IP Library Granted Patent US 9,229,078
Granted Patent B2
US 9,229,078 · App. 13/723,423 · Granted Jan 5, 2016

Method for reducing mechanical vibrations in a magnetic resonance imaging system

View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 9,229,078
App. No.
13/723,423
Granted
Jan 5, 2016
Kind
B2
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.

Claims (36)

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.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Nov 21, 2016
From: SIEMENS AKTIENGESELLSCHAFT
To: SIEMENS HEALTHCARE GMBH
Reel/Frame 040656/0054 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 2, 2013
From: DIETZ, PETER; KRUG, ANDREAS
To: SIEMENS AKTIENGESELLSCHAFT
Reel/Frame 031699/0903 →