JPH04268496A - Device and method for diagnostic abnormality of reactor - Google Patents
Device and method for diagnostic abnormality of reactorInfo
- Publication number
- JPH04268496A JPH04268496A JP3028571A JP2857191A JPH04268496A JP H04268496 A JPH04268496 A JP H04268496A JP 3028571 A JP3028571 A JP 3028571A JP 2857191 A JP2857191 A JP 2857191A JP H04268496 A JPH04268496 A JP H04268496A
- Authority
- JP
- Japan
- Prior art keywords
- steam generator
- steam
- piping
- main steam
- leakage
- 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.)
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Links
Classifications
-
- Y—GENERAL 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
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E30/00—Energy generation of nuclear origin
- Y02E30/30—Nuclear fission reactors
Landscapes
- Monitoring And Testing Of Nuclear Reactors (AREA)
Abstract
Description
【0001】[発明の目的][Object of the invention]
【0002】0002
【産業上の利用分野】本発明は加圧水型原子炉(以下、
PWRと記す)における蒸気発生器内の伝熱管からの一
次系冷却材の漏洩を診断する原子炉の異常診断装置およ
びその診断方法に関する。[Industrial Application Field] The present invention relates to a pressurized water nuclear reactor (hereinafter referred to as
The present invention relates to a nuclear reactor abnormality diagnosis device and its diagnosis method for diagnosing leakage of primary coolant from heat transfer tubes in a steam generator in a nuclear reactor (referred to as PWR).
【0003】0003
【従来の技術】図1により従来の加圧水型原子力発電所
の概略を説明する。図中、符号1は原子炉建屋、2は原
子炉格納容器、3は原子炉容器をそれぞれ示している。
原子炉容器3内の炉心4で加熱された一次系冷却材は一
次系配管5を流れて蒸気発生器6内の伝熱管7に流入す
る。蒸気発生器6内の二次系冷却材は伝熱管7と熱交換
して加熱され高温蒸気となって二次系主蒸気配管8を流
れてタービン9へ流入する。タービン9は回転し、発電
機10を駆動して発電する。タービン9で仕事を終えた
蒸気は復水器11に流入し冷却されて復水となる。この
復水は二次系給水管12を流れて蒸気発生器6へ二次系
冷却材として給水される。一方、蒸気発生器6内の伝熱
管7を流れる一次系冷却材は二次系冷却材と熱交換して
冷却され、一次系主冷却配管13からポンプ14により
原子炉容器3内に冷却して炉心4で加熱される。なお、
図中15は制御棒、16は加圧器、17はスプレー管を
それぞれ示している。又、22は排ガス系抽気配管、2
3はタービン排ガス系モニタで、排ガス中の放射性物質
を測定するものである。2. Description of the Related Art A conventional pressurized water nuclear power plant will be schematically explained with reference to FIG. In the figure, reference numeral 1 indicates a reactor building, 2 indicates a reactor containment vessel, and 3 indicates a reactor vessel. The primary coolant heated in the reactor core 4 in the reactor vessel 3 flows through the primary system piping 5 and flows into the heat transfer tube 7 in the steam generator 6 . The secondary coolant in the steam generator 6 exchanges heat with the heat exchanger tubes 7 and is heated to become high-temperature steam, which flows through the secondary main steam piping 8 and flows into the turbine 9. The turbine 9 rotates and drives the generator 10 to generate electricity. The steam that has completed its work in the turbine 9 flows into the condenser 11, where it is cooled and becomes condensed water. This condensate flows through the secondary system water supply pipe 12 and is supplied to the steam generator 6 as a secondary system coolant. On the other hand, the primary coolant flowing through the heat transfer tubes 7 in the steam generator 6 is cooled by exchanging heat with the secondary coolant, and is cooled from the primary main cooling pipe 13 into the reactor vessel 3 by the pump 14. It is heated in the reactor core 4. In addition,
In the figure, 15 is a control rod, 16 is a pressurizer, and 17 is a spray pipe. In addition, 22 is an exhaust gas system bleed pipe, 2
3 is a turbine exhaust gas system monitor that measures radioactive substances in the exhaust gas.
【0004】ところで、蒸気発生器6内には逆U字状の
細管からなる多数本の伝熱管7が管板に取着されており
、これらの伝熱管7の全数について定期検査時に点検を
行い健全性を確認している。原子炉運転中に仮に伝熱管
7が破損して一次系冷却材の漏洩が発生した場合、漏洩
した放射性物質は二次系主蒸気配管8を通り、タービン
9へ移行し、さらに復水器11を通り給水系に戻ること
になる。PWRでは復水器11から一部の蒸気(ガス)
を排ガス系抽気配管22を通し抽気しており、抽気した
蒸気中に放射性物質が警報設定値以上含まれている場合
には排ガスモニタ23により警報が発せられるように構
成している。By the way, in the steam generator 6, a large number of heat transfer tubes 7 made of inverted U-shaped thin tubes are attached to a tube plate, and all of these heat transfer tubes 7 are inspected during regular inspections. The soundness has been confirmed. If the heat transfer tubes 7 are damaged during reactor operation and primary coolant leaks, the leaked radioactive materials will pass through the secondary main steam piping 8 and move to the turbine 9, and then to the condenser 11. It will return to the water supply system through. In PWR, some steam (gas) from condenser 11
The exhaust gas monitor 23 is configured to issue an alarm if the extracted steam contains radioactive substances exceeding a set alarm value.
【0005】[0005]
【発明が解決しようとする課題】従来のPWRでは、一
次系冷却材が漏洩した場合、放射性物質が排ガスモニタ
23警報設定値を超える量の漏洩に達した時点において
警報が発せられることになる。ところが、図1に示した
ように排ガスモニタ23は二次系の系統でも終端部の復
水器11から導出された排ガス系抽気配管22に位置し
ている。
蒸気発生器6内の伝熱管7の破損に伴って二次系に漏洩
する一次系冷却材の主要線源核種であるN16(半減期
7秒)やC15(半減期2秒)のような短半減期核種は
、排ガスモニタ23に到達するまで減衰して、ほとんど
計測されなくなる。このため、一次系冷却材の漏洩によ
る排ガスモニタ23が対象としている放射性核種は希ガ
ス,腐食生成物,核分裂生成物等である。ところが、一
次系冷却材中に存在するこれらの放射性核種はN16や
C15に比べて、もともと量が少ない上に主蒸気中に漏
洩した一部を抽気して測定していることから、微量の漏
洩に際しては検知し難くなっている。このように、微量
漏洩による異常徴候が検知できない装置となっている。
又、漏洩した放射性物質の濃度および異常の状態を把握
できない等の課題がある。[Problems to be Solved by the Invention] In the conventional PWR, when the primary coolant leaks, an alarm is issued when the amount of radioactive material leaked exceeds the alarm setting value of the exhaust gas monitor 23. However, as shown in FIG. 1, the exhaust gas monitor 23 is located in the exhaust gas system bleed pipe 22 led out from the condenser 11 at the terminal end even in the secondary system. Short-term radionuclides such as N16 (half-life: 7 seconds) and C15 (half-life: 2 seconds), which are the main source nuclides of the primary system coolant, leak into the secondary system due to damage to the heat transfer tubes 7 in the steam generator 6. The half-life nuclide decays until it reaches the exhaust gas monitor 23 and is hardly measured. Therefore, the radionuclides targeted by the exhaust gas monitor 23 due to leakage of the primary coolant are rare gases, corrosion products, nuclear fission products, and the like. However, the amount of these radionuclides present in the primary coolant is smaller than that of N16 and C15, and since the part of the radioactive nuclides that leaked into the main steam is extracted and measured, it is possible that a trace amount of leakage may occur. It becomes difficult to detect. In this way, the device is unable to detect any signs of abnormality due to trace leakage. Additionally, there are problems such as the inability to grasp the concentration of leaked radioactive materials and abnormal conditions.
【0006】本発明は上記課題を解決するためになされ
たもので、加圧水型原子炉における蒸気発生器内の伝熱
管からの一次系冷却材の微量漏洩を速やかに検知するこ
とができる原子炉の異常診断装置およびその診断方法を
提供することにある。
[発明の構成]The present invention has been made to solve the above-mentioned problems, and is a nuclear reactor that can quickly detect a small amount of leakage of primary coolant from a heat transfer tube in a steam generator in a pressurized water reactor. An object of the present invention is to provide an abnormality diagnosis device and a diagnosis method thereof. [Structure of the invention]
【0007】[0007]
【課題を解決するための手段】第1の本発明は加圧水型
原子炉容器に一次系配管を介して加圧器および蒸気発生
器が接続され、この蒸気発生器の二次系出口からタービ
ンまでに二次系主蒸気配管が接続され、この二次系主蒸
気配管に放射線検出器が接続され、この放射線検出器に
演算処理系が接続されてなることを特徴とする。[Means for Solving the Problems] In the first aspect of the present invention, a pressurizer and a steam generator are connected to a pressurized water reactor vessel via a primary system piping, and from the secondary system outlet of the steam generator to the turbine. It is characterized in that a secondary main steam piping is connected, a radiation detector is connected to the secondary main steam piping, and a calculation processing system is connected to the radiation detector.
【0008】第2の本発明は加圧水型原子炉容器に一次
系配管を介して加圧器および蒸気発生器が接続され、こ
の蒸気発生器の二次系出口からタービンまでに接続され
た二次系主蒸気配管に測定点として少なくとも2個の放
射線検出器を設け、これらの放射線検出器で検出した短
半減期核種を線源核種として測定したそれぞれの線量率
の減衰率から蒸気流速を算出し、前記測定点における放
射能濃度を蒸気発生器の二次系出口まで逆算して算出す
ることを特徴とする。[0008] In the second aspect of the present invention, a pressurizer and a steam generator are connected to a pressurized water reactor vessel via a primary system piping, and a secondary system is connected from a secondary system outlet of the steam generator to a turbine. At least two radiation detectors are installed as measurement points in the main steam piping, and the steam flow rate is calculated from the attenuation rate of each dose rate measured using short half-life nuclides detected by these radiation detectors as source nuclides, The method is characterized in that the radioactivity concentration at the measurement point is calculated by back-calculating up to the secondary system outlet of the steam generator.
【0009】[0009]
【作用】第1の発明における異常診断装置では、放射線
検出器を二次系主蒸気配管の流路の上流側(蒸気発生器
に近い位置)に設置し、短半減期核種のN16やC15
が減衰する前に検知することにより、微量の放射性物質
漏洩に伴う初期徴候の診断が可能となる。これは、蒸気
発生器内の伝熱管破損による主蒸気へ漏洩する一次系冷
却材には放射性の希ガス,腐食生成物,核分裂生成物,
N16やC15等が含まれるが、通常原子炉運転時の一
次系冷却材単位体積当りに含まれるN16やC15の量
は最も多く、且つ主蒸気系へ移行しやすいため早期発見
が可能となる。次に、二次系主蒸気配管からの線量率は
その配管中の放射能濃度に比例することから、予め計算
により任意の濃度で測定点における線量率を求め、放射
線検出器により得られた線量率の実測値と前記計算によ
り算出された線量率の計算値との比(実測値/計算値)
を前記計算の際に用いた濃度に規格化して実測値の線量
率に対する放射能濃度を演算処理系により算出する。[Operation] In the abnormality diagnosis device according to the first invention, the radiation detector is installed on the upstream side of the flow path of the secondary main steam piping (at a position close to the steam generator), and the
By detecting radioactivity before it decays, it becomes possible to diagnose early signs associated with the leakage of minute amounts of radioactive material. This means that the primary coolant that leaks into the main steam due to heat exchanger tube breakage in the steam generator contains radioactive rare gases, corrosion products, nuclear fission products, etc.
It contains N16, C15, etc., but the amount of N16 and C15 contained per unit volume of primary system coolant during normal reactor operation is the largest, and because it easily transfers to the main steam system, early detection is possible. Next, since the dose rate from the secondary main steam piping is proportional to the radioactivity concentration in that piping, the dose rate at the measurement point is determined at an arbitrary concentration by calculation in advance, and the dose rate obtained by the radiation detector is calculated in advance. Ratio between the measured value of the dose rate and the calculated value of the dose rate calculated by the above calculation (actual value/calculated value)
is normalized to the concentration used in the calculation, and a calculation processing system calculates the radioactivity concentration for the dose rate of the actual measurement value.
【0010】第2の発明における異常診断方法では、複
数箇所の放射線検出器で測定することにより、まず得ら
れたデータの自己診断を行う。これは、漏洩が発生した
場合、主蒸気の流路に沿って上流,下流の順番で測定値
に変化が現れ、到達時間の差分だけ測定値に差が出てく
ることになるが、放射線検出器の故障又はノイズであれ
ば一方の測定結果にしか現れないことから判断する。次
に、その値が正常な状態の値に比べ有意な差があれば、
漏洩と判定されるとともに測定値の差(減衰率)より上
流側の測定点から下流側の測定点までの蒸気の到達時間
が算出できる。漏洩放射能量を推定する方法を示す。[0010] In the abnormality diagnosis method in the second aspect of the invention, self-diagnosis is first performed on the data obtained by measuring with radiation detectors at a plurality of locations. This means that if a leak occurs, the measured values will change in the order of upstream and downstream along the main steam flow path, and the measured values will differ by the difference in arrival time, but radiation detection If it is a device failure or noise, it can be determined because it only appears in one measurement result. Next, if the value is significantly different from the normal value,
It is determined that there is a leak, and the arrival time of the steam from the upstream measurement point to the downstream measurement point can be calculated from the difference in measured values (attenuation rate). A method for estimating the amount of leaked radioactivity is shown.
【0011】N/N0 =e(−λt)t=ln(N/
N0 )/(−λ)
ここで、N0 は上流側測定値、Nは下流側測定値、λ
は定数で核種によって決まっている。tが上流側の測定
点から下流側の測定点までの蒸気の到達時間である。さ
らに、前記測定点間の流路長さが分っていれば、蒸気の
流速S(m/秒)が以下の式で算出できる。
S=l/t(m/秒)
ここで、lは測定点間の流路長さ(m)、tは前記到達
時間(秒)である。算出された蒸気の流速と測定点から
蒸気発生器の二次系出口までの配管距離をもとに、前記
同様に蒸気の到達時間を求め、先に算出した濃度を逆算
して主蒸気発生器の二次系出口における漏洩放射能量を
推定できる。[0011]N/N0 = e(-λt)t=ln(N/
N0 )/(-λ) Here, N0 is the upstream measured value, N is the downstream measured value, and λ
is a constant and is determined by the nuclide. t is the arrival time of steam from the upstream measuring point to the downstream measuring point. Furthermore, if the length of the flow path between the measurement points is known, the flow velocity S (m/sec) of steam can be calculated using the following formula. S=l/t (m/sec) where l is the flow path length (m) between measurement points, and t is the arrival time (sec). Based on the calculated steam flow velocity and the piping distance from the measurement point to the secondary system outlet of the steam generator, the arrival time of the steam is determined in the same way as above, and the concentration calculated earlier is calculated backwards to reach the main steam generator. The amount of leaked radioactivity at the secondary system outlet can be estimated.
【0012】0012
【実施例】図面を参照しながら本発明の第1および第2
の実施例を説明する。図1は本発明の実施例を含んだ加
圧水型原子力発電所の概略を示している。図中、符号1
は原子炉建屋、2は原子炉格納容器、3は原子炉容器を
それぞれ示している。原子炉容器3内の炉心4で加熱さ
れた一次系冷却材は一次系配管5を流れて蒸気発生器6
内の多数本の伝熱管7に流入する。蒸気発生器6内の二
次系冷却材は伝熱管7と熱交換して加熱され高温蒸気と
なって二次系主蒸気配管8を流れてタービン9へ流入す
る。タービン9は回転し、発電機10を駆動して発電す
る。タービン9で仕事を終えた蒸気は復水器11に流入
し冷却されて復水となる。この復水は二次系給水管12
を流れて蒸気発生器6へ二次系冷却材として給水される
。一方、蒸気発生器6内の伝熱管7を流れる一次系冷却
材は二次系冷却材と熱交換して冷却され、一次系主冷却
配管13からポンプ14により原子炉容器3内に冷却し
て炉心4で加熱される。なお、図中15は制御棒、16
は加圧器、17はスプレー管をそれぞれ示している。[Example] First and second embodiments of the present invention with reference to the drawings
An example will be explained. FIG. 1 schematically shows a pressurized water nuclear power plant including an embodiment of the present invention. In the figure, code 1
2 indicates the reactor building, 2 indicates the reactor containment vessel, and 3 indicates the reactor vessel. The primary coolant heated in the reactor core 4 in the reactor vessel 3 flows through the primary system piping 5 to the steam generator 6.
It flows into a large number of heat exchanger tubes 7 inside. The secondary coolant in the steam generator 6 exchanges heat with the heat exchanger tubes 7 and is heated to become high-temperature steam, which flows through the secondary main steam piping 8 and flows into the turbine 9. The turbine 9 rotates and drives the generator 10 to generate electricity. The steam that has completed its work in the turbine 9 flows into the condenser 11, where it is cooled and becomes condensed water. This condensate is transferred to the secondary system water supply pipe 12
The water is supplied to the steam generator 6 as a secondary coolant. On the other hand, the primary coolant flowing through the heat transfer tubes 7 in the steam generator 6 is cooled by exchanging heat with the secondary coolant, and is cooled from the primary main cooling pipe 13 into the reactor vessel 3 by the pump 14. It is heated in the reactor core 4. In addition, 15 in the figure is a control rod, 16
1 indicates a pressurizer, and 17 indicates a spray tube.
【0013】ここで、第1の実施例(第1の発明)では
二次系主蒸気配管8内の蒸気中の放射能を測定するため
、その配管8に面して、測定点Aとして第1の放射線検
出器18が設けられている。この第1の放射線検出器1
8は演算処理系20に信号ケーブル21によって接続さ
れている。In the first embodiment (first invention), in order to measure the radioactivity in the steam in the secondary main steam pipe 8, a measurement point A is set facing the pipe 8. One radiation detector 18 is provided. This first radiation detector 1
8 is connected to the arithmetic processing system 20 by a signal cable 21.
【0014】第1の実施例における第1の放射線検出器
18の位置は蒸気発生器6の出口6aに近い方が望まし
い。放射線検出器18は電離箱型又はプラスチックシン
チレーション型等を用い線量率又は計数率としてMCS
(マルチチャンネル・スケーリング)モードで連続測定
する。測定データはリアルタイムで同軸ケーブル又は光
ケーブル等の信号ケーブル21でデータの入出力、演算
機能を備えた演算処理装置(パソコン等)で構成する演
算処理系20に転送される。この演算処理系20では平
滑化二次微分等によるピークの探索を行い、正常値の統
計変動の3倍(3σ)を超えるかどうかを一つの基準と
して漏洩の有無を判定するとともに、線量率を放射能濃
度に換算しその値および変化量を出力し、その結果をも
とに漏洩の推移を予測する。又、予め測定対象放射性核
種の一次系冷却材中の放射能濃度と蒸気発生器6内にお
ける二次系主蒸気配管8への移行割合を求めておくこと
により、漏洩した際の主蒸気中の放射能濃度の値から伝
熱管7の破損部の規模を推定できる。The position of the first radiation detector 18 in the first embodiment is preferably close to the outlet 6a of the steam generator 6. The radiation detector 18 uses an ionization chamber type or a plastic scintillation type, and detects MCS as the dose rate or count rate.
(Multi-channel scaling) mode for continuous measurement. Measured data is transferred in real time via a signal cable 21 such as a coaxial cable or an optical cable to an arithmetic processing system 20 comprising an arithmetic processing device (such as a personal computer) equipped with data input/output and arithmetic functions. This arithmetic processing system 20 searches for peaks using smoothed second derivatives, etc., and determines the presence or absence of leakage based on whether the statistical fluctuation exceeds three times (3σ) of the normal value, and determines the dose rate. Convert it to radioactivity concentration, output the value and amount of change, and predict the leakage transition based on the results. In addition, by determining in advance the radioactivity concentration of the radionuclide to be measured in the primary coolant and the transfer rate from the steam generator 6 to the secondary main steam piping 8, it is possible to predict the concentration of the radionuclide in the main steam in the event of a leak. The scale of the damaged portion of the heat exchanger tube 7 can be estimated from the value of the radioactivity concentration.
【0015】しかして、第1の実施例によれば蒸気発生
器6とタービン9をつなぐ二次系主蒸気配管8に面して
、主蒸気の流路に沿って上流側(蒸気発生器に近い位置
)に放射線検出器18を設置した線量率測定系と、この
測定系から得られたデータをもとに正常状態時との比較
を行い漏洩による異常徴候の有無の判断および線量率か
ら測定点における主蒸気中の放射能濃度の算出を行い、
経時変化で処理できる演算処理系とからなっている。も
し、蒸気発生器6内の伝熱管7が破損した場合、一次系
冷却材の放射性物質は数秒で前記放射線検出器18の位
置へ到達することになる。なお、本来から正常状態時に
おける主蒸気中放射能濃度はゼロに等しいので、検出器
の出力は顕著に変化すると思われる。特にN16やC1
5が線源となった場合は放出されるガンマ線のエネルギ
ーが高い(6MeV ,5MeV )ため二次系主蒸気
配管(肉厚2〜3cm)8の外側においても、微量でも
十分に検知することができる。According to the first embodiment, the secondary main steam pipe 8 connecting the steam generator 6 and the turbine 9 is facing the upstream side (toward the steam generator) along the main steam flow path. A dose rate measurement system with a radiation detector 18 installed at a nearby location) and the data obtained from this measurement system are compared with normal conditions to determine whether there are abnormal signs due to leakage and to measure from the dose rate. Calculate the radioactivity concentration in the main steam at the point,
It consists of an arithmetic processing system that can process changes over time. If the heat transfer tube 7 in the steam generator 6 is damaged, the radioactive substances in the primary coolant will reach the radiation detector 18 in a few seconds. Note that since the radioactivity concentration in the main steam under normal conditions is originally equal to zero, the output of the detector is expected to change significantly. Especially N16 and C1
When 5 is used as a radiation source, the energy of the emitted gamma rays is high (6 MeV, 5 MeV), so even a minute amount can be sufficiently detected even outside the secondary main steam pipe (wall thickness 2 to 3 cm) 8. can.
【0016】次に本発明の第2の実施例(第2の発明)
を図1および図2を参照しながら説明する。なお、図1
は第1の実施例の説明とほぼ同様なため、主要構成部分
のみの説明にとどめる。本発明の第2の実施例において
は、図1中のA,Bはそれぞれ二次系主蒸気配管8の上
流側と下流側の測定点であり、その場所に第1および第
2の放射線検出器18,19を設置する。これらの放射
線検出器18,19は演算処理系20に信号ケーブル2
1によって接続されており、電離箱型又はプラスチック
シンチレーション型等を用い線量率又は計数率としてM
CS(マルチチャンネル・スケーリング)モードで連続
測定する。もし、蒸気発生器6内の伝熱管7が破損して
一次系冷却材の漏洩が発生した場合はA,Bの順番で測
定値に変化が現れ、到達時間の差分だけ測定値に差が出
てくることになり、放射線検出器の故障又はノイズであ
れば一方の測定結果にしか現れないはずである。前記、
測定値を演算処理系20において自己診断を行った後、
平滑化二次微分等によるピークの探索を行い、正常値の
統計変動の3倍(3σ)を超えるかどうかを一つの判断
基準とする。ここで、有意な漏洩の徴候であると判断し
た場合、直ちに予め算出してある線量率と放射能濃度の
換算係数から測定値を放射能濃度に換算し、さらに測定
点AとBとの減衰率から主蒸気の流速を算出し、測定点
と蒸気発生器6の二次系出口6aまでの配管距離から到
達時間を求め、前記A又はBの放射能濃度を時間を遡っ
て逆算して蒸気発生器6の二次系出口6aにおける一次
系から漏洩した放射能濃度を算出する。前記一連のデー
タは演算処理系において経時変化として処理することに
より、異常の推移が即時に予測でき、又、予め測定対象
放射性核種の一次系冷却材中の放射能濃度と蒸気発生器
6内における主蒸気系への移行割合を求めておくことに
より、漏洩した際の主蒸気中の放射能濃度の値から破損
部の規模の推定が可能となる。ちなみに、診断可能な漏
洩量を以下の仮定を交え推定してみる。伝熱管7内の一
次系冷却材中のN16放射能濃度を40(μCi/g)
とし、二次系の主蒸気流量を1700(T/h) と
した時の伝熱管7からL(g/s) の漏洩が生じた場
合、時間当りの漏洩量は 144L(mCi/h) と
なる。この内、50%が主蒸気流量1500T/h に
移行すると、約L×5×10−5(μCi/g) が主
蒸気中に存在していることになる。ここで、計算により
主蒸気配管中にN16が1(μCi/g) ある時、主
蒸気配管(650A)表面における線量率はおよそ30
(mR/h)になることから、L×5×10−5(μC
i/g) の放射能濃度では、L×1×10−3(mR
/h)となり、放射線検出器の測定下限を 0.1(m
R/h)としても漏洩率Lは 100(g/s) とな
る。この量は、主蒸気発生器1基当りの一次系冷却材流
量 15000(T/h) 、1基当り3382本の蒸
気発生器6内の伝熱管7とした時の伝熱管1本当りの流
量1200(g/s) の0.08%程度である。Next, a second embodiment of the present invention (second invention)
will be explained with reference to FIGS. 1 and 2. In addition, Figure 1
Since this is almost the same as the explanation of the first embodiment, only the main components will be explained. In the second embodiment of the present invention, A and B in FIG. 1 are measurement points on the upstream side and downstream side of the secondary main steam piping 8, respectively, and the first and second radiation detection stations are installed at those locations. Install containers 18 and 19. These radiation detectors 18 and 19 are connected to a signal cable 2 to an arithmetic processing system 20.
1, and using an ion chamber type or plastic scintillation type, etc., the dose rate or count rate is M
Measure continuously in CS (multichannel scaling) mode. If the heat transfer tube 7 in the steam generator 6 is damaged and leakage of the primary coolant occurs, the measured values will change in the order of A and B, and the measured values will differ by the difference in arrival time. Therefore, if there is a failure or noise in the radiation detector, it should appear in only one measurement result. Said,
After performing self-diagnosis on the measured values in the arithmetic processing system 20,
The peak is searched for by smoothing second-order differential, etc., and one judgment criterion is whether the statistical variation exceeds three times (3σ) of the normal value. If it is determined that there is a sign of significant leakage, the measured value is immediately converted to radioactivity concentration using the dose rate and radioactivity concentration conversion coefficient calculated in advance, and the attenuation at measurement points A and B is further calculated. The main steam flow rate is calculated from the rate, the arrival time is determined from the piping distance from the measurement point to the secondary system outlet 6a of the steam generator 6, and the radioactivity concentration of A or B is calculated backward in time to determine the steam flow rate. The radioactivity concentration leaked from the primary system at the secondary system outlet 6a of the generator 6 is calculated. By processing the above-mentioned series of data as changes over time in the processing system, the transition of abnormality can be predicted immediately. By determining the transfer rate to the main steam system, it is possible to estimate the scale of the damaged part from the radioactivity concentration in the main steam at the time of leakage. By the way, let's estimate the amount of leakage that can be diagnosed using the following assumptions. The N16 radioactivity concentration in the primary coolant in the heat exchanger tube 7 was set to 40 (μCi/g).
If the main steam flow rate in the secondary system is 1700 (T/h) and a leak of L (g/s) occurs from the heat exchanger tube 7, the leakage amount per hour is 144 L (mCi/h). Become. If 50% of this is transferred to the main steam flow rate of 1500 T/h, approximately L x 5 x 10-5 (μCi/g) will exist in the main steam. Here, according to calculations, when there is 1 (μCi/g) of N16 in the main steam pipe, the dose rate at the surface of the main steam pipe (650A) is approximately 30
(mR/h), so L×5×10-5(μC
i/g), L x 1 x 10-3 (mR
/h), and the lower measurement limit of the radiation detector is 0.1 (m
R/h), the leakage rate L is 100 (g/s). This amount is the primary coolant flow rate per main steam generator unit of 15000 (T/h), and the flow rate per heat exchanger tube when the heat exchanger tubes 7 in the steam generator 6 are 3382 per unit. It is about 0.08% of 1200 (g/s).
【0017】第2の実施例(第2の発明)によれば、蒸
気発生器6とタービン9をつなぐ二次系主蒸気配管8に
面して、蒸気の流路に沿って上流側(蒸気発生器に近い
位置)と下流側(タービンに近い位置)に間隔をあけた
複数の放射線検出器18,19を設置した線量率測定系
と、この線量率測定系から得られた複数のデータをもと
にノイズか有意な信号かの自己診断を行うとともに正常
状態時との比較を行い、漏洩による異常徴候の有無の判
定、および線量率から各測定点における主蒸気中の放射
能濃度の算出、さらに流路に沿って得られた複数の線量
率から蒸気発生器6の二次系出口6aから測定点A,B
までの主蒸気到達時間を求める。よって蒸気発生器6の
二次系出口6aにおける漏洩放射能濃度の算出を経時変
化で診断することができる。According to the second embodiment (second invention), the steam pipe is located on the upstream side (steam A dose rate measurement system is installed with a plurality of radiation detectors 18 and 19 spaced apart (a position close to the generator) and a downstream side (a position near the turbine), and a plurality of data obtained from this dose rate measurement system are installed. Based on this, self-diagnosis is performed to determine whether the signal is noise or a significant signal, and a comparison is made with normal conditions to determine whether there are abnormal signs due to leakage, and the radioactivity concentration in the main steam at each measurement point is calculated from the dose rate. , and further from the secondary system outlet 6a of the steam generator 6 to the measurement points A and B based on the plurality of dose rates obtained along the flow path.
Find the main steam arrival time. Therefore, calculation of the leaked radioactivity concentration at the secondary system outlet 6a of the steam generator 6 can be diagnosed based on changes over time.
【0018】[0018]
【発明の効果】本発明によれば、蒸気発生器内の伝熱管
から僅かでも一次系冷却材が二次系冷却材中に漏洩した
場合にも、発生点から近いため直ちに測定系の線量率に
変化が現れて、異常現象の初期徴候の診断が可能となる
とともに、このデータを経時変化として処することによ
り異常の推移が予測でき、且つ異常箇所の状態を診断で
きる。According to the present invention, even if even a small amount of primary coolant leaks into the secondary coolant from the heat exchanger tubes in the steam generator, the dose rate of the measurement system will be reduced immediately because it is close to the point of occurrence. When a change appears in , it is possible to diagnose the early signs of an abnormal phenomenon, and by processing this data as a change over time, it is possible to predict the course of the abnormality and to diagnose the state of the abnormal location.
【図1】本発明の一実施例を含む加圧水型原子力発電所
を概略的に示す構成図。FIG. 1 is a block diagram schematically showing a pressurized water nuclear power plant including an embodiment of the present invention.
【図2】本発明における測定系と演算処理系のブロック
ダイヤグラム。FIG. 2 is a block diagram of a measurement system and an arithmetic processing system in the present invention.
1…原子炉建屋、2…原子炉格納容器、3…原子炉容器
、4…炉心、5…一次系配管、6…蒸気発生器、7…伝
熱管、8…二次系主蒸気配管、9…タービン、10…発
電機、11…復水器、12…二次系給水管、13…一次
系主冷却配管、14…ポンプ、15…制御棒、16…加
圧器、17…スプレー管、18…第1の放射線検出器、
19…第2の放射線検出器、20…演算処理系、21…
信号ケーブル、22…排ガス系抽気配管、23…タービ
ン排ガス系モニタ。1...Reactor building, 2...Reactor containment vessel, 3...Reactor vessel, 4...Reactor core, 5...Primary system piping, 6...Steam generator, 7...Heat transfer tube, 8...Secondary system main steam piping, 9 ... Turbine, 10 ... Generator, 11 ... Condenser, 12 ... Secondary system water supply pipe, 13 ... Primary system main cooling pipe, 14 ... Pump, 15 ... Control rod, 16 ... Pressurizer, 17 ... Spray pipe, 18 ...first radiation detector,
19... Second radiation detector, 20... Arithmetic processing system, 21...
Signal cable, 22...Exhaust gas system extraction piping, 23...Turbine exhaust gas system monitor.
Claims (2)
して加圧器および蒸気発生器が接続され、この蒸気発生
器の二次系出口からタービンまでに二次系主蒸気配管が
接続され、この二次系主蒸気配管に放射線検出器が接続
され、この放射線検出器に演算処理系が接続されてなる
ことを特徴とする原子炉の異常診断装置。Claim 1: A pressurizer and a steam generator are connected to a pressurized water reactor vessel via a primary system piping, and a secondary system main steam piping is connected from a secondary system outlet of the steam generator to a turbine, A nuclear reactor abnormality diagnosis device characterized in that a radiation detector is connected to the secondary main steam piping, and a calculation processing system is connected to the radiation detector.
して加圧器および蒸気発生器が接続され、この蒸気発生
器の二次系出口からタービンまでに接続された二次系主
蒸気配管に測定点として少なくとも2個の放射線検出器
を設け、これらの放射線検出器で検出した短半減期核種
を線源核種として測定したそれぞれの線量率の減衰率か
ら蒸気流速を算出し、前記測定点における放射能濃度を
蒸気発生器の二次系出口まで逆算して算出することを特
徴とする原子炉の異常診断方法。[Claim 2] A pressurizer and a steam generator are connected to the pressurized water reactor vessel via a primary system piping, and a secondary system main steam piping is connected from the secondary system outlet of the steam generator to the turbine. At least two radiation detectors are provided as measurement points, and the vapor flow rate is calculated from the attenuation rate of each dose rate measured using short half-life nuclides detected by these radiation detectors as source nuclides. A nuclear reactor abnormality diagnosis method characterized by calculating the radioactivity concentration back to the secondary system exit of the steam generator.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3028571A JPH04268496A (en) | 1991-02-22 | 1991-02-22 | Device and method for diagnostic abnormality of reactor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3028571A JPH04268496A (en) | 1991-02-22 | 1991-02-22 | Device and method for diagnostic abnormality of reactor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH04268496A true JPH04268496A (en) | 1992-09-24 |
Family
ID=12252311
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3028571A Pending JPH04268496A (en) | 1991-02-22 | 1991-02-22 | Device and method for diagnostic abnormality of reactor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH04268496A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US9494695B2 (en) | 2014-03-28 | 2016-11-15 | Mitsubishi Electric Corporation | Radiation monitor |
-
1991
- 1991-02-22 JP JP3028571A patent/JPH04268496A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US9494695B2 (en) | 2014-03-28 | 2016-11-15 | Mitsubishi Electric Corporation | Radiation monitor |
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