CN107230505A - A kind of reactor nucleus power monitoring method and system - Google Patents

A kind of reactor nucleus power monitoring method and system Download PDF

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Publication number
CN107230505A
CN107230505A CN201710475532.4A CN201710475532A CN107230505A CN 107230505 A CN107230505 A CN 107230505A CN 201710475532 A CN201710475532 A CN 201710475532A CN 107230505 A CN107230505 A CN 107230505A
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China
Prior art keywords
reactor
signal
spectral density
cross
circuit
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CN201710475532.4A
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Inventor
刘才学
彭翠云
曾杰
何攀
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Nuclear Power Institute of China
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Nuclear Power Institute of China
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    • GPHYSICS
    • G21NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21CNUCLEAR REACTORS
    • G21C17/00Monitoring; Testing ; Maintaining
    • G21C17/10Structural combination of fuel element, control rod, reactor core, or moderator structure with sensitive instruments, e.g. for measuring radioactivity, strain
    • G21C17/104Measuring reactivity
    • 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

Abstract

The invention discloses a kind of reactor nucleus power monitoring method and system, its method includes A, after reactor power level is stable, and the neutronic noise signal of reactor is measured using two neutron being arranged symmetrically gamma compensated ionization chambers;B, the FFT to two groups of neutronic noise signal of change time signals, calculate cross-spectral density φXYAnd normalized;C, cross-spectral density is fitted, and calculates frequencies omega1When cross-spectral density φXY1);D, the parameter obtained according to fitting, obtain reactor fission rate F, so as to obtain reactor absolute power P.It carries out parameter measurement under not disturbing reaction heap normally operation, it is adaptable to all reactors, and measurement is convenient and quick.

Description

A kind of reactor nucleus power monitoring method and system
Technical field
Field is monitored the present invention relates to reactor nucleus power, and in particular to one kind is reacted based on neutronic noise signal come scale Core power monitor method and system.
Background technology
In reactor zero power physics testing, to ensure that operation power is no more than related nuclear safety codes and operation limit The requirement of value and condition, while also providing input parameter to check theoretical calculation, needs the absolute power of knowing reaction heap.
In thermal neutron zero power reactor, scale absolute power generally uses activation analysis, and this method modifying factor is very Many, data processing is also more complicated, for swimming pool reactor or zero-energy reactor, because the arrangement of active region often changes, The absolute power of reactor is measured, just necessary often scale, it appears fairly cumbersome.Also one kind is passed in and out according to reactor coolant Mouthful temperature difference and total flow are come the method that calculates absolute power, but it is only applicable to the higher power reactor of power.It is anti-for low-power Answer heap or the temperature difference is small, system radiating amount very big swimming pool reactor, the absolute power error determined in this way is very big.Other sides Method such as source introduction method, due to neutron source active strength dyscalculia, there is uncertainty in neutron source reactivity worth, therefore, survey Measure result less reliable.
The content of the invention
In order to solve the above-mentioned technical problem the present invention provides a kind of reactor nucleus power monitoring method and system, and it is not being done Disturb and parameter measurement is carried out under normal reactor operation, it is adaptable to all reactors, measurement is convenient and quick.
The present invention is achieved through the following technical solutions:
A kind of reactor nucleus power monitoring method, comprises the following steps:
A, after reactor is stable up to critical power level, in order to which the space for reducing reactor in-core neutron flux is imitated Should, the neutronic noise signal of reactor is measured using two neutron being arranged symmetrically gamma compensated ionization chambers;
B, the FFT to two groups of neutronic noise signal of change time signals, calculate cross-spectral density φXYAnd at normalization Reason;
C, cross-spectral density is fitted, obtains cross-spectral density matched curve, frequency is obtained in matched curve Rate ω1When cross-spectral density φ 'XY1);
D, the parameter obtained according to fitting, obtain reactor fission rate F, so as to obtain reactor absolute power P.
The method part of this programme includes pile neutron noise signal measuring process and power measurement step, wherein, step Rapid B, C, D belong to power measurement step, obtain cross-spectral density by neutron noise signal analyze and are fitted To dynamic parameter, so as to obtain absolute power.Measured and obtained under not disturbing reaction heap normally operation using the data of this method, Suitable for all reactors, it is not necessary to which frequent scale, measurement is convenient and quick, and its measurement accuracy is high, effectively solve existing There is the problems such as error is greatly in low-power reactor power measurement and process is numerous and diverse.
Preferably, in step B, in addition to the smoothing processing of cross-spectral density, the number of times of the smoothing processing is big In equal to 8 times.Cross-spectral density is smoothed, the interference of random noise, the number of times of smoothing processing can be effectively reduced At 8 times, the influence of random noise can be excluded or reduced substantially.
Further, the method for the smoothing processing is specially:Current cross-spectral density was effectively measured with last time Calculate obtained cross-spectral density to be averaged, obtain the average cross-spectral density of two groups of noise signals, and draw mutual work( Rate spectrum density curve.
Preferably, cross-spectral density φ ' after normalizationXYFor:
Wherein, A is related to reactor power level, ionisation chamber detection efficient normal Number;β is effective delayed neutron fraction;ω is angular frequency;ι is prompt neutron removal lifetime;
Further, step C is fitted using nonlinear least square method, is specially:Using non-linear least square Method fitting parameter input parameter A, ι, β fitting initial value, the installation warrants reactor core physical theory of initial value, which is calculated, to be obtained The dynamic parameter value obtained is configured, and obtains Reactor dynamic parameters A, ι, β of fitting.
Preferably, in the step D, reactor fission rate F is:
Wherein, D refers to driven factor, and β is effective delayed neutron fraction;
Reactor absolute power P is:P=P0F, wherein, P0Refer to the energy that a nuclear fission is discharged.
The measuring method be using the average current or the statistic fluctuation of voltage caused by a large amount of neutrons as Fundamentals of Measurement, Further according to the output signal of reactor Reactor dynamic parameters are determined around the change of its steady-state average value random statistical fluctuation And absolute power.This technology has the advantages that the not normal operating measurement parameter of disturbing reaction heap, and suitable for swimming pool Reactor, is that measurement absolute power is more convenient, efficiently measuring method.
A kind of reactor nucleus power monitoring system, including:
Two sets of neutron gamma compensated ionization chambers for word noise signal in symmetrical collection reactor;
Micro-current for being amplified to neutron gamma compensated ionization chamber output current signal and be converted to voltage signal is put Big device;
Signal transacting is carried out to micro current amplifier output signal and DC level signal and neutronic noise signal will be exported The signal conditioning circuit for being converted to data signal;
Reactor nucleus power is analyzed and processed and realized to micro-current magnification according to signal conditioning circuit output signal Device, the data analysis of the control of signal conditioning circuit and processing unit.
The signal conditioning circuit includes isolation circuit, DC offset circuit, noise amplifier circuit, the low pass being sequentially connected Filter circuit, buffer circuit, by isolation circuit, output signal and buffering circuit output signal are converted to the A/D of data signal all the way Change-over circuit.
The present invention compared with prior art, has the following advantages and advantages:
1st, caused by the inventive method using a large amount of neutrons average current or the statistic fluctuation of voltage as Fundamentals of Measurement, Measure and obtain under not disturbing reaction heap normally operation, it is adaptable to all reactors, it is not necessary to frequent scale, measurement it is convenient and Fast, its measurement accuracy is high, the problem of effectively solving big error in existing low-power reactor power measurement and numerous and diverse process.
Brief description of the drawings
Accompanying drawing described herein is used for providing further understanding the embodiment of the present invention, constitutes one of the application Point, do not constitute the restriction to the embodiment of the present invention.In the accompanying drawings:
Fig. 1 is the structural representation of apparatus of the present invention.
Fig. 2 installs and uses situation map for the present apparatus.
Embodiment
For the object, technical solutions and advantages of the present invention are more clearly understood, with reference to embodiment and accompanying drawing, to this Invention is described in further detail, and exemplary embodiment and its explanation of the invention is only used for explaining the present invention, does not make For limitation of the invention.
Embodiment 1
A kind of reactor nucleus power monitoring method, comprises the following steps:
A, after reactor power level is stable, measure reactors using two neutron being arranged symmetrically gamma compensated ionization chambers In
Sub- noise signal;
B, the FFT to two groups of neutronic noise signal of change time signals, calculate cross-spectral density φXYAnd at normalization Reason;
C, cross-spectral density is fitted, and calculates a certain specific frequency ω1When cross-spectral density φ 'XY1);
D, the parameter obtained according to fitting, obtain reactor fission rate F, so as to obtain reactor absolute power P.
The measuring method be using the average current or the statistic fluctuation of voltage caused by a large amount of neutrons as Fundamentals of Measurement, Further according to the output signal of reactor Reactor dynamic parameters are determined around the change of its steady-state average value random statistical fluctuation And absolute power.This technology has the advantages that the not normal operating measurement parameter of disturbing reaction heap, and suitable for swimming pool Reactor, is that measurement absolute power is more convenient, efficiently measuring method, realizes the survey of the automation to reactor absolute power Amount.
Power measurement step is specially:
To the FFT of two groups of obtained neutronic noise signal of change time signals, i.e. fast Fourier transform;Then mutual work(is calculated Rate spectrum density φXY, drafting cross-spectral density curve after the smoothing processing of at least 8 times is carried out to cross-spectral density.
The method of smoothing processing is specially:After current cross-spectral density and last time averaging process are restarted most The cross-spectral density once calculated afterwards is averaged, and obtains the average cross-spectral density of two groups of noise signals, and is painted Go out cross-spectral density curve.
According to Koln noise equivalent neutron source it is assumed that the reactor in critical condition, what two ionisation chambers were measured Reactor noise cross-spectral density is:
Wherein:WX、WYThe detector efficiency of respectively two ionisation chambers;The factor, i.e. driven factor, to U235Make the reactor of fuel, D=0.795;F is exhausted for reactor To fission rate;The mean charge converted by one neutron of every detection;H (ω) is the transmission function of reactor.
The average current of ionisation chamber output is represented by:
For critical pile, transmission function can approximate representation be:
Wherein:It is in for reactor under delayed criticality state and obtains prompt neutron decay often Number;β is effective delayed neutron fraction;ω is angular frequency.
Thus convertible export:
Cross-spectral density is normalized, the cross-spectral density φ ' after being normalizedXY
Wherein:VX、VYRespectively two groups noise signal voltage magnitudes;AX、AYRespectively two groups Noise signal multiplication factor.
Then cross-spectral density expression formula is transformed to
Parameter fitting model y=f (x, a are set up by above formulai) nonlinear function, reflect ω and φ 'XYDependence close System, A, ι, β are equivalent to aiFor undetermined parameter.Using Labview Software Development Platform for Virtual Instruments, with non-linear least square Method fitting tool, i.e., using the least square set that parameter is determined using Levenberg-Marquardt algorithms, the set is defeated Enter the best fit of data point (x, y), data point can be by nonlinear function y=f (x, ai) represent, wherein aiIt is the set of parameter.
Using Non-linear least-square curve fitting parameter input parameter A, ι, β fitting initial value, the setting of initial value according to According to reactor core physical theory calculate obtain dynamic parameter value be configured, obtain fitting Reactor dynamic parameters A, ι, β。
And cross-spectral density is obtained using fitting, calculate a certain specific frequency ω of Frequency1When crosspower spectrum it is close Spend φ 'XY1), selected ω1λ should be metmax《ω1《αc, λmax=14 be the maximum of six delayed-neutron precursor decay coefficients Value, i.e., 14《ω1, therefore desirable f1=3, ω1》18.84, αcIt is changing value, and ω1Value it is the smaller the better, typically take 18.84.
The cross-spectral density of neutronic noise signal is after normalized, and reactor fission rate F should be expressed as
The parameter and the cross-spectral density φ ' of calculating obtained by using curve matchingXY1), calculate reactor Fission rate.
Reactor absolute power P=P0F, wherein, P0Refer to the energy that a nuclear fission is discharged.One single U235Core About 3.2 × 10 can be sent during fission-11W/s energy.For using U235As the reactor of fuel, according to P=3.2 × 10-11F can calculate reactor absolute power P.
Embodiment 2
As shown in figure 1, a kind of reactor nucleus power monitoring system based on the above method, including:
Two sets of neutron gamma compensated ionization chambers for word noise signal in symmetrical collection reactor;
Micro-current for being amplified to neutron gamma compensated ionization chamber output current signal and be converted to voltage signal is put Big device;
Signal transacting is carried out to micro current amplifier output signal and DC level signal and neutronic noise signal will be exported The signal conditioning circuit for being converted to data signal;
Reactor nucleus power is analyzed and processed and realized to micro-current magnification according to signal conditioning circuit output signal Device, the data analysis of the control of signal conditioning circuit and processing unit.
Two sets of neutron gamma compensated ionization chambers constitute primary instrument, micro current amplifier, signal conditioning circuit and data analysis Secondary meter is constituted with processing unit.Specifically, as shown in Fig. 2 being arranged symmetrically 2 between reactor core peripheral board and bracketplant DL125 type neutron gamma compensated ionization chambers, for gathering pile neutron noise signal.The design and assembly of neutron gamma compensated ionization chamber into Kit form, ionization chamber enclosure shape is in suspended state, to reduce interference.High voltage power supply is used to be supplied for neutron gamma compensated ionization chamber Electricity, the excitation type converter type high voltage power supply for employing 2 independent continuously adjustabes provides required positive/negative electricity to two ionisation chambers Pressure, adjusts converter drive signal amplitude, reaches the purpose of adjustment output high pressure, output voltage:0~± 500V continuously adjustabes; Low-tension supply is supplied to the necessary dc source of low current normal amplifier operation.
The current signal of 2 neutron gamma compensated ionization chamber outputs is transferred to micro current amplifier by double-shielded cable, Micro current amplifier is amplified to current signal and is converted to 0~10V voltage signal.Micro current amplifier is provided with different Multiplication factor gear, data analysis putting according to the current signal size adjust automatically low current amplifier of acquisition with processing unit Big gear.
Signal conditioning circuit has two-way, each is attached on two neutron gamma compensated ionization chambers, it includes what is be sequentially connected Isolation circuit, DC offset circuit, noise amplifier circuit, low-pass filter circuit, buffer circuit and A/D change-over circuits.
The two-way DC level signal that signal conditioning circuit receives micro current amplifier output is carried out after isolation processing to it Direct current signal is transmitted directly to A/D change-over circuits all the way, and another road is passed after DC compensation, programming amplifying and low-pass filtering treatment Give A/D change-over circuits.It is controlled by data analysis and processing unit for DC offset circuit, noise amplifier circuit, is passed through 16 DA arbitrarily regulations are directly added into direct current biasing component, complete DC compensation, its dc offset range:0~10V, direct current is mended Repay precision:±1mV.The arbitrary disposition of programming amplifying can also be realized simultaneously, specific multiplication factor has:1、10、50、100、200、 500.The size of signal amplitude adjust automatically DC compensation and the putting of signal of the data analysis with processing unit according to collection feedback Big multiple.
Data analysis includes processor, operating system and application program with processing unit, completes the analysis and processing of signal. Its application program is completed based on the method in embodiment 1, and the development platform of software is used as using Labview virtual instrument techniques;Should Realized with program and low current amplifier gear is configured and read, control its fluid drive, and its output amplitude is carried out Detection;DC level is compensated automatically;Signal adaptation unit gain and filtering parameter are configured and read;To A/D Sample frequency and sampling length are configured;Control A/D conversion start and stop;The data cached readings of A/D and display;From power Spectrum density is analyzed with showing with cross-spectral density;Nonlinear least square method dynamic parameter is fitted;Absolute power is calculated.
Based on the system, it is embodied as process and is:
When reactor starts lifting power, startup power monitoring system, system is by automatic measurement reactor noise.Micro- electricity Stream amplifier is provided with different multiplication factor gears, as reactor capability constantly rises, is automatically controlled by Labview softwares Micro current amplifier constantly converts gear, reduces multiplication factor, during opposite power reduction, low current amplifier will increase times magnification Count, then low current amplifier converts a signal into voltage signal output.
After reactor capability is stable, pile neutron noise signal is nursed one's health and gathered, two compensated neutron γ Two groups of neutronic noise current signals of compensated ionization chamber's measurement are respectively divided into two-way, are all the way DC level passage, direct measurement is straight Flow level magnitude;Another road is neutronic noise passage, and noise signal conditioning is carried out to neutronic noise, and signal condition step is as follows:
DC compensation:Level according to neutronic noise passage carries out DC compensation to neutron noise signal, in removal Flip-flop in sub- noise signal, compensation way uses negative feedback control, and dc offset accuracy is 2mv, i.e., neutronic noise is led to Road When, DC compensation will be carried out automatically, and v is neutronic noise channel voltage, and A is current noise multiplication factor.
Noise amplifies:Neutron noise signal is amplified step by step after DC compensation, signal condition equipment multiplication factor has: 1、10、50、100、200、500.Neutronic noise signal is precalculated according to A1After amplifying again, judge whether noise signal outranges (± 5V), does not outrange such as, then it is A to set noise signal multiplication factor1, then A is amplified in precomputation again2Times noise signal is No to outrange, noise signal will continue to amplify if not outranging, then outranged, and reduction multiplication factor is back to A1Times.
LPF:Corner frequency ω according to the cross-spectral density of reactor is equal to prompt neutron decay constant αcI.e. The π f=α of ω=2c, then signal analysis frequencyTherefore noise signal selects setting to be more than firstFrequency carries out low pass filtered Ripple, signal condition equipment LPF gear has:100Hz、200Hz、300Hz、500Hz.
When lifting or decline occurs in reactor power level, then low current amplifier amplification gear changes, now in Sub- noise channel multiplication factor will be set to 1 times, and after then power level is stable, system will be filtered to noise signal again The operations such as ripple, DC compensation, noise amplification.
Two-way neutronic noise passage synchronizes collection after signal condition with two-way DC level passage, obtains two groups The DC level and neutronic noise signal of neutron gamma compensated ionization chamber.
System of the present invention using based on PXI buses standardization and modular technology, improve system reliability and Servicing ease.Realize the automatic measurement to reactor absolute power and improve measurement accuracy, efficiently solve existing There is the problems such as error is greatly in low-power reactor power measurement and process is numerous and diverse.
Above-described embodiment, has been carried out further to the purpose of the present invention, technical scheme and beneficial effect Describe in detail, should be understood that the embodiment that the foregoing is only the present invention, be not intended to limit the present invention Protection domain, within the spirit and principles of the invention, any modification, equivalent substitution and improvements done etc. all should be included Within protection scope of the present invention.

Claims (8)

1. a kind of reactor nucleus power monitoring method, it is characterised in that comprise the following steps:
A, after reactor power level is stable, measured using two neutron being arranged symmetrically gamma compensated ionization chambers in reactors Sub- noise signal;
B, the FFT to two groups of neutronic noise signal of change time signals, calculate cross-spectral density φXYAnd normalized;
C, cross-spectral density is fitted, and calculates frequencies omega1When cross-spectral density φ 'XY1);
D, the parameter obtained according to fitting, obtain reactor fission rate F, so as to obtain reactor absolute power P.
2. a kind of reactor nucleus power monitoring method according to claim 1, it is characterised in that:In step B, in addition to pair The smoothing processing of cross-spectral density, the number of times of the smoothing processing is more than or equal to 8 times.
3. a kind of reactor nucleus power monitoring method according to claim 2, it is characterised in that the side of the smoothing processing Method is specially:The cross-spectral density that current cross-spectral density and last time effective survey calculation are obtained is averaged, and is obtained The average cross-spectral density of two groups of noise signals is obtained, and draws cross-spectral density curve.
4. a kind of reactor nucleus power monitoring method according to claim 1, it is characterised in that crosspower spectrum after normalization Density φ 'XYFor:
Wherein, A is the constant related to reactor power level, ionisation chamber detection efficient;β is Effective delayed neutron fraction;ω is angular frequency;ι is prompt neutron removal lifetime.
5. a kind of reactor nucleus power monitoring method according to claim 4, it is characterised in that step C is using non-linear Least square method is fitted, and is specially:Fitting using Non-linear least-square curve fitting parameter input parameter A, ι, β is initial Value, the installation warrants reactor core physical theory of initial value calculates the dynamic parameter value obtained and is configured, and obtains fitting Reactor dynamic parameters A, ι, β.
6. a kind of reactor nucleus power monitoring method according to claim 1, it is characterised in that in the step D, reaction Heap fission rate F is:
Wherein, D refers to driven factor, and β is effective delayed neutron fraction;
Reactor absolute power P is:P=P0F, wherein, P0Refer to the energy that a nuclear fission is discharged.
7. a kind of reactor nucleus power monitoring system, it is characterised in that including:
Two sets of neutron gamma compensated ionization chambers for word noise signal in symmetrical collection reactor;
For being amplified to neutron gamma compensated ionization chamber output current signal and being converted to the micro current amplifier of voltage signal;
Signal transacting is carried out to micro current amplifier output signal and turns output DC level signal and neutronic noise signal It is changed to the signal conditioning circuit of data signal;
Reactor nucleus power is analyzed and processed according to signal conditioning circuit output signal and realized to micro current amplifier, letter The data analysis of the control of number modulate circuit and processing unit.
8. a kind of reactor nucleus power monitoring system according to claim 1, it is characterised in that the signal conditioning circuit Including the isolation circuit being sequentially connected, DC offset circuit, noise amplifier circuit, low-pass filter circuit, buffer circuit, will isolation Output signal and buffering circuit output signal are converted to the A/D change-over circuits of data signal to circuit all the way.
CN201710475532.4A 2017-06-21 2017-06-21 A kind of reactor nucleus power monitoring method and system Pending CN107230505A (en)

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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109256226A (en) * 2018-11-05 2019-01-22 三门核电有限公司 A kind of reactor Critical lattice monitor system and method
CN111627581A (en) * 2020-06-09 2020-09-04 中国原子能科学研究院 Method and device for measuring fast reactor power distribution
CN112133462A (en) * 2020-09-24 2020-12-25 中国核动力研究设计院 Power calibration method for critical device
CN113295924A (en) * 2021-05-25 2021-08-24 中国核动力研究设计院 Neutron noise measurement method and device suitable for nuclear instrument system with frequency output
CN115295179A (en) * 2022-08-22 2022-11-04 中国原子能科学研究院 Compensation method for reactor power measurement

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1374256A (en) * 2001-03-09 2002-10-16 肖藻生 Waste alkali liquor oxidizing, decomposing, neutralizing and saponifying treatment with cyclohexane
CN101685678A (en) * 2008-09-27 2010-03-31 中国核动力研究设计院 Vibration monitoring system of reactor and reactor internals
CN103049610A (en) * 2012-12-20 2013-04-17 西北核技术研究所 Reactor designing method
CN104933245A (en) * 2015-06-15 2015-09-23 南华大学 Ship reactor shielding design optimization method based on neural network and genetic algorithm

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1374256A (en) * 2001-03-09 2002-10-16 肖藻生 Waste alkali liquor oxidizing, decomposing, neutralizing and saponifying treatment with cyclohexane
CN101685678A (en) * 2008-09-27 2010-03-31 中国核动力研究设计院 Vibration monitoring system of reactor and reactor internals
CN103049610A (en) * 2012-12-20 2013-04-17 西北核技术研究所 Reactor designing method
CN104933245A (en) * 2015-06-15 2015-09-23 南华大学 Ship reactor shielding design optimization method based on neural network and genetic algorithm

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
彭翠云等: "基于反应堆噪声技术的零功率绝对功率测量系统设计", 《核电子学与探测技术》 *

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109256226A (en) * 2018-11-05 2019-01-22 三门核电有限公司 A kind of reactor Critical lattice monitor system and method
CN109256226B (en) * 2018-11-05 2020-07-03 三门核电有限公司 Reactor critical extrapolation monitoring system and method
CN111627581A (en) * 2020-06-09 2020-09-04 中国原子能科学研究院 Method and device for measuring fast reactor power distribution
CN111627581B (en) * 2020-06-09 2022-06-28 中国原子能科学研究院 Method and device for measuring fast reactor power distribution
CN112133462A (en) * 2020-09-24 2020-12-25 中国核动力研究设计院 Power calibration method for critical device
CN113295924A (en) * 2021-05-25 2021-08-24 中国核动力研究设计院 Neutron noise measurement method and device suitable for nuclear instrument system with frequency output
CN115295179A (en) * 2022-08-22 2022-11-04 中国原子能科学研究院 Compensation method for reactor power measurement
CN115295179B (en) * 2022-08-22 2023-12-12 中国原子能科学研究院 Compensation Method for Reactor Power Measurement

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