WO2016031045A1 - 炉外核計装装置 - Google Patents
炉外核計装装置 Download PDFInfo
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- WO2016031045A1 WO2016031045A1 PCT/JP2014/072723 JP2014072723W WO2016031045A1 WO 2016031045 A1 WO2016031045 A1 WO 2016031045A1 JP 2014072723 W JP2014072723 W JP 2014072723W WO 2016031045 A1 WO2016031045 A1 WO 2016031045A1
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/16—Measuring radiation intensity
- G01T1/17—Circuit arrangements not adapted to a particular type of detector
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- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21C—NUCLEAR REACTORS
- G21C17/00—Monitoring; Testing ; Maintaining
- G21C17/10—Structural combination of fuel element, control rod, reactor core, or moderator structure with sensitive instruments, e.g. for measuring radioactivity, strain
- G21C17/108—Measuring reactor flux
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N23/00—Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00
- G01N23/005—Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by using neutrons
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T3/00—Measuring neutron radiation
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- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21C—NUCLEAR REACTORS
- G21C17/00—Monitoring; Testing ; Maintaining
- G21C17/10—Structural combination of fuel element, control rod, reactor core, or moderator structure with sensitive instruments, e.g. for measuring radioactivity, strain
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2223/00—Investigating materials by wave or particle radiation
- G01N2223/30—Accessories, mechanical or electrical features
- G01N2223/304—Accessories, mechanical or electrical features electric circuits, signal processing
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- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03G—CONTROL OF AMPLIFICATION
- H03G1/00—Details of arrangements for controlling amplification
- H03G1/0005—Circuits characterised by the type of controlling devices operated by a controlling current or voltage signal
- H03G1/0088—Circuits characterised by the type of controlling devices operated by a controlling current or voltage signal using discontinuously variable devices, e.g. switch-operated
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E30/00—Energy generation of nuclear origin
- Y02E30/30—Nuclear fission reactors
Definitions
- the present invention relates to an out-of-core nuclear instrumentation device that monitors a neutron flux outside a reactor vessel, and in particular, a detector signal processing circuit (I / I) installed in an out-of-core nuclear instrumentation board constituting the out-of-core nuclear instrumentation device This is related to labor saving in the calibration work of the neutron detector by improving the E amplifier.
- An out-of-core nuclear instrumentation device continuously monitors the neutron flux outside the reactor vessel of a pressurized water reactor (PWR) to monitor the state of the reactor during start-up and operation, and the neutron flux When an abnormality is detected in this state, the reactor is protected by outputting an alarm signal or an emergency stop signal of the reactor.
- the reactor core instrumentation apparatus mainly comprises a neutron detector that measures a neutron flux and converts it into a current value, and an reactor core instrumentation panel that performs an arithmetic process on the converted current value and converts it into the signal. .
- the neutron measurement range of the nuclear reactor instrumentation device is divided into a neutron source region, an intermediate region, and an output region (operation region) according to the level of neutron flux from the reactor shutdown state to power operation.
- the structures and functions of the neutron detector and the outer nuclear instrumentation board differ from region to region, and a detector signal processing circuit (I / E amplifier, that is, a current / voltage amplifier) is used for the calculation processing in the output region.
- the applicant uses the detector signal processing circuit to convert a current value converted by the neutron detector into a voltage value corresponding to the current value and a voltage value converted by the current / voltage conversion unit. And a variable gain amplifying unit for amplifying, and by configuring the variable gain amplifying unit from a current level corresponding resistor circuit capable of gain selection and a D / A converter for adjusting the gain, the neutron detection current is obtained.
- An out-of-core nuclear instrumentation device that can output a voltage level corresponding to the reactor power level and obtain an accurate measurement value of the neutron flux has been already proposed (see Patent Document 1).
- the detector current is converted into a voltage by the current / voltage converter 21 and input to the variable gain amplifier 22.
- the gains of the current / voltage converter 21 and the fixed gain converter 23 to be described later are constant.
- the detector current is measured by the detector current indicator output unit 24, and the output signal V 1 is input to the inverting amplifier 51 of the variable gain amplifying unit 22.
- the D / A converter 53 is adjusted by the adjustment control means 25 in advance to calibrate the output to a voltage value corresponding to the furnace output, whereby the output V3 of the detector signal processing circuit 8 is adjusted. Is determined. Then, the output signal V2 of the variable gain amplifying unit 22 is amplified by the inverting amplifier 71 of the fixed gain amplifying unit 23, and the output signal V3 is input to a signal processing card described later.
- the output V3 is a voltage value corresponding to the furnace output, and a certain level corresponding to the furnace output is required for the arithmetic processing after the signal processing card. Therefore, the detector current is the current / voltage converter 21. And the voltage value is amplified by a variable gain amplifier.
- the proposed conventional neutron detector calibration apparatus uses the selective adjustment control means for adjusting the gain of the D / A converter based on the current value indicated by the detector current indicator output unit, so that the output voltage is adjusted.
- Manual adjustment was sequentially performed to achieve the target value. For this reason, it is necessary for the operator to adjust the output voltage to the target value by the increase / decrease buttons on the operation unit while confirming the current value indicated by the detector current indicator output unit.
- Instruments such as indicators and indicators had to be constantly monitored, requiring manpower and time.
- this adjustment may be performed during the operation of the reactor, the burden on the operator is increased even at night, and there is a possibility that the input current may be adjusted incorrectly depending on the operator.
- the present invention has been made to solve the above-described problems, eliminates the need for manual adjustment by an operator so that the output voltage always becomes a target value by an operator, and eliminates the need for neutron detector signal input.
- An object of the present invention is to provide an out-of-core nuclear instrumentation apparatus that promotes labor saving and high accuracy of calibration work by automating the calibration work of neutron flux level signal output.
- An out-of-core nuclear instrumentation apparatus uses a neutron detector that measures a neutron flux outside a reactor vessel and converts it into a current value, and a current value from the neutron detector using a detector signal processing circuit.
- the detector signal processing circuit is a current value converted by the neutron detector
- a gain / voltage conversion unit that converts the current value into a voltage value corresponding to the current value and an operational amplifier with a D / A converter, and a variable gain amplification that amplifies the voltage value converted by the current / voltage conversion unit
- an adjustment control means for adjusting the gain of the D / A converter, and an output voltage amplified by the variable gain amplification section is automatically compared based on a preset reference value and output to the adjustment control means. With a comparator is there.
- the nuclear reactor instrumentation apparatus of the present invention it is possible to reduce the burden on the worker especially during night work, prevent human error, and output a neutron flux level signal for a highly reliable neutron detector signal input. It is possible to save labor in the calibration work.
- FIG. 5 is a circuit configuration diagram showing a detector signal processing circuit in a second embodiment.
- FIG. 6 is a circuit configuration diagram showing a detector signal processing circuit in a third embodiment.
- FIG. 4 is a circuit diagram showing a specific configuration example of a comparator in the first to third embodiments. It is a basic circuit block diagram which shows the conventional detector signal processing circuit.
- FIG. 1 is a configuration diagram showing a general configuration of an out-of-core nuclear instrumentation device in an output region.
- the neutron detector 3 of the out-of-core nuclear instrumentation device 14 is provided around the outside of the reactor vessel 16 installed in the reactor containment vessel 15.
- the neutron detector 3 detects the neutron leaking from the upper part of the reactor vessel 16 and converts it into a current value
- the lower detector detects the neutron leaking from the lower part of the reactor vessel 16 and converts it into a current value.
- the detector 5 is integrated.
- the current value converted by the upper detector 4 is detected in the reactor core instrument board 1 of the reactor core instrument 14 installed outside the reactor containment vessel 15 via the upper detector cable 6. Is input to the signal processing circuit 8.
- the current value converted by the lower detector 5 is also input to the detector signal processing circuit 8 via the lower detector cable 7.
- the detector signal processing circuit 8 includes a circuit corresponding to the upper detector 4 and a circuit corresponding to the lower detector 5, and the detector signal processing circuit 8 converts the current value into the output voltage 9 for the upper detector and the lower detection. It is converted into a dexterous output voltage 10. Both output voltages 9 and 10 are input to the signal processing card 11 in the out-of-core nuclear instrument panel 1.
- the signal processing card 11 performs A / D (analog / digital) conversion and engineering value conversion, and outputs various signals to the operation panel 12 and the input / output card 13 in the reactor protection system 2.
- FIG. 2 is a basic circuit configuration diagram showing the detector signal processing circuit 8 of the neutron detector 3.
- the detector signal processing circuit 8 includes a current / voltage conversion unit 21 that converts the current value Iu obtained by converting the neutron flux detected by the upper detector 3 or the lower detector 4 into a voltage value V1, and the voltage value V1
- a variable gain amplifying unit 22 that amplifies the voltage value V2 as a first step, a fixed gain amplifying unit 23 that amplifies the voltage value V2 once amplified as a second step and outputs it as an output voltage V3 from the detector signal processing circuit 8; Obtained from the detector current indicator output unit 24 for displaying the voltage value V1 converted by the current / voltage conversion unit 21, the adjustment control means 25 for adjusting the amplification width of the variable gain amplification unit 22, and the variable gain amplification unit 22.
- the fixed gain amplifying unit 23 is disposed at the subsequent stage of the variable gain amplifying section 22, but the variable gain amplifying section 22 may be disposed at the subsequent stage of the fixed gain amplifying section 23.
- the current Iu measured by the neutron detector is input to the inverting amplifier 31 using the operational amplifier in the current / voltage conversion unit 21, and the voltage value V 1 corresponding to the current Iu. Is output.
- the input impedance of the operational amplifier is very high, and all current flows to the resistor 32 without flowing into the inverting amplifier 31.
- the output voltage of the inverting amplifier 31 is ⁇ (resistance value 32 ⁇ detector current).
- the output voltage can be set to 0 to 2 V by adjusting the gain with the variable gain amplifier 22.
- the fixed gain amplifying unit 23 constitutes a non-inverting amplifier, the gain is (1 + R73 / 75), and the output is about 5 times 0 to 10V.
- the gains of the current / voltage converter 21 and the fixed gain amplifier 23 described later are constant.
- a detector current indicator output unit 24 Connected to the output side of the current / voltage conversion unit 21 is a detector current indicator output unit 24 for displaying the detector current by the voltage value V1.
- the voltage value V1 is calculated by the variable gain amplification unit 22. It is input to an inverting amplifier 51 which is an amplifier.
- the D / A converter 53 is adjusted by an adjustment control means 25 for calibrating the output voltage V3 to a voltage value corresponding to the furnace output in advance and a comparator 29 connected to this input stage.
- the output voltage V3 of the detector signal processing circuit 8 is determined. That is, the amplification width of the variable gain amplification unit 22 is adjusted by the comparator 29 connected to the adjustment control means 25. This adjustment is performed after the neutron detector 3 (FIG. 1) is installed, and arises from the reactor power, the amount of neutron leakage from the reactor vessel 16, the error of the installed detector, and its installation location. Absorbs detection accuracy.
- the D / A converter 53 is an electronic circuit (for example, a 12-bit circuit) that converts the digital electric signal from the adjustment control means 25 into an analog electric signal (resistance value), and converts the resistance value to a fine resistance value of about 1/10000. obtain.
- the output voltage value V2 of the variable gain amplifier 22 is amplified by a non-inverting amplifier 71 that is an operational amplifier of the fixed gain amplifier 23, and the output voltage V3 of the output signal is input to the signal processing card 11 (FIG. 1).
- the output voltage V3 of the output signal is a voltage value corresponding to the furnace output (for example, a voltage value 3.3V corresponding to the furnace output 100%), and the arithmetic processing after the signal processing card 11 corresponds to the furnace output. Since a voltage value of a certain level is required, the detector current Iu is converted into a voltage value and amplified by the detector signal processing circuit 8.
- Reference numeral 54 is a fixed resistor, and 52 and 72 to 75 are resistors.
- FIG. 3 is a circuit configuration diagram showing the detector signal processing circuit (I / E amplifier) according to Embodiment 1 of the present invention. Differences from the detector signal processing circuit of FIG. 1 will be mainly described. In each figure, the same numerals indicate the same or corresponding parts.
- the fixed resistor 54 (FIG. 2) of the variable gain amplifying unit 22 is configured by a current level corresponding resistor circuit 61 capable of selecting a gain.
- the current level corresponding resistor circuit 61 is configured by a parallel body in which a plurality of series bodies each having a resistor and an analog switch connected in series are connected in parallel. 62 to 64 are resistors, and 65 to 67 are analog switches. As a result, the analog switch can be selectively closed to provide a high resistance circuit for low current levels.
- the current level corresponding resistor circuit 61 can also be configured by a variable resistor.
- the gain of the inverting amplifier 51 can be selected by selecting the resistance of the current level corresponding resistor circuit 61.
- the comparator 29 for comparing the voltage value obtained from the variable gain amplifying unit 22 with a preset value as a reference and the selection adjustment control means 26 are controlled so as to select a desired resistance by turning on / off the analog switch. Thereby, the width of the gain of the variable gain amplifying unit 22 can be widened compared to the fixed resistance value. When the current Iu measured by the neutron detector 3 is small, a large resistance value is selected.
- the gain of the variable gain amplifying unit 22 can be varied by adjusting the resistance value of the D / A converter 53 by a digital electric signal in accordance with an instruction from the comparator 29 connected to the selection adjustment control means 26.
- the current level corresponding resistor circuit 61 When the resistance value is adjusted only by the D / A converter 53 with a fixed resistance, if the lower limit of the current input range falls to, for example, 1 ⁇ A, the gain setting count value (digital electric signal) in the D / A converter 53 The voltage change width becomes larger and the accuracy deteriorates. Therefore, in FIG.
- the current level corresponding resistor circuit 61 selects a large gain, By finely adjusting the gain with the D / A converter 53, a highly accurate gain can be automatically adjusted.
- the selection of the current level corresponding resistor circuit 61 by the selection adjustment control means 26 of the variable gain amplifier 22 of the first embodiment, the adjustment of the D / A converter 53, and the function of the comparator 29 will be described.
- the neutron detector current Iu corresponding to the reactor output 100% level is input to the current / voltage converter 21, it is converted into a voltage value V1 by the inverting amplifier 31 and output.
- the detector current is displayed on the detector current indicator output unit 24 and the voltage value V1 is input to the inverting amplifier 51 of the variable gain amplifying unit 22.
- the comparator 29 compares the upper limit voltage reference value and the lower limit voltage reference value in the comparator 29 set in advance, and adjusts to a voltage level range of a certain level required for the arithmetic processing after the signal processing card 11.
- the resistance value of the D / A converter is automatically adjusted via the control means 26.
- FIG. 6 is a specific circuit example composed of a combination of two-stage comparators X and Y.
- the target value is 7.143V
- the inverting input ( ⁇ ) of the converter X is set to the lower reference value 7.142V.
- Aiming for the target value (7.143V) by presetting the upper reference value of 7.144V to the inverting input (-) of the converter Y and inputting V3 to the non-inverting input (+) of both converters. Automatically adjusts to be within the span of the upper and lower limits.
- the automatic adjustment count value is sent to the D / A converter 53 by depressing an automatic button of the selection and adjustment control unit provided on the panel surface of the operation device, and the gain can be automatically adjusted. Therefore, the detector current instruction output unit 24 merely displays the detector current, and the operator does not need to check the detector current instruction output unit 24 one by one as in the prior art.
- the resistors 62 of the current level corresponding resistor circuit 61 are turned on and off by the analog switches 65 to 67.
- the resistance value is switched by selecting ⁇ 64, and further, the resistance value of the D / A converter 53 is adjusted to change the gain of the variable gain amplifying unit 22, and the output voltage V3 of the detector signal processing circuit 8 is changed. It can be adjusted to the required voltage level.
- the resistance value including the resistance value of the D / A converter 53, the resistance value selected by the current level corresponding resistance circuit 61, and the on-resistance value of the analog switch is finely adjusted. Can be adjusted. For this reason, the gain width of the variable gain amplifying unit 22 can be automatically and accurately changed by the comparator connected to the selective adjustment control compared to the conventional case, and as a result, the width of the neutron detector current that can be measured is increased. Can be enlarged.
- FIG. FIG. 4 is a circuit configuration diagram showing the detector signal processing circuit (I / E amplifier) 8 in the second embodiment.
- the variable level amplifying unit 22 is added and the current level corresponding resistor circuit 61 composed of the resistor and the analog switch is added to perform the switching control has been described.
- the second embodiment as shown in FIG. 1 is added to the current / voltage converter 21 with a current level corresponding resistor circuit 41 including a resistor and an analog switch.
- Reference numerals 42 to 44 are resistors, and 45 to 47 are analog switches. Then, the resistance value in the current level corresponding resistance circuit 41 is automatically switched by the comparator 29 connected to the selection adjustment control means 27.
- the analog switches 45 to 47 are turned on / off by the comparator 29 connected to the selection adjustment control means 27.
- the width of the gain of the detector signal processing circuit can be automatically and accurately changed with a selective adjustment control additionally provided with a comparator as compared with the conventional method. Can be enlarged.
- FIG. 5 is a circuit configuration diagram showing the detector signal processing circuit (I / E amplifier) 8 according to the third embodiment.
- the D / A converter of the variable gain amplifier 22 has a two-stage configuration compared to FIG. Thus, two D / A converters 55 (DAC1) and 56 (DAC2) are connected in series.
- One D / A converter 55 corresponds to the current level corresponding resistance circuit 61 of the first embodiment, and the selection adjustment control means 28 selects a large resistance value based on the comparator 29, and the other D / A converter 56.
- the resistance value is finely adjusted by the selection adjustment control means 28 based on the comparator 29.
- the gain selection / adjustment is performed by taking the output voltage V3 of the fixed gain amplifier into the comparator.
- the present invention is not limited to this, and the output voltage V2 of the variable gain amplifier is directly used as the comparator. It goes without saying that the count value may be commanded and controlled by the selection adjustment control means.
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Abstract
Description
図1は、出力領域における炉外核計装装置の一般的な構成を示す構成図である。図1において、原子炉格納容器15内に設置される原子炉容器16の外部の周辺に炉外核計装装置14の中性子検出器3が設けられる。中性子検出器3は、原子炉容器16の上部から漏洩する中性子を検出し電流値に変換する上部検出器4と、この原子炉容器16の下部から漏洩する中性子を検出し電流値に変換する下部検出器5を一体にしたものである。上部検出器4で変換された電流値は上部検出器ケーブル6を経由して、通常原子炉格納容器15の外部に設置される炉外核計装装置14の炉外核計装盤1内にある検出器信号処理回路8に入力される。下部検出器5で変換された電流値も同様に、下部検出器ケーブル7を経由して検出器信号処理回路8に入力される。
図2では上記電流/電圧変換部21及び後述する固定ゲイン増幅部23のゲインは一定である。上記電流/電圧変換部21の出力側には電圧値V1により検出器電流を表示する検出器電流指示計出力部24を接続されており、また、前記電圧値V1は可変ゲイン増幅部22の演算増幅器である反転増幅器51に入力される。
電流レベル対応用抵抗回路61は、抵抗とアナログスイッチを直列に接続した直列体を複数個並列に接続した並列体で構成されている。62~64は抵抗、65~67はアナログスイッチである。それにより、アナログスイッチを選択的に閉じて、低電流レベル対応用の高抵抗回路にすることができる。なお、電流レベル対応用抵抗回路61は可変抵抗器でも構成できる。
従って、検出器電流指示出力部24は検出器電流を単に表示するのみであり、作業者は従来のように、逐一、検出器電流指示出力部24を確認する必要がない。
図4は、実施の形態2における検出器信号処理回路(I/Eアンプ)8を示す回路構成図である。実施の形態1では、可変ゲイン増幅部22に抵抗とアナログスイッチからなる電流レベル対応用抵抗回路61を追加して切り替え制御をする場合について述べたが、実施の形態2では図4に示すように、図1の基本的回路構成に対して、電流/電圧変換部21に抵抗とアナログスイッチからなる電流レベル対応用抵抗回路41を追加する。なお、42~44は抵抗、45~47はアナログスイッチである。そして電流レベル対応用抵抗回路41における抵抗値を、選択調整制御手段27に接続したコンパレータ29により自動的に切り替える。
図5は実施の形態3における検出器信号処理回路(I/Eアンプ)8を示す回路構成図であり、図1に対して、可変ゲイン増幅部22のD/Aコンバータが二段構成となるように、D/Aコンバータ55(DAC1)、56(DAC2)を2つ直列に接続したものである。
14 炉外核計装装置、16 原子炉容器、21 電流/電圧変換部、
22 可変ゲイン増幅部、23 固定ゲイン増幅部、
24 検出器電流指示計出力部、25 調整制御手段、
26、27、28 選択調整制御手段、29 コンパレータ、
41 電流レベル対応用抵抗回路、42~44 抵抗、
45~47 アナログスイッチ、53、55、56 D/Aコンバータ、
61 電流レベル対応用抵抗回路、62~64 抵抗、
65~67 アナログスイッチ。
Claims (6)
- 原子炉容器の外の中性子束を計測して電流値に変換する中性子検出器と、前記中性子検出器からの電流値を検出器信号処理回路を用いて演算処理して原子炉の運転時の中性子束の状態を出力する炉外核計装盤とを備える炉外核計装装置において、前記検出器信号処理回路は、前記中性子検出器で変換された電流値を、その電流値に応じた電圧値に変換する電流/電圧変換部と、D/Aコンバータを付設した演算増幅器を有し前記電流/電圧変換部で変換された電圧値を増幅する可変ゲイン増幅部と、前記D/Aコンバータのゲインを調整する調整制御手段と、前記可変ゲイン増幅部で増幅された出力電圧を予め設定された基準値を基に比較して前記調整制御手段に出力するコンパレータとを備えたことを特徴とする炉外核計装装置。
- 前記検出器信号処理回路は、
前記中性子検出器で変換された電流値を、その電流値に応じた電圧値に変換する電流/電圧変換部と、
前記電流/電圧変換部で変換された電圧値から前記中性子検出器で変換された電流値を指示する検出器電流指示計出力部と、
ゲインを選択できる電流レベル対応用抵抗回路及び、ゲインを調整するD/Aコンバータを持つ演算増幅器を有し、前記電流/電圧変換部で変換された電圧値を増幅する可変ゲイン増幅部と、
前記電流レベル対応用抵抗回路のゲインを選択し、前記D/Aコンバータのゲインを調整する選択調整制御手段に接続し、可変ゲイン増幅部から得られる電圧値をあらかじめ設定された値を基準に自動比較するコンパレータと、
を備えることを特徴とする請求項1記載の炉外核計装装置。 - 前記検出器信号処理回路は、
ゲインを選択できる電流レベル対応用抵抗回路を持つ演算増幅器を有し、前記中性子検出器で変換された電流値を、その電流値に応じた電圧値に増幅して変換する電流/電圧変換部と、
前記電流/電圧変換部で増幅して変換された電圧値より前記中性子検出器で変換された電流値を指示する検出器電流指示計出力部と、
ゲインを調整するD/Aコンバータを持つ演算増幅器を有し、前記電流/電圧変換部で増幅して演算された電圧値を増幅する可変ゲイン増幅部と、
前記電流レベル対応用抵抗回路のゲインを選択し、前記D/Aコンバータのゲインを調整する選択調整制御手段に接続し、可変ゲイン増幅部から得られる電圧値をあらかじめ設定された基準値を基に自動比較するためのコンパレータと、
を備えることを特徴とする請求項1記載の炉外核計装装置。 - 前記電流レベル対応用抵抗回路は、抵抗とアナログスイッチの直列体の複数個で構成されることを特徴とする請求項2あるいは請求項3に記載の炉外核計装装置。
- 前記検出器信号処理回路は、
前記中性子検出器で変換された電流値を、その電流値に応じた電圧値に変換する電流/電圧変換部と、
前記電流/電圧変換部で変換された電圧値より前記中性子検出器で変換された電流値を指示する検出器電流指示計出力部と、
直列接続された2つのD/Aコンバータを持ち、一方のD/Aコンバータで前記中性子検出器で変換された電流値レベルに対応してゲインを選択し、他方のD/Aコンバータでゲインを調整する演算増幅器を有し、前記電流/電圧変換部で変換された電圧値を増幅する可変ゲイン増幅部と、
前記2つのD/Aコンバータのゲインを選択、調整する選択調整制御手段に接続し、可変ゲイン増幅部から得られる電圧値をあらかじめ設定された値を基準に自動比較するためのコンパレータと、
を備えることを特徴とする請求項1記載の炉外核計装装置。 - 前記コンパレータは、上限基準値と下限基準値を予め所定の値に設定しておくことで、所定の目標値を目指して上記上下限基準値内のスパンに入るように自動調整されるようにしたことを特徴とする請求項1から3および請求項5のいずれか1項に記載の炉外核計装装置。
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US15/306,614 US20170047132A1 (en) | 2014-08-29 | 2014-08-29 | Ex-core nuclear instrumentation device |
EP14900613.2A EP3188193A4 (en) | 2014-08-29 | 2014-08-29 | Excore nuclear instrumentation device |
JP2016545188A JPWO2016031045A1 (ja) | 2014-08-29 | 2014-08-29 | 炉外核計装装置 |
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US10441114B2 (en) | 2012-07-11 | 2019-10-15 | Kenrick Rampersad | Disposable finger tongs for handling a food product |
JP2020531820A (ja) * | 2017-08-18 | 2020-11-05 | ウエスチングハウス・エレクトリック・カンパニー・エルエルシー | 絶縁分離された核計装出力信号のスケーリング方法および当該方法を用いたシステム |
JP7378378B2 (ja) | 2020-10-13 | 2023-11-13 | 三菱電機株式会社 | 炉外核計装装置 |
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WO2017042876A1 (ja) * | 2015-09-08 | 2017-03-16 | 三菱電機株式会社 | 炉内核計装装置 |
CA2980051A1 (en) * | 2017-05-31 | 2018-11-30 | Atomic Energy Of Canada Limited / Energie Atomique Du Canada Limitee | System and method for stand-off monitoring of nuclear reactors using neutron detection |
CN109192343B (zh) * | 2018-07-11 | 2020-06-05 | 岭澳核电有限公司 | 减少压水反应堆堆外核测量系统的测量偏差方法及装置 |
CN109546983A (zh) * | 2018-11-20 | 2019-03-29 | 上海东软载波微电子有限公司 | 一种自动增益控制装置以及自动增益控制方法 |
CN113295924A (zh) * | 2021-05-25 | 2021-08-24 | 中国核动力研究设计院 | 适用于频率输出的核仪表系统的中子噪声测量方法和装置 |
CN113436766B (zh) * | 2021-06-07 | 2023-05-26 | 中国核动力研究设计院 | 一种用于核电厂的堆外核仪表系统设备 |
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- 2014-08-29 EP EP14900613.2A patent/EP3188193A4/en not_active Withdrawn
- 2014-08-29 CN CN201480081565.5A patent/CN106605269A/zh active Pending
- 2014-08-29 WO PCT/JP2014/072723 patent/WO2016031045A1/ja active Application Filing
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JP7227959B2 (ja) | 2017-08-18 | 2023-02-22 | ウエスチングハウス・エレクトリック・カンパニー・エルエルシー | 絶縁分離された核計装出力信号のスケーリング方法および当該方法を用いたシステム |
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US20170047132A1 (en) | 2017-02-16 |
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