23 1949-01-18 J A Zurn Mfg Co Magnetic separator for fluid systems
US2478290A (en) * 1946-10-18 1949-08-09 Hpm Dev Corp Apparatus for removing foreign matter from fluid
US2622699A (en) * 1950-11-15 1952-12-23 Internat Derrick And Equipment Gear case with magnetic lubricant purifying means
US3676337A (en) * 1970-07-09 1972-07-11 Massachusetts Inst Technology Process for magnetic separation
US3873448A (en) * 1973-05-09 1975-03-25 Tenneco Chem Magnetic separator
US3912634A (en) * 1974-05-01 1975-10-14 Eriez Mfg Co Filter cartridge for a magnetic separator
US4046681A (en) * 1975-07-10 1977-09-06 Sala Magnetics, Inc. Multiple matrix assembly and matrix unit for magnetic separator with simplified sealing
US4079002A (en) * 1976-04-15 1978-03-14 Aquafine Corporation Thin-section-matrix magnetic separation apparatus and method
US4142479A (en) * 1975-10-06 1979-03-06 Daidotokushuko Kabushikikaisha Magnetic separators and apparatus for making the same
US4157297A (en) * 1974-10-31 1979-06-05 Max Alth Non-ferrous metal separation by induced attraction system and device
US4209394A (en) * 1979-02-05 1980-06-24 Massachusetts Institute Of Technology Magnetic separator having a multilayer matrix, method and apparatus
US4539040A (en) * 1982-09-20 1985-09-03 Mawardi Osman K Beneficiating ore by magnetic fractional filtration of solutes
WO1987001608A1 (en) * 1985-09-16 1987-03-26 Coulter Electronics, Inc. Flux diverting flow chamber for high gradient magnetic separation of particles from a liquid medium
WO1987001607A1 (en) * 1985-09-16 1987-03-26 Coulter Electronics, Inc. Apparatus for acoustically removing particles from a magnetic separation matrix
US5092987A (en) * 1984-12-05 1992-03-03 Akademi Der Wissenschaften Der Ddr Matrix for magnetic separators
US5275292A (en) * 1992-05-18 1994-01-04 Brugger Richard D Eddy current separator
US5700376A (en) * 1994-10-20 1997-12-23 Carpenter; Roland K. Method and apparatus for magnetically treating flowing liquids
US6068768A (en) * 1998-04-13 2000-05-30 Carpenter; Roland K. Apparatus for magnetically treating flowing liquids

Cited By (21)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2452220A (en) * 1942-05-19 1948-10-26 Bower William Leslie Magnetic separator
US2459534A (en) * 1945-03-23 1949-01-18 J A Zurn Mfg Co Magnetic separator for fluid systems
US2478290A (en) * 1946-10-18 1949-08-09 Hpm Dev Corp Apparatus for removing foreign matter from fluid
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