JPS58122404A - Measuring method of thickness of copper film on inside surface of clad pipe for nuclear fuel - Google Patents
Measuring method of thickness of copper film on inside surface of clad pipe for nuclear fuelInfo
- Publication number
- JPS58122404A JPS58122404A JP57004221A JP422182A JPS58122404A JP S58122404 A JPS58122404 A JP S58122404A JP 57004221 A JP57004221 A JP 57004221A JP 422182 A JP422182 A JP 422182A JP S58122404 A JPS58122404 A JP S58122404A
- Authority
- JP
- Japan
- Prior art keywords
- nuclear fuel
- thickness
- pipe
- eddy current
- copper film
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B7/00—Measuring arrangements characterised by the use of electric or magnetic techniques
- G01B7/02—Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness
- G01B7/06—Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness for measuring thickness
- G01B7/10—Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness for measuring thickness using magnetic means, e.g. by measuring change of reluctance
- G01B7/105—Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness for measuring thickness using magnetic means, e.g. by measuring change of reluctance for measuring thickness of coating
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は銅皮“膜の厚み測定に関し、詳細には核燃料被
覆管の内面に形成される銅皮膜の厚み測定方法および装
置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to measuring the thickness of a copper coating, and more particularly to a method and apparatus for measuring the thickness of a copper coating formed on the inner surface of a nuclear fuel cladding tube.
従来、核燃料被覆管は一般に長さ数メートル。Traditionally, nuclear fuel cladding tubes are typically several meters long.
内110 ミIJメートル程度の細長い管であってその
材料としてはジルコニウム合金が一般使用されて満足す
kき効果が得られている。しかしながらそれを使用する
原子炉の負荷変動が大きい場合1.1はジルコニウム合
金は核分裂生成物の影響に上り応力腐食を起こし易い傾
向を有する。従ってf11宋原子炉の負荷を急激に変え
ることのないように特別の配慮が必要であった。この問
題を解決するためにシルコニ、ラム合金からなる被覆管
の内壁にフルコニウムの酸化皮膜を形成し、その上に更
に銅皮膜を設けた。いわゆる銅バリア型被覆管の使用が
提案されている。すなわち銅バリア型破覆管における銅
皮膜は核分裂生成物に対する障壁として機能する。従っ
て銅皮膜の厚さは犬である程障壁としての機能は向上す
る。しかしながら原子炉の運転効率の面から言えば、銅
材料の中性子吸収横断面積が大きい為、その厚さは小さ
い方が良い。It is a long and narrow tube with a diameter of approximately 110 mm, and zirconium alloy is generally used as the material, and a satisfactory effect has been obtained. However, if the load fluctuation of the nuclear reactor in which it is used is large, 1.1 the zirconium alloy has a tendency to be affected by nuclear fission products and to cause stress corrosion. Therefore, special consideration was required to avoid sudden changes in the load on the F11 Song reactor. In order to solve this problem, a fluoronium oxide film was formed on the inner wall of the cladding tube made of silconi and ram alloy, and a copper film was further provided on top of it. The use of so-called copper barrier type cladding has been proposed. In other words, the copper coating in the copper barrier type rupture tube functions as a barrier against fission products. Therefore, the thicker the copper film, the better the barrier function. However, from the standpoint of operating efficiency of the nuclear reactor, since the neutron absorption cross-sectional area of copper material is large, it is better to have a smaller thickness.
この相反する要求の妥協点として5μm の厚さが推奨
されており、この厚さがこの値からずれるとそのずれの
方向によりバリアとしての機能まだは原子炉の運転効率
が大きく影響される。従ってこの厚さの管理は極めて正
確に行わなければならない。A thickness of 5 μm is recommended as a compromise between these conflicting requirements, and if the thickness deviates from this value, the function as a barrier and the operating efficiency of the reactor will be greatly affected depending on the direction of the deviation. Therefore, this thickness must be controlled extremely accurately.
一方、設けられた銅皮膜の厚み測定は核燃料被覆管を破
壊し1重量法、金相学的方法、あるいは電気化学的方法
で行われているが、これらの方法は破壊測定であること
に加えて測定そのものに時間がかかり経済性に劣るもの
である。On the other hand, the thickness of the provided copper coating is measured by destroying the nuclear fuel cladding and using the 1 gravimetric method, the metallurgical method, or the electrochemical method, but these methods are not only destructive measurements but also This process takes time and is uneconomical.
他方、非破壊測定法としては螢光X線法および超音波法
が使用されている。螢光X線法は精度も良く、近年急激
に普及しつつある測定方法であるが、管内面への適用に
は極めて問題が多い。これに対して超音波法は反射波を
利用するものであるから管内面への適用が容易である。On the other hand, fluorescent X-ray method and ultrasonic method are used as non-destructive measurement methods. Although the fluorescent X-ray method has good accuracy and is a measurement method that has become rapidly popular in recent years, there are many problems in its application to the inner surface of tubes. On the other hand, since the ultrasonic method uses reflected waves, it can be easily applied to the inner surface of a tube.
しかしながらこの方法による結果はその精度に問題があ
る。いずれにしてもこれら従来の非破壊測定法では核燃
料被覆管内面の5±1郷程度の銅皮膜を有効に測定する
ことは出来ない。However, the accuracy of the results obtained using this method is problematic. In any case, these conventional non-destructive measurement methods cannot effectively measure a copper coating of about 5±1 mm on the inner surface of a nuclear fuel cladding tube.
本発明の目的は非破壊法により短時間でしかも連続的に
核燃料被覆管内面の銅皮膜厚を測定する方法および装置
を提供することである。An object of the present invention is to provide a method and apparatus for measuring the copper film thickness on the inner surface of a nuclear fuel cladding tube continuously in a short period of time by a non-destructive method.
本発明によれば長さ数メートル、内径約10ミリメート
ルの核燃料被覆管内面に形成された銅皮膜の厚さ測定に
渦電流法が適用される。According to the present invention, the eddy current method is applied to the thickness measurement of a copper coating formed on the inner surface of a nuclear fuel cladding tube having a length of several meters and an inner diameter of about 10 mm.
渦電流法とは交番磁界を与えたコイルを金属に近づける
とコイル自体のインピーダンスが変化することを利用す
るものであり、主に表皮効果を利用するものである。す
なわち、銅とジルコニウム合金の固有、抵抗の比は約2
5=1であって比較的太であり、この差により銅被覆の
ある場合とゾ 。The eddy current method utilizes the fact that when a coil to which an alternating magnetic field is applied is brought close to metal, the impedance of the coil itself changes, and mainly utilizes the skin effect. In other words, the specific resistance ratio of copper and zirconium alloy is approximately 2.
5 = 1 and is relatively thick, and this difference makes it different from the case with copper coating.
ルコニウム合金単独の場合とではコイルのインピ−ダン
スが明らかに異ったものになること、そしてこのインピ
ーダンスの変化分が特定の条件下で銅皮膜の厚さと明確
な相関性を示すという事実に立脚して本発明は構成され
ている。This is based on the fact that the impedance of the coil is clearly different from that of the ruconium alloy alone, and that the change in impedance shows a clear correlation with the thickness of the copper coating under certain conditions. The present invention is configured as follows.
上記における特定の条件の一つは試験周波数である。こ
の試験周波数が低過ぎると下地であるジルコニウム合金
の例えば管の肉厚等の影響を強く受け、それにより測定
精度が低下する。これに対して試験周波数が高過ぎると
インピーダンス変化分に対する銅皮膜の厚さの関係に直
線性が得られなくなる。従ってこの試験周波数の選択は
重要である。すなわち問題とする銅皮膜厚に対して直線
性が良く、且つジルコニウム合金管の肉厚が多少変動し
ても充分な測定精度が得られるような周波数を選択しな
ければならない。One of the specific conditions above is the test frequency. If this test frequency is too low, it will be strongly influenced by the underlying zirconium alloy, such as the wall thickness of the tube, thereby reducing measurement accuracy. On the other hand, if the test frequency is too high, linearity cannot be obtained in the relationship between the change in impedance and the thickness of the copper film. Therefore, the selection of this test frequency is important. That is, it is necessary to select a frequency that has good linearity for the copper coating thickness in question and that provides sufficient measurement accuracy even if the wall thickness of the zirconium alloy tube varies somewhat.
他の条件は特に内そう型渦電流測定子を使用する場合の
渦電流測定子と核燃料被覆管内面との間隙である。すな
わち、測定子を用いて材料を掃引する場合には測定子と
管内面との間にある程度の間隙が必要であるが、この間
隙は雑音の低減、検出感度の向上およびインピーダンス
変化分と皮膜浮量の直線性の向上の点から出来るだけ小
さい方が望ましい。Another condition is the gap between the eddy current measuring element and the inner surface of the nuclear fuel cladding tube, especially when an internal hollow type eddy current measuring element is used. In other words, when sweeping a material using a probe, a certain amount of space is required between the probe and the inner surface of the tube, but this gap reduces noise, improves detection sensitivity, and reduces impedance changes and film lift. From the viewpoint of improving linearity of quantity, it is desirable that it be as small as possible.
これら条件は測定対象を目安としである程度経験的に求
めることが出来る。例えばジルコニウム合金をジルカロ
イ−2とし、被覆管の長さを4メートル、内径を10.
8ミリメートルとし、銅皮膜の厚さを6〜7μmとし、
被覆管の肉厚公差を±0.08龍、所要の測定精度を±
0.2μ扉とした場合に試験周波数は100〜1000
KHz、測定子と被覆管内壁との間隙は0.2〜0.7
ynxが適当であることがわかった。These conditions can be determined empirically to some extent using the measurement target as a guide. For example, the zirconium alloy is Zircaloy-2, the length of the cladding tube is 4 meters, and the inner diameter is 10.
8 mm, and the thickness of the copper film is 6 to 7 μm,
The wall thickness tolerance of the cladding tube is ±0.08, and the required measurement accuracy is ±0.08.
When using a 0.2μ door, the test frequency is 100 to 1000.
KHz, the gap between the probe and the inner wall of the cladding tube is 0.2 to 0.7
It turns out that ynx is suitable.
これらの諸点を図面に示す次の実施例により明らかにす
る。These points will be made clear by the following examples shown in the drawings.
実施例 1
外径12.5 Ill 内& 10.8 m、長さ4m
の内面に銅皮膜を有しない核燃料被覆管に挿入された2
個の渦電流測定子(5)の出力端子を渦電流測定装置(
1)のブリッジ回路に接続し平衡をとる。次に内−1に
厚さ1μmから10μmの範囲の銅皮膜を設けた上記と
同様の核燃料被覆管(2)を架台(3)に固定治具(4
)により固定する。Example 1 Outer diameter 12.5 Ill Inner & 10.8 m, length 4 m
2 inserted into a nuclear fuel cladding tube that does not have a copper coating on its inner surface.
Connect the output terminals of the eddy current probes (5) to the eddy current measuring device (
Connect to the bridge circuit in 1) to maintain balance. Next, a nuclear fuel cladding tube (2) similar to the above with a copper coating of 1 μm to 10 μm thick on the inner side (1) is attached to a fixing jig (4) on a pedestal (3).
) to fix it.
次に上記銅皮膜を有しない核燃料被覆管内の渦電流測定
子の一方をとり出し上記銅皮膜を有する核燃料被覆管内
に挿入し、乾燥器(7)を介してコンプレッサ(6)か
ら空気圧力を加えることにより止め板(8)の位置まで
送り込む。Next, one of the eddy current probes in the nuclear fuel cladding tube that does not have the copper coating is taken out and inserted into the nuclear fuel cladding tube that has the copper coating, and air pressure is applied from the compressor (6) via the dryer (7). By doing so, it is fed to the position of the stop plate (8).
次にこの渦電流測定子(5)を掃引装置(9)により8
WL/f+の速度でビームスイッチ(10)の位置とな
るまで引き出して被覆管を掃引し、それを記録装置(1
1)により記録する。Next, this eddy current measuring element (5) is
Pull it out at a speed of WL/f+ until it reaches the beam switch (10) position, sweep the cladding tube, and record it on the recording device (10).
Record according to 1).
以上の操作を試験周波数をパラメータとしてインビーダ
ンス変化分と銅皮膜厚間の直線性の検討結果を肉厚変動
が±0.0811での測定精度と共に第1表に示す。Table 1 shows the results of examining the linearity between the impedance change and the copper film thickness using the test frequency as a parameter in the above operation, along with the measurement accuracy when the wall thickness variation is ±0.0811.
第1表
450〜9 ±0.6
90 0〜8 ±0.2
2700〜8 ±0.2
5400〜8 ±0.2
1080 0〜7 ±0.2
2160、 0〜5 ±0,1
以上の結果から6〜7μm間の直線性が良く且つ測定精
度も良好な試験周波数範囲は100〜1000KHzで
あることがわかる。Table 1 450~9 ±0.6 90 0~8 ±0.2 2700~8 ±0.2 5400~8 ±0.2 1080 0~7 ±0.2 2160, 0~5 ±0.1 or more From the results, it can be seen that the test frequency range with good linearity between 6 and 7 μm and good measurement accuracy is 100 to 1000 KHz.
実施例 2
測定子(5)との間隙が0.1〜0.5諺の核燃料被覆
管内面に1〜10μmの銅皮膜を形成し実施例1と同様
の操作により試験周波数540 KHzで測定を行った
。第2表に測定子(5)の搬送、掃引の可否。Example 2 A copper film of 1 to 10 μm was formed on the inner surface of the nuclear fuel cladding tube with a gap of 0.1 to 0.5 between the measuring element (5) and measurements were carried out at a test frequency of 540 KHz using the same procedure as in Example 1. went. Table 2 shows whether the probe (5) can be transported and swept.
掃引時の雑音、測定の際の感度すなわち皮膜1μm当り
の振幅、直線性を示す皮膜厚範囲を示す。It shows the noise during sweeping, the sensitivity during measurement, that is, the amplitude per 1 μm of film, and the film thickness range showing linearity.
0.1 否 −−−〇、2
可 0.05 10 0〜8
0.3 可 0.05 10
0〜80.4 町 0.05
10 0〜80.5 #
0.05 9 0〜70.7
町 0.06 8 0〜71.0
可 0.11 5 0
〜5以上の結果から、搬送と掃引が可能であり雑音も小
さく、しかも感度及び銅皮膜厚6〜7μmの範囲での直
線性の良好な間隙は0.2〜0.7關であることがわか
る。0.1 No ---〇, 2
Possible 0.05 10 0~8
0.3 Possible 0.05 10
0-80.4 Town 0.05
10 0~80.5 #
0.05 9 0~70.7
Town 0.06 8 0~71.0
Possible 0.11 5 0
~5 From the above results, it was determined that the gap is 0.2 to 0.7, which allows conveyance and sweeping, has low noise, and has good sensitivity and linearity in the range of copper coating thickness of 6 to 7 μm. Recognize.
以上説明したように本発明によれば核燃料被覆管を破壊
することなく核燃料被覆管内面に設けた。As explained above, according to the present invention, the nuclear fuel cladding tube can be provided on the inner surface of the nuclear fuel cladding tube without destroying it.
6〜7μmの範囲の銅皮膜厚を短時間でしかも連続的に
測定することが出来1作業性を大幅に改善することが出
来る。The copper coating thickness in the range of 6 to 7 μm can be measured continuously in a short period of time, and work efficiency can be greatly improved.
なお、以上の説明においては銅皮膜の厚さの測定に限定
しているが1本発明は銅皮膜の欠陥及0・ジルコニウム
酸化層の欠陥をも検出すること可能にするものである。Although the above description is limited to the measurement of the thickness of the copper coating, the present invention also makes it possible to detect defects in the copper coating and defects in the 0.zirconium oxide layer.
すなわち銅皮膜の欠陥については銅が部分的に析出され
ずに下地のジルカロイ−2の露出している欠陥面を0.
1 mm”程度迄検出可能である。またジルコニウム酸
化層に関しては酸化層の欠落面を最低1 xm、2程度
迄検出可能である。In other words, regarding defects in the copper film, copper is not partially deposited and the exposed defect surface of the underlying Zircaloy-2 is 0.
It is possible to detect the missing surface of the zirconium oxide layer to a minimum of 1 x m and about 2 mm.
第1図は本発明による銅皮膜厚測定に使用される装置の
概略図である。
l・・・満電流測定装置 2・・・核燃料被覆管3・
・・架台 4・・・固定治具 5・・・渦電流測定子6
・・・コンプレッサ 7・・・乾燥器 8・・・止め板
9・・・測定子掃引装置 10・・・ビームスイッチ1
1・・・記録計 12・・・ガイドFIG. 1 is a schematic diagram of an apparatus used to measure copper film thickness according to the present invention. l... Full current measuring device 2... Nuclear fuel cladding tube 3.
... Frame 4 ... Fixing jig 5 ... Eddy current probe 6
...Compressor 7...Dryer 8...Stop plate 9...Measure head sweep device 10...Beam switch 1
1...Recorder 12...Guide
Claims (1)
にその内径より0.2〜0.7 myx小さい外径を有
する内そう型渦電流測定子をそう人し、この測定子に1
00〜1000KHzの範囲の試験周波数を供給しつつ
上記被覆管内面に沿って上記測定子を掃引することを特
徴とする上記銅皮膜の厚さを連続的に測定する核燃料被
覆管内面の銅皮膜厚測定方法。An inner hollow type eddy current probe having an outer diameter 0.2 to 0.7 myx smaller than the inner diameter is placed inside a nuclear fuel cladding tube having a copper coating of 1.6 to 7 μm on the inner surface, and a 1.
The thickness of the copper coating on the inner surface of the nuclear fuel cladding tube is continuously measured by sweeping the measuring element along the inner surface of the cladding tube while supplying a test frequency in the range of 00 to 1000 KHz. Measuring method.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57004221A JPS58122404A (en) | 1982-01-14 | 1982-01-14 | Measuring method of thickness of copper film on inside surface of clad pipe for nuclear fuel |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57004221A JPS58122404A (en) | 1982-01-14 | 1982-01-14 | Measuring method of thickness of copper film on inside surface of clad pipe for nuclear fuel |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS58122404A true JPS58122404A (en) | 1983-07-21 |
Family
ID=11578542
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57004221A Pending JPS58122404A (en) | 1982-01-14 | 1982-01-14 | Measuring method of thickness of copper film on inside surface of clad pipe for nuclear fuel |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58122404A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0585902A2 (en) * | 1992-09-04 | 1994-03-09 | Sumitomo Electric Industries, Ltd. | Method and apparatus for measuring length of conduit and for diagnosing inside of conduit |
-
1982
- 1982-01-14 JP JP57004221A patent/JPS58122404A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0585902A2 (en) * | 1992-09-04 | 1994-03-09 | Sumitomo Electric Industries, Ltd. | Method and apparatus for measuring length of conduit and for diagnosing inside of conduit |
EP0585902A3 (en) * | 1992-09-04 | 1994-12-07 | Sumitomo Electric Industries | Method and apparatus for measuring length of conduit and for diagnosing inside of conduit. |
US5528938A (en) * | 1992-09-04 | 1996-06-25 | Sumitomo Electric Industries, Ltd. | Method and apparatus for measuring length of conduit and for diagnosing inside of conduit |
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