Method for determining average wall thickness for pipes and tubes using guided waves

• US 5,970,434 A
• Filed: 01/29/1998
• Issued: 10/19/1999
• Est. Priority Date: 01/29/1998
• Status: Expired due to Term

• Current Assignee: Southwest Research Institute
• Original Assignee: Southwest Research Institute
• Inventors: Kwun, Hegeon, Brophy, Joseph W.
• Primary Examiner(s): Barlow, John
• Assistant Examiner(s): VO, HIEN XUAN
• Application Number:
  US09/015,133
• Time in Patent Office: 628 Days
• Field of Search: 702/170, 73/584, 73/622, 73/620, 73/625, 73/629, 73/632, 73/628, 73/627, 324/220, 324/226
• US Class Current: 702/170
• CPC Class Codes: G01B 17/02 for measuring thickness
• CPC Class Codes: G01N 2291/02854 Length, thickness
• CPC Class Codes: G01N 2291/0421 Longitudinal waves
• CPC Class Codes: G01N 2291/101 one transducer
• CPC Class Codes: G01N 2291/2636 cylindrical from inside
• CPC Class Codes: G01N 29/2412 using the magnetostrictive properties of the material to be examined, e.g. electromagnetic acoustic transducers [EMAT]; investigating the presence of flaws using eddy currents G01N27/90, magnetostrictive transducers B06B1/08, measuring magnetostrictive properties G01R33/18
• 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
• CPC Class Codes: G01N 29/46 by spectral analysis, e.g. Fourier analysis or wavelet analysis spectral signal processing per se G06F17/14
• CPC Class Codes: G01N 29/50 using auto-correlation techniques or cross-correlation techniques

Abstract

A method for determining changes in the average wall thickness or the mean radius of a pipe or tube using ultrasonic and/or magnetostrictive wave probes by analyzing the dispersive behavior of waves traveling in the tube wall volume. The method examines certain wave propagation modes and identifies a cut-off frequency that is characteristic for a particular wall thickness or tube diameter. This method permits the rapid and accurate inspection of a length of pipe or tube from a single location on the inside diameter of the pipe and permits a comparison of data gathered with similar data for the structure in its original condition. Changes in the cut-off frequency, indirectly determined by the method of the present invention are inversely related to changes in the wall thickness and/or the mean radius for the cylindrical structure. In this manner the method of the present invention provides a mechanism for determining the remaining service life for such pipes and tubes.

Claims

1. A method for measuring changes in an average wall thickness for a longitudinal section of pipe from a single location comprising the steps of:

directing interrogating mechanical waves into a wall of said pipe at said single location;

receiving a multifrequency return signal, said multifrequency return signal resulting from a dispersion of said interrogating mechanical waves throughout said longitudinal section of pipe;

analyzing said return signal by determining the ratio of wave group velocity at a first selected frequency to wave group velocity at a second selected frequency, said first and second selected frequencies being discrete frequencies offset from a cut-off frequency, said cut-off frequency being a frequency range over which said return signal is significantly attenuated due to the original geometry of said pipe;

comparing said ratio of wave group velocities with a baseline ratio for said pipe; and

correlating a change in said ratio with a respective change in said average wall thickness for said longitudinal section of pipe.

2. The method of claim 1 wherein said step of analyzing said return signal further comprises analyzing the L(0,1) and L(0,2) longitudinal propagation modes for said dispersion of said interrogating mechanical waves.

3. The method of claim 1 wherein said first selected frequency is significantly less than said cut-off frequency and said second selected frequency is close to said cut-off frequency.

4. The method of claim 1 wherein said step of directing interrogating mechanical waves comprises placing an ultrasonic transducer in mechanical contact with an inside wall of said pipe and driving said transducer with an AC electrical signal.

5. The method of claim 1 wherein said step of directing interrogating mechanical waves comprises positioning a magnetostrictive transducer in proximity to an inside wall of said pipe and driving said transducer with an AC electrical signal.

6. A method for measuring changes in an average wall thickness for a longitudinal section of pipe from a single location on said longitudinal section of pipe, comprising the steps of:

directing interrogating mechanical waves into an inside wall of said pipe;

receiving a multifrequency return signal, said multifrequency return signal resulting from a dispersion of said interrogating mechanical waves throughout said longitudinal section of pipe;

analyzing said return signal by determining a shift in a cut-off frequency identified within said return signal, said cut-off frequency being a frequency range over which said return signal is significantly attenuated due to the original geometry of said pipe;

correlating said shift in said cut-off frequency with a respective change in said average wall thickness for said longitudinal section of pipe.

7. The method of claim 6 wherein said step of analyzing said return signal further comprises determining said shift in said cut-off frequency by analyzing the L(0,1) and L(0,2) longitudinal propagation modes for said dispersion of said interrogating mechanical waves.

8. The method of claim 6 further comprising the step of initially determining said cut-off frequency for said length of pipe by calculating said cut-off frequency according to the equation;

F_c =V/2π

B;

wherein F_c is the cut-off frequency;

V is the Rod velocity limit; and

B is the mean radius of said pipe.