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JP2013088266A - Radiation monitor - Google Patents

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JP2013088266A
JP2013088266A JP2011228420A JP2011228420A JP2013088266A JP 2013088266 A JP2013088266 A JP 2013088266A JP 2011228420 A JP2011228420 A JP 2011228420A JP 2011228420 A JP2011228420 A JP 2011228420A JP 2013088266 A JP2013088266 A JP 2013088266A
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JP2013088266A5 (en
JP5743844B2 (en
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Kenichi Mogi
健一 茂木
Tatsuro Kobayashi
達郎 小林
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Mitsubishi Electric Corp
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Abstract

【課題】応答性を犠牲にしないで標準偏差に関係する機器誤差を低減した高精度の検出を行うことができる放射線モニタを提供する。
【解決手段】放射線をデジタルパルスとして定周期で計数して計数値を出力するカウンタ3と、演算器4は、計数率を、今回演算周期から前回演算周期の計数率に演算周期時間を乗じた値を減算して求めた加減差を、前回演算周期の加減差積算値に加算して今回演算周期の加減差積算値とし、当該今回演算周期の加減差積算値の小数点以下を切り捨てた加減差積算自然数を求め、今回演算周期の加減差積算自然数と前回演算周期の加減差積算自然数とを比較し、異なる場合には、今回演算周期および前回演算周期の加減差積算自然数の平均値を求め、当該平均値に標準偏差に基づく重み付け係数を乗じて標準偏差が一定になるように演算して計数率とするか、同一の場合には、前回演算周期の計数率を今回演算周期の計数率とし、警報判定を行う。
【選択図】図1
A radiation monitor capable of performing highly accurate detection with reduced instrument errors related to standard deviation without sacrificing responsiveness is provided.
A counter 3 that counts radiation as a digital pulse at a constant cycle and outputs a count value, and a calculator 4 multiply the count rate of the previous calculation cycle from the current calculation cycle by the calculation cycle time. The addition / subtraction obtained by subtracting the value is added to the addition / subtraction integration value of the previous calculation cycle to obtain the addition / subtraction integration value of the current calculation cycle. Find the integrated natural number, compare the addition / subtraction integration natural number of the current calculation cycle with the addition / subtraction integration natural number of the previous calculation cycle, and if different, find the average value of the addition / subtraction integration natural number of the current calculation cycle and the previous calculation cycle, Multiply the average value by a weighting factor based on the standard deviation to calculate the standard deviation to be constant, or use the same as the count rate in the previous calculation cycle. , Alarm judgment Cormorant.
[Selection] Figure 1

Description

この発明は、原子炉施設、使用済燃料再処理施設等の放出管理あるいは放射線管理に用いられる放射線モニタに関し、特に、機器誤差を圧縮するものである。   The present invention relates to a radiation monitor used for emission management or radiation management of a nuclear reactor facility, a spent fuel reprocessing facility, etc., and in particular, compresses equipment errors.

従来の原子炉施設、使用済燃料再処理施設等で使用される放射線モニタは、放射線を検出した結果としての信号パルスの繰り返し周波数が10cpm程度から10cpm程度までの広いレンジをカバーし、レンジ切換なしで要求の精度を確保して測定することが求められている。また、放射線検出器の出力パルスの繰り返し周波数が、バックグラウンドレベルから高警報点を含む高計数率領域へ変化した場合に、計数率の速い応答が求められている。このため、計数率に反比例して時定数が変化すると共に標準偏差が一定になるように、入力パルスの繰り返し周波数に対してそれを測定した結果として得られる計数率が時定数の1次遅れで応答するようにし、入力パルスの繰り返し周波数と計数率に対応したフィードバックパルスの繰り返し周波数がバランスさせて計数率を測定する仕組みが広く導入されている(例えば、特許文献1参照)。 The radiation monitor used in the conventional nuclear reactor facility, spent fuel reprocessing facility, etc. covers a wide range where the repetition frequency of the signal pulse as a result of detecting the radiation ranges from about 10 cpm to about 10 7 cpm. There is a need to ensure the required accuracy without switching. Further, when the repetition frequency of the output pulse of the radiation detector changes from the background level to a high count rate region including a high alarm point, a response with a fast count rate is required. For this reason, the count rate obtained as a result of measuring it with respect to the repetition frequency of the input pulse is the first-order delay of the time constant so that the time constant changes in inverse proportion to the count rate and the standard deviation becomes constant. A mechanism for measuring the count rate by making the response and balancing the repetition frequency of the input pulse and the repetition frequency of the feedback pulse corresponding to the count rate has been widely introduced (see, for example, Patent Document 1).

特開平11−326523号公報JP-A-11-326523

従来の放射線モニタは、上記のようなものにて計数率を測定しているので、入力パルスとフィードバックパルスのそれぞれの繰り返し周波数がバランスしたときに、最大1パルス入力分のゆらぎが発生し、好適な応答性かつ高精度で放射線量を測定する場合に、標準偏差に依存して機器固有の誤差が大きくなるという問題点があった。   Since the conventional radiation monitor measures the counting rate with the above-mentioned, when the repetition frequency of each of the input pulse and the feedback pulse is balanced, fluctuations of up to one pulse input occur, which is preferable. When measuring the radiation dose with high responsiveness and high accuracy, there is a problem that the error inherent to the device increases depending on the standard deviation.

この発明は上記のような課題を解決するためになされたものであり、応答性を犠牲にすることなく機器誤差を圧縮した放射線モニタを提供することを目的とする。   The present invention has been made to solve the above-described problems, and an object thereof is to provide a radiation monitor in which instrument errors are compressed without sacrificing responsiveness.

この発明の放射線モニタは、
放射線を検出するとアナログ信号パルスを出力する放射線検出手段と、
上記アナログ信号パルスを入力して許容範囲内にあるとデジタルパルスとして出力する波高弁別手段と、
上記デジタルパルスを入力して定周期で計数して計数値を出力する計数手段と、
上記定周期の計数率を演算し、当該計数率を工学値に変換し、当該工学値について警報判定を行う演算手段とを有し、
上記演算手段は、上記計数率を、
今回演算周期の計数値から前回演算周期の計数率に演算周期時間を乗じた値を減算して求めた加減差を、上記前回演算周期の加減差積算値に加算して今回演算周期の加減差積算値とし、当該今回演算周期の加減差積算値の小数点以下を切り捨てた加減差積算自然数を求め、上記今回演算周期の加減差積算自然数と上記前回演算周期の加減差積算自然数とを比較し、
異なる場合には、上記今回演算周期の加減差積算自然数および上記前回演算周期の加減差積算自然数の平均値を求め、当該平均値に標準偏差に基づく重み付け係数を乗じて標準偏差が一定になるように演算して計数率とするか、
同一の場合には、上記前回演算周期の計数率を上記今回演算周期の計数率とするものである。
The radiation monitor of the present invention is
Radiation detecting means for outputting an analog signal pulse when detecting radiation;
A pulse height discriminating means for inputting the analog signal pulse and outputting it as a digital pulse within an allowable range;
Counting means for inputting the digital pulse, counting at a fixed period, and outputting a count value;
Calculating the count rate of the fixed period, converting the count rate into an engineering value, and having an arithmetic means for performing a warning determination on the engineering value,
The calculation means calculates the count rate as follows:
Addition / subtraction obtained by subtracting the value calculated by multiplying the count rate of the previous calculation cycle by the calculation cycle time from the count value of the previous calculation cycle is added to the accumulated value of the previous calculation cycle to add or subtract the current calculation cycle. As an integrated value, an addition / subtraction integration natural number obtained by rounding down the decimals of the addition / subtraction integration value of the current calculation cycle is calculated, and the addition / subtraction integration natural number of the current calculation cycle is compared with the addition / subtraction integration natural number of the previous calculation cycle,
If they are different, the average value of the addition / subtraction integration natural number of the current calculation cycle and the addition / subtraction integration natural number of the previous calculation cycle are obtained, and the standard deviation is made constant by multiplying the average value by a weighting factor based on the standard deviation. To calculate the counting rate,
In the same case, the count rate of the previous calculation cycle is set as the count rate of the current calculation cycle.

また、この発明の放射線モニタは、
放射線を検出してアナログ信号パルスを出力する放射線検出手段と、
上記アナログ信号パルスを入力して許容範囲内にあるとデジタルパルスとして出力する波高弁別手段と、
上記デジタルパルスを加算入力し、パルス発生手段から出力されたフィードバッグパルスを減算入力し、その結果を加減差積算値として出力する加減差積算手段と、
上記加減差積算手段に入力される上記デジタルパルスおよび上記フィードバッグパルスを標準偏差に基づいて重み付けして積算する積算制御手段と、
上記デジタルパルスの繰り返し周波数に対して時定数の一次遅れで応答する繰り返し周波数を上記フィードバックパルスとして上記加減差積算手段に出力するパルス発生手段と、
定周期で計数率を演算し、当該計数率を工学値に変換し、当該工学値について警報判定を行う演算手段とを備え、
上記演算手段は、上記計数率を、
前回演算周期の加減差積算値と今回演算周期の加減差積算値とを比較し、
異なる場合には、上記前回演算周期の加減差積算値および上記今回演算周期の加減差積算値の平均値を求め、当該平均値を標準偏差が一定になるように演算して上記計数率とするか、
同一の場合には、上記前回演算周期の計数率を上記今回演算周期の計数率とするものである。
The radiation monitor of the present invention is
Radiation detecting means for detecting radiation and outputting analog signal pulses;
A pulse height discriminating means for inputting the analog signal pulse and outputting it as a digital pulse within an allowable range;
Addition input of the digital pulse, subtraction input of the feedback pulse output from the pulse generation means, addition / subtraction integration means for outputting the result as an addition / subtraction integration value,
Integration control means for weighting and integrating the digital pulse and feedback pulse input to the addition / subtraction integration means based on a standard deviation;
Pulse generating means for outputting a repetition frequency that responds with a first order delay of a time constant to the repetition frequency of the digital pulse as the feedback pulse to the addition / subtraction integration means;
A calculation rate is calculated at a fixed period, the count rate is converted into an engineering value, and an arithmetic means for performing alarm determination on the engineering value is provided.
The calculation means calculates the count rate as follows:
Compare the accumulated value of the previous calculation cycle with the accumulated value of the current calculation cycle,
If they are different, the average value of the addition / subtraction integration value of the previous calculation cycle and the addition / subtraction integration value of the current calculation cycle is obtained, and the average value is calculated so that the standard deviation is constant to obtain the count rate. Or
In the same case, the count rate of the previous calculation cycle is set as the count rate of the current calculation cycle.

この発明の放射線モニタは、
放射線を検出するとアナログ信号パルスを出力する放射線検出手段と、
上記アナログ信号パルスを入力して許容範囲内にあるとデジタルパルスとして出力する波高弁別手段と、
上記デジタルパルスを入力して定周期で計数して計数値を出力する計数手段と、
上記定周期の計数率を演算し、当該計数率を工学値に変換し、当該工学値について警報判定を行う演算手段とを有し、
上記演算手段は、上記計数率を、
今回演算周期の計数値から前回演算周期の計数率に演算周期時間を乗じた値を減算して求めた加減差を、上記前回演算周期の加減差積算値に加算して今回演算周期の加減差積算値とし、当該今回演算周期の加減差積算値の小数点以下を切り捨てた加減差積算自然数を求め、上記今回演算周期の加減差積算自然数と上記前回演算周期の加減差積算自然数とを比較し、
異なる場合には、上記今回演算周期の加減差積算自然数および上記前回演算周期の加減差積算自然数の平均値を求め、当該平均値に標準偏差に基づく重み付け係数を乗じて標準偏差が一定になるように演算して計数率とするか、
同一の場合には、上記前回演算周期の計数率を上記今回演算周期の計数率とするので、
応答性を犠牲にしないで標準偏差に関係する機器誤差を低減した高精度の検出を行うことができる。
The radiation monitor of the present invention is
Radiation detecting means for outputting an analog signal pulse when detecting radiation;
A pulse height discriminating means for inputting the analog signal pulse and outputting it as a digital pulse within an allowable range;
Counting means for inputting the digital pulse, counting at a fixed period, and outputting a count value;
Calculating the count rate of the fixed period, converting the count rate into an engineering value, and having an arithmetic means for performing a warning determination on the engineering value,
The calculation means calculates the count rate as follows:
Addition / subtraction obtained by subtracting the value calculated by multiplying the count rate of the previous calculation cycle by the calculation cycle time from the count value of the previous calculation cycle is added to the accumulated value of the previous calculation cycle to add or subtract the current calculation cycle. As an integrated value, an addition / subtraction integration natural number obtained by rounding down the decimals of the addition / subtraction integration value of the current calculation cycle is calculated, and the addition / subtraction integration natural number of the current calculation cycle is compared with the addition / subtraction integration natural number of the previous calculation cycle,
If they are different, the average value of the addition / subtraction integration natural number of the current calculation cycle and the addition / subtraction integration natural number of the previous calculation cycle are obtained, and the standard deviation is made constant by multiplying the average value by a weighting factor based on the standard deviation. To calculate the counting rate,
In the case of the same, since the count rate of the previous calculation cycle is the count rate of the current calculation cycle,
It is possible to perform highly accurate detection with reduced instrument errors related to standard deviation without sacrificing responsiveness.

また、この発明の放射線モニタは、
放射線を検出してアナログ信号パルスを出力する放射線検出手段と、
上記アナログ信号パルスを入力して許容範囲内にあるとデジタルパルスとして出力する波高弁別手段と、
上記デジタルパルスを加算入力し、パルス発生手段から出力されたフィードバッグパルスを減算入力し、その結果を加減差積算値として出力する加減差積算手段と、
上記加減差積算手段に入力される上記デジタルパルスおよび上記フィードバッグパルスを標準偏差に基づいて重み付けして積算する積算制御手段と、
上記デジタルパルスの繰り返し周波数に対して時定数の一次遅れで応答する繰り返し周波数を上記フィードバックパルスとして上記加減差積算手段に出力するパルス発生手段と、
定周期で計数率を演算し、当該計数率を工学値に変換し、当該工学値について警報判定を行う演算手段とを備え、
上記演算手段は、上記計数率を、
前回演算周期の加減差積算値と今回演算周期の加減差積算値とを比較し、
異なる場合には、上記前回演算周期の加減差積算値および上記今回演算周期の加減差積算値の平均値を求め、当該平均値を標準偏差が一定になるように演算して上記計数率とするか、
同一の場合には、上記前回演算周期の計数率を上記今回演算周期の計数率とするので、
応答性を犠牲にしないで標準偏差に関係する機器誤差を低減した高精度の検出を行うことができる。
The radiation monitor of the present invention is
Radiation detecting means for detecting radiation and outputting analog signal pulses;
A pulse height discriminating means for inputting the analog signal pulse and outputting it as a digital pulse within an allowable range;
Addition input of the digital pulse, subtraction input of the feedback pulse output from the pulse generation means, addition / subtraction integration means for outputting the result as an addition / subtraction integration value,
Integration control means for weighting and integrating the digital pulse and feedback pulse input to the addition / subtraction integration means based on a standard deviation;
Pulse generating means for outputting a repetition frequency that responds with a first order delay of a time constant to the repetition frequency of the digital pulse as the feedback pulse to the addition / subtraction integration means;
A calculation rate is calculated at a fixed period, the count rate is converted into an engineering value, and an arithmetic means for performing alarm determination on the engineering value is provided.
The calculation means calculates the count rate as follows:
Compare the accumulated value of the previous calculation cycle with the accumulated value of the current calculation cycle,
If they are different, the average value of the addition / subtraction integration value of the previous calculation cycle and the addition / subtraction integration value of the current calculation cycle is obtained, and the average value is calculated so that the standard deviation is constant to obtain the count rate. Or
In the case of the same, since the count rate of the previous calculation cycle is the count rate of the current calculation cycle,
It is possible to perform highly accurate detection with reduced instrument errors related to standard deviation without sacrificing responsiveness.

この発明の実施の形態1の放射線モニタの構成を示すブロック図である。It is a block diagram which shows the structure of the radiation monitor of Embodiment 1 of this invention. 図1に示した放射線モニタの演算器の演算処理を示すフローチャートである。It is a flowchart which shows the arithmetic processing of the calculator of the radiation monitor shown in FIG. この発明の実施の形態2の放射線モニタの構成を示すブロック図である。It is a block diagram which shows the structure of the radiation monitor of Embodiment 2 of this invention. 図3に示した放射線モニタの演算器の演算処理を示すフローチャートである。It is a flowchart which shows the arithmetic processing of the calculator of the radiation monitor shown in FIG. この発明の実施の形態3の放射線モニタの構成を示すブロック図である。It is a block diagram which shows the structure of the radiation monitor of Embodiment 3 of this invention. 図5に示した放射線モニタの演算器の入出力特性を示す図である。It is a figure which shows the input / output characteristic of the calculator of the radiation monitor shown in FIG. 図5に示した放射線モニタの演算器の演算処理を示すフローチャートである。It is a flowchart which shows the arithmetic processing of the calculator of the radiation monitor shown in FIG. この発明の実施の形態4の放射線モニタの構成を示すブロック図である。It is a block diagram which shows the structure of the radiation monitor of Embodiment 4 of this invention. 図8に示した放射線モニタのタイミングチャートを示す図である。It is a figure which shows the timing chart of the radiation monitor shown in FIG.

実施の形態1.
以下、本願発明の実施の形態について説明する。図1はこの発明の実施の形態1における放射線モニタの構成を示すブロック図、図2は図1に示した放射線モニタの演算器の演算処理を示すフローチャートである。図1において、放射線を検出するとアナログ信号パルスを出力する放射線検出手段としての放射線検出器1と、放射線検出器1から出力されたアナログ信号パルスを入力し、そのアナログ信号パルスが許容範囲内であるか否かを、例えば、アナログ信号パルスの電圧レベルが設定されたレベル以上である場合、あるいは設定されたレベルの範囲内である場合、入力されたアナログ信号パルスを許容範囲内であるとみなしてデジタルパルスとして出力し、それ以外の設定された条件を逸脱した場合、入力されたアナログ信号パルスをノイズとみなしてデジタルパルスを出力しない波高別手段としての波高弁別器2とを備える。
Embodiment 1 FIG.
Embodiments of the present invention will be described below. FIG. 1 is a block diagram showing a configuration of a radiation monitor according to Embodiment 1 of the present invention, and FIG. 2 is a flowchart showing a calculation process of a calculator of the radiation monitor shown in FIG. In FIG. 1, a radiation detector 1 serving as radiation detecting means for outputting an analog signal pulse when radiation is detected, and an analog signal pulse output from the radiation detector 1 are input, and the analog signal pulse is within an allowable range. For example, if the voltage level of the analog signal pulse is equal to or higher than the set level, or is within the set level range, the input analog signal pulse is regarded as being within the allowable range. A pulse height discriminator 2 is provided as a pulse height discriminating means that outputs a digital pulse and deviates from other set conditions and regards the input analog signal pulse as noise and does not output the digital pulse.

さらに、波高弁別器2から出力されたデジタルパルスを入力し、定周期で計数して計数値ΔNを出力する計数手段としてのカウンタ3と、カウンタ3から出力された今回演算周期の計数値ΔN(今回)および標準偏差に基づき後述のようにして定周期で計数率を演算し、その計数率を工学値に変換し、その工学値について警報判定を行い、工学値および警報判定結果を出力する演算手段としての演算器4と、演算器4の演算に必要な演算手順、各設定値、データなどを格納するメモリ5と、演算器4から出力された工学値および警報判定結果を表示すると共に、画面から設定値入力および警報リセット等の操作を行うことができる表示器6とにて構成される。尚、工学値は用途により計数率そのもの(計数率=工学値)である場合、また、工学値を放射線量に変換する定数を乗じたものである場合などがある。ここでは説明の便宜上、工学値=計数率の場合にて説明する。   Further, the digital pulse output from the wave height discriminator 2 is input, the counter 3 as a counting means for counting at a constant cycle and outputting the count value ΔN, and the count value ΔN (current count) output from the counter 3 ( This time, based on the standard deviation and the count rate, the count rate is calculated at regular intervals, the count rate is converted into an engineering value, the engineering value is judged as an alarm, and the engineering value and the alert judgment result are output. While displaying the arithmetic unit 4 as a means, the memory 5 for storing the calculation procedure necessary for the calculation of the arithmetic unit 4, each set value, data, etc., the engineering value and the alarm judgment result output from the arithmetic unit 4, It is comprised with the indicator 6 which can perform operation, such as setting value input and alarm reset, from a screen. The engineering value may be the counting rate itself (counting rate = engineering value) depending on the application, or may be a product of the engineering value multiplied by a constant for converting the radiation dose. Here, for the sake of convenience of explanation, the case of engineering value = counting rate will be described.

次に上記のように構成された実施の形態1の放射線モニタの動作について説明する。
まず、演算器4における標準偏差一定の計数率mを求める演算について説明する。前回演算周期の計数率をm(前回)、前回演算周期の加減差積算値をM(前回)、演算周期毎のカウンタの計数値をΔN、計数時間(演算周期時間をさす)をΔT、今回演算周期の加減差積算値をM(今回)とし、前回演算周期の加減差積算値の小数点以下を切り捨てた自然数をM(前回:自然数)、今回演算周期の加減差積算値の小数点以下を切り捨てた自然数をM(今回:自然数)、今回演算周期の計数率をm(今回)とする。そして、M(今回)およびm(今回)はそれぞれ下記(1)式、(2)式により求めることができる。
M(今回)=M(前回)+{ΔN(今回)−m(前回)×ΔT}・・・(1)
m(今回)=exp{γ×2α×M(今回:自然数平均値)}・・・(2)
Next, the operation of the radiation monitor of the first embodiment configured as described above will be described.
First, the calculation for obtaining the count rate m with a constant standard deviation in the calculator 4 will be described. The count rate of the previous calculation cycle is m (previous), the addition / subtraction integrated value of the previous calculation cycle is M (previous), the counter value of the counter for each calculation cycle is ΔN, the count time (refers to the calculation cycle time) is ΔT, this time The integration value of the calculation cycle is M (current), the natural number of the previous calculation cycle is rounded down to the natural number M (previous: natural number), and the decimal point of the current cycle of the addition / subtraction integration value is rounded down. The natural number is M (current time: natural number), and the count rate of the current calculation cycle is m (current time). M (current) and m (current) can be obtained by the following equations (1) and (2), respectively.
M (current) = M (previous) + {ΔN (current) −m (previous) × ΔT} (1)
m (current) = exp {γ 1 × 2 α × M (current: natural number average value)} (2)

上記(2)式で求められた計数率m(今回)は、下記(3)式に示すように標準偏差σ=一定で制御される。
σ=1/(2mτ)1/2=一定・・・(3)
また、時定数τは、下記(4)式のように計数率mに反比例し、標準偏差の2乗に反比例し、γに反比例する。γは、下記(5)式のように標準偏差の2乗に比例し、例えば、計数の重み付けに係わる定数αを用いて2αで重み付けして計数することにより、上記(2)式から求められる計数率m(今回)は、波高弁別器2の出力パルスの繰り返し周波数の変化に時定数τの一次遅れで追従して応答する。
τ=1/(2mσ)=1/(mγ)・・・(4)
γ=2σ=2α×2−11×ln2=γ×2α=定数・・・(5)
The count rate m (current) obtained by the above equation (2) is controlled with a standard deviation σ = constant as shown in the following equation (3).
σ = 1 / (2mτ) 1/2 = constant (3)
The time constant τ is inversely proportional to the count rate m, inversely proportional to the square of the standard deviation, and inversely proportional to γ, as shown in the following equation (4). γ is proportional to the square of the standard deviation as shown in the following equation (5), and is obtained from the above equation (2) by, for example, counting by weighting with 2α using a constant α relating to the weighting of the count. The count rate m (current time) responds by following the change in the repetition frequency of the output pulse of the wave height discriminator 2 with a first order delay of the time constant τ.
τ = 1 / (2mσ 2 ) = 1 / (mγ) (4)
γ = 2σ 2 = 2 α × 2 −11 × ln2 = γ 1 × 2 α = constant (5)

上記(2)式において2αで計数の重み付けすることにより、α=0の重み付け2=1を基準とすると、計数α=2の重み付け2=4で、τは1/4、α=4の重み付け2=16で、τは1/16、α=6の重み付け2=64で、τは1/64と、計数の重み付けを大きくすることにより応答は順次速くなる。 By weighting the count by 2 alpha in the above (2), when the reference weighted 2 0 = 1 alpha = 0, weighting 2 2 = 4 counts alpha = 2, tau is 1/4, alpha = When the weighting of 4 is 2 4 = 16, τ is 1/16, the weighting of α = 6 is 2 6 = 64, and τ is 1/64.

次に上記のように構成された実施の形態1の放射線モニタの演算器4の演算処理手順について図2に基づいて説明する。まず、α、高警報設定値、低警報設定値、m(前回)、M(前回)、M(前回:自然数)、ΔN(今回)をメモリ5から入力する(図2のステップS1)。次に、上記(1)式によりM(今回)を求める(図2のステップS2)。次に、M(今回)の小数点以下を切り捨てたM(今回:自然数)を求め(図2のステップS3)、M(今回:自然数)≠M(前回:自然数)か否かの判定を行う(図2のステップS4)。次に、異なる場合(YES)には、M(今回:自然数平均値)={M(前回:自然数)+M(今回:自然数)}/2を求める(図2のステップS5)。次に、M(今回:自然数平均値)に基づいて、上記(2)式でm(今回)を求める(図2のステップS6)。   Next, the calculation processing procedure of the calculator 4 of the radiation monitor according to the first embodiment configured as described above will be described with reference to FIG. First, α, high alarm set value, low alarm set value, m (previous), M (previous), M (previous: natural number), and ΔN (current) are input from the memory 5 (step S1 in FIG. 2). Next, M (current) is obtained by the above equation (1) (step S2 in FIG. 2). Next, M (current: natural number) obtained by rounding down the decimal point of M (current) is obtained (step S3 in FIG. 2), and it is determined whether M (current: natural number) ≠ M (previous: natural number) ( Step S4 in FIG. Next, if different (YES), M (current: natural number average value) = {M (previous: natural number) + M (current: natural number)} / 2 is obtained (step S5 in FIG. 2). Next, based on M (current: natural number average value), m (current) is obtained by the above equation (2) (step S6 in FIG. 2).

一方、ステップS4で、同一の場合(NO)ならば、m(前回)をm(今回)とし出力する(図2のステップS7)。次に、m(今回)≧高警報設定値か否かの判定を行う(図2のステップS8)。次に、YESならば高警報を出力し(図2のステップS9)、例えば表示器6に高警報であることを表示し、今回演算周期を終了してステップS1に戻る。一方、ステップS8でNOならば、m(今回)≦低警報設定値かの判定を行う(図2のステップS10)。次に、YESならば低警報を出力し(図2のステップS11)、例えば表示器6に低警報であることを表示し、今回演算周期を終了してステップS1に戻る。一方、ステップS10でNOならば、今回演算周期を終了してステップS1に戻る。   On the other hand, if they are the same in step S4 (NO), m (previous) is output as m (present) (step S7 in FIG. 2). Next, it is determined whether m (current) ≧ high alarm set value (step S8 in FIG. 2). Next, if YES, a high alarm is output (step S9 in FIG. 2), for example, the display 6 indicates that the alarm is high, ends the current calculation cycle, and returns to step S1. On the other hand, if NO in step S8, it is determined whether m (current) ≤ low alarm set value (step S10 in FIG. 2). Next, if YES, a low alarm is output (step S11 in FIG. 2), for example, the display 6 indicates that the alarm is low, ends the current calculation cycle, and returns to step S1. On the other hand, if “NO” in the step S10, the current calculation cycle is ended and the process returns to the step S1.

計数率は、測定レンジ下限から測定レンジ上限まで、測定精度からの要求で決まる標準偏差σになるように、σ=一定で計数率が演算される。低計数率を測定する用途では応答性が優先され、大きな標準偏差に設定される。例えば、標準偏差σが0.104と大きい場合の誤差の圧縮について説明する。標準偏差0.104に対応して決まる計数の重み付けは2=64であり、上記(2)式においてM(今回:自然数平均値)に計数の重み64が乗ぜられ、さらに定数γが乗ぜられたものに基づき計数率m(今回)が求められる。上記(5)式においてγは”2−11×ln2=一定”として求めることができ、”3.38×10−4”となる。10.0cpmのときMは、”ln(計数率)/γ=ln10/(3.38×10−4)=6812”で、Mが計数の重み64だけ増加すると計数率は”exp(3.38×10−4×6876)=10.2cpm”に増加する。 The count rate is calculated with σ = constant so that the count rate becomes the standard deviation σ determined by the request from the measurement accuracy from the measurement range lower limit to the measurement range upper limit. In applications where a low count rate is measured, responsiveness is given priority and a large standard deviation is set. For example, error compression when the standard deviation σ is as large as 0.104 will be described. The weight of the count determined corresponding to the standard deviation of 0.104 is 2 6 = 64. In the above equation (2), M (current: natural number average value) is multiplied by the count weight 64, and further the constant γ 1 is multiplied. The counting rate m (this time) is obtained based on the obtained information. In the above equation (5), γ 1 can be obtained as “2 −11 × ln2 = constant”, and becomes “3.38 × 10 −4 ”. When 10.0 cpm, M is “ln (count rate) / γ = ln10 / (3.38 × 10 −4 ) = 6812”, and when M is increased by the count weight 64, the count rate is “exp (3. 38 × 10 −4 × 6876) = 10.2 cpm ″.

平衡状態においてM(今回:自然数)に基づき計数率を求めると10.0cpmと10.2cpmでゆらぐことになるが、M(今回:自然数)がM(前回:自然数)から変化した場合にM(今回:自然数平均値)に基づき計数率を求めることにより計数率は”exp(3.38×10−4×6844)=10.1cpm”で安定する。例えば、演算周期を1秒とすると、10cpmの等間隔のパルス列では6秒毎に加減差積算値に1パルスが加算され、その6秒間に1パルスが減算され、1パルスの加減算のタイミングを含めた全てのタイミングで計数率は安定する。 If the count rate is calculated based on M (current time: natural number) in an equilibrium state, it will fluctuate between 10.0 cpm and 10.2 cpm, but if M (current time: natural number) changes from M (previous: natural number), M ( The count rate is stabilized at “exp (3.38 × 10 −4 × 6844) = 10.1 cpm” by calculating the count rate based on the current value (natural number average value). For example, if the calculation cycle is 1 second, one pulse is added to the addition / subtraction integrated value every 6 seconds in a 10 cpm equidistant pulse train, and 1 pulse is subtracted every 6 seconds, including the timing of addition / subtraction of 1 pulse. The count rate is stable at all timings.

上記のように構成された実施の形態1の放射線モニタによれば、演算器は、前回演算周期から今回演算周期で加減差積算値の小数点以下を切り捨てた自然数が変化する場合に、その平均値に基づき計数率を求めるようにしたので、入力の繰り返し周波数が平衡状態にある場合には、全てのタイミングで計数率を安定させることができ、応答性を犠牲にしないで標準偏差に関係する機器誤差を低減して高精度で放射線を測定できる。   According to the radiation monitor of the first embodiment configured as described above, the arithmetic unit calculates the average value when the natural number obtained by rounding down the decimal point of the addition / subtraction integrated value changes from the previous calculation cycle to the current calculation cycle. Since the count rate is calculated based on the above, when the input repetition frequency is in an equilibrium state, the count rate can be stabilized at all timings, and the equipment related to the standard deviation without sacrificing responsiveness It is possible to measure radiation with high accuracy by reducing errors.

実施の形態2.
上記実施の形態1では、波高弁別器2から出力されたデジタルパルスをカウンタ3が定周期で計数して計数値ΔNを出力し、演算器4が、カウンタ3から出力された今回演算周期の計数値ΔN(今回)および標準偏差に基づき定周期で計数率を演算したが、本実施の形態2においては、図3に示すように、カウンタ3の代わりにアップダウンカウンタ7と、積算制御回路8と、パルス発生器9とを備える。
Embodiment 2. FIG.
In the first embodiment, the counter 3 counts the digital pulses output from the wave height discriminator 2 at a constant cycle and outputs a count value ΔN, and the calculator 4 counts the current calculation cycle output from the counter 3. Although the count rate is calculated at regular intervals based on the numerical value ΔN (current) and the standard deviation, in the second embodiment, an up / down counter 7 and an integration control circuit 8 are used instead of the counter 3 as shown in FIG. And a pulse generator 9.

アップダウンカウンタ7は、波高弁別器2から出力されたデジタルパルスを加算入力端子71に入力し、パルス発生器9から出力されたフィードバッグパルスを減算入力端子72に入力し、その結果の加減差積算値を出力する。積算制御回路8は、アップダウンカウンタ7の加算入力および減算入力を標準偏差に基づき重み付けして計数するようにアップダウンカウンタ7を制御する。パルス発生器9は、クロック91の出力に分周器92を接続し、分周器92の出力にレートマルチプライヤ93を接続し、アップダウンカウンタ7から出力された加減差積算値を入力して分周器92とレートマルチプライヤ93とを制御し、レートマルチプライヤ93の出力パルスの繰り返し周波数に変換してフィードバッグパルスとしてアップダウンカウンタ7の減算入力端子72に入力する。尚、クロック91は、演算器4に標準装備されているクロック(図示せず)と共用してもよい。   The up / down counter 7 inputs the digital pulse output from the pulse height discriminator 2 to the addition input terminal 71, inputs the feedback pulse output from the pulse generator 9 to the subtraction input terminal 72, and adds or subtracts the result. Output the integrated value. The integration control circuit 8 controls the up / down counter 7 so that the addition input and subtraction input of the up / down counter 7 are counted based on the standard deviation. The pulse generator 9 connects a frequency divider 92 to the output of the clock 91, connects a rate multiplier 93 to the output of the frequency divider 92, and inputs the addition / subtraction integrated value output from the up / down counter 7. The frequency divider 92 and the rate multiplier 93 are controlled, converted to a repetition frequency of the output pulse of the rate multiplier 93, and input to the subtraction input terminal 72 of the up / down counter 7 as a feedback pulse. Note that the clock 91 may be shared with a clock (not shown) provided as a standard in the arithmetic unit 4.

次に上記のように構成された実施の形態2の放射線モニタの動作について説明する。
まず、演算器4は、アップダウンカウンタ7から出力された今回演算周期の加減差積算値M(今回)を入力し、図4のフローチャートに示すようにM(今回:平均値)を求め、その値に基づき(6)式により計数率を求める。アップダウンカウンタ7の加算入力および減算入力の計数の重みに関しては、上記実施の形態1と同様であるため説明は省略する。
m(今回)=exp{γ×2α×M(今回:平均値)}・・・(6)
Next, the operation of the radiation monitor of the second embodiment configured as described above will be described.
First, the arithmetic unit 4 inputs the addition / subtraction integrated value M (current) of the current calculation cycle output from the up / down counter 7, calculates M (current: average value) as shown in the flowchart of FIG. Based on the value, the count rate is obtained by equation (6). The counting weights of the addition input and the subtraction input of the up / down counter 7 are the same as those in the first embodiment, and the description thereof is omitted.
m (current) = exp {γ 1 × 2α × M (current: average value)} (6)

次に上記のように構成された実施の形態2の放射線モニタの演算器の演算処理手順について図4に基づいて説明する。まず、α、高警報設定値、低警報設定値、m(前回)、M(前回)、M(前回:平均値)、M(今回)をメモリ5から入力する(図4のステップS21)。次に、M(今回)≠M(前回)か否かの判定を行う(図4のステップS22)。次に、異なる場合(YES)ならば、M(今回:平均値)={M(前回)+M(今回)}/2を求める(図4のステップS23)。次に、M(今回:平均値)に基づき上記(6)式でm(今回)を求める(図4のステップS24)。一方、同一の場合(NO)ならば、m(前回)をm(今回)として出力する(図4のステップS25)。   Next, the calculation processing procedure of the calculator of the radiation monitor according to the second embodiment configured as described above will be described with reference to FIG. First, α, high alarm set value, low alarm set value, m (previous), M (previous), M (previous: average value), and M (current) are input from the memory 5 (step S21 in FIG. 4). Next, it is determined whether or not M (current) ≠ M (previous) (step S22 in FIG. 4). Next, if different (YES), M (current: average value) = {M (previous) + M (current)} / 2 is obtained (step S23 in FIG. 4). Next, m (current) is obtained by the above equation (6) based on M (current: average value) (step S24 in FIG. 4). On the other hand, if they are the same (NO), m (previous) is output as m (present) (step S25 in FIG. 4).

次に、以下、上記実施の形態1と同様の動作にて、m(今回)≧高警報設定値か否かの判定を行う(図4のステップS8)。次に、YESならば高警報を出力し(図4のステップS9)、例えば表示器6に高警報であることを表示し、今回演算周期を終了してステップS21に戻る。一方、ステップS8でNOならば、m(今回)≦低警報設定値か否かの判定を行う(図4のステップS10)。次に、YESならば低警報を出力し(図4のステップS11)、例えば表示器6に低警報であることを表示し、今回演算周期を終了してステップS21に戻る。一方、ステップS10でNOならば、今回演算周期を終了してステップS21に戻る。   Next, it is determined whether m (current) ≧ high alarm set value by the same operation as in the first embodiment (step S8 in FIG. 4). Next, if YES, a high alarm is output (step S9 in FIG. 4), for example, the display 6 indicates that the alarm is high, ends the current calculation cycle, and returns to step S21. On the other hand, if NO in step S8, it is determined whether m (current) ≦ low alarm set value (step S10 in FIG. 4). Next, if YES, a low alarm is output (step S11 in FIG. 4), for example, the display 6 indicates that the alarm is low, ends the current calculation cycle, and returns to step S21. On the other hand, if “NO” in the step S10, the current calculation cycle is ended and the process returns to the step S21.

例えば、演算周期を1秒とすると、10cpmの等間隔のパルス列では6秒毎に加減差積算値に1パルスが加算され、その6秒間に1パルスが減算され、1パルスの加減算のタイミングを含めた全てのタイミングで計数率は安定する。   For example, if the calculation cycle is 1 second, one pulse is added to the addition / subtraction integrated value every 6 seconds in a 10 cpm equidistant pulse train, and 1 pulse is subtracted every 6 seconds, including the timing of addition / subtraction of 1 pulse. The count rate is stable at all timings.

上記のように構成された実施の形態2の放射線モニタは、演算器が、前回演算周期から今回演算周期で加減差積算値が変化する場合に、その平均値に基づき計数率を求めるようにしたので、入力の繰り返し周波数が平衡状態にある場合には、全てのタイミングで計数率を安定させることができ、応答性を犠牲にしないで標準偏差に関係する機器誤差を低減して高精度で放射線を測定できる。   In the radiation monitor according to the second embodiment configured as described above, when the addition / subtraction integrated value changes from the previous calculation cycle to the current calculation cycle, the calculator calculates the count rate based on the average value. Therefore, when the input repetition frequency is in an equilibrium state, the count rate can be stabilized at all timings, and the instrument error related to the standard deviation can be reduced without sacrificing responsiveness, and radiation can be performed with high accuracy. Can be measured.

実施の形態3.
上記実施の形態2では、アップダウンカウンタ7で加減積算値Mを出力するようにしたが、本実施の形態3では、図5に示すように、アップダウンカウンタ7を仮数部73と指数部74との2つのエリアに分け、仮数部73の加減差積算値Cおよび指数部74の加減差積算値Eをそれぞれ出力する。そして、演算器4は、A=定数、B=定数としたときに図6に示すように指数関数に近似した計数率rを下記(7)式で求める。尚、Cの計数の重み付けは、上記実施の形態2と同様であるので説明を省略する。
r(今回)={A+C(今回:平均値)}/B×2E(今回)・・・(7)
Embodiment 3 FIG.
In the second embodiment, the up / down counter 7 outputs the addition / subtraction integrated value M. However, in the third embodiment, the up / down counter 7 includes the mantissa part 73 and the exponent part 74 as shown in FIG. And the addition / subtraction integration value C of the mantissa part 73 and the addition / subtraction integration value E of the exponent part 74 are respectively output. Then, the arithmetic unit 4 obtains a count rate r approximated to an exponential function by the following equation (7) as shown in FIG. 6 when A = constant and B = constant. Note that the weighting of the C count is the same as in the second embodiment, and a description thereof will be omitted.
r (current) = {A + C (current: average value)} / B × 2 E (current) (7)

次に上記のように構成された実施の形態3の放射線モニタの演算器の演算処理手順について図7に基づいて説明する。まず、α、高警報設定値、低警報設定値、r(前回)、C(前回)、C(前回:平均値)、C(今回)をメモリ5入力する(図7のステップS41)。次に、C(今回)≠C(前回)か否かの判定を行う(図7のステップS42)。
そして、異なる場合(YES)ならば、C(今回:平均値)={C(前回)+C(今回)}/2を求める(図7のステップS43)。次に、C(今回:平均値)に基づき上記(7)式でr(今回)を求める(図7のステップS44)。
Next, the calculation processing procedure of the calculator of the radiation monitor according to the third embodiment configured as described above will be described with reference to FIG. First, α, high alarm set value, low alarm set value, r (previous), C (previous), C (previous: average value), and C (current) are input to the memory 5 (step S41 in FIG. 7). Next, it is determined whether or not C (current) .noteq.C (previous) (step S42 in FIG. 7).
If they are different (YES), C (current: average value) = {C (previous) + C (current)} / 2 is obtained (step S43 in FIG. 7). Next, r (current) is obtained by the above equation (7) based on C (current: average value) (step S44 in FIG. 7).

一方、同一の場合(NO)ならば、r(前回)をr(今回)として出力する(図7のステップS45)。次に、以下、上記各実施の形態と同様の動作にて、r(今回)≧高警報設定値か否かの判定を行う(図7のステップS46)。そして、YESならば高警報を出力し(図7のステップS9)、例えば表示器6に高警報であることを表示し、今回演算周期を終了してステップS41に戻る。一方、ステップS8でNOならば、r(今回)≦低警報設定値か否かの判定を行う(図7のステップS48)。一方、ステップS8でNOならば、r(今回)≦低警報設定値かの判定を行う(図7のステップS48)。次に、YESならば低警報を出力し(図7のステップS11)、例えば表示器6に低警報であることを表示し、今回演算周期を終了してステップS41に戻る。一方、ステップS48でNOならば、今回演算周期を終了してステップS41に戻る。   On the other hand, if they are the same (NO), r (previous) is output as r (current) (step S45 in FIG. 7). Next, it is determined whether r (current) ≧ high alarm set value by the same operation as in the above embodiments (step S46 in FIG. 7). If YES, a high alarm is output (step S9 in FIG. 7), for example, the display 6 indicates that the alarm is high, ends the current computation cycle, and returns to step S41. On the other hand, if NO in step S8, it is determined whether r (current) ≦ low alarm set value (step S48 in FIG. 7). On the other hand, if NO in step S8, it is determined whether r (current) ≤ low alarm set value (step S48 in FIG. 7). Next, if YES, a low alarm is output (step S11 in FIG. 7), for example, the display 6 indicates that the alarm is low, ends the current calculation cycle, and returns to step S41. On the other hand, if “NO” in the step S48, the current calculation cycle is ended and the process returns to the step S41.

上記のように構成された実施の形態3の放射線モニタは、演算器が、前回演算周期から今回演算周期でアップダウンカウンタの仮数部の加減積算値が変化する場合に、その平均値に基づき計数率を求めるようにしたので、入力の繰り返し周波数が平衡状態にある場合には、全てのタイミングで計数率を安定させることができ、応答性を犠牲にしないで標準偏差に関係する機器誤差を低減して高精度で放射線を測定できる。   In the radiation monitor according to the third embodiment configured as described above, the computing unit counts based on the average value when the addition / subtraction integrated value of the mantissa part of the up / down counter changes from the previous computation cycle to the current computation cycle. Since the rate is calculated, when the input repetition frequency is in a balanced state, the count rate can be stabilized at all timings, and the instrument error related to the standard deviation is reduced without sacrificing responsiveness. Radiation can be measured with high accuracy.

実施の形態4.
上記実施の形態2では、パルス発生器9についてクロック91の出力に分周器92を接続し、分周器92の出力にレートマルチプライヤ93を接続し、レートマルチプライヤ93のフィードバッグパルスをアップダウンカウンタ7の減算入力端子72に入力するようにしたが、本実施の形態4では、図8に示すように、パルス発生器90は、クロック91の出力にレートマルチプライヤ930を接続し、レートマルチプライヤ930の出力に分周器920を接続し、分周器920のフィードバッグパルスをアップダウンカウンタ7の減算入力端子72に入力する。
Embodiment 4 FIG.
In the second embodiment, the divider 92 is connected to the output of the clock 91 in the pulse generator 9, the rate multiplier 93 is connected to the output of the divider 92, and the feedback pulse of the rate multiplier 93 is increased. In the fourth embodiment, as shown in FIG. 8, the pulse generator 90 connects the rate multiplier 930 to the output of the clock 91, and the rate is input to the subtraction input terminal 72 of the down counter 7. A frequency divider 920 is connected to the output of the multiplier 930, and a feedback pulse of the frequency divider 920 is input to the subtraction input terminal 72 of the up / down counter 7.

このように制御したので、図9に示すように、ある一定時間において定められた数の出力パルスを、まずレートマルチプライヤ930がランダムに抜き出す。次に、この抜き出したパルスを分周器920に適用してフィードバッグパルスを得る。このフィードバッグパルスはクロック信号数周期分の誤差はあるものの、繰り返し周波数が高い場合には演算周期中のパルス数に対して無視できる程度の割合であり、繰り返し周波数が低い場合にはパルス間隔を一定に整えることができる。尚、パルス発生器90以外の動作は、上記実施の形態2と同様に行うことができる。   Since control is performed in this way, as shown in FIG. 9, the rate multiplier 930 first extracts a predetermined number of output pulses in a certain period of time at random. Next, this extracted pulse is applied to a frequency divider 920 to obtain a feedback pulse. This feedback pulse has an error equivalent to the number of cycles of the clock signal, but when the repetition frequency is high, it is a negligible ratio with respect to the number of pulses in the calculation cycle, and when the repetition frequency is low, the pulse interval is It can be fixed. The operations other than the pulse generator 90 can be performed in the same manner as in the second embodiment.

上記のように構成された実施の形態4の放射線モニタによれば、上記実施の形態2と同様の効果を奏するのはもちろんのこと、低計数率領域で精度が要求される、例えば、PWRプラントの高感度型主蒸気管モニタのバックグラウンド4〜10cpmにおいて、減算入力のフィードバッグパルスの間隔を等しくできるために、入力の繰り返し周波数が平衡状態にある場合には、アップダウンカウンタの加算入力と減算入力との交互性が保たれるため、全てのタイミングで計数率を安定させることができ、応答性を犠牲にしないで標準偏差に関係する機器誤差を低減して高精度で放射線を測定できる。   According to the radiation monitor of the fourth embodiment configured as described above, the same effects as those of the second embodiment can be obtained, but accuracy is required in the low count rate region. For example, a PWR plant In the background of 4 to 10 cpm of the high-sensitivity main steam pipe monitor, the interval between the feedback pulses of the subtraction input can be made equal, so that when the input repetition frequency is in a balanced state, the addition input of the up / down counter is Since the alternation with the subtraction input is maintained, the count rate can be stabilized at all timings, and the instrument error related to the standard deviation can be reduced without sacrificing responsiveness, and radiation can be measured with high accuracy. .

尚、本発明は、その発明の範囲内において、各実施の形態において適宜、変形、省略することが可能である。   It should be noted that the present invention can be appropriately modified and omitted in each embodiment within the scope of the present invention.

1 放射線検出器、2 波高弁別器、3 カウンタ、4 演算器、5 メモリ、
6 表示器、7 アップダウンカウンタ、8 積算制御回路、9 パルス発生器、
71 加算入力端子、72 減算入力端子、73 仮数部、74 指数部、
91 クロック、92,920 分周器、93,930 レートマルチプライヤ。
1 radiation detector, 2 wave height discriminator, 3 counter, 4 arithmetic unit, 5 memory,
6 display, 7 up / down counter, 8 integration control circuit, 9 pulse generator,
71 Addition input terminal, 72 Subtraction input terminal, 73 Mantissa part, 74 Exponential part,
91 clock, 92,920 divider, 93,930 rate multiplier.

Claims (8)

放射線を検出するとアナログ信号パルスを出力する放射線検出手段と、
上記アナログ信号パルスを入力して許容範囲内にあるとデジタルパルスとして出力する波高弁別手段と、
上記デジタルパルスを入力して定周期で計数して計数値を出力する計数手段と、
上記定周期の計数率を演算し、当該計数率を工学値に変換し、当該工学値について警報判定を行う演算手段とを有し、
上記演算手段は、上記計数率を、
今回演算周期の計数値から前回演算周期の計数率に演算周期時間を乗じた値を減算して求めた加減差を、上記前回演算周期の加減差積算値に加算して今回演算周期の加減差積算値とし、当該今回演算周期の加減差積算値の小数点以下を切り捨てた加減差積算自然数を求め、上記今回演算周期の加減差積算自然数と上記前回演算周期の加減差積算自然数とを比較し、
異なる場合には、上記今回演算周期の加減差積算自然数および上記前回演算周期の加減差積算自然数の平均値を求め、当該平均値に標準偏差に基づく重み付け係数を乗じて標準偏差が一定になるように演算して計数率とするか、
同一の場合には、上記前回演算周期の計数率を上記今回演算周期の計数率とすることを特徴とする放射線モニタ。
Radiation detecting means for outputting an analog signal pulse when detecting radiation;
A pulse height discriminating means for inputting the analog signal pulse and outputting it as a digital pulse within an allowable range;
Counting means for inputting the digital pulse, counting at a fixed period, and outputting a count value;
Calculating the count rate of the fixed period, converting the count rate into an engineering value, and having an arithmetic means for performing a warning determination on the engineering value,
The calculation means calculates the count rate as follows:
Addition / subtraction obtained by subtracting the value calculated by multiplying the count rate of the previous calculation cycle by the calculation cycle time from the count value of the previous calculation cycle is added to the accumulated value of the previous calculation cycle to add or subtract the current calculation cycle. As an integrated value, an addition / subtraction integration natural number obtained by rounding down the decimals of the addition / subtraction integration value of the current calculation cycle is calculated, and the addition / subtraction integration natural number of the current calculation cycle is compared with the addition / subtraction integration natural number of the previous calculation cycle,
If they are different, the average value of the addition / subtraction integration natural number of the current calculation cycle and the addition / subtraction integration natural number of the previous calculation cycle are obtained, and the standard deviation is made constant by multiplying the average value by a weighting factor based on the standard deviation. To calculate the counting rate,
In the case of being the same, the radiation monitor characterized in that the count rate of the previous computation cycle is set to the count rate of the current computation cycle.
放射線を検出してアナログ信号パルスを出力する放射線検出手段と、
上記アナログ信号パルスを入力して許容範囲内にあるとデジタルパルスとして出力する波高弁別手段と、
上記デジタルパルスを加算入力し、パルス発生手段から出力されたフィードバッグパルスを減算入力し、その結果を加減差積算値として出力する加減差積算手段と、
上記加減差積算手段に入力される上記デジタルパルスおよび上記フィードバッグパルスを標準偏差に基づいて重み付けして積算する積算制御手段と、
上記デジタルパルスの繰り返し周波数に対して時定数の一次遅れで応答する繰り返し周波数を上記フィードバックパルスとして上記加減差積算手段に出力するパルス発生手段と、
定周期で計数率を演算し、当該計数率を工学値に変換し、当該工学値について警報判定を行う演算手段とを備え、
上記演算手段は、上記計数率を、
前回演算周期の加減差積算値と今回演算周期の加減差積算値とを比較し、
異なる場合には、上記前回演算周期の加減差積算値および上記今回演算周期の加減差積算値の平均値を求め、当該平均値を標準偏差が一定になるように演算して上記計数率とするか、
同一の場合には、上記前回演算周期の計数率を上記今回演算周期の計数率とすることを特徴とする放射線モニタ。
Radiation detecting means for detecting radiation and outputting analog signal pulses;
A pulse height discriminating means for inputting the analog signal pulse and outputting it as a digital pulse within an allowable range;
Addition input of the digital pulse, subtraction input of the feedback pulse output from the pulse generation means, addition / subtraction integration means for outputting the result as an addition / subtraction integration value,
Integration control means for weighting and integrating the digital pulse and feedback pulse input to the addition / subtraction integration means based on a standard deviation;
Pulse generating means for outputting a repetition frequency that responds with a first order delay of a time constant to the repetition frequency of the digital pulse as the feedback pulse to the addition / subtraction integration means;
A calculation rate is calculated at a fixed period, the count rate is converted into an engineering value, and an arithmetic means for performing alarm determination on the engineering value is provided.
The calculation means calculates the count rate as follows:
Compare the accumulated value of the previous calculation cycle with the accumulated value of the current calculation cycle,
If they are different, the average value of the addition / subtraction integration value of the previous calculation cycle and the addition / subtraction integration value of the current calculation cycle is obtained, and the average value is calculated so that the standard deviation is constant to obtain the count rate. Or
In the case of being the same, the radiation monitor characterized in that the count rate of the previous computation cycle is set to the count rate of the current computation cycle.
上記加減差積算手段は、アップダウンカウンタにて構成されたことを特徴とする請求項2記載の放射線モニタ。 3. The radiation monitor according to claim 2, wherein the addition / subtraction integration means is constituted by an up / down counter. 上記アップダウンカウンタは、仮数部と指数部とにて構成されたことを特徴とする請求項3記載の放射線モニタ。 4. The radiation monitor according to claim 3, wherein the up / down counter comprises a mantissa part and an exponent part. 上記パルス発生手段は、クロックの出力にレートマルチプライヤを接続し、
上記レートマルチプライヤの出力に分周器を接続して構成され、
上記分周器から出力されるパルスを上記フィードバッグパルスとすることを特徴とする請求項2ないし請求項4のいずれか1項に記載の放射線モニタ。
The pulse generating means connects a rate multiplier to the output of the clock,
A divider is connected to the output of the rate multiplier,
The radiation monitor according to any one of claims 2 to 4, wherein the pulse output from the frequency divider is the feedback pulse.
上記波高弁別手段は、入力した上記アナログ信号パルスの波高レベルが許容範囲内を逸脱するとノイズとして除去する請求項1ないし請求項5のいずれか1項に記載の放射線モニタ。 The radiation monitor according to any one of claims 1 to 5, wherein the wave height discriminating means removes the wave height level of the input analog signal pulse as noise when the wave height level deviates from an allowable range. 上記演算手段は、上記工学値および警報判定結果を出力し、
上記演算手段からの出力を表示する表示手段を備えたことを特徴とする請求項1ないし請求項6のいずれか1項に記載の放射線モニタ。
The arithmetic means outputs the engineering value and the alarm determination result,
The radiation monitor according to any one of claims 1 to 6, further comprising display means for displaying an output from the arithmetic means.
上記演算手段の演算手順、および、演算に必要な設定値及びデータを格納する記憶手段を備えたことを特徴とする請求項1ないし請求項7のいずれか1項に記載の放射線モニタ。 The radiation monitor according to any one of claims 1 to 7, further comprising a storage means for storing a calculation procedure of the calculation means and set values and data necessary for the calculation.
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