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The Design Of Reactor Power Monitor Based On 16N? Energy Spectrum Measurement

Posted on:2021-05-10Degree:MasterType:Thesis
Country:ChinaCandidate:L WangFull Text:PDF
GTID:2392330602488675Subject:Nuclear Science and Technology
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Reactor power is a significant parameter for nuclear power plants'safety and control.Accurate measurement of nuclear reactor power is of great importance to the safe operation of the reactor in many important nodes,such as nuclear reactor start-up,increasing power,full power operation,and power reduction operation.Therefore,the design of the reactor power measurement instrument follows the principle of diversity.Generally multiple measures are adopted to monitor the reactor power to ensure the safety of the reactor,such as various kinds and redundant design.The 16N concentration in the primary loop of the nuclear reactor has a linear relationship with the reactor power.By online monitoring the 16N?radioactivity in the primary loop,the nuclear reactor power can be measured efficiently and quickly.At present,16N power monitor systems mostly use the method of 16N total gamma dose measurement in domestic.that is,it monitors the reactor power by detecting the 16N total?radioactive intensity of main pipe of the primary loop.However,there are many other activated and fission?radionuclides in the primary loop,which is a certain interference to the method of the 16N total?dose monitoring reactor power.This paper studies the reactor power measurement method based on 16N?energy spectrum for purpose of eliminating the interference of other?radionuclides in the water of the main pipe,which can measure the reactor power more accurately.It is of practical value.The main research of the thesis is as follows:1.Establish a theoretical model for monitoring reactor power based on16N?energy spectrum.2.Because 16N?radioactivity is too high in the primary loop,MCNP is used to optimize the simulation of the shielding design of the reactor power monitor based on 16N?energy spectrum measurement.So that after setting a reasonable shielding,the NaI detector can obtain a good 16N?energy spectrum and have a high enough counting rate when running at full power.?1?On account of the source system is large and the particle penetration probability is small,the Monte Carlo simulation result is too small,resulting in a large simulation error,and may not even get the simulation result.In this paper,multiple MCNP simulation methods are used for comparison,such as direct calculation,segmentation and dose estimation.?2?The calculation of the lead chambers with different thicknesses without the collimating aperture is used to select the lead chamber shielding based on shielding most of the?rays of the main pipe and reducing the NaI detector counting rate to a lower range by the source item analysis.The lead thickness is set to18cm eventually.?3?MCNP software is simulated when the size of collimating aperture was selected as 0.5cm,1cm and 2cm.Analyzing through the appropriate range of detector counting rate,the size of collimating aperture is selected as1cm.According to the above simulation data,the lead shielding of 16N monitor was designed and processed.3.Establishing the experimental measurement system based on 16N?energy spectrum monitoring reactor power,the detector was debugged,and the energy calibration experiment was conducted by using PuC source which emits 6.13MeV?ray,137Cs source which emits 0.662MeV?ray,60Co source which emits 1.173MeV and 1.332MeV?rays.
Keywords/Search Tags:16N monitoring reactor power, ? energy spectrum measurement, lead shielding, MCNP simulation, detection efficiency
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