Structured coil electromagnets for magnetic resonance imaging and method for fabricating the same

• US 5,382,904 A
• Filed: 08/06/1992
• Issued: 01/17/1995
• Est. Priority Date: 04/15/1992
• Status: Expired due to Term

• Current Assignee: Houston Advanced Research Center
• Original Assignee: Houston Advanced Research Center
• Inventors: Pissanetzky, Sergio
• Primary Examiner(s): ARANA, LOUIS M
• Application Number:
  US07/926,667
• Time in Patent Office: 894 Days
• Field of Search: 324/300, 324/307, 324/309, 324/318, 324/319, 324/320, 335/299, 335/296, 29/602.1
• US Class Current: 324/319
• CPC Class Codes: G01R 33/3806 Open magnet assemblies for improved access to the sample, e.g. C-type or U-type magnets
• CPC Class Codes: G01R 33/3815 with superconducting coils, e.g. power supply therefor
• CPC Class Codes: G01R 33/3875 using correction coil assemblies, e.g. active shimming
• CPC Class Codes: G01R 33/421 of main or gradient magnetic field
• CPC Class Codes: Y10T 29/4902 Electromagnet, transformer or inductor

Abstract

Superconducting electromagnets suitable for use in the NMR tomography of human organs, and a method of making the same, are disclosed. Each of the disclosed electromagnets are constructed according to a structured coils methodology, where the desired field at locations within the volume of interest and, optionally, outside of the location of the coils is selected; the current magnitude and polarity for a plurality of coil elements locations are then optimized, by way of a computer program, to provide the desired field magnitude at the locations. The magnet construction results in a plurality of coils of varying current polarity, and of irregular shape and size, optimized to provide the uniform field. Magnets may be constructed according to the present invention which provide suitably highly uniform and high magnitude DC magnetic fields at volumes of interest which may be within or outside of the magnet bore, enabling the MRI of human organs without requiring whole body insertion of the patient into the magnet bore.

Claims

1. A method of fabricating an electromagnet, comprising the steps of:

defining a volume of interest;

selecting a magnetic field magnitude to be produced in said volume of interest;

defining a region near said volume of interest within which non-zero zero current density is allowable, and represented as a two-dimensional array of elemental areas;

determining the magnitude and polarity of the current density for each of the elemental areas within the defined region in order to produce the selected magnetic field magnitude in the volume of interest, in such a manner that substantially the same magnitude and polarity of current density is determined for at least one cluster of elemental areas; and

constructing at least one coil for carrying current at locations and at magnitudes corresponding to the result of the determining step.

2. The method of claim 1, wherein said elemental areas correspond to elemental cross-sectional areas of loops about said volume of interest.

3. The method of claim 1, wherein said elemental areas correspond to elemental cross-sectional areas of long bars extending normal to a plane cross-section of said volume of interest.

4. The method of claim 1, wherein the determining step comprises:

selecting a current density limit for said elemental areas;

selecting a target value of magnetic field for a plurality of target locations;

modeling the field produced by the selected current magnitude and polarity for said elemental areas;

calculating the difference between the modeled field and the target value of magnetic field at each of said plurality of target locations to derive a quadratic error form;

adjusting the selected current density magnitude and polarity values for said elemental areas within said current density limit according to constrained quadratic optimization of said quadratic error form.

5. The method of claim 4, wherein said adjusting step comprises:

iteratively performing simplex minimization of said quadratic error form.

6. The method of claim 4, wherein said plurality of target locations comprise target locations within said volume of interest.

7. The method of claim 6, wherein said plurality of target locations comprise target locations at the perimeter of said volume of interest.

8. The method of claim 6, wherein said plurality of target locations further comprise target locations disposed outside of the location of said coil elements.

9. The method of claim 4, wherein said step of calculating the difference comprises

calculating the zonal harmonic coefficients in the field.

10. The method of claim 4, further comprising:

after said minimizing step, calculating the magnetization of iron surrounding the defined region;

and wherein said modeled field further includes the field produced by said magnetization.

11. The method of claim 4, further comprising:

defining current density limits for each of said elemental areas.

12. The method of claim 11, wherein said current density limits correspond to superconducting current densities.

13. The method of claim 1, wherein said defining step comprises:

defining a first array of primary elemental areas near said volume of interest; and

defining a second array of shielding elemental areas disposed outside of the first array of primary elemental areas relative to said volume of interest.

14. The method of claim 1, further comprising:

after the determining step, adjusting the location of the region relative to the volume of interest;

after the adjusting step, repeating the determining step for the elemental areas in the defined region at its adjusted location;

calculating the field in the volume of interest after said adjusting and repeated determining steps; and

repeating said adjusting, determining and calculating steps until the difference between the calculated field and desired field reaches a tolerance limit.

15. The method of claim 1, wherein at least one cluster has a non-rectangular cross-sectional area.

16. The method of claim 1, wherein at least one cluster has a rectangular cross-sectional area.

17. An electromagnet, comprising:

at least one coil for conducting current encircling a bore, wherein the current conducted at a plurality of locations therewithin is determined by a method comprising the steps of;

defining a volume of interest;

selecting a magnetic field magnitude to be produced in said volume of interest;

defining a region within which non-zero current densities are allowed, and comprised of a two-dimensional array of elemental areas; and

determining the magnitude and polarity of current density for each of said elemental areas to produce the selected magnetic field magnitude in the volume of interest, in such a manner that substantially the same magnitude and polarity of current density is determined for at least one cluster of elemental areas within the defined region, each cluster defining the shape, position, and current of a corresponding coil.

18. The magnet of claim 17, wherein the determining step comprises:

selecting a current density limit for said elemental areas;

selecting a target value of magnetic field for a plurality of target locations;

modeling the field produced by the selected current density magnitude and polarity for said elemental areas;

calculating the difference between the modeled field and the target value of magnetic field at each of said plurality of target locations to derive a quadratic error form;

adjusting the selected current density magnitude and polarity values for said elemental areas within said current density limit according to constrained quadratic optimization of said quadratic error form.

19. The magnet of claim 17, wherein the method further comprises:

after the determining step, adjusting the location of the defined region;

after the adjusting step, repeating the determining step for the elemental areas in the defined region at its adjusted location;

calculating the field in the volume of interest after said adjusting and repeated determining steps; and

repeating said adjusting, determining and calculating steps until the difference between the calculated field and desired field reaches a tolerance limit.

20. The magnet of claim 17, further comprising:

means for shielding stray field produced by the coil.

21. The magnet of claim 20, wherein said shielding means comprises a shielding coil disposed outside of said coil relative to said volume of interest.

22. The magnet of claim 17, wherein said shielding means comprises:

an iron shield surrounding the coil.

23. The magnet of claim 20, wherein the determining step comprises:

selecting a current density limit for said elemental areas;

selecting a target value of magnetic field for a plurality of target locations;

modeling the field produced by the selected current magnitude and polarity for said elemental areas;

calculating the difference between the modeled field and the target value of magnetic field at each of said plurality of target locations to derive a quadratic error form;

adjusting the selected current density magnitude and polarity values for said elemental areas within said current density limit according to constrained quadratic optimization of said quadratic error form;

wherein said method further comprises;

after said minimizing step, calculating the magnetization of iron surrounding the defined region;

and wherein said modeled field further includes the field produced by said magnetization.

24. The magnet of claim 17, wherein at least a portion of said volume of interest is located outside of said bore.

25. The magnet of claim 17, wherein said coil comprises superconducting wire.

26. The magnet of claim 17, wherein said coil comprises non-superconducting wire.

27. The magnet of claim 17, wherein at least one cluster has a non-rectangular cross-sectional area.

28. The magnet of claim 17, wherein at least one cluster has a rectangular cross-sectional area.