Eddy current probe system and method for determining the midpoint and depth of a discontinuity

• US 5,864,229 A
• Filed: 06/11/1992
• Issued: 01/26/1999
• Est. Priority Date: 06/11/1991
• Status: Expired due to Term

• Current Assignee: NEWT Holdings Limited
• Original Assignee: Millstrong Limited
• Inventors: Lund, Frank Philip
• Primary Examiner(s): Snow, Walter E.
• Application Number:
  US07/897,120
• Time in Patent Office: 2,420 Days
• Field of Search: 324/239, 324/243, 324/262, 324/236-238, 324/219-221
• US Class Current: 324/240
• CPC Class Codes: G01N 27/902 by moving the sensors

Abstract

A probe for generating a signal indicative of a quantitative measurement of the size of a surface defect, comprising a magnetic field generator for inducing currents in the surface, and a perturbation current sensor arrangement positioned relative to the field to give an output providing the quantitative measure.

Claims

1. A probe for measuring the depth of a defect adjacent to a material surface, comprising:

a magnetic field generator configured to generate an alternating magnetic field having two opposed pole portions of magnetic flux which interact with the material surface in first and second regions spaced apart along a spatial direction in the surface when the probe is positioned against the surface, so as to induce an eddy current flow in the surface between said two regions running across said spatial direction, said eddy current flow exhibiting a current gradient along said spatial direction, so that the defect extending in said spatial direction will give rise to a defect-crossing potential difference across the defect, said defect-crossing potential difference varying along said spatial direction as a potential difference gradient, to give rise to perturbation currents in said eddy currents; and

at least one perturbation current sensor configured to sense a magnetic field normal to the surface corresponding to said perturbation currents in the plane of the surface, positioned asymmetrically relative to said magnetic field generator in the region of said potential difference gradient to provide at least one output signal dependent upon said perturbation currents and hence upon said potential difference gradient, as a quantitative measure of the depth of the defect.

2. The probe according to claim 1, wherein said magnetic field generator is arranged to generate a field having symmetrical field gradient regions about a center along said spatial direction, inducing corresponding symmetrical contra-rotating eddy current regions in the surface along said spatial direction.

3. The probe according to claim 2, wherein said at least one sensor is arranged asymmetrically with regard to said magnetic field produced by said magnetic field generator.

4. The probe according to claim 3, wherein said at least one sensor is disposed substantially to overlie regions of maximum current density gradient in the surface.

5. The probe according to claim 3, wherein said at least one sensor is positioned asymmetrically, relative to said center, in said spatial direction.

6. The probe according to claim 3, wherein said at least one sensor comprises at least one pair of perturbation current sensors positioned centrosymmetrically in said spatial direction.

7. The probe according to claim 6, wherein said at least one pair of said perturbation current sensors are connected in opposition such that induced signals of opposite sign in said sensors are additive in magnitude.

8. The probe according to claim 1, wherein said at least one sensor comprises at least one pair of perturbation current sensors offset in said spatial direction.

9. The probe according claim 1, wherein said at least one sensor comprises a coil in a plane parallel to the surface.

10. The probe according to claim 3, wherein said at least one sensor comprises a coil parallel to the surface, comprising a first lobe and second lobe, aligned in said spatial direction, said first and second lobes inducing opposing current rotations, wherein said opposing current rotations induced in said lobes are additive.

11. The probe according claim 1, wherein said magnetic field generator comprises a solenoid extending in said spatial direction.

12. A measuring assembly comprising a probe according to claim 8 and further comprising signal processing means for combining said signals from said at least one pair of said perturbation current sensors such that induced signals of opposite signs in said sensors are additive in magnitude.

13. The probe according to claim 1, wherein said magnetic field generator and said at least one sensor are packaged for use under water.

14. The probe according to claim 1, wherein said magnetic field sensed by said at least one sensor is orthogonal to said magnetic field generated by said magnetic field generator.

15. The probe according to claim 14, wherein said magnetic field generator and said at least one current sensor each consist of at least one inductance coil, and further wherein an axis of at least one of said plurality of said inductance coils of said at least one current sensor is orthogonal to an axis of said magnetic field generator.

16. The probe according to claim 1, wherein said at least one perturbation current sensor comprises an array of perturbation current sensors.

17. The probe according to claim 1, wherein the probe is shaped to conform to a non-tubular surface.

18. The probe according to claim 1, wherein said magnetic field generator includes a high frequency alternating electric excitation field equal to or greater than approximately one kHz.

19. The probe according to claim 1, wherein said magnetic field generator includes a high frequency alternating electric excitation field equal to or greater than approximately 40 kHz.

20. A method of measuring a depth of a defect in a surface of a material from a position adjacent to the material, comprising the steps of:

generating an AC eddy current in a plane of the surface, said eddy current having a region flowing across a spatial direction in which the defect extends to create a defect-crossing potential difference across the sides of the defect, said defect crossing potential difference varying along the defect in said spatial direction in a gradient along the defect, whereby perturbation currents are generated in the surface;

sensing said perturbation currents at a point in said gradient to provide sensed signals which are responsive to a magnitude of said defect-crossing potential difference; and

deriving from said sensed signals a quantitative indication of the depth of said defect at a point between the ends of said defect.

21. The method according to claim 20, wherein said AC eddy current is induced by a generated magnetic field.

22. The method according to claim 20, wherein said AC eddy current is, in the absence of a defect, centrosymmetrical along said spatial direction and said sensed current perturbations are sensed or processed asymmetrically.

23. The method according to claim 20, wherein said deriving step comprises the step of processing said sensed signals to derive real and imaginary components of said perturbation currents.

24. The method according to claim 20, wherein said surface is a non-tubular surface.

25. The method according to claim 24, wherein said surface comprises a weld between two plates.

26. The method according to claim 20, wherein said generating step includes the step of generating a high frequency alternating electric excitation field equal to or greater than approximately one kHz.

27. The method according to claim 20, wherein said generating step includes the step of generating a high frequency alternating electric excitation field equal to or greater than approximately 40 kHz.