GB2288464A - Wire bundle MRI magnet shim rings - Google Patents
Wire bundle MRI magnet shim rings Download PDFInfo
- Publication number
- GB2288464A GB2288464A GB9408543A GB9408543A GB2288464A GB 2288464 A GB2288464 A GB 2288464A GB 9408543 A GB9408543 A GB 9408543A GB 9408543 A GB9408543 A GB 9408543A GB 2288464 A GB2288464 A GB 2288464A
- Authority
- GB
- United Kingdom
- Prior art keywords
- magnet
- turns
- insulation
- shims
- wire
- 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
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
- G01R33/28—Details of apparatus provided for in groups G01R33/44 - G01R33/64
- G01R33/38—Systems for generation, homogenisation or stabilisation of the main or gradient magnetic field
- G01R33/387—Compensation of inhomogeneities
- G01R33/3873—Compensation of inhomogeneities using ferromagnetic bodies ; Passive shimming
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- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Magnetic Resonance Imaging Apparatus (AREA)
Abstract
A magnet for MRI apparatus includes shims 13, 14 which are fabricated from mutually insulated contiguous turns of iron or steel wire. The insulation reduces eddy currents. The shims may be wound using round or square section wire. Induced voltages may be reduced by reversing the winding sense, or by segmenting. <IMAGE>
Description
IMPROVEMENTS IN OR RELATING TO MAGNETIC
RESONANCE IMAGING APPARATUS
This invention relates to magnetic resonance imaging (MRI) apparatus and more particularly it relates to magnets for use in such apparatus.
The principal of operation of MRI apparatus, (more especially as used for medical applications), and the requirements for design and construction of magnets used in such apparatus is generally well known to those skilled in the art. Accordingly, a detailed discussion of this subject for the purposes of the present invention is believed to be unnecessary, but nevertheless some fundamental requirements for successful operation of the apparatus will now be considered.
One of the principal requirements for high quality imaging is the provision of a highly homogeneous magnetic field in an imaging volume, i.e. a region wherein that part of a patient to be scanned is positioned. Homogeneity is known to be improved by the inclusion of precisely positioned mild steel shimming rings in the 'warm bore' of a cryogenic annular magnet, i.e. shimming rings positioned on the imaging volume side of a cryogenic container or cryostat used to house a super-conducting magnet.
Unfortunately, eddy currents are produced in these shims, as primary magnetic field gradient coils are pulsed on and off, (which pulsing is a fundamental part of the imaging process), which adversely affect the image quality.
In order to minimise this effect, active shielding is provided by means of secondary gradient coils, which generate shielding magnetic fields effective to produce cancellation of the field gradients in predetermined regions. Active magnetic shield gradients are usually designed to produce a zero magnetic field in a region spaced apart by several centimetres from the shims and a compromise design is therefore difficult, if not impossible to produce, especially if the shims are positioned between the primary and secondary gradient coils, or on the 'warm bore' or patient side of the coils, as may be necessary for optimum magnetic homogeneity.
It is an object of the present invention to provide for elimination, or at least a substantial reduction, of eddy currents in shimming rings of an MRI magnet, whereby image quality is improved.
According to the present invention, a magnet for MRI apparatus includes shims which are fabricated from mutually insulated contiguous turns of iron or steel wire.
The wire may be of rectangular or square in cross-section whereby high packing density is achievable.
The ratio of thickness to width of the rectangular cross section wire may be chosen to achieve optimum packing density and/or optimum anti eddy current propagation characteristics.
The insulation used to provide the said mutually insulated turns should preferably be of substantially uniform thickness throughout the length of a winding defined by the turns.
insulation may be defined by an enamel or plastics coating, such as an epoxy resin coating for example.
The insulation may be electrostatically applied using a wet coating process.
Alternatively, the insulation may comprise tape or braiding or the like.
The winding may be arranged to comprise two or more subwindings wound so as substantially to cancel the effects of voltages induced therein which could cause insulation breakdown.
The shims may be wound wet or dry directly onto a profiled former mounted in a cryostat operatively associated with the magnet.
One embodiment of the invention will now be described by way of example only with reference to the accompanying drawing, which is a schematic sectional view of a part of a superconducting magnet used in MRI apparatus.
Referring now to the drawings, a super-conducting magnet for MRI apparatus comprises magnet coils la, lb, ic and 2a, 2b, 2c, which are arranged within a vessel 3 filled with liquid helium.
It will be appreciated that the magnet is symmetrical about its longitudinal axis 4, through which the sectional view is taken and accordingly for simplicity, an upper half only of the sectional view is shown. The magnet is also generally symmetrical about a vertical axis 5 and as can be seen from the drawing, the magnet coils la, ib and ic are positioned to the right of the vertical axis 5 and are similar to the coils 2a, 2b and 2c which are positioned to the left of the vertical axis 5.
The vessel 3 is contained within a wall 6 of a sealed outer chamber, and a space 7 defined between the vessel 3 and the wall 6 of the outer chamber, is evacuated to minimise heat gain by convection and thereby to provide good insulation. Additionally, in the evacuated space 7, inner and outer aluminium cryoshields 8 and 9 respectively, are provided to minimise heat gain by radiation.
A cylindrical region (often described as the 'warm bore' of a magnet) disposed within the annular super-conducting magnet coils la, ib, ic and 2a, 2b, 2c, includes a generally spherical imaging volume as shown by broken line 10, wherein optimum homogeneity of the magnetic field obtains and wherein that part of a patient to be scanned is positioned. In this region, primary gradient coils 11 are positioned, together with secondary shield gradient coils 12, which serve to produce a shield magnetic field in opposition to the field produced by the primary gradient coils.
In order to produce homogeneity of the magnetic field in the 'warm bore', shims 13a, 13b and 14a, 14b are provided between the primary and secondary gradient coils 11 and 12. Although the shims 13a, 13b and 14a, 14b are shown located between the gradient coils 11, 12, they may alternatively be located above the secondary shield gradient coil 12 in a space 15, or below the primary gradient coil 11 in a space 16.
In order to prevent the undesirable build up of eddy currents in the shimming rings 13a, 13b and 14a, 14b, the rings are fabricated, using a winding technique, of turns made of iron or mild steel which are mutually insulated from each other. The magnetic performance of the wire wound shims may be adjusted by means of physical movement of their position in the bore and/or by winding additional balancing turns. The wire used for the balancing turns would be of suitable shape and size, which may or may not correspond to the wire from which the shims are fabricated. Wire winding of the shims allows both ease of manufacture and the possibility of balancing turns on the shims.
Constancy of packing density is maintained by holding the winding tension at a constant level. These factors render wire winding far superior to the other techniques of lamination, e.g.
stacking sheets of steel plate.
In order to provide good packing density, the wire from which the shims are wound is preferably square or rectangular in cross section, the thickness to width ratio being chosen to provide optimum packing density and anti-eddy current propagation characteristics. The wire may be insulated using any suitable technique such as enamel or plastics coating for example, and an electrostatically applied wet coating processed may be used.
Alternatively, however, the insulation may comprise wound tape or a braided cover. It will be appreciated that the quality of the insulation is chosen having regard to the break down voltage required which is dependent upon the voltages produced during gradient pulsing. Prior to being insulated, the wire material will normally be fully annealed to produce suitable soft magnetic properties. Iron or mild steel wire is suitable for the shims having a carbon content of less than .1it. Typically the presence of other residual elements is kept to less than .4%. Conveniently, the wire may be manufactured by a rolling or drawing process, annealing being carried out as a final stage in the manufacturing operation.
Advantageously layers of turns or groups of layers of turns may be wound in opposing directions thereby to cancel out voltages induced during gradient pulsing. Additionally, or alternatively, the winding may be segmented whereby induced voltages are not permitted to build up. Alternatively, in order to prevent the build up of the induced voltages, wire may be used which is not electrically continuous.
Various modifications may be made to the arrangement just before described, without departing from the scope of the invention and for example, although a super-conducting magnet has been just before described, it will be appreciated that similar techniques may be used for other high flux non super-conducting magnet assemblies.
Claims (12)
1. A magnet for MRI apparatus includes shims which are fabricated from mutually insulated contiguous turns of iron or steel wire.
2. A magnet as claimed in claim 1, wherein the wire is of rectangular or square in cross-section.
3. A magnet as claimed in claim 2, wherein the ratio of thickness to width of the wire cross-section is chosen to achieve optimum packing density and/or optimum anti-eddy current propagation characteristics.
4. A magnet as claimed in any preceding claim, wherein the insulation used to provide the said mutually insulated turns is of substantially uniform thickness throughout the length of a winding defined by the turns.
5. A magnet as claimed in any preceding claim, wherein the insulation is defined by an enamel or plastics coating.
6. A magnet as claimed in claim 5, wherein the coating is an epoxy resin.
7. A magnet as claimed in any preceding claim, wherein the insulation is electrostatically applied using a wet coating process.
8. A magnet as claimed in any of claims 1 to 4, wherein the insulation comprises tape or braiding or the like.
9. A magnet as claimed in any preceding claim, wherein a winding defined by the turns comprises two or more subwindings wound so as substantially to cancel the effects of voltages induced therein.
10. A magnet as claimed in any preceding claim, wherein the shims are wound wet or dry directly onto a profiled former mounted in a cryostat operatively associated with the magnet.
11. A magnet as claimed in claim 1 and substantially as hereinbefore described with reference to the accompanying drawing.
12. MRI apparatus including a magnet as claimed in any preceding claim.
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE1995619121 DE69519121T2 (en) | 1994-04-13 | 1995-03-20 | Improvements in or related to magnetic resonance imaging devices |
EP19950104102 EP0677751B1 (en) | 1994-04-13 | 1995-03-20 | Improvements in or relating to magnetic resonance imaging apparatus |
JP7087102A JPH0838454A (en) | 1994-04-13 | 1995-04-12 | Magnet of magnetic resonance image device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB9407309A GB9407309D0 (en) | 1994-04-13 | 1994-04-13 | Improvements in or relating to magnetic resonance imaging apparatus |
Publications (3)
Publication Number | Publication Date |
---|---|
GB9408543D0 GB9408543D0 (en) | 1994-06-22 |
GB2288464A true GB2288464A (en) | 1995-10-18 |
GB2288464B GB2288464B (en) | 1998-01-28 |
Family
ID=10753466
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB9407309A Pending GB9407309D0 (en) | 1994-04-13 | 1994-04-13 | Improvements in or relating to magnetic resonance imaging apparatus |
GB9408543A Revoked GB2288464B (en) | 1994-04-13 | 1994-04-29 | Improvements in or relating to magnetic resonance imaging apparatus |
Family Applications Before (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB9407309A Pending GB9407309D0 (en) | 1994-04-13 | 1994-04-13 | Improvements in or relating to magnetic resonance imaging apparatus |
Country Status (1)
Country | Link |
---|---|
GB (2) | GB9407309D0 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5979937A (en) * | 1996-04-08 | 1999-11-09 | Takata Corporation | Air bag device |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0216404A1 (en) * | 1985-08-26 | 1987-04-01 | Koninklijke Philips Electronics N.V. | Magnetic resonance imaging apparatus including-homogenizing magnetic elements |
GB2219406A (en) * | 1988-04-08 | 1989-12-06 | Magnex Scient Limited | Electromagnets |
US4931759A (en) * | 1989-04-06 | 1990-06-05 | General Atomics | Magnetic resonance imaging magnet having minimally symmetric ferromagnetic shield |
-
1994
- 1994-04-13 GB GB9407309A patent/GB9407309D0/en active Pending
- 1994-04-29 GB GB9408543A patent/GB2288464B/en not_active Revoked
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0216404A1 (en) * | 1985-08-26 | 1987-04-01 | Koninklijke Philips Electronics N.V. | Magnetic resonance imaging apparatus including-homogenizing magnetic elements |
GB2219406A (en) * | 1988-04-08 | 1989-12-06 | Magnex Scient Limited | Electromagnets |
US4931759A (en) * | 1989-04-06 | 1990-06-05 | General Atomics | Magnetic resonance imaging magnet having minimally symmetric ferromagnetic shield |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5979937A (en) * | 1996-04-08 | 1999-11-09 | Takata Corporation | Air bag device |
Also Published As
Publication number | Publication date |
---|---|
GB9407309D0 (en) | 1994-06-08 |
GB2288464B (en) | 1998-01-28 |
GB9408543D0 (en) | 1994-06-22 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
773K | Patent revoked under sect. 73(2)/1977 |