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JPH0227604B2 - - Google Patents
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JPH0227604B2 - - Google Patents

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Publication number
JPH0227604B2
JPH0227604B2 JP58232404A JP23240483A JPH0227604B2 JP H0227604 B2 JPH0227604 B2 JP H0227604B2 JP 58232404 A JP58232404 A JP 58232404A JP 23240483 A JP23240483 A JP 23240483A JP H0227604 B2 JPH0227604 B2 JP H0227604B2
Authority
JP
Japan
Prior art keywords
tube
lining
energy loss
thickness
pipe
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.)
Expired - Lifetime
Application number
JP58232404A
Other languages
Japanese (ja)
Other versions
JPS60123712A (en
Inventor
Susumu Togawa
Toshio Toshima
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.)
Kubota Corp
Original Assignee
Kubota Corp
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 Kubota Corp filed Critical Kubota Corp
Priority to JP23240483A priority Critical patent/JPS60123712A/en
Publication of JPS60123712A publication Critical patent/JPS60123712A/en
Publication of JPH0227604B2 publication Critical patent/JPH0227604B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B17/00Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations
    • G01B17/02Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations for measuring thickness
    • G01B17/025Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations for measuring thickness for measuring thickness of coating

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)

Description

【発明の詳細な説明】 本発明は管内面ライニング厚の測定方法に関
し、特に充水状態の管におけるライニング厚を測
定可能な管内面ライニング厚の測定方法に関す
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring the lining thickness on the inner surface of a tube, and more particularly to a method for measuring the lining thickness on the inner surface of a tube by which the lining thickness of a tube in a water-filled state can be measured.

遠心鋳造等により鋳鉄管を成形した場合には、
通常、防食等の理由により、内面にセメントモル
タル層、樹脂モルタル層、あるいは塗料等のライ
ニングが施される。通水用の管路、配管の維持管
理のため、管内面ライニングの調査、特にその厚
さを調査する場合には、従来、管路、配管の流水
を停止させ、部分的に管を取外して直接調べる
か、あるいは管内カメラによつて調査するなどの
方法がとられている。しかし、いずれにしろ、そ
の期間中、その管路を含むシステムを休止させね
ばならず、問題がある。
When forming cast iron pipes by centrifugal casting, etc.
Usually, for reasons such as corrosion prevention, a cement mortar layer, a resin mortar layer, or a lining of paint is applied to the inner surface. In order to maintain and manage water-flowing conduits and piping, when investigating the inner lining of the pipe, especially its thickness, conventionally, water flow in the conduit or piping is stopped and the pipe is partially removed. Methods such as direct investigation or investigation using in-duct cameras are used. However, in any case, the system including the pipe must be stopped during that period, which poses a problem.

そこで本発明は、管内面ライニング厚を、通水
状態のまま管表面から測定可能なようにすること
を目的とするものである。
SUMMARY OF THE INVENTION Therefore, an object of the present invention is to make it possible to measure the inner lining thickness of a pipe from the pipe surface while water is flowing through the pipe.

この目的を達成するため本発明は、内面にライ
ニングが施された充水状態の鉄管の表面に超音波
探触子を設置して管径方向に超音波を発し、対向
側のライニング内面からの反射波のエネルギ損失
を検出するに際し、管表面と探触子との接触面の
状況と、管内の水の物性と、管の材質と、管の口
径と、ライニングの材質とを一定であるとすると
ともに、管厚を既知であるとして、これらにもと
づくエネルギ損失の値をあらかじめ把握してお
き、ライニング厚とエネルギ損失との関係をあら
かじめ求めておき、そして、検出されたエネルギ
損失値から前記あらかじめ把握されたエネルギ損
失値を減じて、その差からライニング厚を求める
ものである。
In order to achieve this objective, the present invention installs an ultrasonic probe on the surface of a water-filled iron pipe whose inner surface is lined, emits ultrasonic waves in the radial direction of the pipe, and emits ultrasonic waves from the inner surface of the lining on the opposite side. When detecting the energy loss of reflected waves, it is assumed that the condition of the contact surface between the tube surface and the probe, the physical properties of the water in the tube, the material of the tube, the diameter of the tube, and the material of the lining are constant. At the same time, assuming that the pipe thickness is known, the value of the energy loss based on this is known in advance, the relationship between the lining thickness and the energy loss is determined in advance, and the relationship between the lining thickness and the energy loss is calculated in advance from the detected energy loss value. The determined energy loss value is subtracted and the lining thickness is determined from the difference.

したがつて、管表面と探触子との接触面の状
況、管内液体の物性、管材質、管口径、およびラ
イニング材質が一定であるなら、管厚を求めてお
けば、検出された反射波のエネルギ損失はライニ
ング厚のみの関数となり、管内面ライニング厚を
通水状態のまま測定できることになるため、管
路、配管の維持管理を容易に行なうことができる
のみならず、鉄管とライニングと水との3物質の
中の超音波の減衰を扱うものであるため、常識的
には超音波は鉄部で反射した信号しか使えないと
ころを、水を介在させることによりライニング内
面からの反射波を検出することができる。
Therefore, if the condition of the contact surface between the tube surface and the probe, the physical properties of the liquid in the tube, the tube material, the tube diameter, and the lining material are constant, the detected reflected wave can be calculated by determining the tube thickness. The energy loss is a function only of the lining thickness, and the inner lining thickness of the pipe can be measured while water is flowing. This not only makes it easier to maintain and manage the pipes and pipes, but also allows for easy maintenance of pipes, linings, and water. Since it deals with the attenuation of ultrasonic waves in three substances, conventionally, ultrasonic waves can only be used as signals reflected from iron parts, but by interposing water, the waves reflected from the inner surface of the lining can be used. can be detected.

以下、本発明の一実施例を図面にもとづいて説
明する。第1図において1は鋳鉄製の管であり、
その内面にはセメントモルタル層等のライニング
2が施されている。管1内には水3が通され、そ
の表面には超音波探触子4が設置されている。第
2図はシステム図を示し、4は第1図に示した超
音波探触子、5は管1の肉厚を測定するための超
音波厚み計、6はライニング厚を測定する際に反
射エコーを検知するためのブラウン管7付き超音
波検知器で、超音波探傷器をそのまま利用してい
る。8は反射波エコー高さのA/D変換器で、こ
のA/D変換器8と前記超音波厚み計5との出力
は損失エネルギ演算器9で演算処理され、その結
果がライニング厚表示器10および記録計11に
導かれる。
Hereinafter, one embodiment of the present invention will be described based on the drawings. In Fig. 1, 1 is a cast iron pipe;
Its inner surface is provided with a lining 2 such as a layer of cement mortar. Water 3 is passed through the tube 1, and an ultrasonic probe 4 is installed on its surface. Figure 2 shows a system diagram, where 4 is the ultrasonic probe shown in Figure 1, 5 is an ultrasonic thickness gauge for measuring the wall thickness of the pipe 1, and 6 is a reflection device used to measure the lining thickness. This is an ultrasonic detector with a cathode ray tube 7 for detecting echoes, and uses the same ultrasonic flaw detector as is. Reference numeral 8 denotes an A/D converter for the reflected wave echo height, and the output from this A/D converter 8 and the ultrasonic thickness meter 5 is processed by a loss energy calculator 9, and the result is displayed on the lining thickness display. 10 and recorder 11.

第1図に示すように、内部に水3が通されてい
る管1の表面に超音波探触子4を接触させ、半径
方向に超音波12を発射する。すると、超音波1
2は管1の肉を通過し、その一部はライニング2
および水3中を透過し、対向側のライニング面1
3で反射し、その反射波が超音波探触子4にて検
知される。検知信号は、超音波検知器6のブラウ
ン管7で目視できる。
As shown in FIG. 1, an ultrasonic probe 4 is brought into contact with the surface of a tube 1 through which water 3 is passed, and ultrasonic waves 12 are emitted in the radial direction. Then, ultrasound 1
2 passes through the flesh of tube 1, a part of which passes through the lining 2
and water 3, and the opposite lining surface 1
3, and the reflected wave is detected by the ultrasonic probe 4. The detection signal can be visually observed on the cathode ray tube 7 of the ultrasonic detector 6.

反射波のエネルギPrはエコー高さによつて知
ることができる。すなわち、反射波は発射波に比
べエネルギ損失を受け、このエネルギ損失は、 1 探触子4と管1との接触面でのエネルギ損失
ΔPt 2 管1の肉厚部でのエネルギ損失ΔPi〔ただし
ΔPiは管厚tiと管材質miとの関数:ΔPi(ti,mi)〕 3 ライニング2でのエネルギ損失ΔPl〔ただし
ΔPlはライニング厚tlとライニング材質mlとの
関数:ΔPl(tl,ml)〕 4 水3によるエネルギ損失ΔPw にて構成され、全エネルギ損失をΔPrとすると、 ΔPr=ΔPt+ΔPi+ΔPl+ΔPw ……(i) となる。
The energy Pr of the reflected wave can be determined by the echo height. That is, the reflected wave suffers an energy loss compared to the emitted wave, and this energy loss is as follows: 1 Energy loss ΔP t at the contact surface between probe 4 and tube 1 2 Energy loss ΔP i at the thick part of tube 1 [However, ΔP i is a function of pipe thickness t i and pipe material m i : ΔP i (t i , m i )] 3 Energy loss ΔP l in lining 2 [However, ΔP l is a function of lining thickness t l and lining material m Function with l : ΔP l (t l , m l )] 4 Consists of energy loss ΔP w due to water 3, and if the total energy loss is ΔP r , ΔP r = ΔP t + ΔP i + ΔP l + ΔP w ... (i) becomes.

いま、接触面の状況、水(管内液体)の物性、
管材質、管口径およびライニング材質を一定とす
ると、全エネルギ損失ΔPrの変化δΔPrは、 δΔPr=δΔPi(δti)+δΔPl(δtl) ……(ii) として表わせる。すなわち、予め管厚tiとこれに
よるエネルギ損失ΔPiとの関係、およびライニン
グ厚tlとこれによるエネルギ損失ΔPlとの関係が
わかつていると、全エネルギ損失の変化δΔPr
および管厚δtiを知ることによつて、ライニング
厚δtlを求めることができる。
Now, the situation of the contact surface, the physical properties of water (liquid inside the pipe),
Assuming that the pipe material, pipe diameter, and lining material are constant, the change δΔP r in the total energy loss ΔP r can be expressed as δΔP r = δΔP i (δt i ) + δΔP l (δt l ) (ii). That is, if the relationship between the pipe thickness t i and the resulting energy loss ΔP i and the relationship between the lining thickness t l and the resulting energy loss ΔP l are known in advance, the change in total energy loss δΔP r ,
By knowing the pipe thickness δt i and the pipe thickness δt i , the lining thickness δt l can be determined.

第1図〜第2図に示す装置によれば、ひとつの
探触子4によつて、超音波厚み計5を作用させる
ことにより管1の肉厚を測定できるうえに、前述
の反射波の全エネルギ損失の変化δΔPrと前記管
厚との測定結果を演算器9で演算することによ
り、ライニング厚を容易に計算できる。また、反
射波のエネルギ損失は、超音波検知器6として使
用する通常の超音波探傷器のゲートアナログ出力
によつて取出せる。ゲートは、予め入力した管口
径値に応じて設定される。
According to the apparatus shown in FIGS. 1 and 2, the wall thickness of the tube 1 can be measured by using a single probe 4 and the ultrasonic thickness gauge 5, and also the thickness of the tube 1 can be measured by The lining thickness can be easily calculated by calculating the measurement result of the change in total energy loss δΔP r and the pipe thickness using the calculator 9. Further, the energy loss of the reflected wave can be extracted by the gate analog output of a normal ultrasonic flaw detector used as the ultrasonic detector 6. The gate is set according to the pipe diameter value input in advance.

第3図はセメントモルタルライニングされたダ
クタイル鋳鉄管における管厚によるエネルギ損失
の測定結果を示し、また第4図は同鋳鉄管におけ
るライニング厚によるエネルギ損失の測定結果を
示す。第4図より、1mmの精度によつてライニン
グ厚を測定可能なことが理解される。
FIG. 3 shows the measurement results of energy loss depending on the pipe thickness in a ductile cast iron pipe lined with cement mortar, and FIG. 4 shows the measurement results of the energy loss depending on the lining thickness in the same cast iron pipe. From FIG. 4, it is understood that the lining thickness can be measured with an accuracy of 1 mm.

なお、本発明によると、ライニング厚を測定し
てその減厚を調査する場合のみならず、管内の付
着物による管実内径の減少をも測定できる。
Note that, according to the present invention, it is possible not only to measure the lining thickness and investigate the decrease in the thickness, but also to measure the decrease in the inner diameter of the tube due to deposits inside the tube.

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

図面は本発明の一実施例を示し、第1図は超音
波探触子を管表面に設置した状態を示す図、第2
図は測定装置のシステム図、第3図は管厚による
エネルギ損失の測定結果を示す図、第4図はライ
ニング厚によるエネルギ損失の測定結果を示す図
である。 1……管、2……ライニング、3……水、4…
…超音波探触子、6……超音波検知器(超音波探
傷器)、13……ライニング面。
The drawings show one embodiment of the present invention, and FIG. 1 shows an ultrasonic probe installed on the tube surface, and FIG.
This figure is a system diagram of the measuring device, FIG. 3 is a diagram showing the measurement results of energy loss due to pipe thickness, and FIG. 4 is a diagram showing the measurement results of energy loss due to lining thickness. 1...Pipe, 2...Lining, 3...Water, 4...
...Ultrasonic probe, 6... Ultrasonic detector (ultrasonic flaw detector), 13... Lining surface.

Claims (1)

【特許請求の範囲】[Claims] 1 内面にライニングが施された充水状態の鉄管
の表面に超音波探触子を設置して管径方向に超音
波を発し、対向側のライニング内面からの反射波
のエネルギ損失を検出するに際し、管表面と探触
子との接触面の状況と、管内の水の物性と、管の
材質と、管の口径と、ライニングの材質とを一定
であるとするとともに、管厚を既知であるとし
て、これらにもとづくエネルギ損失の値をあらか
じめ把握しておき、ライニング厚とエネルギ損失
との関係をあらかじめ求めておき、そして、検出
されたエネルギ損失値から前記あらかじめ把握さ
れたエネルギ損失値を減じて、その差からライニ
ング厚を求めることを特徴とする管内面ライニン
グ厚の測定方法。
1. An ultrasonic probe is installed on the surface of a water-filled iron pipe that is lined on the inside, emits ultrasonic waves in the pipe radial direction, and detects the energy loss of reflected waves from the inner surface of the lining on the opposite side. Assume that the condition of the contact surface between the tube surface and the probe, the physical properties of the water in the tube, the tube material, the tube diameter, and the lining material are constant, and the tube thickness is known. As such, the value of energy loss based on these is known in advance, the relationship between lining thickness and energy loss is determined in advance, and the previously determined energy loss value is subtracted from the detected energy loss value. , a method for measuring the inner surface lining thickness of a tube, characterized by determining the lining thickness from the difference.
JP23240483A 1983-12-08 1983-12-08 Measuring method of thickness of lining on inner surface of pipe Granted JPS60123712A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23240483A JPS60123712A (en) 1983-12-08 1983-12-08 Measuring method of thickness of lining on inner surface of pipe

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23240483A JPS60123712A (en) 1983-12-08 1983-12-08 Measuring method of thickness of lining on inner surface of pipe

Publications (2)

Publication Number Publication Date
JPS60123712A JPS60123712A (en) 1985-07-02
JPH0227604B2 true JPH0227604B2 (en) 1990-06-19

Family

ID=16938711

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23240483A Granted JPS60123712A (en) 1983-12-08 1983-12-08 Measuring method of thickness of lining on inner surface of pipe

Country Status (1)

Country Link
JP (1) JPS60123712A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB8603010D0 (en) * 1986-02-06 1986-03-12 Britoil Plc Ultrasonic thickness meter
US4669310A (en) * 1986-03-26 1987-06-02 The Babcock & Wilcox Company High frequency ultrasonic technique for measuring oxide scale on the inner surface of boiler tubes
US5661241A (en) * 1995-09-11 1997-08-26 The Babcock & Wilcox Company Ultrasonic technique for measuring the thickness of cladding on the inside surface of vessels from the outside diameter surface

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
BE817121A (en) * 1974-07-01 1974-11-04 DEVICE FOR MEASURING THE PARAMETERS OF THE TALUS OF MATERIAL CONTAINED IN A CYLINDER DRIVEN IN ROTATION AROUND ITS AXIS
JPS5435506A (en) * 1977-08-24 1979-03-15 Toshiba Corp Balancer of turbine rotor

Also Published As

Publication number Publication date
JPS60123712A (en) 1985-07-02

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