JPS6221003A - Thickness measurement of lining pipe - Google Patents

Thickness measurement of lining pipe

Info

Publication number
JPS6221003A
JPS6221003A JP16092985A JP16092985A JPS6221003A JP S6221003 A JPS6221003 A JP S6221003A JP 16092985 A JP16092985 A JP 16092985A JP 16092985 A JP16092985 A JP 16092985A JP S6221003 A JPS6221003 A JP S6221003A
Authority
JP
Japan
Prior art keywords
thickness
tube
pipe
eddy current
liner
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP16092985A
Other languages
Japanese (ja)
Inventor
Masayoshi Iwasaki
岩崎 全良
Akio Suzuki
紀生 鈴木
Manabu Kotani
学 小谷
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Kobe Steel Ltd
Original Assignee
Kobe Steel Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Kobe Steel Ltd filed Critical Kobe Steel Ltd
Priority to JP16092985A priority Critical patent/JPS6221003A/en
Publication of JPS6221003A publication Critical patent/JPS6221003A/en
Pending legal-status Critical Current

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  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)

Abstract

PURPOSE:To measure the thickness of a lining pipe at a high accuracy, by computing the thickness of the lining pipe with the mean of outputs of an eddy current measuring device as reference point as obtained by rotating a single tube made of a base material with the same diameter as the lining pipe to be measured. CONSTITUTION:In a liner covered pipe 1, a Zircaloy tube 8 with the same diameter as the pipe 1 and a pure Zr tube 9 are fixed concentrically. A probe (PB)3 is moved through the tube 8, the tube 8 is turned and the outputs of an eddy current measuring device 5 during one turn thereof are average in terms of frequency to make respective reference points (zero point). Moreover, while the PB 3 is moved through the tube 9, the tube 9 is rotated, the outputs of the measuring device 5 during one turn thereof are averaged in terms of frequency and the results are compared to the respective reference points to set the sensitivity. Then, the PB 3 is shifted into the pipe 1 to be measured and moved turning the tube 1. The reference points are subtracted from the current output at the measuring point and on the basis of the results and the sensitivity, the liner thickness, overall thickness and the zercaloy thickness are calculated 6 and displayed 7.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、渦電流法によりライニング管のライナ層や全
肉厚等の厚みを測定する方法に関し、特にジルコニウム
合金(以下、ジルカロイと称す)管の内面に純ジルコニ
ウムライナ層を形成した原子炉核燃料用の被覆管におけ
るライナ厚さや全肉厚の測定等に好適に適用可能な測定
法に関するものである。     □ 〔従来技術〕 原子炉運転の効率化のためには急激な出力上昇や下降が
不可欠であるが、従来のジルカロイ製の核燃料被覆管で
は、急激な出力変動があると応力腐食割れが懸念される
。そこで、ジルカロイ管の内面に極薄の純ジルコニウム
ライナ層を形成した被覆管が開発されている。このよう
な被覆管においては強度上の問題からライナ層や全肉厚
が所定の厚さを有していることが必要であり、そのため
にこれらの厚さを正確に測定する必要がある。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a method for measuring the thickness of a liner layer, total wall thickness, etc. of a lined pipe by an eddy current method, and particularly relates to a method for measuring the thickness of a liner layer, total wall thickness, etc. of a lined pipe using an eddy current method. The present invention relates to a measurement method that can be suitably applied to the measurement of liner thickness and total wall thickness in cladding tubes for reactor nuclear fuel in which a pure zirconium liner layer is formed on the inner surface of the tube. □ [Prior technology] Rapid increases and decreases in power are essential for efficient nuclear reactor operation, but with conventional Zircaloy nuclear fuel cladding, there are concerns about stress corrosion cracking if there is a sudden change in power. Ru. Therefore, a cladding tube in which an extremely thin pure zirconium liner layer is formed on the inner surface of a Zircaloy tube has been developed. In such a cladding tube, it is necessary that the liner layer and the total wall thickness have a predetermined thickness due to strength issues, and therefore, it is necessary to accurately measure these thicknesses.

一般に、ライニング管のように2種以上の金属からでき
ている管の各層や全体の厚さの測定法としては、破壊的
測定法と非破壊的測定法があるが、破壊的測定法では管
の両端部の測定しかできず、管内面全面の測定が不可欠
な上記被覆管の場合には適用できない。非破壊的測定法
としては超音波法と渦電流法があるが、超音波法は、上
記被覆管においてはライナ層とジルカロイ部の境界面で
のエコー識別が極めて困難であるため適用できない。一
方、渦電流法はジルコニウムライナ層の導電率(1/ρ
、ρ=50μΩ・am)とジルカロイ部の導電率(1/
ρ、ρ=70μΩ・cm)の差を利用することによって
ライナ厚や全肉厚の測定が可能である。即ち、渦電流法
の原理は、交流電流を流したコイルを金属表面に近接さ
せることにより金属表面に渦電流が流れ、その渦電流に
よって誘導磁場が誘起されてコイルのインピーダンスが
変化するため、このインピーダンスの変化量によって金
属表面の情報を得ることができるということであり、ラ
イニング管のライナ厚の変動によってインピーダンスが
変化し、また全肉厚の変動によってもインピーダンスが
変化することも周知のことであり、これによってライナ
厚や管の全肉厚を測定することが原理的には可能である
。
In general, there are two methods for measuring the thickness of each layer and the entire thickness of pipes made of two or more metals, such as lining pipes: destructive measurement methods and non-destructive measurement methods. This method can only measure both ends of the tube, and cannot be applied to the above-mentioned cladding tube, where measurement of the entire inner surface of the tube is essential. Nondestructive measurement methods include the ultrasonic method and the eddy current method, but the ultrasonic method cannot be applied to the above-mentioned cladding tube because it is extremely difficult to identify echoes at the interface between the liner layer and the Zircaloy portion. On the other hand, in the eddy current method, the conductivity of the zirconium liner layer (1/ρ
, ρ = 50μΩ・am) and the electrical conductivity of the Zircaloy part (1/
By using the difference between ρ and ρ=70 μΩ·cm, it is possible to measure the liner thickness and total wall thickness. In other words, the principle of the eddy current method is that when a coil carrying an alternating current is brought close to a metal surface, an eddy current flows on the metal surface, and the eddy current induces an induced magnetic field, which changes the impedance of the coil. This means that information on the metal surface can be obtained from the amount of change in impedance, and it is well known that impedance changes depending on changes in the liner thickness of the lining pipe, and also changes in impedance due to changes in the total wall thickness. This makes it possible in principle to measure the liner thickness and the total wall thickness of the pipe.

このような渦電流法によるライナ厚の具体的な測定法の
一例として、特開昭59−67405号公報に開示され
たものがある。これはコイルと管内面との間の空隙(以
下、リフトオフと称す)の変動に起因するコイルインピ
ーダンス変化方向のインピーダンス成分Vyとそれに直
交する方向のインピーダンス成分Vxを求め、Vxがら
、あるいはVxをvyで補正したものからライナ厚を求
めている。
An example of a specific method for measuring liner thickness using such an eddy current method is disclosed in Japanese Patent Laid-Open No. 59-67405. This is done by determining the impedance component Vy in the direction of coil impedance change due to fluctuations in the air gap between the coil and the inner surface of the tube (hereinafter referred to as lift-off) and the impedance component Vx in the direction orthogonal to it. The liner thickness is calculated from the corrected value.

ところで、測定されたインピーダンス成分をラ  ゛イ
ナ厚に変換する際には基準点が必要であり、そこで上記
公報では既知のライナ層を備えた基準試片を用い、停止
しているこの基準試片の一点におけるインピーダンス成
分Vx−Vyを基準としている。しかし、管内における
インピーダンスの変化を正規化インピーダンス平面に示
した第6図から明らかなように、リフトオフが異なると
基準点が大きく変化するが、上記方法では基準点設定時
のリフトオフを再現性よく設定するのは非常に困難であ
り、再現性の良い基準(零)点設定や感度設定が不可能
で、正確な測定ができないという問題があった。
By the way, a reference point is required when converting the measured impedance component into liner thickness, so in the above publication, a reference specimen with a known liner layer is used, and this reference specimen that is stationary is used. The impedance component Vx-Vy at one point is used as a reference. However, as is clear from Figure 6, which shows the change in impedance in the pipe on the normalized impedance plane, the reference point changes greatly when the liftoff is different, but the above method allows for reproducibility of the liftoff when setting the reference point. It is very difficult to do so, and it is impossible to set a reference (zero) point or sensitivity with good reproducibility, making it impossible to perform accurate measurements.

〔発明の目的〕[Purpose of the invention]

本発明は、上記従来の問題点を解決するためになされた
ものであって、渦電流法によってライニング管の各厚み
を測定する場合、その基準点の再現性を良くしたライニ
ング管の厚み測定法の提供を目的とする。
The present invention has been made to solve the above conventional problems, and is a method for measuring the thickness of a lining tube that improves the reproducibility of reference points when measuring each thickness of a lining tube by the eddy current method. The purpose is to provide.

〔発明の構成〕[Structure of the invention]

本発明のライニング管の厚み測定法は、ライニング管の
厚みを、管内部に電磁誘導試験用コイルを挿入して渦電
流法により測定する際に、被測定ライニング管と同径の
母材単独管を回転させて得られた渦流測定器の出力の平
均値を基準点としてライニング管の厚みを算出し、ライ
ナ層が零の母材管を回転させてリフトオフ量を平均化さ
せることによって零点の再現性を良くしたことを特徴と
するものである。
The method for measuring the thickness of a lined pipe according to the present invention is to measure the thickness of a lined pipe by inserting an electromagnetic induction test coil inside the pipe and using an eddy current method. The thickness of the lining pipe is calculated using the average value of the output of the eddy current measuring device obtained by rotating the eddy current measuring device as a reference point, and the zero point is reproduced by rotating the base material pipe with zero liner layer and averaging the lift-off amount. It is characterized by improved sex.

又、第2の本発明のライニング管の厚み測定法は、さら
に被測定ライニング管と同径のライナ材単独管を回転さ
せて得られた渦流測定器の出力の平均値から感度を設定
してライニング管の厚みを算出し、同様に感度の再現性
も良くしたことを特徴とするものである。
In addition, in the second method of measuring the thickness of a lining pipe according to the present invention, the sensitivity is further set based on the average value of the output of the eddy current measuring device obtained by rotating a single liner pipe having the same diameter as the lining pipe to be measured. The thickness of the lining tube is calculated, and the reproducibility of sensitivity is also improved.

〔実施例〕〔Example〕

次に、本発明をライナ被覆管のライナ厚及び全肉厚の測
定に適用した一実施例を、第1図〜第5図に基づいて説
明する。第1図(a)において、同図(b)示すように
母材管であるジルカロイ管laの内面に純ジルコニウム
のライナ層1bを形成されたライナ被覆管lが回転器2
によりその軸心回りに回転駆動可能に保持され、このラ
イナ被覆管1内に装入可能なプローブ3が装入装置4に
て支持されている。プローブ3内には絶対値型のコイル
が埋め込まれており、そのコイル径は約1鶴である。こ
のコイルからの信号、即ちインピーダンス変化は渦流測
定器5で検知されて例えば電圧に変換され、その出力が
所定の算出式をプログラムされた演算装置6に入力され
てライナ厚、全肉厚及びそれらからジルカロイ厚が演算
され、結果が表示器7に表示されるように構成されてい
る。
Next, an embodiment in which the present invention is applied to the measurement of the liner thickness and total wall thickness of a liner cladding tube will be described based on FIGS. 1 to 5. In FIG. 1(a), as shown in FIG. 1(b), a liner cladding tube l having a liner layer 1b of pure zirconium formed on the inner surface of a Zircaloy tube la, which is a base material tube, is attached to a rotator 2.
A probe 3 is supported by a charging device 4 and is held rotatably around its axis by a probe 3 which can be inserted into the liner cladding tube 1 . An absolute value type coil is embedded in the probe 3, and the diameter of the coil is approximately 1. A signal from this coil, that is, a change in impedance, is detected by an eddy current measuring device 5 and converted into, for example, a voltage, and the output is inputted to an arithmetic device 6 programmed with a predetermined calculation formula to determine the liner thickness, total wall thickness, and other values. The Zircaloy thickness is calculated from the above, and the result is displayed on the display 7.

コイルに印加される試験周波数は、主に全肉厚を測定す
るための500KHzと、主にライナ厚を測定するため
の2MHzと4 M Hzの2重周波数との計3重周波
数が用いられている。このようにライナ厚の測定におい
て、2重周波数にてコイルを励磁すると、周波数によっ
てインピーダンス変化の方向が変わるため、各励磁周波
数を微少変化させたときに生ずる前記コイルのインピー
ダンス変化の方向とそれに直交する方向のインピーダン
ス成分を検出し、これらインピーダンス成分からリフト
オフ量の変動やライナ層とジルカロイ部の導電率の変動
等の影響を無くしてライナ厚を求めることができるので
ある。
The test frequency applied to the coil was a total of three frequencies: 500 KHz, which was mainly used to measure the total wall thickness, and a dual frequency of 2 MHz and 4 MHz, which was mainly used to measure the liner thickness. There is. In measuring liner thickness, when a coil is excited at dual frequencies, the direction of impedance change changes depending on the frequency. The liner thickness can be determined from these impedance components by eliminating the effects of changes in lift-off amount, changes in conductivity between the liner layer and the Zircaloy portion, etc.

前記ライナ被覆管工の一端部には、このライナ被覆管1
と同径のジルカロイ管8及び純ジルコニウム管9が同心
状に固定されている。
This liner cladding tube 1 is attached to one end of the liner cladding tube work.
A Zircaloy tube 8 and a pure zirconium tube 9 having the same diameter are fixed concentrically.

以上の構造における測定手順は、まずプローブ3をジル
カロイ管8内に移動させてジルカロイ管8を回転させ、
その1回転中における渦流測定器5の出力を各周波数毎
にそれぞれ平均化してこれを基準点く零点)とする。さ
らにプローブ3を純ジルコニウム管9内に移動させて純
ジルコニウム管9を回転させ、その一回転中における渦
流測定器5の出力を各周波数毎にそれぞれ平均化し、そ
れを純ジルコニウムのライナ層が無限の場合の出力とし
て前記基準点と対比し、感度を設定する。
The measurement procedure in the above structure is to first move the probe 3 into the Zircaloy tube 8, rotate the Zircaloy tube 8,
The output of the eddy current measuring device 5 during one rotation is averaged for each frequency and used as a reference point (zero point). Furthermore, the probe 3 is moved into the pure zirconium tube 9, the pure zirconium tube 9 is rotated, and the output of the eddy current measuring device 5 during one rotation is averaged for each frequency. The sensitivity is set by comparing the output with the reference point in the case of .

次に、プローブ3を被測定管であるライナ被覆管1内に
移動し、このライナ被覆管1を回転しながらプローブ3
を移動させる。この時の渦流測定器5の各周波数毎の出
力からそれぞれの前記基準点を減算し、その値に基づき
、さらに前記感度に基づいて演算装置6でライナ厚と全
厚肉を算出し、さらに全肉厚からライナ厚を減算するこ
とによってジルカロイ厚を算出し、これらを表示器7に
表示する。
Next, move the probe 3 into the liner cladding tube 1 that is the tube to be measured, and rotate the liner cladding tube 1 while rotating the probe 3.
move. At this time, each reference point is subtracted from the output of the eddy current measuring device 5 for each frequency, and based on that value, the calculation device 6 calculates the liner thickness and total thickness based on the sensitivity, and then The Zircaloy thickness is calculated by subtracting the liner thickness from the wall thickness, and these are displayed on the display 7.

以上の方法で測定した結果を従来法の結果とともに第2
図に示す。これは、ジルカロイ管を基準点(零点)とし
て従来法で9.0μlのライナ層を存するライナ被覆管
を数回測定した際の渦流測定器の出力例と、本発明法に
よって測定した結果を示したものであり、従来法では厚
みの正確な測定は不可能であるが、本発明法では高精度
の測定が可能となっている。
The results measured using the above method are combined with the results of the conventional method.
As shown in the figure. This shows an example of the output of the eddy current measuring device when measuring a liner-coated tube with a liner layer of 9.0 μl using the conventional method several times using the Zircaloy tube as the reference point (zero point), and the results measured using the method of the present invention. Although it is impossible to accurately measure the thickness with the conventional method, the method of the present invention allows highly accurate measurement.

又、上記方法でライナ被覆管のライナ厚、全肉厚及びジ
ルカロイ厚を測定した結果の一例を第3図〜第5図に示
す。これらの結果から、本発明法によれば実測値と高精
度に対応しており、正確な測定が可能なことが認められ
る。
Furthermore, examples of the results of measuring the liner thickness, total wall thickness, and Zircaloy thickness of the liner cladding tube using the above method are shown in FIGS. 3 to 5. From these results, it is recognized that the method of the present invention corresponds to the actual measured value with high accuracy and that accurate measurement is possible.

〔発明の効果〕〔Effect of the invention〕

本発明のライニング管の厚み測定法によれば、以上のよ
うにライニング管の厚みを、管内部に電磁誘導試験用の
コイルを挿入して渦電流法により測定する際に、被測定
ライニング管と同径の母材単独管を回転させて得られた
渦流測定器の出力の平均値を基準点としてライニング管
の厚みを算出するので、ライナ層が零の母材管を回転さ
せてリフトオフ量を平均化することができ、その結果、
零点の再現性を良(することができる。さらに、被測定
ライニング管と同径のライナ材単独管を回転させて得ら
れた渦流測定器の出力の平均値から感度を設定してライ
ニング管の厚みを算出することにより、同様に感度の再
現性も良くすることができる。従って、本発明法によれ
ば、渦電流によってライニング管の厚みを極めて高精度
に測定することが可能となる。
According to the method for measuring the thickness of a lining pipe of the present invention, when the thickness of a lining pipe is measured by the eddy current method by inserting a coil for electromagnetic induction testing inside the pipe as described above, it is possible to The thickness of the lining tube is calculated using the average value of the output of the eddy current measuring device obtained by rotating a single base material tube of the same diameter as a reference point, so the lift-off amount is calculated by rotating the base material tube with zero liner layer. can be averaged, resulting in
The reproducibility of the zero point can be improved.Furthermore, the sensitivity can be set from the average value of the output of the eddy current measuring device obtained by rotating a single liner tube with the same diameter as the lined tube to be measured. By calculating the thickness, it is also possible to improve the reproducibility of the sensitivity. Therefore, according to the method of the present invention, it is possible to measure the thickness of the lining tube with extremely high precision using eddy current.

【図面の簡単な説明】[Brief explanation of drawings]

第1図〜第5図は本発明の一実施例を示し、第1図(a
)は本発明法を実施する装置の概略構成図、同図(b)
は同図(a)のI−I線断面図、同図(C)は同図(a
)の■−■線断面図、同図(d)は同図(a)のm−m
線断面図、第2図は本発明法と従来法によるライナ厚の
測定結果のばらつきを示すグラフ、第3図〜第5図はそ
れぞれライナ厚、全肉厚及びジルカロイ厚の測定値と実
測値の関係を示すグラフ、第6図は基準試験管中でのコ
イルインピーダンスの変化を正ffl化インピ−ダンス
平面で示した図である。 1はライナ被覆管、2は回転機、3はプローブ、5は渦
流測定器、6は演算装置、8はジルカロイ管、9は純ジ
ルコニウム管である。 第6図 第3図 ライナツツ’x差り根L    (7am)第4図 第5図
1 to 5 show an embodiment of the present invention, and FIG.
) is a schematic configuration diagram of an apparatus for carrying out the method of the present invention, and (b) of the same figure
is a cross-sectional view taken along the line I-I of the same figure (a), and the same figure (C) is a cross-sectional view taken along the line I-I of the same figure (a).
), the same figure (d) is m-m of the same figure (a)
Line cross-sectional view, Figure 2 is a graph showing the variation in liner thickness measurement results by the method of the present invention and the conventional method, Figures 3 to 5 are measured values and actual values of liner thickness, total wall thickness, and Zircaloy thickness, respectively. FIG. 6 is a diagram showing the change in coil impedance in a reference test tube on a positive ffl impedance plane. 1 is a liner clad tube, 2 is a rotating machine, 3 is a probe, 5 is an eddy current measuring device, 6 is a calculation device, 8 is a Zircaloy tube, and 9 is a pure zirconium tube. Figure 6 Figure 3 Rainatsu'x difference root L (7am) Figure 4 Figure 5

Claims (1)

【特許請求の範囲】 1、ライニング管の厚みを、管内部に電磁誘導試験用の
コイルを挿入して渦電流法により測定する際に、被測定
ライニング管と同径の母材単独管を回転させて得られた
渦流測定器の出力の平均値を基準点としてライニング管
の厚みを算出することを特徴とするライニング管の厚み
測定法。 2、ライニング管の厚みを、管内部に電磁誘導試験用の
コイルを挿入して渦電流法により測定する際に、被測定
ライニング管と同径の母材単独管を回転させて得られた
渦流測定器の出力の平均値を基準点とし、被測定ライニ
ング管と同径のライナ材単独管を回転させて得られた渦
流測定器の出力の平均値から感度を設定してライニング
管の厚みを算出することを特徴とするライニング管の厚
み測定法。
[Claims] 1. When measuring the thickness of a lined pipe by the eddy current method by inserting a coil for electromagnetic induction testing inside the pipe, a single base material pipe having the same diameter as the lined pipe to be measured is rotated. A method for measuring the thickness of a lining pipe, characterized in that the thickness of the lining pipe is calculated using the average value of the output of an eddy current measuring device obtained as a reference point. 2. When measuring the thickness of a lined pipe using the eddy current method by inserting a coil for electromagnetic induction testing inside the pipe, the eddy current obtained by rotating a single base material pipe with the same diameter as the lined pipe to be measured Using the average value of the output of the measuring device as a reference point, set the sensitivity from the average value of the output of the eddy current measuring device obtained by rotating a single liner tube with the same diameter as the lined tube to be measured, and calculate the thickness of the lined tube. A method for measuring the thickness of a lining pipe.
JP16092985A 1985-07-19 1985-07-19 Thickness measurement of lining pipe Pending JPS6221003A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16092985A JPS6221003A (en) 1985-07-19 1985-07-19 Thickness measurement of lining pipe

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16092985A JPS6221003A (en) 1985-07-19 1985-07-19 Thickness measurement of lining pipe

Publications (1)

Publication Number Publication Date
JPS6221003A true JPS6221003A (en) 1987-01-29

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP16092985A Pending JPS6221003A (en) 1985-07-19 1985-07-19 Thickness measurement of lining pipe

Country Status (1)

Country Link
JP (1) JPS6221003A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007263981A (en) * 2003-10-20 2007-10-11 Ebara Corp Eddy current sensor

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5967405A (en) * 1982-09-30 1984-04-17 Sumitomo Metal Ind Ltd Method for measuring thickness of liner

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5967405A (en) * 1982-09-30 1984-04-17 Sumitomo Metal Ind Ltd Method for measuring thickness of liner

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007263981A (en) * 2003-10-20 2007-10-11 Ebara Corp Eddy current sensor

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