Ultrasonic method and device for detecting and measuring defects in metal media

• US 4,658,649 A
• Filed: 06/06/1985
• Issued: 04/21/1987
• Est. Priority Date: 06/06/1985
• Status: Expired due to Fees

• Current Assignee: Combustion Engineering Incorporated (ABB Limited)
• Original Assignee: Combustion Engineering Incorporated (ABB Limited)
• Inventors: Brook, Mark V.
• Primary Examiner(s): NOT, DEFINED
• Application Number:
  US06/741,699
• Time in Patent Office: 684 Days
• Field of Search: 73/624, 73/628, 73/641, 73/642, 73/610, 73/612, 73/597, 73/598, 73/622, 73/637
• US Class Current: 73/624
• CPC Class Codes: G01N 2291/011 Velocity or travel time
• CPC Class Codes: G01N 2291/0234 Metals, e.g. steel
• CPC Class Codes: G01N 2291/0421 Longitudinal waves
• CPC Class Codes: G01N 2291/0422 Shear waves, transverse waves, horizontally polarised waves
• CPC Class Codes: G01N 2291/0428 Mode conversion
• CPC Class Codes: G01N 2291/044 Internal reflections (echoes), e.g. on walls or defects
• CPC Class Codes: G01N 2291/056 Angular incidence, angular propagation
• CPC Class Codes: G01N 2291/102 one emitter, one receiver
• CPC Class Codes: G01N 2291/2632 flat
• CPC Class Codes: G01N 2291/2634 cylindrical from outside
• CPC Class Codes: G01N 29/0618 synchronised with scanning, e.g. in real-time
• CPC Class Codes: G01N 29/07 by measuring propagation velocity or propagation time of acoustic waves
• CPC Class Codes: G01N 29/11 by measuring attenuation of acoustic waves
• CPC Class Codes: G01N 29/2487 Directing probes, e.g. angle probes directing arrangements G01N29/221
• CPC Class Codes: G01N 29/32 Arrangements for suppressing undesired influences, e.g. temperature or pressure variations , compensating for signal noise
• CPC Class Codes: G01N 29/46 by spectral analysis, e.g. Fourier analysis or wavelet analysis spectral signal processing per se G06F17/14

Abstract

An non-destructive testing method employs an ultrasound generator which provides a beam having an axis which intersects the outer surface of an object to be tested at an angle relative to a line normal to the surface which is in the range of 23° to 28°. A longitudinal mode wave and a shear mode wave are propogated within the object and the shear wave is converted into longitudinal mode waves by reflection from an opposite surface of the object. The propogated and mode converted waves are reflected from different portions of a defect and the echos arrive serially in time at a receiver transducer. The ultrasound generator and receiver transducer are sonically isolated. The received signals have a favorable signal-to-noise ratio and the times of receipt thereof are employed to determine the dimensions of a detected defect.

Claims

1. A method for the measurement of abnormalities in a solid test object having opposed surfaces comprising the steps of:

intermittently transmitting a beam of ultrasonic energy from a first location so as to cause the axis of said beam to intercept a first surface of a test object at an angle in the range of 23°

to 28°

relative to a line normal to said first surface to thereby propogate a shear mode wave and a first longitudinal mode wave in said object, said waves having substantially equal amplitudes;

reflecting said shear mode wave at a second surface of said body which is disposed generally opposite to said first surface to convert a portion of the energy comprising said shear mode wave to a second longitudinal mode wave;

serially receiving echos of said propogated first and said second longitudinal mode waves as reflected from an abnormality within the test object, said echos being received at a second location on the test object first surface which is spaced from said first location, said echos being refracted at said first surface;

acoustically isolating said trasmitted beam prior to interception of the first surface of the test object thereby from said echos subsequent to refraction thereof;

measuring the time delay transmission of a pulse of ultrasonic energy which comprises the intermittently transmitted beam and receipt of the echo commensurate with the reflection of the propogated first longitudinal wave from the abnormality; and

comparing the measured time delay with previously recorded data of time delay vrs. abonormality size to determine the distance from the test object first surface to the beginning of the abnormality.

2. The method of claim 1 wherein the steps of transmitting and receiving each include spacing a piezoelectric crystal from the first surface of the test object.

3. The method of claim 2 wherein the receiving piezoelectric crystal defines an axis which is oriented at an angle in the range of 12°

to 28°

relative to a line normal to the first surface of the object.

4. The method of claim 3 wherein the test object is a tubular member having substantially parallel inner and outer wall surfaces and wherein said first surface is the outer wall surface of the tubular member.

5. The method of claim 4 wherein the steps of spacing include mounting the piezoelectric crystals on members comprised of a material having low acoustic attenuation characteristics and coupling ultrasound energy to and from the crystals via the members.

6. The method of claim 3 wherein the steps of spacing include mounting the piezoelectric crystals on members comprised of a material having low acoustic attenuation characteristics and coupling ultrasound energy to and from the crystals via the members.

7. The method of claim 6 wherein the step of isolating includes positioning a sound insulator between the spacer members.

8. The method of claim 7 wherein the step of isolating includes positioning a sound insulator between the spacer members.

9. The method of claim 1 wherein the step of measuring includes detecting signals commensurate with echos produced upon reflection from the abnormality of said second longitudinal mode wave and employing such detected signals as a verification of the presence of the abnormality.

10. The method of claim 9 wherein the test object is a hollow member having substantially parallel inner and outer wall surfaces and wherein said first surface is the outer wall surface of the hollow member.

11. The method of claim 10 wherein the abnormality is a crack originating at the inner wall surface and wherein the propogated longitudinal mode wave is reflected from the tip of the crack and is the first serially received echo.

12. The method of claim 11 wherein the steps of transmitting and receiving each include spacing a piezoelectric crystal from the outer wall surface of the hollow member.

13. The method of claim 12 wherein the receiving piezoelectric crystal defines an axis which is oriented at an angle in the range of 12°

to 28°

relative to a line normal to the outer wall surface of the hollow member.

14. The method of claim 13 wherein the steps of spacing include mounting the piezoelectric crystals on members comprised of a material having low acoustic attenuation characteristics.

15. The method of claim 14 wherein the step of isolating includes positioning a sound insulator between the spacer members.

16. The method of claim 9 wherein the shear mode wave reflected from the second surface of the test object comprises said second longitudinal mode wave and a third mode converted wave which follows the second surface and wherein said method further comprises the steps of:

detecting signals commensurate with echos produced upon reflection from the abnormality of the third mode converted wave;

determining the time delay between receipt of echos produced upon reflection from the abnormality of said first longitudinal mode wave and said third mode converted wave, said time delay being indicative of the length of the abnormality in a direction generally transverse to the first surface of the test object.