Method of and device for determining the internal structure of a body by means of acoustic beams

• US 4,279,157 A
• Filed: 06/06/1979
• Issued: 07/21/1981
• Est. Priority Date: 06/22/1978
• Status: Expired due to Term

• Current Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Original Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Inventors: Schomberg, Hermann, Tasto, Manfred
• Primary Examiner(s): Kreitman, Stephen A.
• Application Number:
  US06/045,900
• Time in Patent Office: 776 Days
• Field of Search: 73/597, 73/599, 73/618, 73/620, 73/626, 73/606, 73/607, 128/660
• US Class Current: 73/618
• CPC Class Codes: G01H 3/125 for representing acoustic field distribution using optical means G01H9/002; sonar systems for imaging G01S7/56, G01S15/89; acoustic holography G03H3/00
• CPC Class Codes: G01H 5/00 Measuring propagation velocity of ultrasonic, sonic or infrasonic waves , e.g. of pressure waves
• CPC Class Codes: G01N 2291/0289 Internal structure, e.g. defects, grain size, texture
• CPC Class Codes: G01N 29/0672 by acoustic tomography medical tomography A61B8/13
• CPC Class Codes: G01S 15/8913 using separate transducers for transmission and reception

Abstract

A method and device for determining the internal structure of a body by means of acoustic beams. Transit times and intensities of acoustic beams passing through the body in different spatial directions are measured to establish the refractive index distribution and the acoustic absorption coefficient distribution, respectively at the points of a point matrix associated with the body. The non-rectilinear course of the acoustic beams is taken into account in this respect. This results in reconstructed images of higher quality.

Claims

1. In a method for determining the internal structure of a body comprising the steps of:

passing a plurality of acoustic beams through a body in different directions from one or more acoustic transmission elements to one or more separate acoustic reception elements;

measuring the value of the transit time of each of said beams through the body; and

utilizing the measured transit time values to calculate the value of the acoustic refractive index at points in a matrix associated with the body;

the improvement comprising the steps of;

first assuming a distribution of acoustic refractive index values at preselected points in the matrix, which approximate known body structure, said assumed distribution taking into account the geometry of the transmission and reception elements;

using said assumed distribution to calculate the path of each of said beams throught the body;

calculating an assumed transit time for each beam along the determined paths; and

then comparing the assumed transit time with the measured value of the transit time to generate step-wise corrections for the calculated value of the acoustic refractive index at points in the matrix.

2. The method of claim 1 wherein the assumed distribution of acoustic refractive index values is smoothed by forming a weighted mean value of neighboring acoustic refractive index values at points in the matrix.

3. A method as claimed in claim 1 further comprising the steps of:

measuring the intensity of the acoustic beams received by the reception elements;

utilizing the measured intensity to calculate the total absorption value for each of said beams;

determining a distribution of absorption coefficient values at points in the matrix from the calculated total absorption values;

calculating an assumed absorption value for each beam along the determined paths; and

then comparing the assumed absorption values with the calculated absorption values to generate step-wise corrections for the calculated value of the absorption coefficient at points in the matrix.

4. The method of any of claim 1 through 3 wherein the direction of the beams is changed by rotating the acoustic transmission elements and acoustic reception elements around a fixed axis.

5. The method of any of claim 1 through 3 wherein the direction of the acoustic beams is changed by activation of separate acoustic transmission elements and acoustic reception elements which are distributed around the body and whose position remains unchanged with respect to the body.

6. In a device for determining the internal structure of a body of the type comprising:

an acoustic converter disposed around the body which includes separate acoustic transmission elements and acoustic reception elements;

means for selectively activating the transmission and reception elements for the transmission and reception, respectively, of acoustic beams;

means for measuring the value of the transit time of the acoustic beams between the transmission elements and the reception elements; and

means for calculating the acoustic refractive index at points in a matrix which is associated with the body from the measure values of the transit time;

the improvement comprising;

means for determining the paths of the acoustic beams through the body on the basis of an assumed distribution of the values of the acoustic refractive index in the body and for determining theoretical transit time values for acoustic beams following those determined paths; and

means for comparing the measured transit time values with the theoretical transit time values and for correcting the calculated values of the acoustic refractive index at points in the matrix on the basis of the results of the comparison.

7. The device of claim 6 further comprising:

means for measuring the values of the intensity of acoustic beams received at the reception elements;

means for calculating absorption coefficients at points in the matrix on the basis of the measured intensity; and

means for calculating theoretical absorption values for the acoustic beams along the assumed beam paths, for comparing the calculated absorption values with the measured absorption values, and for correcting the calculated values of the absorption coefficients on the basis of the results of the comparison.

8. The device of claim 6 or 7 further comprising a tank which is rotatable about an axis and displaceable in the direction of the axis and wherein the acoustic converter comprises a flat acoustic matrix of transmission elements and a flat acoustic matrix of reception elements, said elements extending in columns and rows which are parallel and perpendicular, respectively, to the axis.

9. The device of claim 8 wherein the acoustic transmission element matrix comprises a single plate-shaped acoustic transmitter.

10. The device of claim 8 wherein the reception element matrix comprises a single plate-shaped acoustic receiver.

11. The device as claimed in claim 10 further comprising means for transmitting the acoustic beams from the acoustic transmission elements as focused acoustic beams by activating concentric circles of separate acoustic transmission elements and by displacing said circles along the rows and columns of the transmission element matrix.

12. The device as claimed in claim 8 wherein the acoustic receive matrix comprises a single plate-shaped acoustic receiver and the acoustic transmission element matrix comprises a row of several acoustic transmission elements.

13. A device as claimed in claim 8 wherein the acoustic transmission element matrix and the reception element matrix comprise a row of individual acoustic transmission elements and acoustic reception elements, respectively, said rows being displaceable in the direction of the axis.

14. A device as claimed in claims 6 or 7 comprising a tank which is rotatable around an axis and displaceable in the direction of the axis wherein the acoustic converter comprises a row of acoustic transmission elements, which are situated one above the other along the direction of the axis and which generate fan-shaped acoustic beams, and a two-dimensional matrix of acoustic reception elements having columns of elements which extend parallel to the direction of the axis and rows of elements which are at least partially curved around the axis.

15. A device as claimed in claim 6 or 7 comprising a tank which is rotatable around an axis and which is displaceable in the direction of the axis wherein the acoustic reception elements are disposed in a ring-like manner around the axis and are situated one above the other in the direction of the axis to form a hollow cylinder which surrounds the body to be examined and wherein the acoustic transmission elements are disposed in rings situated above and below the rings of acoustic reception elments.

16. A device as claimed in claim 15 wherein the acoustic transmission elements are situated within the ring of acoustic reception elements.

17. A device as claimed in claim 16 wherein the acoustic converter comprises a single ring of adjacently situated acoustic reception elements and separate acoustic transmission elements which are disposed between the reception elements and at a distance from each other, the acoustic converter being displaceable in the direction of the axis.