WO2015176553A1 - Method for monitoring 16n leaked by nuclear power reactor steam generator - Google Patents

Method for monitoring 16n leaked by nuclear power reactor steam generator Download PDF

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WO2015176553A1
WO2015176553A1 PCT/CN2015/071668 CN2015071668W WO2015176553A1 WO 2015176553 A1 WO2015176553 A1 WO 2015176553A1 CN 2015071668 W CN2015071668 W CN 2015071668W WO 2015176553 A1 WO2015176553 A1 WO 2015176553A1
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nuclear power
steam generator
energy
power reactor
reactor steam
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PCT/CN2015/071668
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French (fr)
Chinese (zh)
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田志恒
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田志恒
田立
田陆
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/20Measuring radiation intensity with scintillation detectors
    • G01T1/202Measuring radiation intensity with scintillation detectors the detector being a crystal

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  • the invention relates to the field of nuclear power reactor radiation monitoring, in particular to a 16 N monitoring method for leakage from a nuclear power reactor steam generator.
  • the scintillator embedded with the alpha source also has technical problems such as causing uncertainty to the scintillator during the manufacturing process and affecting the monitoring result.
  • the existing NaI(Tl) scintillator also has a problem that the detection efficiency and energy resolution of the 16 N monitoring are relatively low.
  • the object of the present invention is to provide a 16 N monitoring method for leaking out of a nuclear power reactor steam generator, so as to solve the technical problem that the monitoring system has low sensitivity and is prone to false alarms.
  • the present invention provides a 16 N monitoring method for a nuclear power reactor steam generator, comprising the following steps: S01, the scintillator detecting device containing the gamma source is retained after the background peeling The scaled peak of the stable gamma energy spectrum is used to monitor the 16 N leaked by the nuclear power reactor steam generator and generate a monitoring signal; S02, the signal processor is used to process the monitoring signal, and the monitoring result is output.
  • the background peeling means that the scintillator detecting device containing the gamma source is placed in the low background chamber for a sufficiently long period of time to reduce the statistical error of the obtained count to a negligible degree, and the result is obtained.
  • the count is divided by the measurement time to give the count rate of each energy zone and the energy spectrum meter and stored; when the nuclear power reactor is measured in the field, the count rate of the graduated peak region is reserved for stabilizing the gamma energy spectrum, and the scale peak region is deducted. The count rate stored outside.
  • the monitoring result includes a count rate of three energy zones of 0.2-2.2 MeV, 2.2-4.5 MeV, 4.5-7.0 MeV, a peak height count rate of the 16 N characteristic peak, and an integral of the count rate integral.
  • Count, and the count rate of the three energy zones, the peak height count rate of the 16 N characteristic peak, and the integral count of the integral count of the count rate over time, the count rate of each spectrum spectrometer, and the energy spectrum meter The energy score obtained by the count rate integration.
  • the 16 N monitoring method leaked by the nuclear power reactor steam generator further comprises dividing the level of the nuclear power reactor steam generator leakage into a leakage warning level, a leakage level, and a leakage according to a counting rate of the 0.2-2.2 MeV energy region. The second step.
  • the count rate of the three energy zones, the peak height count rate of the 16 N characteristic peak, and the integral count of the count rate integral over time are plotted, and The count rate of each channel of the spectrometer is integrated over the set time T to obtain the energy spectrum.
  • the set time T is shortened as the leak level is increased.
  • the monitoring results are displayed in real time and stored by the memory.
  • the 16 N characteristic peak refers to an energy peak having gamma ray energies of 5.11 MeV, 5.62 MeV, and 6.13 MeV, respectively.
  • the 16 N monitoring method leaked by the nuclear power reactor steam generator also includes the steps of the nuclear power reactor steam generator leakage simulation.
  • the step of simulating the leakage of the nuclear power reactor steam generator means that the scintillation detecting device Ts containing the ⁇ source is irradiated with the 16 N scale source for N times, and the energy spectrum obtained by averaging the N measurements is obtained.
  • the video is shown in K*Ts time, where K is the 16 N scale source and the gamma source-containing scintillator detection device is in the 0.2-2.2 MeV energy zone and the nuclear power reactor steam generator leakage level is in the energy. The ratio of the count rate of the zone.
  • the video of the energy spectrum obtained by averaging the N measurements is fast-released in K*Ts time; if K>1, the energy spectrum obtained by N measurements is averaged. The video of the obtained energy spectrum was slowed down in K*Ts time.
  • the scintillator of the scintillator detecting device containing the ⁇ source is a LaBr 3 :Ce scintillator.
  • the 1.436 MeV ⁇ -ray energy peak of the natural radionuclide 138 La radiation contained in the LaBr 3 :Ce scintillation body and the 0.037 MeV X-ray energy peak of the K electron capture radiation are coincident with the energy peak added to 1.473 MeV.
  • the scale peak region refers to an energy interval in which the gamma ray energy is 1.434 to 1.497 MeV.
  • the 16 N scale source is a 238 Pu- 13 C source.
  • the use of the scintillator containing the gamma source avoids the uncertainty of the packaging process operation such as the embedded source, and solves the technical problem that the monitoring system has low sensitivity and is prone to false alarms and affects the monitoring result.
  • FIG. 1 is a schematic diagram showing the steps of a 16 N monitoring method for a nuclear power reactor steam generator leaking according to the present invention
  • FIG 2 is a monitoring method using LaBr 3 16 N leaking steam generator for nuclear reactor according to the present invention: Ce schematic front peeling detection means measuring the background;
  • FIG 3 is a monitoring method 16 N 3 of the steam generator leaks out by LaBr nuclear reactor according to the present invention: Ce view after peeling detection means measuring the background;
  • FIG 4 is a stack with monitoring method LaBr 3 16 N leaking out of the steam generator according to the present invention, nuclear: Ce detecting means 16 N measured calibration source 50s schematic spectrum;
  • FIG 5 is (Tl) detection means 16 N measured calibration source 50s schematic stack with NaI spectrum monitoring method 16 N leaking out of the steam generator according to the present invention, nuclear power;
  • FIG 6 is a leak monitoring method according to the present invention nuclear reactor steam generator 16 N: Ce-detecting means 16 N measured calibration source spectrum schematic 1800s; and
  • FIG 7 is (Tl) detection means 16 N measured calibration source schematic 1800s spectrum stack monitoring method using NaI 16 N leaking out of the steam generator according to the present invention is nuclear.
  • a 16 N monitoring method for leaking out of a nuclear power reactor steam generator includes the following steps: S01, the scintillator detecting device containing the ⁇ source is left after the background peeling The scaled peak of the stable gamma energy spectrum is used to monitor the 16 N leaked by the nuclear power reactor steam generator and generate a monitoring signal; S02, the monitoring signal is processed by a signal processor, and the monitoring result is output.
  • the use of the scintillator containing the gamma source avoids the uncertainty of the packaging process operation such as the embedded source, and solves the technical problem that the monitoring system has low sensitivity and is prone to false alarms and affects the monitoring result.
  • the background peeling refers to placing the scintillator detecting device containing the gamma source in a low background chamber (such as a lead chamber) for a sufficiently long time to reduce the statistical error of the obtained count to a negligible degree. Dividing the obtained count by the measurement time gives the energy rate of each energy zone and the energy meter (the count rate of the present invention is the net count rate) and stores it; retains the scale peak when the nuclear power reactor is measured in the field. The count rate of the zone is used to stabilize the gamma spectrum while deducting the count rate stored outside of the graduated peak region.
  • the LaBr 3 :Ce scintillator detecting device is preferably a scintillator detecting device containing a ⁇ source, and in other embodiments, other scintillator detecting devices containing a ⁇ source suitable for high-energy gamma ray detection may be selected.
  • the scale peak refers to the 1.473 MeV energy peak of the sum of the 1.436 MeV ⁇ -ray energy peak of the natural radionuclide 138 La radiation and the 0.037 MeV X-ray energy peak of the K electron trapping radiation contained in the LaBr 3 :Ce scintillation body, and the scale peak region is Refers to the energy range of gamma ray energy from 1.434 to 1.497 MeV.
  • is to LaBr 3 containing source: Ce scintillator detecting means described in detail as an example background release: the contents of the source ⁇
  • LaBr 3 Ce scintillator detection means disposed lead measuring chamber for 48 hours, the resulting count by 48*3600 seconds gives the count rate N b1 , N b2 (unit: cps) of each energy region and each spectrum spectrometer (4096 channels in total) and stores it; the gamma ray energy is 1.434-1.497 MeV when measured in the field.
  • the energy interval is the count rate of each channel of the 886-925 channel on the energy spectrum meter for stabilizing the gamma energy spectrum, and subtracting the energy interval, that is, the count rate stored outside the channel interval (that is, each obtained in the field measurement)
  • Figures 2 and 3 show the energy spectra of the substrate before and after stripping (under normal conditions) using a LaBr 3 :Ce detector. After the background peeling, the background count rate of the 0.2-2.2 MeV energy region was measured by the LaBr 3 :Ce scintillator detection device to be only 10 cps. However, the background count of the 0.2-2.2 MeV energy region was measured by the NaI(Tl) scintillator detection device to be 186 cps.
  • the monitoring result includes a count rate of three energy zones of 0.2-2.2 MeV, 2.2-4.5 MeV, 4.5-7.0 MeV, a peak height count rate of 16 N characteristic peaks, and an integral count of the integrals of these count rates, and The count rate of the three energy zones, the peak height count rate of the 16 N characteristic peaks, and the integral count of the integration counts of these count rates over time, the count rate of each spectrum spectrometer, and the count of each channel of the spectrometer The energy spectrum obtained by the rate integral.
  • the count rate of the above three energy zones, the peak height count rate of the 16 N characteristic peak, and the integral count of the integrated count of these count rate integrals are outputted, And the count rate of each of the spectrometers is integrated over the set time T, and further, the set time T is shortened as the leak level is increased.
  • the 16 N characteristic peak refers to an energy peak having gamma ray energies of 5.11 MeV, 5.62 MeV, and 6.13 MeV, respectively.
  • the method of the present invention further comprises dividing the level of leakage of the nuclear power reactor steam generator into a leakage warning level, a leakage level, and a leakage level according to a counting rate of a 0.2-2.2 MeV energy region.
  • the steps, as well as the steps of the simulation of the nuclear power reactor steam generator leak are dividing the level of leakage of the nuclear power reactor steam generator into a leakage warning level, a leakage level, and a leakage level according to a counting rate of a 0.2-2.2 MeV energy region.
  • Ne 500 cps (leakage level)
  • the count rate of the 16 N scale source in the energy range of 0.2-2.2 MeV is 1.21 times that of NaI(Tl) using the LaBr 3 :Ce scintillator detection device (as shown in Table 1).
  • Table 1 is a comparison chart of the counting rate of the 1800s of the 16 N scale source measured by LaBr 3 :Ce and NaI(Tl) using the 16 N monitoring method leaked by the nuclear power reactor steam generator according to the present invention.
  • the three leakage level thresholds of Np, Ne, and Nc are 121 cps, 605 cps, and 10285 cps, respectively. Table 2).
  • Table 2 is a leakage simulation data table of the 16 N monitoring method leaked by the nuclear power reactor steam generator according to the present invention.
  • the leak warning level threshold of the LaBr 3 :Ce scintillator detection device is 12 times (121/10) of its background count rate, which has higher reliability; and the leakage of the NaI (Tl) scintillator detection device is adopted.
  • the warning level threshold is 0.54 times (100/186) of its background count rate, and the leak warning level cannot be set.
  • Figure 4 and Figure 5 show the energy spectrum after averaging the 16 N scale source for 5 seconds using the LaBr 3 :Ce and NaI(Tl) scintillation detectors (the high-energy end of the energy spectrum of the linear coordinate system is shown)
  • this embodiment is magnified 100 times display), according to the energy spectrum of 4096 channels, it is shown that due to the low detection efficiency and poor energy resolution of the NaI(Tl) scintillator, it is also an integral count of 50 seconds, which is not only low in amplitude ( The 6.13 MeV energy peak is 4.2 times lower, the 5.62 MeV energy peak is 2.3 times lower, and the fluctuation is larger. Only some divergent spikes can be seen, and the well-defined 16 N characteristic peak image is not seen.
  • the 16 N scale source is a 238 Pu- 13 C source.
  • Leakage simulation refers to the use of a 16 N scale source to illuminate the scintillator detection device Ts containing the ⁇ source for N times, and the video of the energy spectrum obtained by averaging the N measurements is displayed in K*Ts time.
  • the K is a 16 N scale source illuminating the ratio of the count rate of the scintillator detection device containing the gamma source in the energy range of 0.2-2.2 MeV to the count rate of each leak level of the nuclear power reactor steam generator in the energy region. Further, if K ⁇ 1, the video of the energy spectrum obtained by averaging the N measurements is fast-released in K*Ts time; if K>1, the energy spectrum obtained by N measurements is averaged. The video of the obtained energy spectrum was slowed down in K*Ts time.
  • the leakage simulation of the nuclear power reactor steam generator can be performed according to the counting rate of 2.2-4.5MeV, 4.5-7MeV, 0-7MeV energy region or the peak height counting rate of 5.11MeV, 5.62MeV and 6.13MeV energy peaks. ,As shown in table 2.
  • the energy spectrum (logarithmic coordinates) of the 1800s of the 16 N scale source is measured by the LaBr 3 :Ce and NaI(Tl) scintillator detection device.
  • the former has excellent energy spectrum for the 16 N characteristic peak. In the latter.
  • the method of the present invention provides LaBr 3: Ce scintillator 16 N for measuring the ratio of NaI (Tl) scintillator with a higher detection efficiency and energy resolution, leaving only 1.473MeV energy peak after a background process scale peak release
  • the background count rate in the energy range of 0.2-2.2 MeV and 2.2-4.5 MeV is only 5% and 0.7% of the embedded ⁇ -source NaI(Tl) scintillator, which can balance 0.2-2.2 MeV, 2.2-4.5 MeV, 4.5.
  • the detection system immediately starts the integral counting function for integrating these counting rates, and measures the integral count of each of the three energy zones and the characteristic peak of 16 N as time rises in time, only one or two minutes.
  • the real image of the leak can be displayed, and the true and false alarms are easy to distinguish and there will be no false alarms.
  • the leakage warning level which increases the leakage alarm sensitivity of the nuclear power reactor steam generator by 5 times is increased.
  • the use of the LaBr 3 :Ce scintillator containing the ⁇ source avoids the technical problems such as the inconsistency of the encapsulation process by the embedded source and the like, which affects the monitoring result.

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Abstract

A method for monitoring 16N leaked by a nuclear power reactor steam generator, the method comprising the following steps: S01, enabling a scintillator detection device comprising γ sources to maintain the scale peak of a stable γ energy spectrum to monitor the 16N leaked by a nuclear power reactor steam generator and generate a monitoring signal; S02, utilizing a signal processor to process the monitoring signal, and outputting a monitoring result. Utilizing the scintillator comprising γ sources avoids an uncertainty factor of the scintillator caused by a packaging process operation such as an embedded source, and solves the technical problem of false alarms affecting a monitoring result due to the low sensitivity of a monitoring system.

Description

用于核动力堆蒸汽发生器泄漏出的16N的监测方法16N monitoring method for leakage from nuclear power reactor steam generator 技术领域Technical field
本发明涉及核动力堆辐射监测领域,特别地,涉及一种用于核动力堆蒸汽发生器泄漏出的16N的监测方法.。The invention relates to the field of nuclear power reactor radiation monitoring, in particular to a 16 N monitoring method for leakage from a nuclear power reactor steam generator.
背景技术Background technique
核动力堆采用内嵌241Amα源的NaI(Tl)闪烁体作探测器件监测蒸汽发生器泄漏出的16N技术已有几十年的历史,当前仍广泛使用,其中的α源用于稳定16N的γ能谱,但241Amα粒子在闪烁体中电离产生的3.5MeV等效γ能量峰区较宽(约为3.0-3.7MeV,与内嵌工艺有关),在监测16N技术关注的0.2-4.5MeV能区产生较高的本底计数率,监测系统灵敏度低,易出现误报警。内嵌α源的闪烁体还具有在制作过程中给闪烁体带来不确定性因素从而影响监测结果等技术问题。此外,现有的NaI(Tl)闪烁体还存在对16N监测其探测效率和能量分辨率都比较低的问题。Embedded into nuclear power reactors 241 Amα source NaI (Tl) scintillator for decades history monitoring probe member leaking steam generator 16 N technology, currently still widely used, wherein the source for stabilizing α 16 The gamma spectrum of N, but the 3.5 MeV equivalent gamma energy peak region generated by ionization of 241 Amα particles in the scintillator is wider (about 3.0-3.7 MeV, which is related to the in-line process), and is monitored in the 16 N technique. The -4.5MeV energy zone produces a high background count rate, and the monitoring system has low sensitivity and is prone to false alarms. The scintillator embedded with the alpha source also has technical problems such as causing uncertainty to the scintillator during the manufacturing process and affecting the monitoring result. In addition, the existing NaI(Tl) scintillator also has a problem that the detection efficiency and energy resolution of the 16 N monitoring are relatively low.
发明内容Summary of the invention
本发明目的在于提供一种用于核动力堆蒸汽发生器泄漏出的16N的监测方法,以解决监测系统灵敏度低,易出现误报警的技术问题。The object of the present invention is to provide a 16 N monitoring method for leaking out of a nuclear power reactor steam generator, so as to solve the technical problem that the monitoring system has low sensitivity and is prone to false alarms.
为实现上述目的,本发明提供了一种用于核动力堆蒸汽发生器泄漏出的16N的监测方法,包括如下步骤:S01,将内含γ源的闪烁体探测装置在本底剥离后保留稳定γ能谱的刻度峰,用于监测核动力堆蒸汽发生器泄漏出的16N并生成监测信号;S02,用信号处理机处理监测信号,并输出监测结果。In order to achieve the above object, the present invention provides a 16 N monitoring method for a nuclear power reactor steam generator, comprising the following steps: S01, the scintillator detecting device containing the gamma source is retained after the background peeling The scaled peak of the stable gamma energy spectrum is used to monitor the 16 N leaked by the nuclear power reactor steam generator and generate a monitoring signal; S02, the signal processor is used to process the monitoring signal, and the monitoring result is output.
进一步地,在步骤S01中,本底剥离是指把内含γ源的闪烁体探测装置置于低本底小室内测量足够长的时间使所得计数的统计误差降低到可以忽略的程度,将所得计数除以测量时间给出各能区以及能谱仪各道的计数率并存储之;在核动力堆现场测量时保留刻度峰区的计数率用于稳定γ能谱,而扣除该刻度峰区以外存储的计数率。Further, in step S01, the background peeling means that the scintillator detecting device containing the gamma source is placed in the low background chamber for a sufficiently long period of time to reduce the statistical error of the obtained count to a negligible degree, and the result is obtained. The count is divided by the measurement time to give the count rate of each energy zone and the energy spectrum meter and stored; when the nuclear power reactor is measured in the field, the count rate of the graduated peak region is reserved for stabilizing the gamma energy spectrum, and the scale peak region is deducted. The count rate stored outside.
进一步地,在步骤S02中,监测结果包括0.2-2.2MeV、2.2-4.5MeV、4.5-7.0MeV三个能区的计数率、16N特征峰的峰高计数率和对计数率积分所得的积分计数,以及三个能区的计数率、16N特征峰的峰高计数率和对计数率积分所得的积分计数随时间变化的曲线、能谱仪各道的计数率和对能谱仪各道的计数率积分所得的能谱。 Further, in step S02, the monitoring result includes a count rate of three energy zones of 0.2-2.2 MeV, 2.2-4.5 MeV, 4.5-7.0 MeV, a peak height count rate of the 16 N characteristic peak, and an integral of the count rate integral. Count, and the count rate of the three energy zones, the peak height count rate of the 16 N characteristic peak, and the integral count of the integral count of the count rate over time, the count rate of each spectrum spectrometer, and the energy spectrum meter The energy score obtained by the count rate integration.
进一步地,核动力堆蒸汽发生器泄漏出的16N的监测方法还包括根据0.2-2.2MeV能区的计数率将核动力堆蒸汽发生器泄漏的级别分为泄漏预警级、泄漏一级、泄漏二级的步骤。Further, the 16 N monitoring method leaked by the nuclear power reactor steam generator further comprises dividing the level of the nuclear power reactor steam generator leakage into a leakage warning level, a leakage level, and a leakage according to a counting rate of the 0.2-2.2 MeV energy region. The second step.
进一步地,在监测到核动力堆蒸汽发生器泄漏报警时,输出三个能区的计数率、16N特征峰的峰高计数率和对计数率积分所得的积分计数随时间变化的曲线,以及能谱仪各道的计数率在每隔设定时间T内积分所得的能谱。Further, when the nuclear power reactor steam generator leakage alarm is detected, the count rate of the three energy zones, the peak height count rate of the 16 N characteristic peak, and the integral count of the count rate integral over time are plotted, and The count rate of each channel of the spectrometer is integrated over the set time T to obtain the energy spectrum.
进一步地,设定时间T随泄漏级别的提高而缩短。Further, the set time T is shortened as the leak level is increased.
进一步地,监测结果实时显示并由存储器存储。Further, the monitoring results are displayed in real time and stored by the memory.
进一步地,16N特征峰是指γ射线能量分别为5.11MeV、5.62MeV和6.13MeV的能量峰。Further, the 16 N characteristic peak refers to an energy peak having gamma ray energies of 5.11 MeV, 5.62 MeV, and 6.13 MeV, respectively.
进一步地,核动力堆蒸汽发生器泄漏出的16N的监测方法还包括核动力堆蒸汽发生器泄漏仿真的步骤。Further, the 16 N monitoring method leaked by the nuclear power reactor steam generator also includes the steps of the nuclear power reactor steam generator leakage simulation.
进一步地,核动力堆蒸汽发生器泄漏仿真的步骤是指用16N刻度源照射内含γ源的闪烁体探测装置Ts时间N次,对N次测量得到的能谱进行平均后所得能谱的录像在K*Ts时间内进行放映,其中K为16N刻度源照射内含γ源的闪烁体探测装置在0.2-2.2MeV能区的计数率与核动力堆蒸汽发生器各泄漏级别在该能区的计数率的比值。Further, the step of simulating the leakage of the nuclear power reactor steam generator means that the scintillation detecting device Ts containing the γ source is irradiated with the 16 N scale source for N times, and the energy spectrum obtained by averaging the N measurements is obtained. The video is shown in K*Ts time, where K is the 16 N scale source and the gamma source-containing scintillator detection device is in the 0.2-2.2 MeV energy zone and the nuclear power reactor steam generator leakage level is in the energy. The ratio of the count rate of the zone.
进一步地,若K<1,对N次测量得到的能谱进行平均后所得能谱的录像在K*Ts时间内进行快放;若K>1,对N次测量得到的能谱进行平均后所得能谱的录像在K*Ts时间内进行慢放。Further, if K<1, the video of the energy spectrum obtained by averaging the N measurements is fast-released in K*Ts time; if K>1, the energy spectrum obtained by N measurements is averaged. The video of the obtained energy spectrum was slowed down in K*Ts time.
进一步地,内含γ源的闪烁体探测装置的闪烁体为LaBr3:Ce闪烁体。Further, the scintillator of the scintillator detecting device containing the γ source is a LaBr 3 :Ce scintillator.
进一步地,LaBr3:Ce闪烁体内含的天然放射性核素138La辐射的1.436MeVγ射线能量峰与K电子俘获辐射的0.037MeVχ射线能量峰符合相加为1.473MeV的能量峰为刻度峰。Further, the 1.436 MeV γ-ray energy peak of the natural radionuclide 138 La radiation contained in the LaBr 3 :Ce scintillation body and the 0.037 MeV X-ray energy peak of the K electron capture radiation are coincident with the energy peak added to 1.473 MeV.
进一步地,刻度峰区是指γ射线能量为1.434-1.497MeV的能量区间。Further, the scale peak region refers to an energy interval in which the gamma ray energy is 1.434 to 1.497 MeV.
进一步地,16N刻度源为238Pu-13C源。Further, the 16 N scale source is a 238 Pu- 13 C source.
本发明具有以下有益效果: The invention has the following beneficial effects:
使用内含γ源的闪烁体,避免了内嵌源等封装工艺操作给闪烁体带来不确定性因素,解决了监测系统灵敏度低,易出现误报警从而影响监测结果的技术问题。The use of the scintillator containing the gamma source avoids the uncertainty of the packaging process operation such as the embedded source, and solves the technical problem that the monitoring system has low sensitivity and is prone to false alarms and affects the monitoring result.
除了上面所描述的目的、特征和优点之外,本发明还有其它的目的、特征和优点。下面将参照图,对本发明作进一步详细的说明。In addition to the objects, features and advantages described above, the present invention has other objects, features and advantages. The invention will now be described in further detail with reference to the drawings.
附图说明DRAWINGS
构成本申请的一部分的附图用来提供对本发明的进一步理解,本发明的示意性实施例及其说明用于解释本发明,并不构成对本发明的不当限定。在附图中:The accompanying drawings, which are incorporated in the claims In the drawing:
图1是根据本发明的用于核动力堆蒸汽发生器泄漏出的16N的监测方法的步骤示意图;1 is a schematic diagram showing the steps of a 16 N monitoring method for a nuclear power reactor steam generator leaking according to the present invention;
图2是根据本发明的用于核动力堆蒸汽发生器泄漏出的16N的监测方法的用LaBr3:Ce探测装置测本底剥离前的示意图;FIG 2 is a monitoring method using LaBr 3 16 N leaking steam generator for nuclear reactor according to the present invention: Ce schematic front peeling detection means measuring the background;
图3是根据本发明的用于核动力堆蒸汽发生器泄漏出的16N的监测方法的用LaBr3:Ce探测装置测本底剥离后的示意图;FIG 3 is a monitoring method 16 N 3 of the steam generator leaks out by LaBr nuclear reactor according to the present invention: Ce view after peeling detection means measuring the background;
图4是根据本发明的用于核动力堆蒸汽发生器泄漏出的16N的监测方法的用LaBr3:Ce探测装置测16N刻度源50s能谱示意图;FIG 4 is a stack with monitoring method LaBr 3 16 N leaking out of the steam generator according to the present invention, nuclear: Ce detecting means 16 N measured calibration source 50s schematic spectrum;
图5是根据本发明的用于核动力堆蒸汽发生器泄漏出的16N的监测方法的用NaI(Tl)探测装置测16N刻度源50s能谱示意图;FIG 5 is (Tl) detection means 16 N measured calibration source 50s schematic stack with NaI spectrum monitoring method 16 N leaking out of the steam generator according to the present invention, nuclear power;
图6是根据本发明的用于核动力堆蒸汽发生器泄漏出的16N的监测方法的用LaBr3:Ce探测装置测16N刻度源1800s能谱示意图;以及 3 LaBr FIG 6 is a leak monitoring method according to the present invention nuclear reactor steam generator 16 N: Ce-detecting means 16 N measured calibration source spectrum schematic 1800s; and
图7是根据本发明的用于核动力堆蒸汽发生器泄漏出的16N的监测方法的用NaI(Tl)探测装置测16N刻度源1800s能谱示意图。FIG 7 is (Tl) detection means 16 N measured calibration source schematic 1800s spectrum stack monitoring method using NaI 16 N leaking out of the steam generator according to the present invention is nuclear.
具体实施方式detailed description
以下结合附图对本发明的实施例进行详细说明,但是本发明可以由权利要求限定和覆盖的多种不同方式实施。The embodiments of the present invention are described in detail below with reference to the accompanying drawings.
参见图1至图3,根据本发明的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,包括如下步骤:S01,将内含γ源的闪烁体探测装置在本底剥离后留下稳定γ能谱 的刻度峰,用于监测所述核动力堆蒸汽发生器泄漏出的16N并生成监测信号;S02,用信号处理机处理所述监测信号,并输出监测结果。使用内含γ源的闪烁体,避免了内嵌源等封装工艺操作给闪烁体带来不确定性因素,解决了监测系统灵敏度低,易出现误报警从而影响监测结果的技术问题。Referring to FIG. 1 to FIG. 3, a 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to the present invention includes the following steps: S01, the scintillator detecting device containing the γ source is left after the background peeling The scaled peak of the stable gamma energy spectrum is used to monitor the 16 N leaked by the nuclear power reactor steam generator and generate a monitoring signal; S02, the monitoring signal is processed by a signal processor, and the monitoring result is output. The use of the scintillator containing the gamma source avoids the uncertainty of the packaging process operation such as the embedded source, and solves the technical problem that the monitoring system has low sensitivity and is prone to false alarms and affects the monitoring result.
在步骤S01中,本底剥离是指把内含γ源的闪烁体探测装置置于低本底小室(如铅室)内测量足够长的时间使所得计数的统计误差降低到可以忽略的程度,将所得计数除以测量时间给出各能区以及能谱仪各道的计数率(本发明所指计数率均为净计数率)并存储之;在所述核动力堆现场测量时保留刻度峰区的计数率用于稳定γ能谱,而扣除该刻度峰区以外存储的计数率。在本实施例中优选LaBr3:Ce闪烁体探测装置为内含γ源的闪烁体探测装置,在其它实施例中还可选其它适合高能γ射线探测的内含γ源的闪烁体探测装置。进一步地,刻度峰是指LaBr3:Ce闪烁体内含的天然放射性核素138La辐射的1.436MeVγ射线能量峰与K电子俘获辐射的0.037MeVχ射线能量峰之和的1.473MeV能量峰,刻度峰区是指γ射线能量为1.434-1.497MeV的能量区间。In step S01, the background peeling refers to placing the scintillator detecting device containing the gamma source in a low background chamber (such as a lead chamber) for a sufficiently long time to reduce the statistical error of the obtained count to a negligible degree. Dividing the obtained count by the measurement time gives the energy rate of each energy zone and the energy meter (the count rate of the present invention is the net count rate) and stores it; retains the scale peak when the nuclear power reactor is measured in the field. The count rate of the zone is used to stabilize the gamma spectrum while deducting the count rate stored outside of the graduated peak region. In the present embodiment, the LaBr 3 :Ce scintillator detecting device is preferably a scintillator detecting device containing a γ source, and in other embodiments, other scintillator detecting devices containing a γ source suitable for high-energy gamma ray detection may be selected. Further, the scale peak refers to the 1.473 MeV energy peak of the sum of the 1.436 MeV γ-ray energy peak of the natural radionuclide 138 La radiation and the 0.037 MeV X-ray energy peak of the K electron trapping radiation contained in the LaBr 3 :Ce scintillation body, and the scale peak region is Refers to the energy range of gamma ray energy from 1.434 to 1.497 MeV.
现以内含γ源的LaBr3:Ce闪烁体探测装置为例来详细描述本底剥离:将内含γ源的LaBr3:Ce闪烁体探测装置置于铅室内测量48小时,将所得计数除以48*3600秒给出各能区以及能谱仪各道(总共4096道)的计数率Nb1、Nb2(单位:cps)并存储之;在现场测量时保留γ射线能量为1.434-1.497MeV的能量区间即能谱仪上道址区间为886-925道各道的计数率用于稳定γ能谱,而扣除该能量区间即道址区间以外存储的计数率(即将现场测量时获得的各能区以外及能谱仪各道的计数率减去之前在铅室内测量时获得的各能区但除1.434-1.497MeV能区以外以及能谱仪各道但除886-925道以外的计数率)。图2和图3分别表示用LaBr3:Ce探测装置测本底剥离前和剥离后(置于普通环境下)的能谱图。进行本底剥离后,用LaBr3:Ce闪烁体探测装置测量0.2-2.2MeV能区的本底计数率仅为10cps。但是,用NaI(Tl)闪烁体探测装置测量0.2-2.2MeV能区的本底计数率为186cps。Γ is to LaBr 3 containing source: Ce scintillator detecting means described in detail as an example background release: the contents of the source γ LaBr 3: Ce scintillator detection means disposed lead measuring chamber for 48 hours, the resulting count by 48*3600 seconds gives the count rate N b1 , N b2 (unit: cps) of each energy region and each spectrum spectrometer (4096 channels in total) and stores it; the gamma ray energy is 1.434-1.497 MeV when measured in the field. The energy interval is the count rate of each channel of the 886-925 channel on the energy spectrum meter for stabilizing the gamma energy spectrum, and subtracting the energy interval, that is, the count rate stored outside the channel interval (that is, each obtained in the field measurement) The count rate of the energy spectrum and the energy spectrum of each channel except the energy range of 1.434-1.497MeV and the energy spectrum of each channel except 886-925 ). Figures 2 and 3 show the energy spectra of the substrate before and after stripping (under normal conditions) using a LaBr 3 :Ce detector. After the background peeling, the background count rate of the 0.2-2.2 MeV energy region was measured by the LaBr 3 :Ce scintillator detection device to be only 10 cps. However, the background count of the 0.2-2.2 MeV energy region was measured by the NaI(Tl) scintillator detection device to be 186 cps.
在步骤S02中,监测结果包括0.2-2.2MeV、2.2-4.5MeV、4.5-7.0MeV三个能区的计数率、16N特征峰的峰高计数率和对这些计数率积分的积分计数,以及这三个能区的计数率、16N特征峰的峰高计数率和对这些计数率积分的积分计数随时间变化的曲线、能谱仪各道的计数率和对能谱仪各道的计数率积分所得的能谱。其中,在监测到核动力堆蒸汽发生器泄漏报警时,才输出上述三个能区的计数率、16N特征峰的峰高计数率和对这些计数率积分的积分计数随时间变化的曲线,以及能谱仪各道的计数率在每隔设定时间T内积分所得的能谱,进一步地,该设定时间T随泄漏级别的提高而 缩短。为便于查看和分析,将上述监测结果实时显示并交由存储器存储。进一步地,16N特征峰是指γ射线能量分别为5.11MeV、5.62MeV和6.13MeV的能量峰。In step S02, the monitoring result includes a count rate of three energy zones of 0.2-2.2 MeV, 2.2-4.5 MeV, 4.5-7.0 MeV, a peak height count rate of 16 N characteristic peaks, and an integral count of the integrals of these count rates, and The count rate of the three energy zones, the peak height count rate of the 16 N characteristic peaks, and the integral count of the integration counts of these count rates over time, the count rate of each spectrum spectrometer, and the count of each channel of the spectrometer The energy spectrum obtained by the rate integral. Wherein, when the nuclear power reactor steam generator leakage alarm is detected, the count rate of the above three energy zones, the peak height count rate of the 16 N characteristic peak, and the integral count of the integrated count of these count rate integrals are outputted, And the count rate of each of the spectrometers is integrated over the set time T, and further, the set time T is shortened as the leak level is increased. For easy viewing and analysis, the above monitoring results are displayed in real time and stored in memory. Further, the 16 N characteristic peak refers to an energy peak having gamma ray energies of 5.11 MeV, 5.62 MeV, and 6.13 MeV, respectively.
可选地,本发明方法除了S01、S02的步骤外,还包括根据0.2-2.2MeV能区的计数率将核动力堆蒸汽发生器泄漏的级别分为泄漏预警级、泄漏一级、泄漏二级的步骤,以及和/或核动力堆蒸汽发生器泄漏仿真的步骤。Optionally, in addition to the steps of S01 and S02, the method of the present invention further comprises dividing the level of leakage of the nuclear power reactor steam generator into a leakage warning level, a leakage level, and a leakage level according to a counting rate of a 0.2-2.2 MeV energy region. The steps, as well as the steps of the simulation of the nuclear power reactor steam generator leak.
当前通常划分核动力堆蒸汽发生器泄漏级别时,都采用两级泄漏级别。这两级的泄漏的级别阈值根据内嵌α源的NaI(Tl)闪烁体探测装置测量0.2-2.2MeV能区的计数率来取值:Ne=500cps(泄漏一级),Nc=8500cps(泄漏二级)。鉴于LaBr3:Ce闪烁体用于16N测量有很高的探测效率和能量分辨率以及本底剥离后的低本底计数率,能设置泄漏预警级的阈值Np=100cps,实现提前报警。实验表明,用LaBr3:Ce闪烁体探测装置测量16N刻度源在0.2-2.2MeV能区的计数率是NaI(Tl)的1.21倍(如表1所示),Two-stage leak levels are currently used when dividing the nuclear power reactor steam generator leakage levels. The threshold level of the leakage of these two stages is based on the count rate of the 0.2-2.2 MeV energy zone measured by the NaI(Tl) scintillator detection device embedded with the alpha source: Ne=500 cps (leakage level), Nc=8500 cps (leakage) Level 2). In view of LaBr 3: Ce scintillator 16 N measured for a high detection efficiency and energy resolution and low background count rate after the release of this bottom, the leakage can be provided early warning threshold level Np = 100cps, to achieve early warning. Experiments have shown that the count rate of the 16 N scale source in the energy range of 0.2-2.2 MeV is 1.21 times that of NaI(Tl) using the LaBr 3 :Ce scintillator detection device (as shown in Table 1).
表1是根据本发明的核动力堆蒸汽发生器泄漏出的16N的监测方法的用LaBr3:Ce和NaI(Tl)测16N刻度源1800s的计数率对比示意表
Figure PCTCN2015071668-appb-000001
Table 1 is a comparison chart of the counting rate of the 1800s of the 16 N scale source measured by LaBr 3 :Ce and NaI(Tl) using the 16 N monitoring method leaked by the nuclear power reactor steam generator according to the present invention.
Figure PCTCN2015071668-appb-000001
由此推算出用内含γ源的LaBr3:Ce闪烁体探测装置测量0.2-2.2MeV能区的计数率时,Np、Ne、Nc这三种泄漏级别阈值分别为121cps、605cps和10285cps(如表2所示)。From this, it is estimated that when the count rate of the 0.2-2.2 MeV energy region is measured by the LaBr 3 :Ce scintillator detecting device containing the γ source, the three leakage level thresholds of Np, Ne, and Nc are 121 cps, 605 cps, and 10285 cps, respectively. Table 2).
表2是根据本发明的核动力堆蒸汽发生器泄漏出的16N的监测方法的泄漏仿真数据表Table 2 is a leakage simulation data table of the 16 N monitoring method leaked by the nuclear power reactor steam generator according to the present invention.
Figure PCTCN2015071668-appb-000002
Figure PCTCN2015071668-appb-000002
因此,采用LaBr3:Ce闪烁体探测装置的泄漏预警级阈值是其本底计数率的12倍(121/10),有较高的可靠性;而采用NaI(Tl)闪烁体探测装置的泄漏预警级阈值是其本底计数率的0.54倍(100/186),不能设置泄漏预警级。Therefore, the leak warning level threshold of the LaBr 3 :Ce scintillator detection device is 12 times (121/10) of its background count rate, which has higher reliability; and the leakage of the NaI (Tl) scintillator detection device is adopted. The warning level threshold is 0.54 times (100/186) of its background count rate, and the leak warning level cannot be set.
图4和图5分别为用LaBr3:Ce和NaI(Tl)闪烁体探测装置测量16N刻度源50秒5次进行平均后的能谱(在线性坐标系的能谱图高能端放大显示是通用作法,本实施例放大100倍显示),根据4096道的能谱表明:因NaI(Tl)闪烁体的探测效率低和能量分辨率差,同样是50秒的积分计数,其不仅幅度低(6.13MeV能量峰低4.2倍,5.62MeV能量峰低2.3倍),而且涨落较大,只能看到一些发散的尖刺,看不到包络明晰的16N特征峰图像。优选地,16N刻度源为238Pu-13C源。Figure 4 and Figure 5 show the energy spectrum after averaging the 16 N scale source for 5 seconds using the LaBr 3 :Ce and NaI(Tl) scintillation detectors (the high-energy end of the energy spectrum of the linear coordinate system is shown) As a general method, this embodiment is magnified 100 times display), according to the energy spectrum of 4096 channels, it is shown that due to the low detection efficiency and poor energy resolution of the NaI(Tl) scintillator, it is also an integral count of 50 seconds, which is not only low in amplitude ( The 6.13 MeV energy peak is 4.2 times lower, the 5.62 MeV energy peak is 2.3 times lower, and the fluctuation is larger. Only some divergent spikes can be seen, and the well-defined 16 N characteristic peak image is not seen. Preferably, the 16 N scale source is a 238 Pu- 13 C source.
由于核动力堆蒸汽发生器发生泄漏的概率较低,例如有些核电站从投入运行起至今未发生一起蒸汽发生器的泄漏事故,为获得核动力堆蒸汽发生器泄漏的真实情况,预先知晓泄漏规律,为将来真正发生泄漏时提供依据,进行泄漏仿真非常必要。泄漏仿真是指先用16N刻度源照射内含γ源的闪烁体探测装置Ts时间N次,对N次测量得到的能谱进行平均后所得能谱的录像在K*Ts时间内进行放映,其中所述K为16N刻度源照射内含γ源的闪烁体探测装置在0.2-2.2MeV能区的计数率与核动力堆蒸汽发生器各泄漏级别在该能区的计数率的比值。进一步地,若K<1,对N次测量得到的能谱进行平均后所得能谱的录像在K*Ts时间内进行快放;若K>1,对N次测量得到的能谱进行平均后所得能谱的录像在K*Ts时间内进行慢放。Due to the low probability of leakage of the nuclear power reactor steam generator, for example, some nuclear power plants have not experienced a steam generator leakage accident since the start of operation. In order to obtain the true situation of the nuclear power reactor steam generator leakage, the leakage law is known in advance. To provide a basis for a real leak in the future, it is necessary to perform a leak simulation. Leakage simulation refers to the use of a 16 N scale source to illuminate the scintillator detection device Ts containing the γ source for N times, and the video of the energy spectrum obtained by averaging the N measurements is displayed in K*Ts time. The K is a 16 N scale source illuminating the ratio of the count rate of the scintillator detection device containing the gamma source in the energy range of 0.2-2.2 MeV to the count rate of each leak level of the nuclear power reactor steam generator in the energy region. Further, if K<1, the video of the energy spectrum obtained by averaging the N measurements is fast-released in K*Ts time; if K>1, the energy spectrum obtained by N measurements is averaged. The video of the obtained energy spectrum was slowed down in K*Ts time.
由表1的数据可知,在0.2-2.2MeV能区的计数率分别是Np、Ne、Nc这三种泄漏级别计数率的21.3、4.26和0.25倍(该数值与所用16N刻度源的活度有关)。因此,对图4和图5所有50s能谱的屏幕录像延长至1066s和213s慢放,可仿真蒸汽发生器泄漏预警级和泄漏一级的积分计数随时间的上升情况;同样对图4和图5所有50s能谱的屏幕录像缩短至12.5s快放,可仿真核动力堆蒸汽发生器泄漏二级的积分计数随时间的上升情况。同理,也可根据2.2-4.5MeV、4.5-7MeV、0-7MeV能区的计数率或者5.11MeV、5.62MeV和6.13MeV能量峰的峰高计数率来进行核动力堆蒸汽发生器的泄漏仿真,如表2所示。It can be seen from the data in Table 1 that the count rates in the energy range of 0.2-2.2 MeV are 21.3, 4.26, and 0.25 times of the three leak level count rates of Np, Ne, and Nc, respectively (this value and the activity of the 16 N scale source used). related). Therefore, the screen recording of all 50s spectrum of Figure 4 and Figure 5 is extended to 1066s and 213s slow release, which can simulate the rise of the steam generator leakage warning level and the leakage level of the integral count over time; also for Figure 4 and Figure 5 The screen recording of all 50s energy spectrum is shortened to 12.5s fast release, which can simulate the rise of the integral count of the nuclear power reactor steam generator leakage level over time. Similarly, the leakage simulation of the nuclear power reactor steam generator can be performed according to the counting rate of 2.2-4.5MeV, 4.5-7MeV, 0-7MeV energy region or the peak height counting rate of 5.11MeV, 5.62MeV and 6.13MeV energy peaks. ,As shown in table 2.
如图6、图7所示,用LaBr3:Ce和NaI(Tl)闪烁体探测装置测量16N刻度源1800s的能谱图(对数坐标),前者对16N特征峰的能谱显著优于后者。As shown in Fig. 6 and Fig. 7, the energy spectrum (logarithmic coordinates) of the 1800s of the 16 N scale source is measured by the LaBr 3 :Ce and NaI(Tl) scintillator detection device. The former has excellent energy spectrum for the 16 N characteristic peak. In the latter.
从以上的描述中,可以看出,本发明上述的实施例实现了如下技术效果:From the above description, it can be seen that the above-described embodiments of the present invention achieve the following technical effects:
本发明方法提供的LaBr3:Ce闪烁体用于16N测量比NaI(Tl)闪烁体有更高的探测效率和能量分辨率,经本底剥离处理后只留下1.473MeV能量峰作为刻度峰,在 0.2-2.2MeV和2.2-4.5MeV能区的本底计数率仅为内嵌α源NaI(Tl)闪烁体的5%和0.7%,能兼顾0.2-2.2MeV、2.2-4.5MeV、4.5-7.0MeV三个能区的计数率以及16N特征峰的峰高计数率变化。尤其是当发生泄漏报警后探测系统立即启动对这些计数率积分的积分计数功能,实时测定这三个能区各自的积分计数以及16N的特征峰随时间上升的情况,只需一两分钟就可将泄漏的真实状况形象的展示出来,真假报警极易分辨,不会出现误报警。鉴于所选闪烁体具有探测效率高以及进行本底剥离后其本底计数率低的优势,增加了将核动力堆蒸汽发生器的泄漏报警灵敏度提高了5倍的泄漏预警级。使用内含γ源的LaBr3:Ce闪烁体,避免了内嵌源等封装工艺操作给闪烁体带来不确定性因素从而影响监测结果等技术问题。The method of the present invention provides LaBr 3: Ce scintillator 16 N for measuring the ratio of NaI (Tl) scintillator with a higher detection efficiency and energy resolution, leaving only 1.473MeV energy peak after a background process scale peak release The background count rate in the energy range of 0.2-2.2 MeV and 2.2-4.5 MeV is only 5% and 0.7% of the embedded α-source NaI(Tl) scintillator, which can balance 0.2-2.2 MeV, 2.2-4.5 MeV, 4.5. The count rate of the three energy regions of -7.0 MeV and the peak height count rate of the 16 N characteristic peak. Especially when the leak alarm occurs, the detection system immediately starts the integral counting function for integrating these counting rates, and measures the integral count of each of the three energy zones and the characteristic peak of 16 N as time rises in time, only one or two minutes. The real image of the leak can be displayed, and the true and false alarms are easy to distinguish and there will be no false alarms. In view of the fact that the selected scintillator has the advantages of high detection efficiency and low background count rate after background stripping, the leakage warning level which increases the leakage alarm sensitivity of the nuclear power reactor steam generator by 5 times is increased. The use of the LaBr 3 :Ce scintillator containing the γ source avoids the technical problems such as the inconsistency of the encapsulation process by the embedded source and the like, which affects the monitoring result.
以上所述仅为本发明的优选实施例而已,并不用于限制本发明,对于本领域的技术人员来说,本发明可以有各种更改和变化。凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。 The above description is only the preferred embodiment of the present invention, and is not intended to limit the present invention, and various modifications and changes can be made to the present invention. Any modifications, equivalent substitutions, improvements, etc. made within the spirit and scope of the present invention are intended to be included within the scope of the present invention.

Claims (15)

  1. 一种用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,包括如下步骤:A 16 N monitoring method for leakage from a nuclear power reactor steam generator, comprising the steps of:
    S01,将内含γ源的闪烁体探测装置在本底剥离后保留稳定γ能谱的刻度峰,用于监测所述核动力堆蒸汽发生器泄漏出的16N并生成监测信号;S01, the scintillator detecting device containing the gamma source retains a stable peak of the stable gamma spectrum after the background is stripped, and is used for monitoring the 16 N leaked by the nuclear power reactor steam generator and generating a monitoring signal;
    S02,用信号处理机处理所述监测信号,并输出监测结果。S02: The monitoring signal is processed by a signal processor, and the monitoring result is output.
  2. 根据权利要求1所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,在步骤S01中,所述本底剥离是指把所述内含γ源的闪烁体探测装置置于低本底小室内测量足够长的时间使所得计数的统计误差降低到可以忽略的程度,将所得计数除以测量时间给出各能区以及能谱仪各道的计数率并存储之;在所述核动力堆现场测量时保留刻度峰区的计数率用于稳定γ能谱,而扣除该刻度峰区以外存储的计数率。The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to claim 1, wherein in the step S01, the background peeling refers to the scintillating body containing the γ source. The detection device is placed in the low background chamber for a sufficient period of time to reduce the statistical error of the obtained count to a negligible degree, and the obtained count is divided by the measurement time to give the count rate of each energy region and the energy spectrum meter and store The count rate of the scale peak region is retained during the on-site measurement of the nuclear power reactor for stabilizing the gamma energy spectrum, and the count rate stored outside the scale peak region is subtracted.
  3. 根据权利要求1所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,A 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to claim 1, wherein
    在步骤S02中,所述监测结果包括0.2-2.2MeV、2.2-4.5MeV、4.5-7.0MeV三个能区的计数率、16N特征峰的峰高计数率和对所述计数率积分所得的积分计数,以及所述三个能区的计数率、16N特征峰的峰高计数率和对所述计数率积分所得的积分计数随时间变化的曲线、能谱仪各道的计数率和对能谱仪各道的计数率积分所得的能谱。In step S02, the monitoring result includes a count rate of three energy regions of 0.2-2.2 MeV, 2.2-4.5 MeV, 4.5-7.0 MeV, a peak height count rate of a 16 N characteristic peak, and an integral of the count rate. The integral count, and the count rate of the three energy zones, the peak height count rate of the 16 N characteristic peak, and the curve of the integral count obtained by integrating the count rate with time, the count rate of each channel of the spectrometer, and the pair The energy spectrum obtained by integrating the count rate of each spectrum spectrometer.
  4. 根据权利要求1至3任一所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,还包括根据0.2-2.2MeV能区的计数率将核动力堆蒸汽发生器泄漏的级别分为泄漏预警级、泄漏一级、泄漏二级的步骤。The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to any one of claims 1 to 3, characterized in that it further comprises generating nuclear power reactor steam according to a counting rate of a 0.2-2.2 MeV energy region. The level of leakage is divided into the steps of leakage warning level, leakage level, and leakage level.
  5. 根据权利要求3所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,在监测到所述核动力堆蒸汽发生器泄漏报警时,输出所述三个能区的计数率、16N特征峰的峰高计数率和对所述计数率积分所得的积分计数随时间变化的曲线,以及能谱仪各道的计数率在每隔设定时间T内积分所得的能谱。The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to claim 3, wherein the three energy zones are outputted when the nuclear power reactor steam generator leakage alarm is detected The count rate, the peak height count rate of the 16 N characteristic peak, and the curve of the integral count obtained by integrating the count rate over time, and the count rate of each track of the spectrometer are integrated every set time T Energy spectrum.
  6. 根据权利要求5所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,所述设定时间T随泄漏级别的提高而缩短。 The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to claim 5, wherein the set time T is shortened as the leakage level is increased.
  7. 根据权利要求1至3任一所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,所述监测结果实时显示并由存储器存储。The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to any one of claims 1 to 3, characterized in that the monitoring result is displayed in real time and stored by a memory.
  8. 根据权利要求3或5所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,所述16N特征峰是指γ射线能量分别为5.11MeV、5.62MeV和6.13MeV的能量峰。The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to claim 3 or 5, wherein the 16 N characteristic peak means that the gamma ray energy is 5.11 MeV, 5.62 MeV and 6.13, respectively. The energy peak of MeV.
  9. 根据权利要求8所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,还包括核动力堆蒸汽发生器泄漏仿真的步骤。The 16 N monitoring method for a nuclear power reactor steam generator leak according to claim 8, further comprising the step of simulating the nuclear power reactor steam generator leakage simulation.
  10. 根据权利要求9所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,所述核动力堆蒸汽发生器泄漏仿真的步骤是指用16N刻度源照射内含γ源的闪烁体探测装置Ts时间N次,对N次测量得到的能谱进行平均后所得能谱的录像在K*Ts时间内进行放映,其中所述K为16N刻度源照射内含γ源的闪烁体探测装置在0.2-2.2MeV能区的计数率与核动力堆蒸汽发生器各泄漏级别在该能区的计数率的比值。The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to claim 9, wherein the step of simulating the nuclear power reactor steam generator leakage means that the 16 N scale source is irradiated with the content The gamma source scintillator detecting device Ts takes N times, and the video of the energy spectrum obtained by averaging the N measurements is displayed in K*Ts time, wherein the K is a 16 N scale source illuminating γ The ratio of the count rate of the source scintillator detection device in the 0.2-2.2 MeV energy region to the count rate of each leakage level of the nuclear power reactor steam generator in the energy region.
  11. 根据权利要求10所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,若K<1,对N次测量得到的能谱进行平均后所得能谱的录像在K*Ts时间内进行快放;若K>1,对N次测量得到的能谱进行平均后所得能谱的录像在K*Ts时间内进行慢放。The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to claim 10, wherein if K < 1, the average energy spectrum obtained by averaging the N measurements is recorded. The K*Ts time is fast-release; if K>1, the spectrum of the energy spectrum obtained by averaging the N measurements is slowed down in K*Ts time.
  12. 根据权利要求1、2或10任一所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,所述内含γ源的闪烁体探测装置的闪烁体为LaBr3:Ce闪烁体。The 16 N monitoring method for leakage from a nuclear power reactor steam generator according to any one of claims 1, 2 or 10, wherein the scintillator of the gamma source-containing scintillator detecting device is LaBr 3 : Ce scintillator.
  13. 根据权利要求12所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,所述LaBr3:Ce闪烁体内含的天然放射性核素138La辐射的1.436MeVγ射线能量峰与K电子俘获辐射的0.037MeVχ射线能量峰符合相加为1.473MeV的能量峰为刻度峰。The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to claim 12, wherein the LaBr 3 :Ce scintillation body contains 1.436 MeV γ ray energy of the natural radionuclide 138 La radiation. The 0.037 MeV X-ray energy peak of the peak and K electron trapping radiation is equal to the energy peak added to 1.473 MeV as the scale peak.
  14. 根据权利要求2所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,所述刻度峰区是指γ射线能量为1.434-1.497MeV的能量区间。The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to claim 2, wherein the scale peak region refers to an energy interval in which the gamma ray energy is 1.434 - 1.497 MeV.
  15. 根据权利要求10所述的用于核动力堆蒸汽发生器泄漏出的16N的监测方法,其特征在于,所述16N刻度源为238Pu-13C源。 The 16 N monitoring method for leaking out of a nuclear power reactor steam generator according to claim 10, wherein the 16 N scale source is a 238 Pu- 13 C source.
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