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JPH07101238B2 - Wide area neutron flux measurement and monitoring device - Google Patents
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JPH07101238B2 - Wide area neutron flux measurement and monitoring device - Google Patents

Wide area neutron flux measurement and monitoring device

Info

Publication number
JPH07101238B2
JPH07101238B2 JP61093826A JP9382686A JPH07101238B2 JP H07101238 B2 JPH07101238 B2 JP H07101238B2 JP 61093826 A JP61093826 A JP 61093826A JP 9382686 A JP9382686 A JP 9382686A JP H07101238 B2 JPH07101238 B2 JP H07101238B2
Authority
JP
Japan
Prior art keywords
signal
output
amplifier
neutron flux
phi
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
JP61093826A
Other languages
Japanese (ja)
Other versions
JPS62250396A (en
Inventor
潤 浜田
勇 豊吉
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP61093826A priority Critical patent/JPH07101238B2/en
Publication of JPS62250396A publication Critical patent/JPS62250396A/en
Publication of JPH07101238B2 publication Critical patent/JPH07101238B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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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

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  • Measurement Of Radiation (AREA)
  • Monitoring And Testing Of Nuclear Reactors (AREA)

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は、原子炉圧力容器内の起動系領域ならびに中間
系領域にある中性子束を計測および表示し、原子炉の平
均出力または局部出力が異常に上昇する等の過渡現象を
示した場合に制御棒引抜阻止信号やスクラム信号を発生
する広域系中性子束計測監視装置に関する。
DETAILED DESCRIPTION OF THE INVENTION Object of the Invention (Industrial field of application) The present invention measures and displays the neutron flux in the start-up system region and the intermediate system region in a reactor pressure vessel, and displays the average of the reactor. The present invention relates to a wide area neutron flux measurement and monitoring device that generates a control rod withdrawal prevention signal and a scrum signal when a transient phenomenon such as an abnormal increase in output or local output is shown.

(従来の技術) 一般に原子炉圧力容器内に中性子束レベルは、広い測定
レンジ(たとえば、沸騰水形原子炉では11桁の測定レン
ジ)を持っており、一つの測定手段で測定することは技
術的に困難である。このため、従来から三つの測定手段
を組み合せて使用している。
(Prior Art) In general, the neutron flux level in a reactor pressure vessel has a wide measurement range (for example, a boiling water reactor has an 11-digit measurement range), and it is technically difficult to measure with one measurement means. Is difficult. For this reason, conventionally, three measuring means are used in combination.

第一の測定手段は低中性子束レンジ(起動系領域)によ
るもので、この領域では炉出力が計数率に比例するの
で、低レンジ6桁をパルス計測方による計数で計数率を
求めて中性子束レベルを測定している。第二の測定手段
は中間の中性子束レンジ(中間領域)によるもので、こ
の領域では炉出力が出力信号のゆらぎ成分の二乗平均値
に比例することに着目し、キャンベル法を用いて測定す
る。つまり、検出器出力信号の交流成分の実効値の二乗
によって測定する。第三の測定手段は高中性子束レンジ
(出力領域)によるもので、この領域では炉出力が直流
電流に比例することに着目し、検出器からの直流電流を
測定するものである。
The first measurement means is in the low neutron flux range (start-up system area). In this area, the reactor output is proportional to the count rate. The level is being measured. The second measuring means is based on the intermediate neutron flux range (intermediate region). In this region, the reactor power is proportional to the root mean square value of the fluctuation components of the output signal, and the Campbell method is used for the measurement. That is, it is measured by the square of the effective value of the AC component of the detector output signal. The third measuring means is based on the high neutron flux range (output region), in which the direct current from the detector is measured, paying attention to the fact that the reactor output is proportional to the direct current.

これらの測定手段では、起動系領域用検出器4個、中間
系領域用検出器8個、出力系領域用検出器100〜200個を
それぞれ炉心内に設置し、各系ごとに検出器を検出回路
に接続して中性子束レベルを測定している。
In these measuring means, four detectors for the starting system area, eight detectors for the intermediate system area, and 100 to 200 detectors for the output system area are installed in the core, and the detectors are detected for each system. It is connected to a circuit to measure the neutron flux level.

また、上述の測定手段を原子炉の安全系として使用する
場合の取り扱い方もそれぞれ異なっている。一般に出力
がe(自然対数の底)倍になるまでの時間Tをペリオド
と定義し出力変化の指標とする。起動系においては、中
性子束の時間変化率を直接微分回路により計測し、この
値が一定値を超えた場合に制御棒引抜阻止信号が出力さ
れる。中間系の場合は、出力表示方式にレンジ切換リニ
ア表示方式を採用しているため、各レンジごとの指示値
が一定値以上になった時にスクラム信号が出力される。
出力系では、その出力指示値が一定値たとえば定格の12
0%出力を超えた場合にスクラム信号が出力される。こ
こで、起動系および中間系は急激な出力上昇を防止し、
また,出力系は定格出力を超えないように監視して原子
炉の安全性を確保する。
In addition, the handling method when the above-mentioned measuring means is used as a safety system of a nuclear reactor is also different. Generally, the time T until the output becomes e (base of natural logarithm) times is defined as a period and is used as an index of output change. In the start-up system, the time rate of change of neutron flux is directly measured by a differentiating circuit, and when this value exceeds a certain value, a control rod withdrawal prevention signal is output. In the case of the intermediate system, since the range switching linear display system is adopted as the output display system, the scrum signal is output when the indication value for each range becomes a certain value or more.
In the output system, the output instruction value is a constant value, for example, the rated value of 12
The scrum signal is output when the output exceeds 0%. Here, the start system and the intermediate system prevent a sudden output increase,
In addition, the output system is monitored so that the rated output is not exceeded to ensure reactor safety.

第5図は、従来の起動系領域における中性子束計測監視
装置のブロック図である。この起動系領域における中性
子束計測監視装置は、起動系領域における中性子束を検
出する検出器(核分裂計数管)1と、この検出器1の出
力信号を増幅するパルス系用増幅器2と、このパルス系
用増幅器2によって増幅された信号を信号パルスとノイ
ズ成分に弁別する波高弁別回路および信号パルスの計数
率を計測するカウンタを備えた起動系出力処理回路3
と、この起動系出力処理回路3の出力を微分して中性子
束の時間変化率を直接に求める微分回路を有し、この微
分回路によって求められた中性子束の時間変化率と設定
値との比較を行い、前記中性子束の時間変化率が前記設
定値より大きい場合に制御棒引抜阻止信号を出力するペ
リオド回路4と、前記中性子束の時間変化率を表示する
表示器5とを備えている。
FIG. 5 is a block diagram of a conventional neutron flux measurement / monitoring device in the startup system region. The neutron flux measurement and monitoring device in this start-up system region comprises a detector (fission counter) 1 for detecting a neutron flux in the start-up system region, a pulse system amplifier 2 for amplifying the output signal of this detector 1, and this pulse. Start-up system output processing circuit 3 including a pulse height discrimination circuit that discriminates the signal amplified by the system amplifier 2 into a signal pulse and a noise component, and a counter that measures the counting rate of the signal pulse.
And a differentiation circuit for differentiating the output of the startup system output processing circuit 3 to directly obtain the time change rate of the neutron flux, and comparing the time change rate of the neutron flux obtained by this differentiation circuit with the set value. And a period circuit 4 that outputs a control rod withdrawal inhibition signal when the time change rate of the neutron flux is larger than the set value, and a display 5 that displays the time change rate of the neutron flux.

第6図は、従来の中間系領域における中性子束監視装置
のブロック図である。この中間系領域における中性子束
監視装置は、中間系領域における中性子束を検出する検
出器6と、この検出器6の出力信号を増幅するキャンベ
ル系用増幅器7と、このキャンベル系用増幅器7によっ
て増幅された信号を二乗する二乗回路8、およびこの二
乗回路8の出力信号を平滑化する平滑回路9を有する中
間系出力処理回路10と、この中間系出力処理回路10の出
力を表示する表示器11と、中間系出力処理回路10の出力
と設定値の比較を行い、中間系出力処理回路10の出力が
前記設定値以上の場合にスクラム信号を発生する比較回
路12を備えている。なお、二乗回路8にはレンジ切換増
幅器が内蔵されており、プラントの運転員は表示器11の
出力レベルを確認しながら、比較回路12からスクラム信
号が発生しないように、適切なレンジ切換信号を入力し
ながら原子炉出力の上昇を行なう。
FIG. 6 is a block diagram of a conventional neutron flux monitoring device in the intermediate region. The neutron flux monitoring device in the intermediate system region includes a detector 6 for detecting the neutron flux in the intermediate system region, a Campbell system amplifier 7 for amplifying an output signal of the detector 6, and an amplification by the Campbell system amplifier 7. An intermediate output processing circuit 10 having a squaring circuit 8 for squaring the generated signal and a smoothing circuit 9 for smoothing an output signal of the squaring circuit 8, and a display 11 for displaying the output of the intermediate output processing circuit 10. And a comparison circuit 12 that compares the output of the intermediate system output processing circuit 10 with a set value and generates a scrum signal when the output of the intermediate system output processing circuit 10 is equal to or more than the set value. It should be noted that the squaring circuit 8 has a built-in range switching amplifier, and the operator of the plant checks the output level of the display 11 and outputs an appropriate range switching signal from the comparison circuit 12 so as not to generate a scrum signal. While inputting, increase the reactor power.

このような特性上の差異のため、パルス系による測定と
キャンベル系による測定とを同一の測定装置で行なうこ
とは不可能と考えられ、従前は別々の装置によりその出
力を表示していた。
Due to such a difference in characteristics, it is considered impossible to perform the measurement by the pulse system and the measurement by the Campbell system with the same measuring device, and the output has been displayed by different devices before.

第7図は、上記の問題点を解決するための手段として開
発された従来の広域系中性子束計測監視装置である。こ
の従来の広域系中性子束計測監視装置は、核分裂計数管
等を有する広域系用検出器20と、この広域系用検出器20
の出力を周波数帯域分離し、高周波数帯域増幅可能なパ
ルス系用増幅器22および低ノイズ中間周波数帯域増幅可
能なキャンベル系用増幅器23を並列接続してなる広域前
置増幅器21と、パルス系用増幅器22の出力側に第5図と
同様に接続された起動系出力処理回路3、ペリオド回路
4、および表示器5と、キャンベル系用増幅器23の出力
側に第6図と同様に接続された二乗回路8および平滑回
路9を有する中間系出力処理回路10、比較回路12および
表示器11とを備えている。パルス系用増幅器22およびキ
ャンベル系用増幅器23は図示していない入力インピーダ
ンスと結合コンデンサの適当な組み合せによって周波数
分離を行なう。すなわち、起動系では高周波成分のみが
パルス系用増幅器22により増幅され、また中間系では中
間周波数帯成分のみがキャンベル系用増幅器23により増
幅されることになり、起動系における計数率特性と中間
系におけるS/N特性のいずれも満足できるとともに、そ
れぞれの増幅器利得をも適切な値に設定できる。したが
って1個の広域用検出器20によって起動系中性子束およ
び中間系中性子束の検出が可能となるが広域前置増幅器
21以降の計測監視手段は、それぞれ単独の第5図に示さ
れた起動系領域の中性子束計測監視手段および第6図に
示された中間系領域の中性子束計測監視手段と何ら変わ
るところはなく、同じ問題点を含んでいる。すなわち、
起動系領域でのペリオド回路4は中性子束の時間変化率
を直接求める微分回路を含んでいることから回路ノイズ
等の微変動により出力信号が大きく変わり、系が不安定
になりやすい。また、中性子束信号にのってくるノイズ
成分により出力信号が大幅に変動するため、このノイズ
成分除去のために回路が複雑になっている。制御棒引抜
き等により正の反応度が加わった場合、原子炉は短時間
で一旦出力が急上昇し、以後安定した上昇率で出力上昇
するという現象を示し、この短時間の出力上昇は即発ジ
ャンプと呼ばれている。しかし、出力上昇の時間が極め
て短く出力上昇もそれ程大きくならないことから原子炉
の安全上特に問題となる現象ではないにもかかわらず、
微分回路があると、この短時間の入力信号を微分するた
め、出力信号である中性子束の時間変化率は急激に大き
くなる。そのため中性子束の時間変化率は設定値以上と
なり、ペリオド回路は制御棒引抜阻止信号をだす可能性
があり、微分回路の存在は、運転性能を低下させる要因
となる。そのため、この即発ジャンプの影響をとり除く
必要から複雑な回路構成をとらざるを得ない。また中間
系領域の中性子束計測監視装置では、運転員は表示器11
で原子炉の出力レベルを確認しつつ、スクラム信号が発
生しないよう適切なレンジに切換えて原子炉の出力上昇
を行なう必要があるため、運転員の負担軽減および運転
上の省力化にはなり得なかった。
FIG. 7 shows a conventional wide area neutron flux measurement and monitoring device developed as a means for solving the above problems. This conventional wide area neutron flux measurement and monitoring device includes a wide area system detector 20 having a fission counter and the like, and a wide area system detector 20.
Wide-area preamplifier 21 in which the pulse system amplifier 22 capable of high frequency band amplification and the Campbell system amplifier 23 capable of low noise intermediate frequency band amplification are connected in parallel, and the pulse system amplifier A start-up output processing circuit 3, a period circuit 4, and an indicator 5 connected to the output side of 22 in the same manner as in FIG. 5, and a square connected to the output side of the Campbell amplifier 23 in the same manner as in FIG. An intermediate output processing circuit 10 having a circuit 8 and a smoothing circuit 9, a comparison circuit 12, and a display 11 are provided. The pulse system amplifier 22 and the Campbell system amplifier 23 perform frequency separation by an appropriate combination of an input impedance (not shown) and a coupling capacitor. That is, in the starting system, only the high frequency component is amplified by the pulse system amplifier 22, and in the intermediate system, only the intermediate frequency band component is amplified by the Campbell system amplifier 23. All of the S / N characteristics in can be satisfied, and each amplifier gain can be set to an appropriate value. Therefore, it is possible to detect the start-up system neutron flux and the intermediate system neutron flux with one wide-area detector 20.
The measurement and monitoring means after 21 are no different from the neutron flux measurement and monitoring means in the starting system area shown in FIG. 5 and the neutron flux measurement and monitoring means in the intermediate system area shown in FIG. 6, respectively. , Contains the same problem. That is,
Since the period circuit 4 in the start-up system region includes a differentiating circuit that directly obtains the time change rate of the neutron flux, the output signal greatly changes due to a slight fluctuation such as circuit noise, and the system is likely to become unstable. Further, since the output signal fluctuates significantly due to the noise component carried on the neutron flux signal, the circuit becomes complicated to remove this noise component. When a positive reactivity is added due to pulling out of the control rod, etc., the reactor shows a phenomenon that the output power suddenly increases in a short time and then increases at a stable rate of increase. being called. However, since the power rise time is extremely short and the power rise does not increase so much, it is not a phenomenon that poses a particular problem to reactor safety,
If there is a differentiating circuit, this short-time input signal is differentiated, so that the time change rate of the neutron flux, which is the output signal, rapidly increases. Therefore, the time change rate of the neutron flux becomes higher than the set value, the period circuit may output the control rod withdrawal prevention signal, and the presence of the differential circuit causes a decrease in operating performance. Therefore, it is necessary to take a complicated circuit configuration because it is necessary to remove the influence of the prompt jump. Also, in the neutron flux measurement and monitoring device in the intermediate region, the operator
Since it is necessary to check the output level of the reactor with, and to increase the reactor output by switching to an appropriate range so that a scrum signal does not occur, it is possible to reduce the burden on the operator and save labor in operation. There wasn't.

(発明が解決しようとする問題点) 本発明は、起動系領域または中間系領域にある中性子束
を分離計測することなく、これらの中性子束を自動計測
および自動監視し、かつ即発ジャンプ等の影響を除去す
るための複雑な回路構成を有しない広域系中性子束計測
監視装置を提供することを目的とする。
(Problems to be Solved by the Invention) The present invention does not separately measure the neutron flux in the start-up system region or the intermediate system region, automatically measures and monitors these neutron fluxes, and the influence of prompt jumps and the like. It is an object of the present invention to provide a wide-area neutron flux measurement and monitoring device that does not have a complicated circuit configuration for removing the neutrons.

〔発明の構成〕[Structure of Invention]

(問題点を解決するための手段および作用) 本発明は、原子炉圧力容器内の起動系領域にある中性子
束、および中間系領域にある中性子束を検出する広域中
性子束検出器と、この広域中性子束検出器によって検出
された広域中性子束の信号を周波数帯域分離し、この周
波数帯域分離された高周波数成分が入力されるパルス系
用増幅器、および中間周波数成分が入力されるキャンベ
ル系用増幅器を備えた広域前置増幅器と、前記パルス系
用増幅器の出力を入力して波高弁別し、かつ計数率を計
測して波高弁別された信号を起動系信号φaとして出力
する起動系出力処理回路と、前記キャンベル系用増幅器
の出力信号を入力とし、この入力の二乗平均値を平滑化
し中間系信号φbとして出力する中間系出力処理回路
と、前記起動系出力処理回路によって出力された前記起
動系信号φaの計数率が予め設定した設定値以上のとき
に切換指示信号を出力する出力比較回路と、前記出力比
較回路の出力である切換指示信号に基づいて、前記起動
系信号φaの計数率が前記設定値以上のとき前記中間系
信号φbを通過させ、前記起動系信号φaの計数率が前記
設定値未満のときは、前記起動系信号φaを通過させる
ように接続を切換える切換器と、第一の増幅器、第一の
ローパスフィルタ、および第一の信号比較回路を備え、
前記起動系信号φaの計数率が前記設定値未満の場合の
み前記切換器によって前記起動系出力処理回路に接続さ
れ、前記起動系信号φaが前記第一の増幅器および前記
第一のローパスフィルタを通過した後の信号φa′と前
記起動系信号φaを前記第一の信号比較回路で比較し、
前記起動系信号φaの大きさが前記信号φa′の大きさ以
上のときに制御棒引抜阻止信号を出力する第一のペリオ
ド計測監視手段と、第二の増幅器、第二のローパスフィ
ルタおよび第二の信号比較回路を備え、前記起動系信号
φaの計数率が前記設定値以上のとき前記切換器によっ
て前記中間系出力処理回路に接続され、前記中間系出力
信号φbが前記第二の増幅器および第二のローパスフィ
ルタを通過した後の信号φb′と前記中間系信号φbを前
記第二の信号比較回路で比較し、前記中間系信号φb
大きさが前記信号φb′の大きさ以上のときに制御棒引
抜阻止信号を出力する第二のペリオド計測監視手段と、
第三の増幅器、第三のローパスフィルタおよび第三の信
号比較回路を備え、前記第二のペリオド計測監視手段と
並列に配置され、前記起動系信号φaの計数率が前記設
定値以上のとき前記切換器によって前記中間系出力処理
回路に接続され、前記中間系信号φbが前記第三の増幅
器および前記第三のローパスフィルタを通過した後の信
号φc′と前記中間系信号φbを前記第三の信号比較回路
で比較し、前記中間系信号φbの大きさが前記信号φc
の大きさ以上のときにスクラム信号を発生する第三のペ
リオド計測監視手段とを具備していることを特徴とする
ものである。
(Means and Actions for Solving Problems) The present invention relates to a wide-area neutron flux detector that detects a neutron flux in a start-up system region in a reactor pressure vessel and a neutron flux in an intermediate-system region, and a wide-range neutron flux detector. A wide band neutron flux signal detected by the neutron flux detector is frequency band separated, and a pulse system amplifier to which the high frequency component separated by this frequency band is input and a Campbell system amplifier to which the intermediate frequency component is input are provided. A wide area preamplifier provided, and a start system output processing circuit for inputting the output of the pulse system amplifier to perform wave height discrimination, and measuring a count rate and outputting the wave height discriminated signal as a start system signal φ a. , it receives the output signal of the Campbell system amplifier, and the intermediate system output processing circuit for outputting a mean square value of this input as a intermediate system signal phi b smoothes the activation system output processing circuit An output comparison circuit outputted the activation system signal phi a of the count rate outputs a switching instruction signal when above predetermined set value Te, based on the switching instruction signal is output from the output comparison circuit, wherein when the counting rate of the activation system signal phi a of more than the set value is passed through the intermediate system signal phi b, when the count rate of the activation system signal phi a is less than the set value, the activation system signal phi a A switching device that switches the connection so that it passes, a first amplifier, a first low-pass filter, and a first signal comparison circuit,
Only when the count rate of the start-up signal φ a is less than the set value is connected to the start-up output processing circuit by the switch, the start-up signal φ a is the first amplifier and the first low-pass filter. The signal φ a ′ after passing through and the starting system signal φ a are compared in the first signal comparison circuit,
First period measurement and monitoring means for outputting a control rod withdrawal prevention signal when the magnitude of the activation system signal φ a is greater than or equal to the magnitude of the signal φ a ′, a second amplifier, a second low pass filter, and A second signal comparison circuit, which is connected to the intermediate system output processing circuit by the switch when the count rate of the starting system signal φ a is equal to or more than the set value, and the intermediate system output signal φ b is the second compared with the amplifier and a second low-pass filtered signal phi b 'and the intermediate system signal phi b of the second signal comparison circuit after passing the magnitude is the signal of the intermediate system signal phi b phi b Second period measurement and monitoring means for outputting a control rod withdrawal prevention signal when the size is equal to or greater than ‘
A third amplifier, a third low-pass filter and a third signal comparison circuit, arranged in parallel with the second period measurement and monitoring means, when the count rate of the activation system signal φ a is equal to or more than the set value. The intermediate system output processing circuit is connected to the intermediate system output processing circuit by the switch, and the intermediate system signal φ b is passed through the third amplifier and the third low-pass filter to output the signal φ c ′ and the intermediate system signal φ b . The magnitude of the intermediate signal φ b is compared by the third signal comparison circuit, and the magnitude of the intermediate signal φ b is the signal φ c ′.
And a third period measuring and monitoring means for generating a scrum signal when the value is equal to or larger than the above value.

(実施例) 第1図は、本発明による広域系中性子束計測監視装置の
一実施例を示すブロック図である。この広域系中性子束
計測監視装置は、原子炉内に設置された広域中性子束検
出器(たとえば核分裂計数管)30と、この広域中性子束
検出器30の出力信号を周波数帯域分離し、この周波数帯
域分離された高周波数成分が入力されるパルス系用増幅
器32、および中間周波数成分が入力されるキャンベル系
用増幅器33を有する広域前置増幅器31と、パルス系用増
幅器32の出力を波高弁別し、計数率を計測し、起動系信
号φaとして出力する起動系出力処理回路34と、キャン
ベル系用増幅器33の出力信号を入力とし、この入力の二
乗平均値を平滑化し中間系信号φbとして出力する中間
系出力処理回路35と、起動系出力処理回路34によって出
力された起動系信号φaの計数率が予め設定した設定値
以上のときに切換指示信号を出力する出力比較回路40
と、この出力比較回路40の出力である切換指示信号に基
づいて、起動系信号φaの計数率が前記設定値以上のと
き中間系信号φbを通過させ、起動系信号φaの計数率が
前記設定値未満のときは、前記起動系信号φaを通過さ
せるように接続を切換える切換器41と、第一の増幅器37
a、第一のローパスフィルタ38a、および第一の信号比較
回路39aを備え、起動系信号φaの計数率が前記設定値未
満の場合のみ切換器41によって起動系出力処理回路34に
接続され、起動系信号φaが第一の増幅器37aおよび第一
のローパスフィルタ38aを通過した後の信号φa′と起動
系信号φaを第一の信号比較回路39aで比較し、起動系信
号φaの大きさが信号φa′の大きさ以上のときに制御棒
引抜阻止信号を出力する第一のペリオド計測監視手段36
aと、この第一のペリオド計測監視手段36aに接続され、
起動系信号を表示する表示器42aと、第二の増幅器37b
第二のローパスフィルタ38bおよび第二の信号比較回路3
9bを備え、起動系信号φaの計数率が前記設定値以上の
とき切換器41によって中間系出力処理回路35に接続さ
れ、中間系出力信号φbが第二の増幅器37bおよび第二の
ローパスフィルタ38bを通過した後の信号φb′と中間系
信号φbを第二の信号比較回路39bで比較し、中間系信号
φbの大きさが信号φb′の大きさ以上のときに制御棒引
抜阻止信号を出力する第二のペリオド計測監視手段36b
と、起動系信号φaの計数率が前記設定値以上のときに
中間系信号φbを表示する第二の表示器42bと、第三の増
幅器37c、第三のローパスフィルタ38cおよび第三の信号
比較回路37cを備え、第二のペリオド計測監視手段36b
並列に配置され、起動系信号φaの計数率が前記設定値
以上のとき切換器41によって中間系出力処理回路35に接
続され、中間系信号φc(=φb)が第三の増幅器37c
よび第三のローパスフィルタ37cを通過した後の信号
φc′と中間系信号φcを第三の信号比較回路37cで比較
し、中間系信号φcの大きさが信号φc′の大きさ以上の
ときにスクラム信号を発生する第三のペリオド計測監視
手段36cとを具備している。またパルス系用増幅器32は
インピーダンスR1と結合コンデンサC1の適当な組み合せ
により、キャンベル系用増幅器33はインピーダンスR2
結合コンデンサC2の適当な組み合せにより周波数分離を
行なっている。起動系出力処理回路34からは起動系領域
における中性子束レベルに相当する信号が起動系信号φ
aとして出力され、中間系出力処理回路35からは中問系
領性子束レベルに相当する信号が中間系信号φbと域に
おける中して出力される。ペリオド計測監視手段36a,36
b,36cにおけるそれぞれの入力信号φa,φb,φcと、こ
れらの入力信号φa,φb,φcがそれぞれ増幅器37a,3
7b,37cおよびローパスフィルタ38a,38b,38cを通過した
後の信号φa′,φb′,φb′との関係は次の式に表現
される。
(Embodiment) FIG. 1 is a block diagram showing an embodiment of a wide area neutron flux measurement and monitoring apparatus according to the present invention. This wide-area neutron flux measurement and monitoring device separates a wide-area neutron flux detector (for example, a nuclear fission counter) 30 installed in a nuclear reactor and an output signal of the wide-area neutron flux detector 30 into frequency bands, A pulse system amplifier 32 to which the separated high frequency component is input, and a wide area preamplifier 31 having a Campbell system amplifier 33 to which an intermediate frequency component is input, and pulse height discrimination of the output of the pulse system amplifier 32, The output signal of the startup system output processing circuit 34 that measures the counting rate and outputs it as the startup system signal φ a and the output signal of the Campbell system amplifier 33 are input, and the root mean square value of this input is smoothed and output as the intermediate system signal φ b. Intermediate output processing circuit 35 and output comparison circuit 40 that outputs a switching instruction signal when the count rate of the startup system signal φ a output by the startup system output processing circuit 34 is equal to or greater than a preset set value.
If, on the basis of the switching instruction signal output from the output comparison circuit 40, start system when the counting rate of the signal phi a of more than the set value is passed through an intermediate system signal phi b, count rate activation system signal phi a Is less than the set value, the switch 41 for switching the connection so as to pass the start-up signal φ a and the first amplifier 37.
a , a first low-pass filter 38 a , and a first signal comparison circuit 39 a, and is connected to the startup system output processing circuit 34 by the switch 41 only when the count rate of the startup system signal φ a is less than the set value. The start-up signal φ a is compared with the signal φ a ′ after the start-up signal φ a has passed through the first amplifier 37 a and the first low-pass filter 38 a and the start-up signal φ a in the first signal comparison circuit 39 a , First period measurement and monitoring means 36 which outputs a control rod pull-out prevention signal when the magnitude of the starting system signal φ a is equal to or greater than the magnitude of the signal φ a ′.
and a, is connected to the first Periodo measurement monitoring means 36 a,
An indicator 42a for displaying a start-up signal, a second amplifier 37b ,
The second low pass filter 38 b and the second signal comparison circuit 3
9 b , the starter signal φ a is connected to the intermediate system output processing circuit 35 by the switcher 41 when the count rate is equal to or more than the set value, and the intermediate system output signal φ b outputs the second amplifier 37 b and the second amplifier 37 b . The signal φ b ′ after passing through the low-pass filter 38 b and the intermediate system signal φ b are compared by the second signal comparison circuit 39 b , and the magnitude of the intermediate system signal φ b is equal to or larger than the magnitude of the signal φ b ′. Second period measurement and monitoring means 36 b that outputs a control rod pull-out prevention signal when
When, a second indicator 42 b of the counting rate of the activation system signal phi a displays an intermediate system signal phi b when more than the set value, the third amplifier 37 c, a third low-pass filter 38 c and comprising a third signal comparison circuit 37 c, arranged in parallel with the second Periodo measurement monitoring means 36 b, an intermediate system output processing circuit by switching unit 41 when the counting rate of the activation system signal phi a of more than the set value The intermediate signal φ c (= φ b ) connected to the signal 35 is passed through the third amplifier 37 c and the third low-pass filter 37 c , and the intermediate signal φ c ′ and the intermediate signal φ c are converted to the third signal. compared with the comparison circuit 37 c, which includes the intermediate system signal third Periodo measurement monitoring means for generating a scram signal when phi magnitude of c is greater than or equal the magnitude of the signal phi c '36 c. Further, the pulse system amplifier 32 performs frequency separation by a suitable combination of the impedance R 1 and the coupling capacitor C 1 , and the Campbell system amplifier 33 performs frequency separation by a suitable combination of the impedance R 2 and the coupling capacitor C 2 . A signal corresponding to the neutron flux level in the startup system region is output from the startup system output processing circuit 34 as the startup system signal φ.
The signal is output as a, and the intermediate system output processing circuit 35 outputs a signal corresponding to the intermediate system conjunctive child bundle level as the intermediate system signal φ b . Period measurement and monitoring means 36 a , 36
The input signals φ a , φ b , and φ c at b and 36 c and the input signals φ a , φ b , and φ c are respectively amplified by the amplifiers 37 a and 3
The relationship with the signals φ a ′, φ b ′, φ b ′ after passing through 7 b , 37 c and the low pass filters 38 a , 38 b , 38 c is expressed by the following equation.

ここで、i=a,b,c φi(t):ペリオド計測監視手段36iの入力信号 φi′(t):増幅器37iおよびローパスフィルタ38i
通過した信号 Gi:増幅器37iのゲイン λi:1/RCi RCi:ローパスフィルタ38iの時定数 (1)式は中性子束がペリオドτiで上昇すると解析的
に解け で与えられる。
Here, i = a, b, c φ i (t): input signal Periodo measurement monitoring means 36 i φ i '(t) : amplifiers 37 i and the low-pass filter 38 the signal has passed through the i G i: amplifier 37 i Gain λ i : 1 / RC i RC i : time constant of low-pass filter 38 i Equation (1) can be analytically solved when the neutron flux rises at period τ i. Given in.

(φi(t)=φi(o)et/τ ) さらにt=∞においてφi′=φiとなることを利用する
と RCi=(Gi−1)・τi……(3) となりローパスフィルタ38iの時定数RCiとゲインGiの関
係が与えられる。したがって、このペリオド計測監視手
段36iにおいてRCiとGiを設定するとペリオドτiが与え
られることになり、あるペリオド(例えば10秒)で制御
棒引抜阻止信号またはスクラム信号を出したい時にはそ
れに対応するRCiとGiの組み合せを設定すれば良い。
i (t) = φ i (o) e t / τ i ) Furthermore, by utilizing the fact that φ i ′ = φ i at t = ∞, RC i = (G i −1) · τ i …… ( 3) relationship constant RC i and the gain G i when next low-pass filter 38 i is provided. Therefore, when RC i and G i are set in the period measurement / monitoring means 36 i, the period τ i is given, and when a control rod withdrawal prevention signal or a scrum signal is to be issued at a certain period (for example, 10 seconds), it corresponds to that. You can set the combination of RC i and G i .

さらにこのペリオド計測監視手段36iの設定ペリオドτS
iに対して炉の出力上昇がペリオドτiに起った時にφi
≧φi′となるまでに要する時間Tiを決めるとTiは、 で与えられるため一義的にGiが決まる。このGiと(3)
式を用いてRCiを決定すれば 「ペリオドτiの出力上昇が起った時からTi時間後に制
御棒引抜阻止信号またはスクラム信号を出すペリオド計
測監視手段」 が与えられることになる。
Furthermore, the setting period τ S of this period measurement and monitoring means 36 i
when the output increase of the furnace had happened to Periodo τ i for the i φ i
When the time T i required until ≧ φ i ′ is determined, T i is Since it is given by, G i is uniquely determined. This G i and (3)
If RC i is determined by using the formula, “a period measurement and monitoring means for issuing a control rod withdrawal prevention signal or scrum signal after T i time from the time when the output of period τ i rises” will be given.

例えばRCi=10秒、Gi=2とすると、トリップ設定ペリ
オドτiは(3)式よりτi=10秒となり炉の出力上昇が
ペリオドτSi=9秒で起った場合、(4)式よりTi=15
秒後にトリップ信号を出力する。
For example, if RC i = 10 seconds and G i = 2, the trip setting period τ i is τ i = 10 seconds from equation (3), and if the reactor power rise occurs at period τ Si = 9 seconds, (4) From the formula, T i = 15
A trip signal is output after a second.

以上のように本発明による広域系中性子束計測監視装置
は、直接中性子束の信号を微分することなく原子炉の出
力上昇のペリオドが設定ペリオド以下であるかどうかを
監視できる。
As described above, the wide area neutron flux measurement and monitoring apparatus according to the present invention can monitor whether or not the period of the reactor power increase is equal to or less than the set period without directly differentiating the neutron flux signal.

第2図は、起動系領域において制御棒引抜阻止信号を発
生した場合の応答例を示した図である。符号43aは起動
系信号φaを示し、符号44aはペリオド計測監視手段36a
の増幅器37aおよびローパスフィルタ38aを通過後の信号
φa′を示しており、交点46で制御棒引抜阻止信号が発
生している。
FIG. 2 is a diagram showing a response example when a control rod pull-out prevention signal is generated in the activation system area. Reference numeral 43 a indicates a starting system signal phi a, numeral 44 a is Periodo measuring monitoring means 36 a
The signal φ a ′ after passing through the amplifier 37 a and the low-pass filter 38 a of FIG. 4 is shown, and the control rod pull-out prevention signal is generated at the intersection point 46.

第3図は、中間系領域において制御棒引抜阻止信号およ
びスクラム信号を発生した場合の応答例を示した図であ
る。符号43bは中間系信号φbを示し、符号44bはペリオ
ド計測監視手段36bの構成要素である増幅器37bおよびロ
ーパスフィルタ38bを通過後の信号φb′を示し、符号45
はペリオド計測監視手段36cの構成要素である増幅器37c
およびローパスフィルタ38cを通過後の信号φc′を示し
ており、交点46で制御棒引抜阻止信号、交点47でスクラ
ム信号が発生している。
FIG. 3 is a diagram showing a response example when the control rod pull-out prevention signal and the scrum signal are generated in the intermediate system region. Reference numeral 43 b indicates the intermediate signal φ b , reference numeral 44 b indicates the signal φ b ′ after passing through the amplifier 37 b and the low-pass filter 38 b , which are components of the period measuring and monitoring means 36 b , and the reference numeral 45.
Amplifier is a component of Periodo measurement monitoring means 36 c 37 c
The signal φ c ′ after passing through the low-pass filter 38 c is shown, and the control rod pull-out prevention signal is generated at the intersection point 46 and the scrum signal is generated at the intersection point 47.

第4図は中間系領域において、ペリオド計測監視手段の
入力信号と前記ペリオド計測監視手段の構成要素である
増幅器およびローパスフィルタを通過後の信号の時間に
対する変化を示したグラフである。符号48はペリオド計
測監視手段の入力信号を示し符号49は前記増幅器および
前記ローパスフィルタ通過後の信号を示している。
FIG. 4 is a graph showing changes with time of the input signal of the period measuring and monitoring means and the signal after passing through the amplifier and the low pass filter which are the constituent elements of the period measuring and monitoring means in the intermediate region. Reference numeral 48 indicates an input signal of the period measuring and monitoring means, and reference numeral 49 indicates a signal after passing through the amplifier and the low-pass filter.

〔発明の効果〕〔The invention's effect〕

本発明による広域中性子束計測監視装置は、起動系領域
または中間系領域にある中性子束を自動計測および自動
監視することができ、ペリオド計測監視手段に微分回路
を使用しないで増幅器、ローパスフィルタおよび信号比
較回路を備えさせているため極めて単純な構成となって
おり、かつ前記増幅器のゲインおよびローパスフィルタ
の時定数を適切に選ぶことにより即発ジャンプ等の影響
を除去することができる。
The wide area neutron flux measurement and monitoring apparatus according to the present invention can automatically measure and automatically monitor the neutron flux in the start-up system region or the intermediate system region, and an amplifier, a low-pass filter and a signal without using a differentiating circuit in the period measurement and monitoring means. Since the comparator circuit is provided, the configuration is extremely simple, and the effects of prompt jump and the like can be eliminated by appropriately selecting the gain of the amplifier and the time constant of the low-pass filter.

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

第1図は本発明による広域系中性子束計測監視装置の一
実施例を示したブロック図、第2図は起動系領域におい
て制御棒引抜阻止信号を発生した場合の応答例を示した
図、第3図は中間系領域において制御棒引抜阻止信号お
よびスクラム信号を発生した場合の応答例を示した図、
第4図は中間系領域においてペリオド計測監視手段の入
力信号と前記ペリオド計測監視手段の構成要素である増
幅器およびローパスフィルタを通過後の信号の時間に対
する変化を示したグラフ、第5図は従来の起動系領域に
おける中性子束計測監視装置のブロック図、第6図は従
来の中間系領域における中性子束計測監視装置のブロッ
ク図、第7図は従来の広域系中性子束計測監視装置のブ
ロック図である。 30……広域中性子束検出器、31……広域前置増幅器、32
……パルス系用増幅器、33……キャンベル系用増幅器、
34……起動系出力処理回路、35……中間系出力処理回
路、36a,36b,36c……ペリオド計測監視手段、37a,37b,3
7c……増幅器、38a,38b,38c……ローパスフィルタ、3
9a,39b,39c……信号比較回路、40……出力比較回路、41
……切換器、42a,42b……表示器。
FIG. 1 is a block diagram showing an embodiment of a wide area neutron flux measurement and monitoring device according to the present invention, and FIG. 2 is a diagram showing an example of a response when a control rod withdrawal prevention signal is generated in an activation system region. FIG. 3 is a diagram showing a response example when the control rod pull-out prevention signal and the scrum signal are generated in the intermediate system region,
FIG. 4 is a graph showing changes with time in the input signal of the period measuring and monitoring means and the signal after passing through the amplifier and the low-pass filter which are the constituent elements of the period measuring and monitoring means in the intermediate region, and FIG. FIG. 6 is a block diagram of a neutron flux measurement and monitoring device in the start-up region, FIG. 6 is a block diagram of a conventional neutron flux measurement and monitoring device in the intermediate region, and FIG. 7 is a block diagram of a conventional wide area neutron flux measurement and monitoring device. . 30 …… Wide area neutron flux detector, 31 …… Wide area preamplifier, 32
...... Pulse system amplifier, 33 …… Campbell system amplifier,
34 ...... activation system output processing circuit, 35 ...... intermediate system output processing circuit, 36 a, 36 b, 36 c ...... Periodo measurement monitoring means, 37 a, 37 b, 3
7 c …… Amplifier, 38 a , 38 b , 38 c …… Low pass filter, 3
9 a , 39 b , 39 c …… Signal comparison circuit, 40 …… Output comparison circuit, 41
...... Switch, 42 a , 42 b ...... Display.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】原子炉圧力容器内の起動系領域にある中性
子束、および中間系領域にある中性子束を検出する広域
中性子束検出器と、この広域中性子束検出器によって検
出された広域中性子束の信号を周波数帯域分離し、この
周波数帯域分離された高周波数成分が入力されるパルス
系用増幅器、および中間周波数成分が入力されるキャン
ベル系用増幅器を備えた広域前置増幅器と、前記パルス
系用増幅器の出力を入力して波高弁別し、かつ計数率を
計測して波高弁別された信号を起動系信号φaとして出
力する起動系出力処理回路と、前記キャンベル系用増幅
器の出力信号を入力とし、この入力の二乗平均値を平滑
化し中間系信号φbとして出力する中間系出力処理回路
と、前記起動系出力処理回路によって出力された前記起
動系信号φaの計数率が予め設定した設定値以上のとき
に切換指示信号を出力する出力比較回路と、前記出力比
較回路の出力である切換指示信号に基づいて、前記起動
系信号φaの計数率が前記設定値以上のとき前記中間系
信号φbを通過させ、前記起動系信号φaの計数率が前記
設定値未満のときは、前記起動系信号φaを通過させる
ように接続を切換える切換器と、第一の増幅器、第一の
ローパスフィルタ、および第一の信号比較回路を備え、
前記起動系信号φaの計数率が前記設定値未満の場合の
み前記切換器によって前記起動系出力処理回路に接続さ
れ、前記起動系信号φaが前記第一の増幅器および前記
第一のローパスフィルタを通過した後の信号φa′と前
記起動系信号φaを前記第一の信号比較回路で比較し、
前記起動系信号φaの大きさが前記信号φa′の大きさ以
上のときに制御棒引抜阻止信号を出力する第一のペリオ
ド計測監視手段と、第二の増幅器、第二のローパスフィ
ルタおよび第二の信号比較回路を備え、前記起動系信号
φaの計数率が前記設定値以上のとき前記切換器によっ
て前記中間系出力処理回路に接続され、前記中間系出力
信号φbが前記第二の増幅器および第二のローパスフィ
ルタを通過した後の信号φb′と前記中間系信号φbを前
記第二の信号比較回路で比較し、前記中間系信号φb
大きさが前記信号φb′の大きさ以上のときに制御棒引
抜阻止信号を出力する第二のペリオド計測監視手段と、
第三の増幅器、第三のローパスフィルタおよび第三の信
号比較回路を備え、前記第二のペリオド計測監視手段と
並列に配置され、前記起動系信号φaの計数率が前記設
定値以上のとき前記切換器によって前記中間系出力処理
回路に接続され、前記中間系信号φbが前記第三の増幅
器および前記第三のローパスフィルタを通過した後の信
号φc′と前記中間系信号φbを前記第三の信号比較回路
で比較し、前記中間系信号φbの大きさが前記信号φc
の大きさ以上のときにスクラム信号を発生する第三のペ
リオド計測監視手段とを具備していることを特徴とする
広域系中性子束計測監視装置。
1. A wide-area neutron flux detector for detecting a neutron flux in a start-up system region in a reactor pressure vessel and a neutron flux in an intermediate-system region, and a wide-range neutron flux detected by this wide-range neutron flux detector. A wide-area preamplifier including a pulse system amplifier to which the high frequency component separated by the frequency band separation is input, and a Campbell system amplifier to which the intermediate frequency component is input, and the pulse system For inputting the output of the amplifier for use in the pulse height discrimination, measuring the count rate, and outputting the signal subjected to the pulse height discrimination as the activation system signal φ a , and inputting the output signal of the Campbell amplifier and then, counting rate of the intermediate system output processing circuit for smoothing the mean square value of the input and output as an intermediate system signal phi b, the starting system the activation system signal outputted by the output processing circuit phi a An output comparator circuit for outputting a switching instruction signal when the above setting value set in advance, based on the switching instruction signal is output from the output comparison circuit, the counting rate of the activation system signal phi a of more than the set value when passed through the intermediate system signal phi b, wherein when the count rate of the activation system signal phi a is less than the set value, a switching device for switching a connection to pass the activation system signal phi a, the first An amplifier, a first low-pass filter, and a first signal comparison circuit,
Only when the count rate of the start-up signal φ a is less than the set value is connected to the start-up output processing circuit by the switch, the start-up signal φ a is the first amplifier and the first low-pass filter. The signal φ a ′ after passing through and the starting system signal φ a are compared in the first signal comparison circuit,
First period measurement and monitoring means for outputting a control rod withdrawal prevention signal when the magnitude of the activation system signal φ a is greater than or equal to the magnitude of the signal φ a ′, a second amplifier, a second low pass filter, and A second signal comparison circuit, which is connected to the intermediate system output processing circuit by the switch when the count rate of the starting system signal φ a is equal to or more than the set value, and the intermediate system output signal φ b is the second compared with the amplifier and a second low-pass filtered signal phi b 'and the intermediate system signal phi b of the second signal comparison circuit after passing the magnitude is the signal of the intermediate system signal phi b phi b Second period measurement and monitoring means for outputting a control rod withdrawal prevention signal when the size is equal to or greater than ‘
A third amplifier, a third low-pass filter and a third signal comparison circuit, arranged in parallel with the second period measurement and monitoring means, when the count rate of the activation system signal φ a is equal to or more than the set value. The intermediate system output processing circuit is connected to the intermediate system output processing circuit by the switch, and the intermediate system signal φ b is passed through the third amplifier and the third low-pass filter to output the signal φ c ′ and the intermediate system signal φ b . The magnitude of the intermediate signal φ b is compared by the third signal comparison circuit, and the magnitude of the intermediate signal φ b is the signal φ c ′.
And a third period measurement / monitoring means for generating a scrum signal when the magnitude is equal to or larger than the above.
JP61093826A 1986-04-23 1986-04-23 Wide area neutron flux measurement and monitoring device Expired - Lifetime JPH07101238B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61093826A JPH07101238B2 (en) 1986-04-23 1986-04-23 Wide area neutron flux measurement and monitoring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61093826A JPH07101238B2 (en) 1986-04-23 1986-04-23 Wide area neutron flux measurement and monitoring device

Publications (2)

Publication Number Publication Date
JPS62250396A JPS62250396A (en) 1987-10-31
JPH07101238B2 true JPH07101238B2 (en) 1995-11-01

Family

ID=14093200

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61093826A Expired - Lifetime JPH07101238B2 (en) 1986-04-23 1986-04-23 Wide area neutron flux measurement and monitoring device

Country Status (1)

Country Link
JP (1) JPH07101238B2 (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000275383A (en) * 1999-03-26 2000-10-06 Toshiba Corp Reactor neutron flux level measurement device
CN104795117A (en) * 2015-04-09 2015-07-22 中国核动力研究设计院 H2 filter based method for performing delay elimination on signals of rhodium self-powered detector
CN104778984A (en) * 2015-04-09 2015-07-15 中国核动力研究设计院 H2 filtration-based signal delay elimination method for rhodium self-powered detector
CN104778981A (en) * 2015-04-09 2015-07-15 中国核动力研究设计院 Luenberger form H2/H<infinity> mixed filtration-based signal delay elimination method for rhodium detector

Also Published As

Publication number Publication date
JPS62250396A (en) 1987-10-31

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