Non-destructive measurement of pipe wall thickness

• US 6,561,032 B1
• Filed: 05/15/2000
• Issued: 05/13/2003
• Est. Priority Date: 05/15/2000
• Status: Expired due to Term

• Current Assignee: Mueller International LLC (Mueller Water Products Incorporated)
• Original Assignee: National Research Council Canada
• Inventors: Hunaidi, Osama
• Primary Examiner(s): CHAPMAN JR, JOHN E
• Application Number:
  US09/570,922
• Time in Patent Office: 1,093 Days
• Field of Search: 735/97, 735/98, 735/92, 736/22, 702/39, 702/170, 702/171
• US Class Current: 73/597
• CPC Class Codes: G01B 17/02 for measuring thickness
• CPC Class Codes: G01N 2291/02854 Length, thickness
• CPC Class Codes: G01N 2291/2626 Wires, bars, rods
• CPC Class Codes: G01N 2291/2634 cylindrical from outside
• CPC Class Codes: G01N 29/07 by measuring propagation velocity or propagation time of acoustic waves

Abstract

The average wall thickness of a pipe carrying a fluid is determined by sensing disturbances in the pipe at two spaced locations, determining the propagation velocity of coupled propagation mode signals at low frequencies resulting from the disturbances, and calculating the average pipe wall thickness between the two locations from the propagation velocity and known constants for the pipe and fluid.

Claims

1. A method of measuring the wall thickness of a pipe carrying a fluid medium, comprising sensing disturbances in the pipe at two spaced locations, determining the propagation velocity of coupled propagation mode signals at low frequencies resulting from said disturbances, and calculating the average pipe wall thickness between said two locations from said propagation velocity and known constants for said pipe and fluid medium.

2. A method as claimed in claim 1, wherein said disturbances result from ambient noise existing in the pipe.

3. A method as claimed in claim 1, wherein said disturbances are induced by external action.

4. A method as claimed in claim 3, wherein said disturbances are induced by simulating a leak in the pipe.

5. A method as claimed in claim 4, wherein said propagation velocity is measured using a time-of-flight method.

6. A method as claimed in claim 4, wherein said propagation velocity is determined from cross-correlation and impulse functions, and phase angle method in the frequency domain.

7. A method as claimed in claim 1, wherein said average pipe wall thickness is determined from the relationship:

$c=c_o<br><br>\sqrt{\frac{1}{\left[1+a<br><br>\left(D/e\right)<br><br>\left(K_w/E_{\mathrm{\rho <br><br>}}\right)\right]}}$

where c is the propagation velocity of leak signals in the pipe, c₀ is the propagation velocity of sound in an infinite body of water equal to {square root over (K_w/ρ

)}, K_w is the bulk modulus of elasticity of the fluid medium, ρ

is density of the fluid medium and E_ρ

is the modulus of elasticity of the pipe material, D is internal diameter of the pipe, e is the thickness of the pipe wall, and α

is constant that depends on the constraints of longitudinal movement of the pipe.

8. A method as claimed in claim 7, wherein said signals are detected using. accelerometers.

9. A method as claimed in claim 7, wherein said signals are detected using hydrophones.

10. A method as claimed in claim 1, wherein said pipe forms part of a water, gas, oil or other fluid distribution and transmission systems.

11. An apparatus for measuring pipe wall thickness, comprising a pair of sensors for detecting coupled mode signals at spaced locations on a pipe, and a processor for determining the propagation velocity of said coupled mode signals between said locations, said processor further determining the average pipe wall thickness between said locations from the propagation velocity and known constants for said pipe and fluid.

12. An apparatus as claimed in claim 11, wherein said sensors comprise hydrophones.

13. An apparatus as claimed in claim 11, wherein said sensors comprise accelerometers.

14. An apparatus for measuring pipe wall thickness as claimed in claim 11, wherein said processor is programmed to determine the average pipe wall thickness from the propagation velocity using the relationship:

$c=c_o<br><br>\sqrt{\frac{1}{\left[1+a<br><br>\left(D/e\right)<br><br>\left(K_w/E_{\mathrm{\rho <br><br>}}\right)\right]}}$

where c is the propagation velocity of leak signals in the pipe, c₀ is the propagation velocity of sound in an infinite body of the fluid medium equal to {square root over (K_w/ρ

)}, K_w is the bulk modulus of elasticity of the fluid medium water, ρ

is density of the fluid medium and E_ρ

is the modulus of elasticity of the pipe material, D is internal diameter of the pipe, e is the thickness of the pipe wall, and α

is constant that depends on the constraints of longitudinal movement of the pipe.

15. A method of determining the type of pipe carrying a fluid medium, comprising sensing disturbances in the pipe at two spaced locations, determining the propagation velocity of coupled propagation mode signals at low frequencies resulting from said disturbances, and determining the type of pipe material from said propagation velocity and known constants for said pipe and fluid medium.