Apparatus for quantitative measurements of ultrasonic wave power distribution

• US 5,463,593 A
• Filed: 03/14/1994
• Issued: 10/31/1995
• Est. Priority Date: 03/14/1994
• Status: Expired due to Term

• Current Assignee: Claudio I. Zanelli
• Original Assignee: Claudio I Zanelli Intec Research Company
• Inventors: Whitehead, Frank R., Zanelli, Claudio I.
• Primary Examiner(s): PIHULIC, DANIEL T
• Application Number:
  US08/212,759
• Time in Patent Office: 596 Days
• Field of Search: 367/13, 73/1 DV
• US Class Current: 367/13
• CPC Class Codes: G01H 9/00 Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means

Abstract

A schlieren imaging system provides quantitative images suitable for testing medical equipment. One embodiment includes precision optics which form an image of a volume of a medium through which an ultrasonic acoustic wave propagates. A spatial filter passes diffracted light but blocks other light. A camera forms an image of the medium from the diffracted light so that regions of the medium which diffract light have higher light intensity in the image. From image intensities, a processor determines acoustic pressures or intensities, typically as a value indicating an integral of the acoustic pressure or intensity along an optical path through the volume. Integrated pressure is determined from a look-up table which relates predicted light intensity to pressure values which cause the predicted light intensity. The system is calibrated by forming an image of a reference ultrasonic acoustic wave and determining a relation between the image intensities and predicted intensities. The system may include a timing circuit which periodically activates and deactivates a transducer and causes emission of synchronized pulses of light. The pulses of light are synchronized with a selected delay after activations of the transducer, so that an image is formed which shows an ultrasonic acoustic wave that has evolved during the delay.

Claims

1. An apparatus for quantitatively measuring a characteristic of ultrasonic acoustic waves, comprising:

an immersion tank to contain a medium through which said ultrasonic waves are passed;

a source of substantially parallel light oriented with respect to said medium so that said substantially parallel light enters said medium along a first axis;

a spatial filter positioned to block a portion of light that emerges from said medium, wherein said portion of light blocked includes zero-th order diffracted light that emerges from said medium in a direction substantially parallel to said first axis;

a camera positioned to image said light emerging from said medium that is not blocked by said spatial filter; and

a quantitative analyzer coupled to said camera wherein said quantitative analyzer generates a quantitative measure of said characteristic of said ultrasonic waves passing through said medium.

2. The apparatus of claim 1, further comprising an optical system positioned between said immersion tank and said spatial filter so as to focus said light emerging from said medium.

3. The apparatus of claim 2, wherein said spatial filter is positioned in a plane where said optical system forms an image of said light emerging from said medium.

4. The apparatus of claim 3, wherein said spatial filter comprises a planar surface having an opaque region wherein said opaque region blocks said portion of said light emerging from said medium after said light emerging from said medium is focused by said optical system.

5. The apparatus of claim 4, wherein said opaque region comprises an opaque circular region.

6. The apparatus of claim 1, further comprising a timing circuit coupled to said source of substantially parallel light, wherein said timing circuit synchronizes pulses of light from said source of substantially parallel light with a user selected delay from activations of a transducer.

7. The apparatus of claim 6, wherein said user selected delay is constant.

8. The apparatus of claim 6, wherein said user selected delay varies in a user selected manner.

9. The apparatus of claim 6, wherein said timing circuit further comprises circuitry for periodically activating said transducer for a user selected time interval.

10. The apparatus of claim 1, wherein said characteristic of said ultrasonic waves is an integral of acoustic pressure along a path through said medium.

11. The apparatus of claim 10, wherein said quantitative analyzer further comprises a look-up table including a plurality of predicted light intensity values and an integrated pressure value for each of said plurality of predicted intensity values.

12. The apparatus of claim 1, wherein said characteristic of said ultrasonic waves is an integral of acoustic intensity along a path through said medium.

13. The apparatus of claim 1, wherein said characteristic of said ultrasonic waves is total acoustic power.

14. The apparatus of claim 1, wherein said characteristic of said ultrasonic waves is acoustic energy in a user selected section of said ultrasonic acoustic waves.

15. A schlieren imaging system, comprising:

a first optical system which provides light diffracted from pressure changes in a volume of a medium, wherein said pressure changes are caused by propagation of an ultrasonic acoustic wave;

a spatial filter positioned to receive said light from said first optical system, wherein said spatial filter blocks zero-th order diffracted light from said first optical system;

a second optical system positioned to receive unblocked light from said spatial filter, wherein said second optical system forms an image using said unblocked light;

an optical sensor positioned to receive said image, wherein said second optical system generates an array of light intensity values, each light intensity value indicating a light intensity for a region of said image; and

a quantitative analyzer coupled to received said array of light intensity values from said optical sensor, wherein said quantitative analyzer generates from said array of light intensity values an array of characteristic values which quantify a characteristic of said ultrasonic acoustic wave.

16. The schlieren imaging system of claim 15, wherein each characteristic value indicates an integral of acoustic pressure changes along a path through said volume of said medium.

17. The schlieren imaging system of claim 15, wherein each characteristic value indicates an integral of acoustic intensity along a path through said volume of said medium.

18. An apparatus for quantitatively measuring a characteristic of ultrasonic acoustic waves, comprising:

a collimating lens;

an approximate point light source located at a focal point of said collimating lens;

a tank which contains a medium through which said ultrasonic acoustic waves are passed, said tank including a first optical window and a second optical window, said first and said second optical windows being located on opposite walls of said tank so that light traversing said tank along a first axis enters through said first optical window and exits through said second optical window, said tank being positioned so that light emerging from said collimating lens along an optical axis of said collimating lens enter said first optical window along said first axis;

a converging lens positioned so that light emerging from said tank along said first axis enters said converging lens along an optical axis of said converging lens;

a spatial filter positioned to block light that enters said converging lens parallel to said optical axis of said converging lens;

an imaging lens positioned to form an image of a volume in said tank; and

a quantitative analyzer which converts said image into a quantitative measure of said characteristic of said ultrasonic waves passing through said medium.

19. The apparatus of claim 18, wherein said point source of light emits light has a bandwidth less than 200 nm.

20. The apparatus of claim 18, wherein said point source of light further comprises an optical filter which limits a bandwidth of light emitted by said point source of light.

21. The apparatus of claim 18, wherein said point source of light comprises a laser diode.

22. The apparatus of claim 18, wherein said first and said second optical windows have surfaces which variations that are no larger than λ

/10 where λ

is the average wavelength of light emitted from said point source of light.

23. The apparatus of claim 22, wherein said point source of light emits light having a bandwidth less than 200 nm.

24. The apparatus of claim 18, further comprising:

a transducer pulser;

a variable delay circuit coupled to the transducer pulser; and

a light pulser coupled to the variable delay circuit and to the point light source.

25. The apparatus of claim 18, wherein the converging and diverging lenses are identical and have a diameter greater than 5 cm.

26. A method for providing a quantitative image of an ultrasonic acoustic wave, comprising the steps of:

generating a light beam that travels along a first direction through a medium;

generating a first ultrasonic acoustic wave which propagates through said medium;

spatially filtering light exiting from said medium, wherein said spatial filtering blocks light that exits said medium along said first direction and transmits light diffracted by a pressure change caused in said medium by said first ultrasonic acoustic wave, wherein said light transmitted is at one or more non-zero angles relative to said first direction;

forming a first image of said medium from said light transmitted during spatial filtering;

measuring a first light intensity value for a region in said first image; and

generating from said first light intensity value a quantitative value characteristic of a property of said ultrasonic acoustic wave.

27. The method of claim 26, further comprising the steps of:

generating a second ultrasonic acoustic wave which propagates through said medium, wherein said second ultrasonic acoustic wave has a known power distribution;

forming a second image of said medium using light diffracted by pressure change caused in said medium by said second ultrasonic acoustic wave;

measuring a second light intensity value for a region in said second image; and

determining a constant which relates said second light intensity value to a predicted light intensity value which was predicted based on said known power distribution of said second ultrasonic acoustic wave.

28. The method of claim 27, wherein the step of generating a value characteristic of a property of said ultrasonic acoustic wave further comprises the steps of:

providing a look-up table which relates each of a plurality of pressure values to a correspond predicted light intensity values;

normalizing said first light intensity value according to said constant;

matching said normalized first light intensity value with a predicted light intensity value in said look-up table; and

identifying a pressure value in said look-up table which corresponds to the predicted light intensity value matched with said normalized first intensity value.

29. The method of claim 26, further comprising the steps of:

generating a second ultrasonic acoustic wave which propagates through said medium, wherein said second ultrasonic acoustic wave has a known power;

forming a second image of said medium using light diffracted by pressure change caused by said second ultrasonic acoustic wave;

measuring a set of light intensity values for a region extending across said second image; and

determining a constant which relates a sum of said set of light intensity values to said known power of said second ultrasonic acoustic wave.

30. The method of claim 29, wherein the step of generating a value characteristic of a property of said ultrasonic acoustic wave further comprises the step of generating an acoustic intensity value indicating an integral of acoustic intensity along a path through said ultrasonic acoustic wave, wherein said intensity value equals the product of said first light intensity value by said constant.