# US 5,341,678 A · Method for determining thickness of ferromagnetic material deposition on nuclear fuel rods

> Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt

- Number: US 5,341,678 A
- Document ID: US5341678A
- Status: Granted
- Kind: A
- Application number: 08/058,152
- Filed: 1993-05-12
- Granted: 1994-08-30
- Earliest claimed: 1993-05-12
- Assignees: General Electric Company
- Inventors: John A. Kervinen
- Web page: https://patentgrep.com/patent/US5341678A

## CPC

- G01N 27/9053: {Compensating for probe to workpiece spacing}
- G01B 7/105: {for measuring thickness of coating}
- G01N: INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES (measuring or testing apparatus or processes other than immunoassay, involving enzymes or microorganisms C12M, C12Q)
- G01B: MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS

## Abstract

A method for determining the thickness of ferromagnetic material deposited on a nuclear fuel rod. Calibration samples of known thickness and known permeability are placed between the probe of an eddy current sensor and a conductive surface. A plurality of calibration points are plotted to provide a characteristic complex impedance diagram for a probe excited at a predetermined frequency. Then the complex impedance of the probe excited at the selected frequency is measured when in proximity to a fuel rod having a corrosion layer of unknown thickness and unknown magnetic permeability. For each probe position, the two components of the complex impedance, i.e., the inductive reactance and the resistance, are determined and plotted on the characteristic complex impedance diagram. The position of the measured data point relative to the calibration points enables one to determine the lift-off error due to the presence of ferromagnetic material.

## Claims

### Claim 1

A method for determining the thickness of a coating of substantially electrically insulating material formed on the surface of an electrically conductive component when said substantially electrically insulating material includes ferromagnetic material, said coating having an unknown thickness and an unknown permeability, comprising the steps of:
mapping a plurality of complex impedance data points for a probe of an eddy current sensor excited with an alternating current having a predetermined frequency, each data point being acquired in the presence of ferromagnetic material having a different respective effective permeability;
placing said probe in contact with said layer of substantially electrically insulating material of unknown thickness and unknown permeability;
exciting said probe with an alternating current having said predetermined frequency;
measuring the complex impedance of said excited probe in contact with said layer;
comparing said measured complex impedance of said probe to said data points; and
determining the portion of the inductive reactance component of said measured complex impedance which is attributable to the permeability of said layer of substantially electrically insulating material.

### Claim 2 (depends on 1)

The method as defined in claim 1, wherein said step of mapping a plurality of data points comprises the steps of:
placing said probe in proximity to an uncoated electrically conductive component, with a selected one of a multiplicity of calibration samples being installed between said probe and said uncoated electrically conductive component, each of said calibration samples being made of substantially electrically insulating material including different known amounts of ferromagnetic material;
exciting said probe with an alternating current having said predetermined frequency; and
plotting the complex impedance of said excited probe when said probe is in contact with an installed calibration sample, said plotting step being repeated for each calibration sample.

### Claim 3 (depends on 1)

The method as defined in claim 1, further comprising the step of subtracting said portion of the inductive reactance component of said measured complex impedance which is attributable to the effective permeability of said layer of substantially electrically insulating material from the inductive reactance component of said measured complex impedance, the resulting value being used to determine the lift-off caused by said layer of substantially electrically insulating material.

### Claim 4 (depends on 3)

The method as defined in claim 3, wherein said electrically conductive component is a tube made of metal or alloy.

### Claim 5 (depends on 4)

The method as defined in claim 4, wherein said electrically conductive component is cladding of a nuclear fuel rod.

### Claim 6 (depends on 1)

The method as defined in claim 1, wherein said predetermined frequency is less than 10.sup.6 Hz.

### Claim 7 (depends on 1)

The method as defined in claim 1, wherein said predetermined frequency is selected so that a phase angle between a lift-off locus in the absence of ferromagnetic material and a permeability locus in the presence of ferromagnetic material is about 110 degrees or less.

### Claim 8 (depends on 2)

The method as defined in claim 2, wherein each respective calibration sample comprises a strip of electrically insulating material having a different number of layers of ferromagnetic paint coated thereon.

### Claim 9

A method for determining the thickness of a coating of substantially electrically insulating material formed on the surface of an electrically conductive component when said substantially electrically insulating material includes ferromagnetic material, said coating having an unknown thickness and an unknown permeability, comprising the steps of:
placing a probe of an eddy current sensor in proximity to an uncoated electrically conductive component, with a selected one of a multiplicity of calibration samples being installed between said probe and said uncoated electrically conductive component, each of said calibration samples being made of substantially electrically insulating material including different known amounts of ferromagnetic material;
exciting said probe with an alternating current having a predetermined frequency;
calibrating the complex impedance of said excited probe when said probe is in contact with an installed calibration sample, said calibrating step being repeated for each calibration sample;
placing said probe in contact with said coated electrically conductive component;
measuring the complex impedance of said excited probe when said probe is in contact with said layer of substantially electrically insulating material of unknown thickness and unknown permeability;
comparing said measured complex impedance of said probe with said calibrated complex impedances of said probe; and
determining the portion of the inductive reactance component of said measured complex impedance which is attributable to the effective permeability of said layer of substantially electrically insulating material.

### Claim 10 (depends on 9)

The method as defined in claim 9, further comprising the step of subtracting said portion of the inductive reactance component of said measured complex impedance which is attributable to the effective permeability of said layer of substantially electrically insulating material from the inductive reactance component of said measured complex impedance, the resulting value being used to determine the thickness of said layer of substantially electrically insulating material.

### Claim 11 (depends on 10)

The method as defined in claim 10, wherein said electrically conductive component is a tube made of metal or alloy.

### Claim 12 (depends on 11)

The method as defined in claim 11, wherein said electrically conductive component is cladding of a nuclear fuel rod.

### Claim 13 (depends on 9)

The method as defined in claim 9, wherein said predetermined frequency is less than 10.sup.6 Hz.

### Claim 14 (depends on 9)

The method as defined in claim 9, wherein said predetermined frequency is selected so that a phase angle between a lift-off locus in the absence ferromagnetic material and a permeability locus in the presence of ferromagnetic material is about 110 degrees or less.

### Claim 15 (depends on 9)

The method as defined in claim 9, wherein each respective calibration sample comprises a strip of electrically insulating material having a different number of layers of ferromagnetic paint coated thereon.
