Technique for eliminating ambiguity when making pulse-echo timing measurements

• US 6,009,380 A
• Filed: 09/10/1997
• Issued: 12/28/1999
• Est. Priority Date: 05/03/1996
• Status: Expired due to Fees

• Current Assignee: Ultrafast, Inc.
• Original Assignee: Ultrafast, Inc.
• Inventors: Kotas, Donald E., Kibblewhite, Ian E., Vecchio, Christopher J.
• Primary Examiner(s): ASSOUAD, PATRICK J
• Application Number:
  US08/968,459
• Time in Patent Office: 839 Days
• Field of Search: 702/142, 702/143, 702/149, 702/189, 73/597, 73/589, 73/570, 73/579, 73/627, 73/629, 73/760, 73/761, 73/615, 367/87, 367/99
• US Class Current: 702/142
• CPC Class Codes: G01H 5/00 Measuring propagation velocity of ultrasonic, sonic or infrasonic waves , e.g. of pressure waves
• CPC Class Codes: G01L 5/246 using acoustic waves
• CPC Class Codes: G01N 2291/02827 Elastic parameters, strength or force
• CPC Class Codes: G01N 2291/044 Internal reflections (echoes), e.g. on walls or defects
• CPC Class Codes: G01N 2291/2691 Bolts, screws, heads
• CPC Class Codes: G01N 29/07 by measuring propagation velocity or propagation time of acoustic waves
• CPC Class Codes: G01N 29/348 with frequency characteristics, e.g. single frequency signals, chirp signals measuring frequency of mechanical vibrations or acoustic waves in general G01H1/06, G01H3/04; measuring frequency or analysing frequency spectra G01R23/00

Abstract

A method of measuring in a material a time-of flight of a signal having a first signal burst and a second signal burst, the first signal burst having a first set of cycles and the second signal burst having a second set of cycles. The method includes identifying a cycle in the second signal burst corresponding to a cycle in the first signal burst, to measure the time-of-flight of the signal.

Claims

1. A method of measuring in a material a time-of flight of a signal, said method comprising:

(a) transmitting into the material a signal having a predetermined fixed frequency, said signal having a first signal burst and a second signal burst, and said first signal burst having a first set of cycles and said second signal burst having a second set of cycles;

(b) identifying a cycle in said second set of cycles in said second signal burst corresponding to a cycle in said first set of cycles in said first signal burst; and

(c) subtracting the time-of-flight of said identified cycle in said first signal burst from the time-of-flight of said identified cycle in said second signal burst, to measure the time-of-flight of the signal.

3. A method according to claim 1, wherein said step of identifying corresponding cycles on said first signal burst and said second signal burst comprises the steps of:

(a) applying to the material a first signal having a first signal burst and a second signal burst, wherein said first signal burst has a first set of cycles and said second signal burst has a second set of cycles corresponding to said first set of cycles and said first signal has a first frequency;

(b) collecting a first set of times-of-fight, relative to an arbitrary point in time, for each cycle of said first set of cycles of said first signal burst and each cycle from said second set of corresponding cycles of said second signal burst;

(c) calculating first difference absolute values between said times-of-flight of each cycle in said first set of cycles in said first signal burst and each cycle in said second set of corresponding cycles in said second signal burst;

(d) applying to the material a second signal having a third signal burst and a fourth signal burst, wherein said third signal burst has a third set of cycles and said fourth signal burst has a fourth set of cycles corresponding to said third set of cycles and wherein said second signal has a second frequency;

(e) collecting a second set of times-of-flight, relative to an arbitrary point in time, for each cycle in said third set of cycles of said third signal burst and each cycle in said fourth set of cycles of said fourth signal burst;

(f) calculating second difference absolute values between said times-of-flight of each cycle in said third set of cycles of said third signal burst and each cycle in said fourth set of cycles of said fourth signal burst;

(g) calculating third difference absolute values between said first difference absolute values and said second difference absolute values;

(h) matching identical and similar third difference values; and

(i) identifying the third difference value closest to a predetermined value.

4. A method according to claim 1, wherein said step of identifying corresponding cycles on said first signal burst and said second signal burst comprises the steps of:

(a) applying to the material a first signal, said first signal having a first portion at a first frequency and a second portion at a second frequency different from said first frequency;

(b) aligning a first zero crossing of one cycle of said first signal burst and a second zero crossing of one cycle of said second signal burst;

(c) calculating the absolute values of the differences in time of the zero crossings for each cycle from a first set of remaining cycles of said first signal burst and each cycle from a corresponding second set of remaining cycles of said second signal burst;

(d) summing the absolute values of said differences;

(e) successively shifting said second signal burst one cycle is forward and one cycle backward relative to said alignment of said first zero crossing of one cycle of said first signal burst and said second zero crossing of said second signal burst; and

(f) repeating steps (b)-(e) until the lowest cumulative zero crossing time difference of said differences is identified.

5. The method according to claim 4, wherein said first signal is transmitted and received with a transducer selected from the group consisting of piezoelectric and electromagnetic transducers.

6. The method according to claim 4, wherein said first signal is transmitted and received with a laser.

7. The method according to claim 5, wherein said second frequency is a resonant frequency of said transducer.

22. A method according to claim 1, wherein said signal is an ultrasonic wave.

24. A method according to claim 1, wherein said signal is transmitted with an ultrasonic signal transmitting means selected from the group consisting of piezoelectric and electromagnetic transducers.

2. A method of measuring in a material a time-of-flight of a first signal through the material using a second signal, said method comprising:

(a) measuring times-of-flight of said first signal having a first predetermined fixed frequency and said second signal having a second predetermined fixed frequency different from said first predetermined fixed frequency; and

(b) identifying times-of-flight in said first signal and said second signal which are independent of frequency.

23. A method according to claim 2, wherein said first and second signals are ultrasonic waves.

25. A method according to claim 2, wherein said first and second signals are transmitted with an ultrasonic signal transmitting means selected from the group consisting of piezoelectric and electromagnetic transducers.

8. A method of measuring the time-of-flight of a signal in a material, said method comprising the steps of:

(a) transmitting a signal burst into the material with an ultrasonic signal transmitting means, said signal burst having a first portion at a first predetermined fixed frequency and a second portion at a second predetermined fixed frequency different from said first predetermined fixed frequency, and a first set of cycles;

(b) receiving a signal burst having a second set of cycles from the material;

(c) identifying one of said received signal burst cycles corresponding to one of said transmitted signal burst cycles; and

(d) calculating said time-of-flight by subtracting the time of said transmitted signal burst cycle from the time of said corresponding received signal burst cycle.

9. A method according to claim 8, wherein said signal is an ultrasonic wave.

10. A method according to claim 9, wherein said time-of-flight measurements are made in a load-bearing member and used to determine a measure of load on said load-bearing member.

11. A method according to claim 8, wherein said step of identifying said received signal burst cycle corresponding to said transmitted signal burst cycle comprises the steps of:

(a) determining the times of the zero crossings of said transmitted signal burst cycles;

(b) measuring the times of the zero crossings of said received signal burst cycles;

(c) applying a correlation technique to match the zero crossings of said received signal burst with the zero crossings of said transmitted signal burst.

12. A method according to claim 11, wherein said correlation technique comprises:

(a) aligning a first zero crossing of one cycle from a first set of cycles of said transmitted signal burst and a second zero crossing of one cycle from a second set of cycles of said received signal burst, said second set of cycles corresponding to said first set of cycles;

(b) calculating absolute values of the differences in the time of the zero crossings for each remaining cycle of said first set of cycles of said transmitted signal burst and each remaining cycle of said second set of corresponding cycles of said received signal burst;

(c) summing said absolute values of said differences;

(d) successively shifting said received signal burst one cycle forward and one cycle backward relative to said alignment of said first zero crossing of one cycle of said transmitted signal burst and said second zero crossing of said received signal burst; and

(e) repeating steps (a)-(d) until a lowest cumulative zero crossing time difference of said differences is identified.

13. A method according to claim 8, wherein said second frequency of said second portion of said transmitted signal burst is a natural resonant frequency of said signal transmitting means.

14. A method according to claim 8, wherein said signal transmitting means is a transducer selected from the group consisting of piezoelectric and electromagnetic transducers.

15. A method according to claim 8, wherein said signal transmitting means is a laser.

16. A method of independently measuring the times-of-flight of a longitudinal ultrasonic wave and a transverse ultrasonic wave in a material, said method comprising:

(a) transmitting into the material said longitudinal and transverse ultrasonic waves at at least two different frequencies with one ultrasonic transmitting means,

(b) measuring the time-of-flight of said longitudinal ultrasonic wave with a first signal at a first predetermined fixed frequency, and

(c) measuring the time-of-flight of said transverse ultrasonic wave with a second signal at a second predetermined fixed frequency.

17. A method according to claim 16, wherein said time-of-flight measurements are made in a load-bearing member and used to determine a measure of load on said load bearing member.

18. A method according to claim 16, wherein said first frequency and said second frequency are chosen such that a wavelength of said longitudinal ultrasonic wave in the material produced by said first frequency is approximately equal to a wavelength of said transverse ultrasonic wave in the material produced by said second frequency.

19. A method according to claim 16, wherein said first frequency is chosen to be approximately a longitudinal wave resonant frequency of said transmitting means and said second frequency is chosen to be approximately a transverse wave resonant frequency of said transmitting means.

20. A method according to claim 16, wherein said ultrasonic signal transmitting means is selected from the group consisting of piezoelectric and electromagnetic transducers.

21. A method according to claim 16, wherein said ultrasonic signal transmitting means is a laser.

26. A method of measuring in a material a time-of flight of a signal, said method comprising:

(a) transmitting a signal having a first signal burst and a second signal burst into the material, said first signal burst having a first set of cycles and said second signal burst having a second set of cycles;

(b) identifying a cycle in said second set of cycles in said second signal burst corresponding to a cycle in said first set of cycles in said first signal burst; and

(c) subtracting the time-of-flight of said identified cycle in said first signal burst from the time-of-flight of said identified cycle in said second signal burst, to measure the time-of-flight of the signal,

wherein said step of identifying corresponding cycles on said first signal burst and said second signal burst comprises the steps of;

(d) applying to the material a first signal having a first signal burst and a second signal burst, and said first signal burst has a first set of cycles and said second signal burst has a second set of cycles corresponding to said first set of cycles and said first signal has a first frequency;

(e) collecting a first set of times-of-flight, relative to an arbitrary point in time,, for each cycle of said first set of cycles of said first signal burst and each cycle from said second set of corresponding cycles of said second signal burst;

(f) calculating first difference absolute values between said times-of-flight of each cycle in said first set of cycles in said first signal burst and each cycle in said second set of corresponding cycles in said second signal burst;

(g) applying to the material a second signal having a third signal burst and a fourth signal burst, wherein said third signal burst has a third set of cycles and said fourth signal burst has a fourth set of cycles corresponding to said third set of cycles and said second signal has a second frequency;

(h) collecting a second set of times-of-flight, relative to an arbitrary point in time, for each cycle in said third set of cycles of said third signal burst and each cycle in said fourth set of cycles of said fourth signal burst;

(i) calculating second difference absolute values between said times-of-flight of each cycle in said third set of cycles of said third signal burst and each cycle in said fourth set of cycles of said fourth signal burst;

(j) calculating third difference absolute values between said first difference absolute values and said second difference absolute values;

(k) matching identical and similar third difference values; and

(l) identifying the third difference values closest to a predetermined value.

27. A method of measuring in a material a time-of flight of a signal, said method comprising:

(a) transmitting a signal having a first signal burst and a second signal burst into the material, said first signal burst having a first set of cycles and said second signal burst having a second set of cycles;

(b) identifying a cycle in said second set of cycles in said second signal burst corresponding to a cycle in said first set of cycles in said first signal burst; and

(c) subtracting the time-of-flight of said identified cycle in said first signal burst from the time-of-flight of said identified cycle in said second signal burst, to measure the time-of-flight of the signal,

wherein said step of identifying corresponding cycles on said first signal burst and said second signal burst comprises the steps of;

(d) applying to the material a first signal, said first signal having a first portion at a first frequency and a second portion at a second frequency different from said first frequency;

(e) aligning a first zero crossing of one cycle of said first signal burst and a second zero crossing of one cycle of said second signal burst;

(f) calculating the absolute values of the differences in time of the zero crossings for each cycle from a first set of remaining cycles of said first signal burst and each cycle from a corresponding second set of remaining cycles of said second signal burst;

(g) summing the absolute values of said differences;

(h) successively shifting said second signal burst one cycle forward and one cycle backward relative to said alignment of said first zero crossing of one cycle of said first signal burst and said second zero crossing of said second signal burst; and

(i) repeating steps (e)-(h) until the lowest cumulative zero crossing time difference of said differences is identified.

28. A method according to claim 27, wherein said first signal is transmitted and received with a transducer selected from the group consisting of piezoelectric and electromagnetic transducers.

29. A method according to claim 27, wherein said first signal is transmitted and received with a laser.

30. A method according to claim 28, wherein said second frequency is a resonant frequency of said transducer.