Process for the modulation of the speed effect of moving parts of a body in a nuclear magnetic resonance density measurement and performance of the process in order to deduce therefrom the speed of the moving parts in question

• US 4,694,253 A
• Filed: 12/12/1985
• Issued: 09/15/1987
• Est. Priority Date: 08/13/1985
• Status: Expired

• Current Assignee: Thomson-Cgr
• Original Assignee: Thomson-Cgr
• Inventors: Le Roux, Patrick
• Primary Examiner(s): Levy, Stewart J.
• Assistant Examiner(s): NOT, DEFINED
• Application Number:
  US06/808,049
• Time in Patent Office: 642 Days
• Field of Search: 324/306, 324/307, 324/309, 324/312, 128/653
• US Class Current: 324/309
• CPC Class Codes: G01N 24/08 by using nuclear magnetic resonance G01N24/12 takes precedence
• CPC Class Codes: G01R 33/56341 Diffusion imaging

Abstract

The present invention relates to a process for modulating the effect of the speed of the moving parts of a body. The machines or processes for measuring the density by nuclear magnetic resonance are too sensitive at the displacement speed of the parts in question. In the invention, the sensitivity of the machines or processes is reduced in such a way that the speed effect can be measured. Prior to the measurement, compensating magnetic field sequences are applied in order to counteract the effect produced by the interfering magnetic field sequences, which are necessary for performing the measurement.

Claims

1. A process for the modulation of the speed effect of the moving parts of a body in a density measurement by nuclear magnetic resonance, comprising the steps of;

exposing said body to an orienting, constant magnetic field for orienting in a single direction the magnetic spin moments of the body;

subjecting said body to a radio frequency magnetic excitation in the presence of and/or followed by the application of a sequence of an interfering magnetic field; and

detecting a magnetic resonance signal emitted in response by the body;

wherein the effect of the speed of the moving parts of the body created by the sequence of the interfering field is modulated by the application, prior to the step of detecting, of a sequence of a compensating magnetic field, an integral of said compensating magnetic field calculated on its duration being zero, and whose history and value are a function of the history and value of the interfering field wherein the sequence of the interfering magnetic field has magnetic field pulses along three orthogonal axes and wherein the sequence of the compensating magnetic field has magnetic field pulses along these three same axes, in order to individually modify the effects of the speed of the moving parts of the body along said three axes wherein the compensating magnetic field pulses are determined a priori by position and duration Γ

; and

,

wherein amplitude λ

is evaluated to obtain the modulation.

4. A process according to one of claims 1, 2 or 3, wherein the sequence of the compensating magnetic fields involves bipolar pairs of pulses.

5. A process according to one of claim 1 or 3, wherein the sequence of compensating magnetic fields involves pairs of pulses, each pulse of a pair being of the same value, shape, duration a nd sign as the other pulse of the pair, said pulses being respectively before and after a second radio frequency pulse.

6. A process according to one of the claims 1 or 2, wherein the integral of the product of the value of the interfering field pulses by the duration separating them from the reading of the emitted signal is compensated by the integral of a same product, obtained with the compensating field pulses.

7. A process according to claim 4, wherein the pulses of the pulse pairs involve pulses which are as far spaced from one another as possible.

8. A process according to one of claims 1 or 3, wherein the radio frequency magnetic excitation involves a first radio frequency pulse for flipping by 90°

the orientation of the magnetic moments of the spins, followed by at least one second radio frequency magnetic pulse for flipping by 180°

the orientation of the magnet moments of the spins and wherein the echo of the signal emitted in response is taken as the magnetic resonance signal after it has been reflected by the second radio frequency pulse.

9. A process according to any one of the claims 1, 2 or 3 wherein the measurement involves the production of the image of a volume, whereof the position and dimensions are determined by sequences of the interfering magnetic field.

10. A process according to any one of the claims 1, 2 or 3 wherein the measurement involves the production of an image of a selection of the body, whose position therein is determined by sequences of the interfering magnetic field.

11. A process according to claim 9, wherein the production of the image is performed in accordance with a three dimensional inverse Fourier transform type process (3DFT).

12. A process according to claim 11, wherein the image is produced in accordance with a bidimensional inverse Fourier transform type process (2DFT).

2. A process for the modulation of the speed effect of the moving parts of a body in a density measurement by nuclear magnetic resonance, comprising the steps of:

exposing said body to an orienting, constant magnetic field for orienting in a single direction the magnetic spin moments of the body;

subjecting said body to a radio frequency magnetic excitation in the presence of and/or followed by the application of a sequence of an interfering magnetic field; and

,

detecting a magentic resonance signal emitted in response by the body;

wherein the effect of the speed of the moving parts of the body created by the sequence of the interfering field is modulated by the application, prior to the step of detecting, of a sequence of a compensating magnetic field, an integral of said compensating magnetic field, calculated on its duration being zero, and whose history and value are a function of the history and value of the interfering field;

wherein the radio frequency magnetic excitation has a radio frequency pulse for flipping by 90°

the orientation of the magnetic moments of the spins, followed by a gradient echo pulse and wherein the echo of the signal emitted in response after being reflected by the gradient echo pulse is acquired as the magnetic resonance signal.

3. A process for the modulation of the speed effect of the moving parts of a body in a sensitivity measurement by nuclear magnetic resonance, comprising the steps of;

exposing said body to an orienting, constant magnetic field for orienting in a single direction the magnetic spin moments of the body;

subjecting said body to a radio frequency magnetic excitation in the presence of and/or followed by the application of a sequence of an interfering magnetic field; and

detecting a magnetic resonance signal emitted in response by the body;

wherein the effect of the speed of the moving parts of the body created by the sequence of the interfering field is modulated by the application, prior to the step of detecting, of a sequence of a compensating magnetic field, an integral of said compensating magnetic field calculated on its duration being zero, and whose history and value are a function of the history and value of the interfering field;

wherein the process is performed on occasions for each of which pluralities of sequences are achieved in order to produce images of theparts of the body;

wherein the process is performed on a first occasion to compensate the effect of the speed and on a second occasion by modifying one or more of the characteristics of the compensating magnetic field but by not nullifying these compensating magnetic field; and

,

wherein the measurements obtained are compared in the two performances in order to deduce therefrom an image of the speed of the moving parts in questions.

13. A performance according to claim 3, wherein the modification relates to the characteristics of the compensating magnetic field relative to one axis in order to deduce therfrom the velocity component of the moving parts along said axis.

14. A performance according to claims 3 or 13 wherein the modification is such that the phase displacement corresponding to the signal emitted by the moving parts moving at a nominal speed is approximately 1 radian.