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JPH0546883B2 - - Google Patents
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JPH0546883B2 - - Google Patents

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Publication number
JPH0546883B2
JPH0546883B2 JP60196956A JP19695685A JPH0546883B2 JP H0546883 B2 JPH0546883 B2 JP H0546883B2 JP 60196956 A JP60196956 A JP 60196956A JP 19695685 A JP19695685 A JP 19695685A JP H0546883 B2 JPH0546883 B2 JP H0546883B2
Authority
JP
Japan
Prior art keywords
phase fluid
group
vibration
tubes
void
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
JP60196956A
Other languages
Japanese (ja)
Other versions
JPS6256825A (en
Inventor
Hironori Shiohata
Shozo Nakamura
Yasuo Mizushina
Michio Kuroda
Noriaki Wada
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP60196956A priority Critical patent/JPS6256825A/en
Publication of JPS6256825A publication Critical patent/JPS6256825A/en
Publication of JPH0546883B2 publication Critical patent/JPH0546883B2/ja
Granted legal-status Critical Current

Links

Classifications

    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E30/00Energy generation of nuclear origin
    • Y02E30/30Nuclear fission reactors

Landscapes

  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
  • Monitoring And Testing Of Nuclear Reactors (AREA)

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は、管群等の異常振動診断方法および装
置に係り、特に、原子力発電プラントにおける冷
却水系統のように、流体が管が構造物の外側を流
れしかもその流体が気体と液体の混在するいわゆ
る二相流体の状態にあるときに、管群や構造物に
発生する異常振動の診断方法および装置に関す
る。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a method and apparatus for diagnosing abnormal vibrations in pipe groups, etc., and in particular, in cases where fluid is piped into a structure, such as a cooling water system in a nuclear power plant. The present invention relates to a method and apparatus for diagnosing abnormal vibrations that occur in a group of pipes or structures when the fluid flows outside and is in a so-called two-phase fluid state in which gas and liquid are mixed.

〔発明の背景〕 熱交換器中の伝熱管群が原子炉内の構造物は、
その外側を流れる流体が、二相流動雰囲気になつ
ている部分が多い。
[Background of the Invention] A group of heat transfer tubes in a heat exchanger is a structure inside a nuclear reactor.
In many parts, the fluid flowing outside is in a two-phase flow atmosphere.

管内を流れる二相流に関する研究や文献は数多
い。ところが、管外を流れる場合については、気
泡流、スラグ流、フロス流、環状流等の流動様式
の分類さえも正確には定められておらず、その判
定も定性的な状態にある。
There are many studies and documents related to two-phase flow inside pipes. However, in the case of flow outside the pipe, even the classification of flow modes such as bubble flow, slug flow, froth flow, annular flow, etc. has not been accurately determined, and the determination thereof is still in a qualitative state.

本発明は、主に管外を流れる二相流に関するも
のであるが、上記のような研究の現状であるか
ら、とりあえず、管内垂直上昇流における二相流
の流動様式を参考として第2図に示す。これら二
相流状態においては、流れの乱れにより、定常的
な励振力が発生し、管や構造物が加振され、振動
する。二相流体の乱れにより発生する累振力の周
波数が管群や構造物の固有振動数に一致したと
き、管群や構造物の振動が大きくなり、異常振動
発生の原因ともなる。異常振動の結果、管と管と
の衝突、あるいは管または構造物支持部の破損が
生ずる惧れがある。
The present invention mainly relates to two-phase flow flowing outside a pipe, but since the current state of the research is as described above, for the time being, the flow pattern of two-phase flow in a vertical upward flow inside a pipe is shown in Figure 2 as a reference. show. In these two-phase flow states, a steady excitation force is generated due to flow turbulence, and the pipes and structures are excited and vibrate. When the frequency of the cumulative force generated by the turbulence of the two-phase fluid matches the natural frequency of the tube group or structure, the vibration of the tube group or structure increases, causing abnormal vibrations. Abnormal vibrations may result in pipe-to-pipe collisions or damage to the pipes or structural supports.

第3図に、a気泡流およびbスラグ流の流動様
式に対する励振力のパワースペクトル密度を示
す。気泡流においては、10Hz以下のピークと60Hz
付近のピークをが存在する。スラグ流において
は、5Hz以下のピークが存在する。一般に、機器
における二相流には、第2図に示した各二相流の
流動様式が単独に存在するわけではなく、むしろ
混在していることが多い。このため二相流体の励
振力の周波数も上記混在する流動様式に対応する
スペクトルを有する。一方、管群または構造物の
固有振動数は、気体と液体の混合割合を示すボイ
ド率により変化する。
FIG. 3 shows the power spectrum density of the excitation force for the flow modes of a bubble flow and b slug flow. In bubble flow, peaks below 10Hz and 60Hz
There are nearby peaks. In the slug flow, a peak of 5 Hz or less exists. Generally, in a two-phase flow in a device, the flow modes of each two-phase flow shown in FIG. 2 do not exist independently, but rather often exist in a mixture. Therefore, the frequency of the excitation force of the two-phase fluid also has a spectrum corresponding to the above-mentioned mixed flow modes. On the other hand, the natural frequency of a tube group or structure changes depending on the void ratio, which indicates the mixing ratio of gas and liquid.

そこで、二相流体の励振力により発生する管群
や構造物の振動周波数分析とボイド率を考慮した
固有振動数の解析結果とを比較すると、管群や構
造物に発生した異常振動の原因が、過大な励振力
か共振現象かを判別可能になると考えられる。
Therefore, by comparing the vibration frequency analysis of pipe groups and structures generated by the excitation force of two-phase fluid with the analysis results of natural frequencies that take void ratio into consideration, it is possible to determine the cause of abnormal vibrations occurring in pipe groups and structures. It is thought that it will be possible to distinguish between excessive excitation force and resonance phenomenon.

なお、上記文献の一例としては、白木他、「二
相流を受ける熱交換器管群の振動」、三菱重工技
報、Vol.19、No.5がある。
An example of the above-mentioned literature is Shiraki et al., "Vibration of heat exchanger tube group subjected to two-phase flow," Mitsubishi Heavy Industries Technical Report, Vol. 19, No. 5.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、二相流体の状態にある管群ま
たは構造物の異常振動発生の原因を特定するため
の異常振動診断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 an abnormal vibration diagnosing method and apparatus for identifying the cause of abnormal vibration in a group of pipes or structures in a two-phase fluid state.

〔発明の概要〕[Summary of the invention]

上記目的を達成するために、本発明は、管群ま
たは構造物の二相流体中の振動を計測しその周波
数を分析する一方、二相流体のボイド率を計測し
このボイド率に対応する管群または構造物の固有
振動数を算出して、振動周波数および固有振動数
を比較することにより、異常振動発生原因を診断
することを特徴とする。
In order to achieve the above object, the present invention measures vibrations in a two-phase fluid of a pipe group or a structure and analyzes its frequency, while also measuring the void ratio of the two-phase fluid and pipes corresponding to this void ratio. It is characterized by diagnosing the cause of abnormal vibration by calculating the natural frequency of a group or structure and comparing the vibration frequency and the natural frequency.

〔発明の実施例〕[Embodiments of the invention]

管外を流れる二相流体に適用した本発明の実施
例を、第1図を参照して詳細に説明する。第1図
は、本発明による異常振動診断装置のブロツク図
である。図において、1は管または構造物、2は
気体と液体の混在する気液二相流体、3はボイド
センサ、4は振動センサ、5は振動計、6は振動
分析器、7はボイド計、8は演算器、9は表示器
である。
An embodiment of the present invention applied to a two-phase fluid flowing outside a tube will be described in detail with reference to FIG. FIG. 1 is a block diagram of an abnormal vibration diagnosis apparatus according to the present invention. In the figure, 1 is a pipe or structure, 2 is a gas-liquid two-phase fluid containing a mixture of gas and liquid, 3 is a void sensor, 4 is a vibration sensor, 5 is a vibration meter, 6 is a vibration analyzer, 7 is a void meter, 8 is a computing unit, and 9 is a display.

二相流体2の乱れによつて発生した管または構
造物1の振動信号は、振動センサ4により検出さ
れ、振動計5で増幅され、振動分析器6において
周波数分析にかけられる。一方、二相流体2のボ
イド信号はボイドセンサ3により検出され、ボイ
ド計7においてボイド率を算出される。演算器8
は、このボイド率を用いて、管または構造物の固
有振動数を求める。固有振動数の求め方について
は後述する。求めた固有振動数と先の振動分析結
果と演算器9に同時に表示する。
A vibration signal of the pipe or structure 1 generated by the turbulence of the two-phase fluid 2 is detected by a vibration sensor 4, amplified by a vibration meter 5, and subjected to frequency analysis in a vibration analyzer 6. On the other hand, a void signal of the two-phase fluid 2 is detected by a void sensor 3, and a void ratio is calculated by a void meter 7. Arithmetic unit 8
calculates the natural frequency of the pipe or structure using this void fraction. The method for determining the natural frequency will be described later. The obtained natural frequency and the previous vibration analysis results are displayed on the calculator 9 at the same time.

第4図にその表示例を示す。第4図の表示例に
おいて、分析結果と二相流体のボイド率から得ら
れる固有振動数が一致しているとき、管は共振状
態にあると診断できる。一方、分析結果の振動ピ
ークが固有振動数と一致しないとき、管に作用す
る励振力は二相流特有の異常な励振力であると診
断できる。
FIG. 4 shows an example of the display. In the display example of FIG. 4, when the analysis result and the natural frequency obtained from the void fraction of the two-phase fluid match, it can be diagnosed that the pipe is in a resonant state. On the other hand, when the vibration peak in the analysis results does not match the natural frequency, it can be diagnosed that the excitation force acting on the pipe is an abnormal excitation force specific to two-phase flow.

次に、演算器8を用いて管または構造物の固有
振動数を求める簡易計算方法について述べる。
Next, a simple calculation method for determining the natural frequency of a pipe or structure using the calculator 8 will be described.

まず、記号の定義をしておくと、 m:管の質量 mTP、ma、mw:付加質量 k:管のばね定数 ρ:液体密度 γ:ボイド率 ω、ωa、ωw、ωTP:管の固有振動数 a:空気中 w:水中 TP:二相流体中 さて、管または構造物がばね−質量系の力学モ
デルに置き換えられたとすると、管の固有振動数
ωは、 ω2=k/m ……(1) で与えられる。また水中における管の固有振動数
ωwは、水の付加質量をmwとすると、 ωw 2=k/(m+mw) ……(2) で得られる。二相流体中の付加質量mTP、空気中
および水中の付加質量にボイド率を導入して、 mTP=γma+(1−γ)mw ……(3) となる。この結果、二相流体中の管の固有振動数
ωTPは ωTP 2=k/(m+mTP =k/m+γma+(1−γ)mw ……(4) で求められる。式(4)は書き換えると、次式にな
る。
First, let's define the symbols: m: mass of the pipe m TP , m a , m w : additional mass k: spring constant of the pipe ρ: liquid density γ: void ratio ω, ω a , ω w , ω TP : natural frequency of the pipe a: in air w: water TP: in two-phase fluid Now, if the pipe or structure is replaced by a mechanical model of a spring-mass system, the natural frequency ω of the pipe is ω 2 =k/m...(1) is given by. Further, the natural frequency ω w of the pipe in water is obtained as follows, where m w is the added mass of water: ω w 2 =k/(m+m w ) (2). Introducing void fraction to the additional mass m TP in the two-phase fluid and the additional mass in air and water, m TP = γm a + (1-γ)m w ...(3). As a result, the natural frequency ω TP of the pipe in the two-phase fluid is determined by ω TP 2 =k/(m+m TP =k/m+γm a +(1−γ)m w ……(4). Equation (4) ) can be rewritten as the following formula.

ωTP 2=k/m{1+γma/m+(1−γ)mw/m}
……(5) 空気中の付加質量maは微小であり、この結果
mam≪1≒0となる。これより式(5)は、 ωTP 2=k/m{1+(1−γ)mw/m} =ω2/1+(1−γ)mw/m ……(6) となる。式(2)より、 mw/m=(ω/ωw2−1 ……(7) を得る。式(7)を式(6)を代入して ωTP 2=ω2/1+(1−γ){(ω/ωw2−1}……
(8) を得る。また管の空気中の固有振動数はma/m
≪1の関係から、近似的に式(1)で得られる値と同
じである。この結果、管1の空気中および水中の
固有振動数を事前に求めておけば、ボイド率γに
おける管の固有振動数を容易に算出できる。
ω TP 2 =k/m{1+γm a /m+(1-γ)m w /m}
...(5) The additional mass m a in the air is small, and as a result
m a m≪1≒0. From this, equation (5) becomes ω TP 2 =k/m{1+(1-γ)m w /m} = ω 2 /1+(1-γ) m w /m (6). From equation (2), m w /m=(ω/ω w ) 2 −1 ...(7) is obtained. Substituting equation (7) into equation (6), ω TP 2 = ω 2 /1+(1-γ) {(ω/ω w ) 2 −1}...
(8) is obtained. Also, the natural frequency of the tube in the air is m a /m
From the relationship <<1, it is approximately the same as the value obtained by equation (1). As a result, if the natural frequencies of the tube 1 in air and water are determined in advance, the natural frequency of the tube at the void ratio γ can be easily calculated.

式(8)中において、空気中および水中にある管の
固有振動数算出にあたつては、実験的あるいは構
造解析等の計算プログラムを用いてもよい。また
空気中(気体)の付加質量が無視できない場合、
式(8)は次式で置き換えられる。
In formula (8), calculation programs such as experimental or structural analysis may be used to calculate the natural frequencies of the pipes in air and water. Also, if the additional mass in the air (gas) cannot be ignored,
Equation (8) can be replaced by the following equation.

ωTP 2=ω2/1+γ{(ω/ωa2−1}+
(1−γ){(ω/ωw2−1}……(9) 式(9)によれば、二相流体中において気体中の付
加質量効果を無視できない場合の固有振動数が求
められる。
ω TP 2 = ω 2 /1+γ{(ω/ω a ) 2 −1}+
(1−γ) {(ω/ω w ) 2 −1}……(9) According to equation (9), the natural frequency when the added mass effect in gas cannot be ignored in a two-phase fluid is found. It will be done.

〔発明の効果〕〔Effect of the invention〕

本発明の異常振動診断方法および装置において
は、二相流体中の管群等の振動を計測してその振
動周波数を分析する一方、二相流体のボイド率を
計算して管の固有振動数を求め、これら振動周波
数と固有振動数とを比較するので、二相流体によ
り発生した管の異常振動が管の固有振動数との共
振によるものか二相流体の異常励振力によるもの
かを適確に診断できる。
In the abnormal vibration diagnosis method and apparatus of the present invention, the vibration of a group of tubes in a two-phase fluid is measured and the vibration frequency is analyzed, while the void fraction of the two-phase fluid is calculated to determine the natural frequency of the tube. Since these vibration frequencies are compared with the natural frequency, it is possible to accurately determine whether the abnormal vibration of the pipe caused by the two-phase fluid is due to resonance with the natural frequency of the pipe or the abnormal excitation force of the two-phase fluid. can be diagnosed.

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

第1図は本発明による異常振動診断装置の一実
施例を示すブロツク図、第2図は管内垂直上昇流
における二相流の流動様式を示す図、第3図は気
泡流およびスラグ流の流動様式に対する励振力の
パワースペクトル密度を示す図、第4図は振動分
析結果と固有振動数とを表示器に同時に表示した
例を示す図である。 1……管群、2……二相流体、3……ボイドセ
ンサ、4……振動センサ、5……振動計、6……
振動分析器、7……ボイド計、8……演算器、9
……表示器。
Figure 1 is a block diagram showing an embodiment of the abnormal vibration diagnosis device according to the present invention, Figure 2 is a diagram showing the flow pattern of two-phase flow in vertical upward flow in a pipe, and Figure 3 is a diagram showing the flow of bubble flow and slag flow. FIG. 4 is a diagram showing the power spectrum density of the excitation force with respect to the mode, and FIG. 4 is a diagram showing an example in which the vibration analysis result and the natural frequency are displayed on the display at the same time. 1... Tube group, 2... Two-phase fluid, 3... Void sensor, 4... Vibration sensor, 5... Vibration meter, 6...
Vibration analyzer, 7... Void meter, 8... Arithmetic unit, 9
……display.

Claims (1)

【特許請求の範囲】 1 二相流体中の管群等の振動を計測しその周波
数を分析する一方、二相流体のボイド率を計測し
このボイド率に対応する管群等の固有振動数を算
出して、前記周波数分析結果とこの固有振動数と
を比較し、二相流体中の管群等の振動の原因が管
群等の共振か二相流体の異常励振力かを判定する
ことを特徴とする管群等の異常振動診断方法。 2 特許請求の範囲第1項において、空気中の管
群等の固有振動数と水中の管群等の固有振動数と
を予め求めておき、二相流体のボイド率に応じて
それらの算入比率を変え、二相流体中の管群等の
固有振動数を算出することを特徴とする管群等の
異常振動診断方法。 3 二相流体中に置かれた管群等の振動を検出す
る振動センサと、検出振動信号を増幅する振動計
と、増幅された信号を周波数分析する振動分析器
と、前記二相流体のボイドを検出するボイドセン
サと、ボイドセンサの信号からボイド率を得るボ
イド計と、そのボイド率をもとに二相流体中の管
群等の固有振動数を算出する演算器と、前記振動
分析器と演算器との出力を重ね合わせて表示する
表示器とからなり、周波数分析結果に生じたピー
ク値と固有振動数とが一致するか否かにより二相
流体中の管群等の振動原因を特定することを特徴
とする管群等の異常振動診断装置。
[Scope of Claims] 1. Vibration of a group of tubes, etc. in a two-phase fluid is measured and its frequency is analyzed, while the void ratio of the two-phase fluid is measured and the natural frequency of the group of tubes, etc. corresponding to this void ratio is determined. The frequency analysis result is compared with this natural frequency to determine whether the cause of vibration of the tube group, etc. in the two-phase fluid is resonance of the tube group, etc. or abnormal excitation force of the two-phase fluid. Characteristic method for diagnosing abnormal vibrations in tube groups, etc. 2 In claim 1, the natural frequencies of a group of tubes, etc. in air and the natural frequencies of a group of tubes, etc. in water are determined in advance, and their inclusion ratio is determined according to the void ratio of the two-phase fluid. A method for diagnosing abnormal vibrations in a group of tubes, etc., characterized in that the natural frequency of the group of tubes, etc. in a two-phase fluid is calculated by changing the . 3 A vibration sensor that detects vibrations of a group of tubes placed in a two-phase fluid, a vibration meter that amplifies the detected vibration signal, a vibration analyzer that analyzes the frequency of the amplified signal, and a void in the two-phase fluid. a void sensor that detects the void ratio, a void meter that obtains the void ratio from the signal of the void sensor, a calculator that calculates the natural frequency of a group of tubes, etc. in a two-phase fluid based on the void ratio, and the vibration analyzer. It consists of a display device that superimposes and displays the output of the computer and the computer, and the cause of vibration in a group of tubes in a two-phase fluid can be determined based on whether the peak value generated in the frequency analysis result matches the natural frequency. An apparatus for diagnosing abnormal vibrations of pipe groups, etc.
JP60196956A 1985-09-06 1985-09-06 Abnormal vibration diagnosis method and device for pipe groups, etc. Granted JPS6256825A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60196956A JPS6256825A (en) 1985-09-06 1985-09-06 Abnormal vibration diagnosis method and device for pipe groups, etc.

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60196956A JPS6256825A (en) 1985-09-06 1985-09-06 Abnormal vibration diagnosis method and device for pipe groups, etc.

Publications (2)

Publication Number Publication Date
JPS6256825A JPS6256825A (en) 1987-03-12
JPH0546883B2 true JPH0546883B2 (en) 1993-07-15

Family

ID=16366442

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60196956A Granted JPS6256825A (en) 1985-09-06 1985-09-06 Abnormal vibration diagnosis method and device for pipe groups, etc.

Country Status (1)

Country Link
JP (1) JPS6256825A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
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JP2003344363A (en) * 2002-05-30 2003-12-03 Ishikawajima Harima Heavy Ind Co Ltd Flow pattern discrimination method for gas-liquid two-phase flow

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