EP0162834A2 - Séparateur magnétique - Google Patents
Séparateur magnétique Download PDFInfo
- Publication number
- EP0162834A2 EP0162834A2 EP85890117A EP85890117A EP0162834A2 EP 0162834 A2 EP0162834 A2 EP 0162834A2 EP 85890117 A EP85890117 A EP 85890117A EP 85890117 A EP85890117 A EP 85890117A EP 0162834 A2 EP0162834 A2 EP 0162834A2
- Authority
- EP
- European Patent Office
- Prior art keywords
- magnetic
- volume
- force
- magnetic separator
- coils
- 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.)
- Granted
Links
Images
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B03—SEPARATION 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
- B03C—MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
- B03C1/00—Magnetic separation
- B03C1/02—Magnetic separation acting directly on the substance being separated
- B03C1/035—Open gradient magnetic separators, i.e. separators in which the gap is unobstructed, characterised by the configuration of the gap
Definitions
- the invention relates to a magnetic separator.
- a magnetic separator Preferably for a coil arrangement that is suitable for isodynamic magnetic separators for high throughput.
- the magnetic separators used industrially today are generally well suited to separating materials with ferromagnetic or strongly paramagnetic properties from other materials with diamagnetic or weakly paramagnetic properties. A separation of materials with only slight differences in their paramagnetic properties is only possible in some magnetic separators that are suitable for laboratory purposes.
- gravity is used as counterforce, which is why it is required that the cutting force density f should be constant over the cutting volume.
- the magnetic field that fulfills these conditions is referred to in this publication as an isodynamic magnetic field.
- Such a magnetic field is approximated by a specially shaped magnetic pole contour of an electromagnet with an iron yoke. If you want to use a different quantity as the counterforce, such as centrifugal force, the density of the separation force f must have the same spatial distribution as the counterforce.
- the level of magnetic induction is essentially limited to the saturation induction of the iron yoke.
- the greatest possible density of the cutting force is defined. If greater cutting force densities are necessary, the maximum magnetic induction must be increased if the geometry remains the same, or the geometric dimension must be reduced if the maximum induction remains the same.
- the object of the invention is to provide a magnetic separator which avoids the disadvantages of the above-mentioned magnetic fields and generates a magnetic field in which, for a certain volume acceptability, the generated separating force is adapted to a corresponding counterforce without being limited by the saturation induction of an iron yoke.
- the magnetic separator according to the invention is characterized in that the magnetic field, which generates the force density in the separating volume which is necessary for the separation with high selectivity and is adapted to the counterforce, is largely induced by the shape and position of the excitation coils.
- the magnetic field is induced by rotationally symmetrical coils, which are arranged symmetrically to the cutting volume and flow through current in opposite directions with respect to the plane of symmetry and comprise the cutting volume and the radius of the center of the cutting volume is smaller than the largest radius of the excitation coils, but larger than the smallest radius of the excitation coils.
- the magnetic field is induced by elongated coils, the long sides of the coil being arranged symmetrically to a plane of symmetry and comprising the sheath volume arranged symmetrically to the plane of symmetry.
- excitation coils are made of normally conductive material. This version is sufficient for certain vaginal problems. It is an economically viable solution.
- the excitation coils are made from superconductors. Weakly magnetic materials can only be separated using magnetic fields that can be generated from superconductors
- one or more iron cores or iron yokes are provided to increase the magnetic induction or to reduce the number of ampere turns.
- one or more iron yokes or a normally conducting or a superconducting surface are provided for shielding the magnetic field.
- a rotationally symmetrical excitation coil arrangement is shown in the figure, 1 denoting the axis of rotation and 2 denoting the plane of symmetry.
- the entire magnetic flux of the upper and the lower two coils between the coil pairs 3, 5 and 4, 6 is pushed through and thereby generates an approximately constant cutting force density in the annular channel-shaped cutting volume 7.
- the counterforce is the centrifugal force which acts in the annular channel-shaped partition volume 7 on the particles moving at the transport speed.
- the magnetic separation force density exerts on the different material particles a different force.
- This magnetic force competes with the counterforce, which is approximately the same for all particles.
- the counterforce is a superimposition of the drag forces in the carrier fluid with the force of gravity.
- the parting volume comes to lie between the excitation coils.
- the desired constancy of the cutting force density over the cutting volume or the desired adaptation to the spatially variable counterforce can be achieved with a coil pair with a non-rectangular cross section or with several coil pairs with a rectangular cross section.
- the desired constancy of the cutting force density can be achieved via the cutting volume or the desired adaptation to the spatially variable counterforce.
Landscapes
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
- Soft Magnetic Materials (AREA)
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| AT1684/84 | 1984-05-22 | ||
| AT0168484A AT379525B (de) | 1984-05-22 | 1984-05-22 | Magnetscheider |
Publications (3)
| Publication Number | Publication Date |
|---|---|
| EP0162834A2 true EP0162834A2 (fr) | 1985-11-27 |
| EP0162834A3 EP0162834A3 (en) | 1986-02-19 |
| EP0162834B1 EP0162834B1 (fr) | 1988-07-27 |
Family
ID=3518753
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| EP19850890117 Expired EP0162834B1 (fr) | 1984-05-22 | 1985-05-21 | Séparateur magnétique |
Country Status (3)
| Country | Link |
|---|---|
| EP (1) | EP0162834B1 (fr) |
| AT (1) | AT379525B (fr) |
| DE (1) | DE3563916D1 (fr) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO1990004458A1 (fr) * | 1988-10-25 | 1990-05-03 | Elin Energieanwendung Gesellschaft M.B.H. | Separateur magnetique a gradient ouvert |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| AT400779B (de) * | 1989-07-19 | 1996-03-25 | Gerhold Juergen Dipl Ing Dr Te | Magnetsystem |
| AT393463B (de) * | 1990-07-13 | 1991-10-25 | Elin Energieanwendung | Isodynamischer trennkanalmagnetscheider |
Family Cites Families (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE2157217A1 (de) * | 1971-11-18 | 1973-05-24 | Preussag Ag | Magnetscheider |
| CH565594A5 (fr) * | 1973-12-07 | 1975-08-29 | Bbc Brown Boveri & Cie | |
| DE2650528A1 (de) * | 1976-11-04 | 1978-05-18 | Kloeckner Humboldt Deutz Ag | Magnetscheider |
| GB2064377B (en) * | 1979-10-12 | 1984-03-21 | Imperial College | Magnetic separators |
| US4340468A (en) * | 1980-11-06 | 1982-07-20 | The United States Of America As Represented By The United States Department Of Energy | Method and apparatus for separating materials magnetically |
-
1984
- 1984-05-22 AT AT0168484A patent/AT379525B/de not_active IP Right Cessation
-
1985
- 1985-05-21 DE DE8585890117T patent/DE3563916D1/de not_active Expired
- 1985-05-21 EP EP19850890117 patent/EP0162834B1/fr not_active Expired
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO1990004458A1 (fr) * | 1988-10-25 | 1990-05-03 | Elin Energieanwendung Gesellschaft M.B.H. | Separateur magnetique a gradient ouvert |
Also Published As
| Publication number | Publication date |
|---|---|
| AT379525B (de) | 1986-01-27 |
| EP0162834A3 (en) | 1986-02-19 |
| EP0162834B1 (fr) | 1988-07-27 |
| ATA168484A (de) | 1985-06-15 |
| DE3563916D1 (en) | 1988-09-01 |
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| PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
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