Method for reducing mechanical vibrations in a magnetic resonance imaging system

Patent metadata

Field	Value
Publication number	US-9229078-B2
Application number	US-201213723423-A
Country	US
Kind code	B2
Filing date	Dec 21, 2012
Priority date	Dec 21, 2011
Publication date	Jan 5, 2016
Grant date	Jan 5, 2016

Abstract

The present embodiments relate to a method for reducing mechanical vibrations in a magnetic resonance imaging system that includes a gradient system having a gradient coil body and an electrically conductive shroud that at least partly encloses the gradient coil body. The method includes determining a mechanical natural vibration mode of the gradient coil body in the magnetic resonance imaging system, and determining excitation force components for the natural vibration mode. The method also includes determining electrically conductive areas of the gradient system, which during operation of the magnetic resonance imaging system, generate a Lorentz force component that contributes to the excitation force components. The method further includes modifying the determined electrically conductive areas such that a minimal number of the Lorentz force components coincide with the excitation force components.

First claim

The invention claimed is:

1. A method for reducing mechanical vibrations in a magnetic resonance imaging system, the magnetic resonance imaging system comprising a gradient system having a gradient coil body with a number of gradient coils and an electrically conductive shroud that at least partially encloses the gradient coil body, the method comprising:
determining a mechanical natural vibration mode of the gradient coil body in the magnetic resonance imaging system;
determining excitation force components for the determined mechanical natural vibration mode;
determining electrically conductive areas of the gradient system that, during operation of the magnetic resonance imaging system, generate a Lorentz force component that contributes to the excitation force components, the electrically conductive areas including the gradient coils and the electrically conductive shroud; and
modifying the determined electrically conductive areas such that a minimal number of the Lorentz force components coincide with the excitation force components for the determined mechanical natural vibration mode.

2. The method as claimed in claim 1 , wherein the electrically conductive shroud has a thickness in a radial direction transverse to a longitudinal extent of the gradient coil body, the thickness corresponding to a skin penetration depth into the shroud.

3. The method as claimed in claim 2 , wherein the electrically conductive shroud completely encloses the gradient coil body in a circumferential direction.

4. The method as claimed in claim 1 , wherein the electrically conductive shroud completely encloses the gradient coil body in a circumferential direction.

5. The method as claimed in claim 4 , wherein the electrically conductive shroud comprises one or more modification elements configured to modify Lorentz forces of induced currents.

6. The method as claimed in claim 5 , wherein the one or more modification elements comprise one or more cutouts in the conductive shroud.

7. The method as claimed in claim 6 , further comprising displacing one or more of the determined Lorentz force components that act on the electrically conductive shroud into a nodal plane of the natural vibration mode, the one or more of the determined Lorentz force components being displaced by modifying eddy current paths in the conductive shroud, the eddy current paths being modified by the one or more modification elements.

8. The method as claimed in claim 1 , wherein the electrically conductive shroud comprises one or more modification elements configured to modify Lorentz forces of induced currents.

9. The method as claimed in claim 8 , wherein the one or more modification elements comprise one or more cutouts in the conductive shroud.

10. The method as claimed in claim 8 , further comprising displacing one or more of the determined Lorentz force components that act on the electrically conductive shroud into a nodal plane of the natural vibration mode, the one or more of the determined Lorentz force components being displaced by modifying eddy current paths in the conductive shroud, the eddy current paths being modified by the one or more modification elements.

11. The method as claimed in claim 1 , further comprising displacing one or more of the determined Lorentz force components that act on the electrically conductive shroud into a nodal plane of the natural vibration mode.

12. The method as claimed in claim 11 , wherein the one or more of the determined Lorentz force components are displaced by modifying eddy current paths in the conductive shroud.

13. The method as claimed in claim 11 , wherein a normal vector of the nodal plane is oriented parallel to a longitudinal extent of the gradient coil body.

14. The method as claimed in claim 1 , further comprising repeating the determining of the mechanical natural vibration mode, the determining of the excitation force components, the determining of the electrically conductive areas, and the modifying for one or more different natural vibration modes.

15. A gradient system comprising:
a gradient coil body having a mechanical natural vibration mode and excitation force components for the mechanical natural vibration mode, the gradient coil body comprising:
a number of gradient coils; and
an electrically conductive shroud that at least partly encloses the gradient coil body; and

electrically conductive areas configured to generate, during operation of a magnetic resonance imaging system, a Lorentz force component that contributes to the excitation force components,
wherein the electrically conductive areas are modified such that a minimal number of the Lorentz force components coincide with the excitation force components for the determined mechanical natural vibration mode.

16. The gradient system as claimed in claim 15 , wherein the electrically conductive shroud has a thickness in a radial direction transverse to a longitudinal extent of the gradient coil body, the thickness corresponding to a skin penetration depth into the shroud.

17. The gradient system as claimed in claim 15 , wherein the electrically conductive shroud completely encloses the gradient coil body in a circumferential direction.

18. The gradient system as claimed in claim 15 , wherein the electrically conductive shroud comprises one or more modification elements configured to modify Lorentz forces of induced currents.

19. The gradient system as claimed in claim 18 , wherein the one or more modification elements comprise one or more cutouts in the conductive shroud.

20. The gradient system as claimed in claim 18 , wherein the one or more modification elements are configured to displace one or more of the determined Lorentz force components that act on the electrically conductive shroud into a nodal plane of the natural vibration mode.

21. A magnetic resonance imaging system comprising:
a gradient system comprising:
a gradient coil body having a number of gradient coils and an electrically conductive shroud that at least partially encloses the gradient coil body, the gradient coil body having a mechanical natural vibration mode and excitation force components for the mechanical natural vibration mode; and
electrically conductive areas configured to generate, during operation of the magnetic resonance imaging system, a Lorentz force component that contributes to the excitation force components,

wherein the electrically conductive areas are modified such that a minimal number of the Lorentz force components coincide with the excitation force components for the determined mechanical natural vibration mode.

22. The magnetic resonance imaging system as claimed in claim 21 , wherein the electrically conductive shroud has an area that is disposed in a nodal plane of the natural vibration mode, and
wherein during operation of the magnetic resonance system, the area conducts the highest current density of eddy currents induced in or on the conductive shroud.

Assignees

• Dietz Peter
• Krug Andreas
• Siemens Ag

Inventors

• Dietz Peter
• Krug Andreas

Classifications

• G01R33/4215

  of the gradient magnetic field, e.g. using passive or active shielding of the gradient magnetic field · CPC title

• G01R33/28

  Details of apparatus provided for in groups G01R33/44 - G01R33/64 · CPC title

• G01R33/44 Primary

  using nuclear magnetic resonance [NMR] (G01R33/24, G01R33/62 take precedence) · CPC title

• G01R33/3854 Primary

  means for active and/or passive vibration damping or acoustical noise suppression in gradient magnet coil systems · CPC title