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为了满足热功率为10μW水平的仅和β放射源活度校准需要,研制了1台活度微量热计测量装置。该装置采用半导体测温元件组合(Bi2Te3+Sb2Te3p型与Bi2Te3+Bi2Se3n型)作为测温元件,采用等温双杯量热计的技术原理和使用计算机软件根据测温信号的极性用电功率在空白测量杯上进行自动补偿确定放射源的热功率。 相似文献
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为了满足热功率为10μW水平的α和β放射源活度校准需要,研制了1台等温双杯活度微量热计测量装置。该装置采用半导体测温元件组合(Bi2Te3+Sb2Te3p型与Bi2Te3+Bi2Se3n型)作为测温元件、采用等温双杯量热计的技术原理和使用计算机软件根据测温信号的极性用电功率在空白测量杯上进行自动补偿确定放射源的热功率。 相似文献
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微量热计测量低活度氚 总被引:1,自引:1,他引:0
针对国际热核聚变实验堆氚增殖系统(ITER-TBS)中微量氚活度的绝对测量需求,设计研制了微量热计。采用固体含氚样品对微量热计的输出热电势(Eout)-输入热功率(P)进行标定,Eout-P关系式具有很好的线性关系,灵敏度系数达到0.13V/W。研制的微量热计最低检测限低于0.2μW,量热杯体积大于500mL,该性能指标预期可定量测量ITER-TBS系统中各种复杂形态的微量氚活度,具有很好的应用前景。 相似文献
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为实现医用同位素核纯度和放射性活度的准确测量,本工作根据量热法测量原理设计一套微量热装置,包括量热系统、温控系统以及测控软件,并对装置的性能进行测试和实验验证。结果表明,同位素量热计的基线电势稳定,复现性良好。最低探测限可至3.1 μW,能够实现医用同位素放射性活度测量的全覆盖。在10 μW~1 mW的测量范围内,当输入热功率<100 μW时,单次测量结果与输入热功率标准值之间的最大偏差<1.5%;当输入功率>100 μW时,测量结果和输入热功率偏差<0.5%。利用该装置成功实现了医用同位素14C样品的活度测量,测量结果与标准值在不确定度范围内相吻合,不产生放射性废物和化学废物,不破坏样品,操作简单方便。后期可通过研究测量预热和保温装置,进一步提高装置的适应能力和探测下限。 相似文献
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裂变热电偶是一种能在强γ辐射环境下测量中子的快响应小型化探测器。本文从理论上估算了裂变热电偶的时间响应,好于1μs,并通过热阶跃响应实验验证了理论计算, 相似文献
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压水反应堆堆内温度测量装置是监测反应堆热功率输出及堆内功率分布情况、保证反应堆安全运行的手段之一。该装置以热电偶作为测量元件,用不锈钢作保护外套。由于热电偶有一定的使用寿命,须定期更换,为此研制了一种适用于核电厂反应堆堆内温度测量的热电偶密封结构。这种结构既能在高温高压下密封牢靠,没有泄漏和渗漏,又能在带放射性环境下方便地逐根更换热电偶。它是一种结构简单实用的新型密封结构。 相似文献
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Amir Zacarias Mesquita Hugo Cesar RezendeRose Mary Gomes do Prado Souza 《Progress in Nuclear Energy》2011,53(8):1197-1203
Since the first nuclear reactor was built, a number of methodological variations have been evolved for the calibration of the reactor thermal power. Power monitoring of reactors is done by means of neutronic instruments, but its calibration is always done by thermal procedures. The purpose of this paper is to present the results of the thermal power calibration carried out on March 5th, 2009 in the IPR-R TRIGA reactor. It was used two procedures: the calorimetric and heat balance methods. The calorimetric procedure was done with the reactor operating at a constant power, with primary cooling system switched off. The rate of temperature rise of the water was recorded. The reactor power is calculated as a function of the temperature-rise rate and the system heat capacity constant. The heat balance procedure consists in the steady-state energy balance of the primary cooling loop of the reactor. For this balance, the inlet and outlet temperatures and the water flow in the primary cooling loop were measured. The heat transferred through the primary loop was added to the heat leakage from the reactor pool. The calorimetric method calibration presented a large uncertainty. The main source of error was the determination of the heat content of the system, due to a large uncertainty in the volume of the water in the system and a lack of homogenization of the water temperature. The heat balance calibration in the primary loop is the standard procedure for calibrating the power of the IPR-R1 TRIGA nuclear reactor. 相似文献
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《Progress in Nuclear Energy》2012,54(8):1197-1203
Since the first nuclear reactor was built, a number of methodological variations have been evolved for the calibration of the reactor thermal power. Power monitoring of reactors is done by means of neutronic instruments, but its calibration is always done by thermal procedures. The purpose of this paper is to present the results of the thermal power calibration carried out on March 5th, 2009 in the IPR-R TRIGA reactor. It was used two procedures: the calorimetric and heat balance methods. The calorimetric procedure was done with the reactor operating at a constant power, with primary cooling system switched off. The rate of temperature rise of the water was recorded. The reactor power is calculated as a function of the temperature-rise rate and the system heat capacity constant. The heat balance procedure consists in the steady-state energy balance of the primary cooling loop of the reactor. For this balance, the inlet and outlet temperatures and the water flow in the primary cooling loop were measured. The heat transferred through the primary loop was added to the heat leakage from the reactor pool. The calorimetric method calibration presented a large uncertainty. The main source of error was the determination of the heat content of the system, due to a large uncertainty in the volume of the water in the system and a lack of homogenization of the water temperature. The heat balance calibration in the primary loop is the standard procedure for calibrating the power of the IPR-R1 TRIGA nuclear reactor. 相似文献
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《Journal of Nuclear Science and Technology》2013,50(6):611-616
A prototype dielectric microcalorimeter was fabricated from 0.99SrTiO3-0.01SrTa2O6, a dielectric material. To estimate the operation performance of the microcalorimeter, a simple evaluation model is introduced by employing the block diagram formalism. Pulse height and fall time constant of the detection signal are analyzed as a function of the thermal conductance of the heat link. The dielectric microcalorimeter maintained at 100mK was irradiated by 5.5 MeV α-particles emitting from an 241Am source. Responsivity was found to be 2.7x10?19C/eV. 相似文献
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Shouqi XIONG 《等离子体科学和技术》2022,24(10):105601
The accurate power measurement is important for an ECRH system in tokamak. The dummy load is designed and developed for the measurement of the millimeter wave power. This work analyzes the dummy load based on the quasi-optical method and the ray tracing method. The reflectivity and thermal deposition of the dummy load have been considered to ensure the safety of the entire system. High-power tests have been carried out at a 105 GHz/500 kW ECRH system. The results of the tests indicate that the designed dummy load is stable and valid. 相似文献
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《Journal of Nuclear Science and Technology》2013,50(12):905-912
In the nuclear power calibration process of JOYO, the first experimental fast breeder reactor in Japan, the indication of the Intermediate Range Monitoring System (IRMS), employing Average Magnitude type Campbelling System (AMCS), was calibrated with the reactor power at 45.82 kW. The reactor power was then decreased and the nonlinear indication lowering of the IRMS was observed. In this paper, we present a derivation of an equation representing the AMCS characteristic and show that the indication lowering occurs when the product of mean arrival rate of pulses and their width is small. The computed values based on the derived equation agreed very well with the observed ones in the JOYO IRMS below 45.82 kW, and it was confirmed that the evaluation method was applicable. Furthermore, it was evident from the evaluation that the indication lowering of the JOYO IRMS above 45.82 kW was negligibly small, and did not affect the reactor power ascension testing. Also, it was proved in a following thermal calibration test above 50 kW that the indication lowering was allowably small indeed in this power region. 相似文献
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《核技术(英文版)》2016,(5):125-130
To obtain multiple monoenergetic neutron sources and realize the on-site calibration of radiation monitoring equipment for nuclear-involved places,the structural characteristics and neutron source features of D-T neutron tube were analyzed;Monte Carlo method was adopted to simulate the effect of interaction between typical materials and different energy neutrons;multilayered shielding materials were combined and optimized to acquire the optimal scheme to shield the neutron sources from the neutron tube.On the base,a tapered alignment filtration construction was designed and Monte Carlo method was employed to simulate the effect of alignment construction.The result showed that the tapered alignment filtration construction can create monoenergetic neutrons including14.1 MeV,0.18 MeV and thermal neutrons and demonstrated good monochrome performance which provides multiple monoenergetic sources for the on-site calibration. 相似文献