Method and apparatus for compensating eddy current effects in a magnetic resonance device having pulsed magnetic field gradients

Claim 3

The method as recited in claim 1, wherein said given time delay starts at a minimum time period substantially equal to zero and increases to a maximum time delay which substantially corresponds to that time wherein it is expected that said eddy current magnetic field will no longer effect said gradient coil magnetic field.

Claim 4

The method as recited in claim 1, wherein said applying step comprises using said correction coefficients to adjust a pre-emphasis filter which is employed with said gradient coil.

Claim 5

The method as recited in claim 1, wherein said applying step comprises using said correction coefficients to cause a computer system to control the generation of said gradient coil pulse.

Claim 6

The method as recited in claim 1, wherein said irradiating step generates free induction decay signals as said MR signals.

Claim 7

The method as recited in claim 1, wherein said calculating step comprises calculating a time constant and coupling coefficient from the peak frequency shift data corresponding to the longest time constant of said eddy current magnetic field which is reliably represented thereby.

Claim 8

The method as recited in claim 1, wherein steps (a)-(e) determine correction coefficients for compensating a monoexponential component of said eddy current magnetic field, and steps (a)-(e) are repeated a plurality of times so as to generate successive sets of correction coefficients, each set substantially compensating for a different mono-exponential component of said eddy current magnetic field.

Claim 9

The method as recited in claim 5, wherein said calculating step comprises calculating a time constant and coupling coefficient from the peak frequency shift data corresponding to the longest time constant of said eddy current magnetic field which is reliably represented thereby.

Claim 10

The method as recited in claim 8, wherein steps (a)-(e) determine correction coefficients for compensating a monoexponential component of said eddy current magnetic field, and steps (a)-(e) are repeated a plurality of times so as to generate successive sets of correction coefficients, each set substantially compensating for a different mono-exponential component of said eddy current magnetic field.

Claim 11

A magnetic resonance (MR) device, comprising: a main magnet having a bore axially formed therethrough in which a base field is formed; gradient coil means positioned inside said bore of said main magnet, responsive to gradient coil pulses for providing a plurality of gradient field pulses along a given coordinate axis inside said bore and said gradient coil means; an MR-active sample positioned inside said bore at a distance remote from an origin of said given coordinate axis; an electrically conductive media located nearby said gradient coil means which produces at least one disturbing magnetic field along said given axis; signal sensing means positioned inside said bore of said magnet for sensing a plurality of successive MR signals generated by said MR active sample after irradiation of said sample by a corresponding plurality of successive RF pulses; and computer means operatively connected with said signal sensing means and said gradient coil means for measuring and storing as data a Fourier transformation of each of said sensed MR signals, for calculating correction coefficients for compensating the magnetic field of said gradient coil means with respect to said disturbing magnetic field using peak frequency shift data determined from the stored data of successive ones of said MR signals which have been Fourier transformed, and for applying said correction coefficients so as to generate pre-distorted gradient coil pulses which will compensate for the affect of said disturbing magnetic field upon said gradient field pulses.

Claim 12

A magnetic resonance (MR) device, comprising: a main magnet having a bore axially formed therethrough in which a base field is formed; gradient coil means positioned inside said bore of said main magnet, responsive to gradient coil pulses for providing a plurality of gradient field pulses along a given coordinate axis inside said bore and said gradient coil means; an MR-active sample positioned inside said bore at a distance remote from an origin of said given coordinate axis; an electrically conductive media located nearby said gradient coil means which produces at least one disturbing magnetic field along said given axis; signal sensing means positioned inside said bore of said magnet for sensing a plurality of successive MR signals generated by said MR active sample after irradiation of said sample by a corresponding plurality of successive RF pulses; and computer means operatively connected with said signal sensing means and said gradient coil means for measuring and storing as data a Fourier transformation of each of said sensed MR signals, for calculating correction coefficients for compensating the magnetic field of said gradient coil means with respect to said disturbing magnetic field using peak frequency shift data determined from the stored data of successive ones of said MR signals which have been Fourier transformed, and for applying said correction coefficients so as to generate pre-distorted gradient coil pulses which will compensate for the affect of said disturbing magnetic field upon said gradient field pulses.

Claim 13

The apparatus of claim 10, wherein said gradient coil means is controlled by said computer means to generate a plurality of time-sequential gradient field pulses and said signal sensing means is controlled by said computer means to irradiate said sample with an RF excitation pulse a given time delay which is increased following application of each of said gradient coil pulses, so as to generate a plurality of time-sequential ones of said MR signals.

Claim 14

The apparatus of claim 11, further including a pre-emphasis filter means coupled to said gradient coil means for providing pre-emphasis to said gradient coil pulses in accordance with the correction coefficients calculated by said computer means.

Claim 15

The apparatus of claim 12, wherein said computer means calculates a time constant and coupling coefficient by analyzing the stored data corresponding to the longest time constant of the disturbing magnetic field reliably represented thereby.