Acoustic imaging device

• US 5,435,312 A
• Filed: 04/25/1994
• Issued: 07/25/1995
• Est. Priority Date: 05/31/1991
• Status: Expired due to Fees

• Current Assignee: Thermotrex Corporation (Thermo Fisher Scientific Incorporated)
• Original Assignee: Thermotrex Corporation (Thermo Fisher Scientific Incorporated)
• Inventors: Martin, Peter I., Otto, Greg, Palmer, Douglas A., Spivey, Brett A.
• Primary Examiner(s): JAWORSKI, FRANCIS J
• Application Number:
  US08/232,741
• Time in Patent Office: 456 Days
• Field of Search: 128/660.01, 128/660.07, 128/661.02, 128/916, 73/602, 364/413.25, 367/103
• US Class Current: 600/448
• CPC Class Codes: A61B 8/13 Tomography A61B8/10, A61B8/12 take precedence; tomography for radiation diagnosis A61B6/02
• CPC Class Codes: A61B 8/463 characterised by displaying multiple images or images and diagnostic data on one display composite display in devices for short-range imaging with acoustic waves G01S7/52074

Abstract

This invention provides an acoustic imaging device which utilizes scattered acoustic wave information to produce an image. The system consists of an array of acoustic transducers which at least partially encircle a medium to be imaged. The medium is sequentially insonified by each transducer with an acoustic signal comprised of at least one discrete frequency. The acoustic signal scatters from the medium and is detected by the remaining transducers. A data set representing the phase and amplitude of each discrete frequency at each transducer is acquired and used by a computer to calculate an image of the medium. Images acquired and calculated at each identifiable discrete frequency are combined in various ways in order to improve the quality of the final image of the medium.

Claims

1. An acoustic imaging device for providing an image of at least a portion of a medium comprising:

A) an acoustic broadcasting means for broadcasting into said medium acoustic signals from at least seven broadcast locations on a circle at least partially surrounding said medium, one location at a time said acoustic signals being at least one discrete frequency and continuous for a period of time equal to at least the travel time of said acoustic signal across said medium,

B) an acoustic signal detection means for detecting, at a plurality of detection locations on said circle at least partially surrounding said medium, acoustic signals broadcast by said broadcasting means,

C) a data collection and comparison means for comparing signals received to said signals broadcast in order to provide with respect to each of said plurality of locations a set of data representing the phases and amplitudes of acoustic signals received at said plurality of locations relative to the phase and amplitude of said signals broadcast from said at least seven locations, and

D) a computing means for mathematically constructing at least one image of at least a portion of said medium utilizing said phase and amplitude data said computing means being programmed to accomplish the following steps;

1) transform said phase and amplitude data into a set of data defining an azimuthal data set in an azimuthal mode space said set of data representing azimuthal modes at the location of said broadcasting means and said detection means,

2) modify said azimuthal data set to account for transducer antenna patterns to produce an antenna independent azimuthal data set, and

3) multiply said antenna independent azimuthal data set by weighting function calculated at a large number of locations in said medium and sum over said azimuthal modes to produce a convolved image of said medium, and

4) deconvolved said convolved image of said medium to produce said image of said medium.

2. An acoustic imaging device as in claim 1 wherein said computing means is programmed to accomplish the additional step of sequentially accomplishing steps A-D at a plurality of discrete frequencies so as to construct a plurality of single frequency complex images.

3. An acoustic imaging device as in claim 2 wherein said computing means is programmed to accomplish the additional step of summing said plurality of single frequency complex images to produce a combined complex image.

4. An acoustic imaging device as in claim 2 wherein said computing means is programmed to accomplish the additional step of summing the magnitudes of said plurality of single frequency complex images to produce a combined image.

5. An acoustic imaging system as in claim 2 wherein said computing means is programmed to accomplish the following additional steps:

A) utilize said plurality of single frequency complex images to construct a set of time data representing a synthesized acoustic pulse which sequentially focuses at said large number of locations in said medium, and

B) utilizing said set of time data, calculate an image of said medium.

6. An acoustic imaging system as in claim 5 wherein said computing means is programmed to utilize said set of time data to determine the time-of-arrival data of said synthesized acoustic pulse from said broadcast locations to said large number of locations within said medium and then to said detection locations said time-of-arrival data forming a time-of-arrival image.

7. An acoustic imaging system as in claim 6 wherein said computer means is programmed to accomplish the additional step of deconvolving a function of said time-of-arrival image to produce a sound speed image.

8. An acoustic imaging device as in claim 7 wherein said function is the diameter of said circle divided by said time-of-arrival image.

9. An acoustic imaging system as in claim 6 wherein said computing means is programmed to accomplish the following additional steps:

A) convolve each said single frequency complex image to produce a plurality of convolved single frequency complex images,

B) multiply each said convolved single frequency complex image by an exponential function of said time-of-arrival image to produce a plurality of phase aberration corrected convolved single frequency complex images,

C) sum said plurality of phase aberration corrected convolved single frequency complex images to produce a phase aberration corrected convolved complex image, and

D) deconvolve said phase aberration corrected convolved complex image to produce a phase aberration corrected complex image.

10. An acoustic imaging device as in claim 9 wherein said computing means is programmed to accomplish the additional step of calculating the magnitude of said phase aberration corrected complex image to produce a phase aberration corrected image.

11. An acoustic imaging system as in claim 9 wherein said computing means is programmed to accomplish the following additional steps:

A) sum a function of the logarithm of said convolved phase aberration corrected complex image with said time-of-arrival image to produce a convolved composite image, and

B) deconvolve said convolved composite image to produce a composite image.

12. An acoustic imaging system as in claim 5 wherein said computing means is programmed to utilize said set of time data to determine the maximum pulse power data of said synthesized acoustic pulse from said broadcast locations to said large number of locations within said medium and then to said detection locations said maximum pulse power data forming a peak pulse power image.

13. An acoustic imaging system as in claim 12 wherein said computing means is programmed to accomplish the additional steps of a function of said maximum pulse power image to produce an attenuation image.

14. An acoustic imaging device as in claim 13 wherein said function is the logarithm of said maximum pulse power image divided by the diameter of said circle.

15. An acoustic imaging system as in claim 2 wherein said computing means is programmed to accomplish the following additional steps:

A) utilize said plurality of single frequency complex images to construct a set of time data representing a synthesized acoustic pulse which sequentially focuses at said large number of locations in said medium,

B) calculate refined set of time data from said set of time data by summing contributions to said synthesized acoustic pulse from said azimuthal modes numerically close to said azimuthal mode data set, and

C) utilizing said refined set of time data, calculate an image.

16. An acoustic imaging system as in claim 15 wherein said computing means is programmed to utilize said refined set of time data to determine the refined time-of-arrival data of said synthesized acoustic pulse from said broadcast locations to said large number of locations within said medium and then to said detection locations said refined time-of-arrival data forming a refined time-of-arrival image.

17. An acoustic imaging system as in claim 16 wherein said computing means is programmed to accomplish the additional step of deconvolving a function of said refined time-of-arrival image to produce a refined sound speed image.

18. An acoustic imaging device as in claim 17 wherein said function is the diameter of said circle divided by said refined time-of-arrival image.

19. An acoustic imaging system as in claim 16 wherein said computing means is programmed to accomplish the following additional steps:

A) convolve each said single frequency complex image to produce a plurality of convolved single frequency complex images,

B) multiply each said convolved single frequency complex image by an exponential function of said refined time-of-arrival image to produce a plurality of refined phase aberration corrected convolved single frequency complex images,

C) sum said plurality of refined phase aberration corrected convolved single frequency complex images to produce a refined phase aberration corrected convolved complex image, and

D) deconvolve said refined phase aberration corrected convolved complex image to produce a refined phase aberration corrected complex image.

20. An acoustic imaging device as in claim 19 wherein said computing means is programmed to accomplish the additional step of calculating the magnitude of said refined phase aberration corrected complex image to produce a refined phase aberration corrected image.

21. An acoustic imaging system as in claim 19 wherein said computing means is programmed to accomplish the following additional steps:

A) sum a function of the logarithm of said refined convolved phase aberration corrected complex image with said refined time-of-arrival image to produce a refined convolved composite image, and

B) deconvolve said refined convolved composite image to produce a refined composite image.

22. An acoustic imaging system as in claim 15 wherein said computing means is programmed to utilize said refined set of time data to determine the refined maximum pulse power data of said synthesized acoustic pulse from said broadcast locations to said large number of locations within said medium and then to said detection locations said refined maximum pulse power data forming a refined peak pulse power image.

23. An acoustic imaging system as in claim 22 wherein said computing means is programmed to accomplish the additional steps of deconvolving a function of said refined maximum pulse power image to produce a refined attenuation image.

24. An acoustic imaging device as in claim 23 wherein said function is the logarithm of said refined maximum pulse power image divided by the diameter of said circle.

25. An acoustic imaging device as in claim 1 wherein said at least discrete frequency is a plurality of discrete frequencies.

26. An acoustic imaging device as in claim 25 wherein said computing means is programmed to accomplish steps 1-4 with respect to said plurality of identifiable discrete frequencies so as to construct a plurality of single frequency complex images.

27. An acoustic imaging device as in claim 26 wherein said computing means is programmed to accomplish the additional step of summing said plurality of single frequency complex images to produce a combined complex image.

28. An acoustic imaging device as in claim 26 wherein said computing means is programmed to accomplish the additional step of summing the magnitudes of said plurality of single frequency complex images to produce a combined image.

29. An acoustic imaging system as in claim 26 wherein said computing means is programmed to accomplish the following additional steps:

A) utilize said plurality of single frequency complex images to construct a set of time data representing a synthesized acoustic pulse which sequentially focuses at said large number of locations in said medium, and

B) utilizing said set of time data, calculate an image.

30. An acoustic imaging system as in claim 29 wherein said computing means is programmed to utilize said set of time data to determine the time-of-arrival data of said synthesized acoustic pulse from said broadcast locations to said large number of locations within said medium and then to said detection locations said time-of-arrival data forming a time-of-arrival image.

31. An acoustic imaging system as in claim 30 wherein said computer means is programmed to accomplish the additional step of deconvolving a function of said time-of-arrival image to produce a sound speed image.

32. An acoustic imaging device as in claim 31 wherein said function is the diameter of said circle divided by said time-of-arrival image.

33. An acoustic imaging system as in claim 29 wherein said computing means is programmed to utilize said set of time data to determine the maximum pulse power data of said synthesized acoustic pulse from said broadcast locations to said large number of locations within said medium and then to said detection locations said maximum pulse power data forming a peak pulse power image.

34. An acoustic imaging system as in claim 33 wherein said computing means is programmed to accomplish the additional steps of deconvolving a function of said maximum pulse power image to produce an attenuation image.

35. An acoustic imaging device as in claim 34 wherein said function is the logarithm of said maximum pulse power image divided by the diameter of said circle.

36. An acoustic imaging system as in claim 26 wherein said computing means is programmed to accomplish the following additional steps:

A) utilize said plurality of single frequency complex images to construct a set of time data representing a synthesized acoustic pulse which sequentially focuses at said large number of locations in said medium,

B) calculate refined set of time data from said set of time data by summing contributions to said synthesized acoustic pulse from said azimuthal modes numerically close to said azimuthal mode data set, and

C) utilizing said refined set of time data, calculate an image of said medium.

37. An acoustic imaging system as in claim 36 wherein said computing means is programmed to utilize said refined set of time data to determine the refined time-of-arrival data of said synthesized acoustic pulse from said broadcast locations to said large number of locations within said medium and then to said detection locations said refined time-of-arrival data forming a refined time-of-arrival image.

38. An acoustic imaging system as in claim 37 wherein said computing means is programmed to accomplish the additional step of deconvolving a function of said refined time-of-arrival image to produce a refined sound speed image.

39. An acoustic imaging device as in claim 38 wherein said function is the diameter of said circle divided by said time-of-arrival image.

40. An acoustic imaging system as in claim 37 wherein said computing means is programmed to accomplish the following additional steps:

A) convolve each said single frequency complex image to produce a plurality of convolved single frequency complex images,

B) multiply each said convolved single frequency complex image by an exponential function of said refined time-of-arrival image to produce a plurality of refined phase aberration corrected convolved single frequency complex images,

C) sum said plurality of refined phase aberration corrected convolved single frequency complex images to produce a refined phase aberration corrected convolved complex image, and

D) deconvolve said refined phase aberration corrected convolved complex image to produce a refined phase aberration corrected complex image.

41. An acoustic imaging system as in claim 45 wherein said computing means is programmed to accomplish the following additional steps:

A) sum a function of the logarithm of said refined convolved phase aberration corrected complex image with said refined time-of-arrival image to produce a refined convolved composite image, and

B) deconvolve said refined convolved composite image to produce a refined composite image.

42. An acoustic imaging system as in claim 36 wherein said computing means is programmed to utilize said refined set of time data to determine the refined maximum pulse power data of said synthesized acoustic pulse from said broadcast locations to said large number of locations within said medium and then to said detection locations said refined maximum pulse power data forming a refined peak pulse power image.

43. An acoustic imaging system as in claim 42 wherein said computing means is programmed to accomplish the additional steps of deconvolving a function of said refined maximum pulse power image to produce a refined attenuation image.

44. An acoustic imaging device as in claim 43 wherein said function is the logarithm of said maximum pulse power image divided by the diameter of said circle.

45. An acoustic imaging system as in claim 36 wherein said computing means is programmed to accomplish the following additional steps:

A) convolve each said single frequency complex image to produce a plurality of convolved single frequency complex images,

B) multiply each said convolved single frequency complex image by an exponential function of said time-of-arrival image to produce a plurality of phase aberration corrected convolved single frequency complex images,

C) sum said plurality of phase aberration corrected convolved single frequency complex images to produce a phase aberration corrected convolved complex image, and

D) deconvolve said phase aberration corrected convolved complex image to produce a phase aberration corrected complex image.

46. An acoustic imaging device as in claim 45 wherein said computing means is programmed to accomplish the additional step of calculating the magnitude of said phase aberration corrected complex image to produce a phase aberration corrected image.

47. An acoustic imaging device as in claim 45 wherein said computing means is programmed to accomplish the additional step of calculating the magnitude of the refined phase aberration corrected complex image to produce a refined phase aberration corrected image.

48. An acoustic imaging system as in claim 45 wherein said computing means is programmed to accomplish the following additional steps:

A) sum a function of the logarithm of said convolved phase aberration corrected complex image with said time-of-arrival image to produce a convolved composite image, and

B) deconvolve said convolved composite image to produce a composite image.