NMR flow imaging using bi-phasic excitation field gradients

• US 4,654,591 A
• Filed: 07/29/1985
• Issued: 03/31/1987
• Est. Priority Date: 07/29/1985
• Status: Expired due to Term

• Current Assignee: Wisconsin Alumni Research Foundation (University of Wisconsin System)
• Original Assignee: Wisconsin Alumni Research Foundation (University of Wisconsin System)
• Inventors: Moran, Paul R.
• Primary Examiner(s): Tokar, Michael J.
• Application Number:
  US06/760,354
• Time in Patent Office: 610 Days
• Field of Search: 128/653, 324/300, 324/306, 324/307, 324/309, 324/311, 324/313, 324/318, 324/322
• US Class Current: 324/306
• CPC Class Codes: G01R 33/563 of moving material, e.g. flow contrast angiography

Abstract

An NMR zeugmatographic scanner is modified to provide flow images. A motion sensitizing, bi-phasic excitation field gradient is applied during each measurement cycle to produce transverse magnetization in paramagnetic nuclei which are moving in the direction of the gradient. The resulting free induction signal is processed using an inverse Fourier transformation to produce images of flowing paramagnetic nuclei.

Claims

1. In a gyromagnetic resonance instrument which performs a measurement cycle in which a FID signal produced by gyromagnetic material having a transverse magnetic moment is detected and processed to produce an indication of the amount of transverse magnetization, the improvement comprising:

an oscillator for producing an excitation signal at the Larmor frequency of the gyromagnetic material;

an excitation field gradient coil coupled to the oscillator and mounted in the instrument to produce a transversely directed magnetic field at the Larmor frequency which has a magnitude gradient in a preset direction; and

control means for producing a motion sensitized FID signal by controlling the excitation signal applied to the excitation field gradient coils such that a bi-phasic excitation field gradient is applied to the gyromagnetic material.

2. The improvement as recited in claim 1 in which the instrument includes means for linking the FID signal produced during each of a plurality of measurement cycles with a location in the gyromagnetic material and the control means produces a plurality of motion sensitized FID signals from various locations in the gyromagnetic material which are processed to form an image indicative of the motion of gyromagnetic material at each of said various locations.

3. The improvement as recited in claim 1 in which the bi-phasic excitation field gradient is produced by coupling the excitation signal to the excitation field gradient coil for a preset time interval and then coupling the inversion of the excitation signal to the excitation field gradient coil for the same preset time interval.

4. In an NMR scanner for producing images from data collected during measurement cycles, a method for producing data during such a measurement cycle which indicates motion in gyromagnetic material, the steps comprising:

applying a first bi-phasic excitation field gradient to the gyromagnetic material;

receiving the FID signal which is produced by the gyromagnetic material in response to the first bi-phasic excitation field gradient;

storing the received FID signal;

applying a second bi-phasic excitation field gradient to the gyromagnetic material;

applying a homogeneous transverse excitation field to the gyromagnetic material;

receiving the FID signal which is produced by the gyromagnetic material in response to the homogeneous transverse excitation field; and

storing the received FID signal.

5. The method as recited in claim 4 in which the bi-phasic excitation field gradient is applied to the gyromagnetic material by:

producing a first signal at the Larmor frequency for a preset time interval;

applying said first signal to a gradient coil;

producing a second signal at the Larmor frequency for the same preset time interval; and

applying said second signal to the gradient coil.

6. The method as recited in claim 5 in which the second signal is substantially 180 degrees out of phase with the first signal.

7. The method as recited in claim 4 in which the homogeneous transverse excitation field produces a 90 degree tip in the net magnetic moment of the gyromagnetic material.