共查询到19条相似文献,搜索用时 187 毫秒
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本文讨论了放射免疫分析法和免疫放射分析法及受体结合分析法的在线和离线数据处理问题。文章认为,放射免疫分析法的数据处理发展较快,其中四参数和五参数Logitic法及四参数单位点质量作用模型较为理想。模型中较合理地考虑了非特异性结合,且适合于不对称的免疫放射分析法的曲线。用放射配基测定受体的技术及其数据处理的方法发展很快,业已证明用目前最常用的Scatchard法处理数据并不理想。尤其当放射配基与受体的亲和力很高时,Clark模型的应用受到很大的限制,而用最小二乘法拟合Clark模型的改进型能得到满意的结果。 相似文献
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锶在土壤中的吸附动力学 总被引:2,自引:0,他引:2
用动态法测定了锶在核废物处置预选场址土壤中的平衡吸附容量,研究了水相pH值、流速、土壤粒度和锶溶液的初始质量浓度对土壤吸附锶的影响。水相pH值、流速、溶液的初始质量浓度越大,土壤平衡吸附容量越大;土壤粒度越小,土壤平衡吸附容量越大。用常用的吸附动力学方程对实验数据进行了拟合,并对吸附机理进行了探讨。实验结果表明,该放射性废物处置预选场址土壤对锶的最大吸附率为48.8%,吸附性能较差。 相似文献
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应用MATLAB对开环式氡析出率测量过程中不同抽气流率下集氡罩内氡浓度随时间的变化规律进行模拟计算,并用实验对计算结果进行了验证。结果表明,在氡析出率测量时保持集氡罩参数不变的情况下,随着抽气流率的增大,集氡罩内平衡氡浓度值减小,达到平衡氡浓度的时间也缩短。实验表明,集氡罩内的平衡氡浓度的减小可最大限度地减小泄露与反扩散的影响;抽气流率的变大使集氡罩内达到平衡氡浓度时间缩短以及集氡罩内的充气均匀性愈好。通过本次实验,获得的抽气流率为1.94-3.0 L·min~(-1),集氡罩底面积为299 cm~2,体积为1.79×10~(-3)m~3。 相似文献
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利用介质阻挡放电低温等离子体技术对甲基红模拟染料废水进行降解研究,降解反应在同心管式反应器中进行。考察了放电功率、溶液初始浓度、初始pH、处理时间、气氛条件等单因素的改变对甲基红降解效果的影响,通过测定甲基红521 nm处的吸光度值、溶液pH及颜色变化,分析了甲基红降解历程,并推测了降解机理。研究结果表明:在本实验中,溶液在115 W低放电功率下的处理效果更好,由于处理效果受温度、湿度等影响,放电功率与处理效果间并不呈正相关关系;溶液的初始浓度越高,达到同样的降解效果所需的时间越长;相同条件下,模拟废水的初始pH越低,其处理后的降解效果越好,即酸性条件下更有利于甲基红断键降解。 相似文献
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生长抑素-葡聚糖的99Tcm标记及体外结合分析 总被引:2,自引:2,他引:2
采用还原氨化方法,将天然生长抑素(SMS)与葡聚糖(Dx20)偶联,并以125I-奥曲肽(125I-Tyr3-Octreotide)为放射配基,进行受体竞争结合实验,测定了SMS-Dx50的IC50;以SnCl2为还原剂对SMS-Dx50进行99Tcm标记,并进行99Tcm- SMS-Dx50受体结合分析,考察其对生长抑素受体的亲合能力。结果表明:SMS-Dx50保持了对SMS 2型受体的高亲和力;其IC50与奥曲肽的IC50(0.79 nmol/L)相近,为5.95 nmol/L;99Tcm- SMS-Dx50标记率>85%, 经PD-10柱分离纯化,其放化纯度>98%;99Tcm- SMS-Dx50对生长抑素2型受体特异性结合为25%~40%,保持了较高的亲和力;SMS-Dx50适合于99Tcm标记,可用于生长抑素受体阳性肿瘤诊断的进一步研究 相似文献
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A study on the influence of void fraction change on plutonium and minor actinides recycling in standard boiling water reactor (BWR) with equilibrium burnup model has been conducted. We considered the equilibrium burnup model since it is a simple time independent burnup method that can handle all possible produced nuclides in any nuclear system.
The uranium enrichment for the criticality of the reactor diminishes significantly for the plutonium and minor actinides recycling case compared to that of the once-through cycle of BWR case. This parameter decreases much lower with the increasing of the void fraction. A similar propensity was also shown in the required natural uranium per annum. The annual required natural uranium was calculated by assuming that the uranium concentration in the tail of the enrichment plant is 0.25 w%. The amount of loaded fuel reduces slightly with the increment of the void fraction for plutonium and minor recycling in BWR. 相似文献
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Lanfranco Monti Ehud Greenspan Marco Sumini Massimiliano Fratoni Ki-Bog Lee Federico Rocchi 《Progress in Nuclear Energy》2008,50(2-6):262-268
This work investigates the effect of initial fuel composition, power density and number of recycles on the pitch-to-diameter (P/D) ratio and TRans-Uranium isotopes (TRU) loading required for attaining one of the most important design goals of the Encapsulated Nuclear Heat Source (ENHS) – nearly zero burnup reactivity swing over the 20 years of core life. It is found that the required P/D ratio is sensitive to, primarily, the initial concentration of the short-lived isotope 241Pu in the fuel loaded into the first core and to the core power density. The longer is the cooling time of the TRU from LWR spent fuel the smaller becomes the relative 241Pu concentration and the smaller becomes the fraction of 241Pu lost via radioactive decay and, hence, the smaller needs be the conversion ratio required for nearly zero burnup reactivity swing and the larger can be the P/D ratio. Likewise, the higher is the ENHS power density, the smaller becomes the fraction of 241Pu lost via radioactive decay and the larger becomes the P/D required for the first core. The optimal P/D ratio tends to increase with the number of times the fuel is recycled from one ENHS core to the next one. The optimal P/D ratio for the equilibrium composition core is in between 1.53 and 1.59. For a given discharge burnup it tends to somewhat increase with the equilibrium core power density. However, if structural materials will be developed to enable a 20 years core life at elevated power densities, the higher the power density the smaller is the required equilibrium P/D ratio. 相似文献
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4A沸石对Sr2+的吸附性能的研究 总被引:4,自引:0,他引:4
采用间歇法研究在不同环境条件下(浓度、pH值、介质、温度),4A沸石(简称四)对Sr^2+的吸附性能影响。结果表明:ZF对Sr^2+的吸附性能比较好,当Sr^2+浓度为0.05mol/L时,ZF对Sr^2+的吸附平衡时间约在14天左右,平衡吸附量为526mg/g。Sr^2+的浓度对ZF的吸附性能影响比较大,其次是溶液的pH值、介质和溶液的温度。ZF对Sr^2+的平衡吸附量随Sr^2+浓度的升高而增大,但平衡吸附率和平衡吸附比随着浓度的增大而降低。pH值增大时ZF对Sr^2+的吸附性能加强。介质溶液含种类、浓度不同的离子时,相对于去离子水介质,ZF对Sr^2+吸附性能有程度不同的下降;但腐殖酸的存在可以削弱这种影响。温度升高时,ZF对Sr^2+吸附性能降低。 相似文献
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The objective of this study is to demonstrate the feasibility of the Kim’s delayed hydride cracking (DHC) model. To this end, this study has investigated the velocity and incubation time of delayed hydride cracking (DHC) for the water-quenched and furnace-cooled Zr-2.5Nb tubes with a different radius of notch tip. DHC tests were carried out at constant KI of 20 MPa √m on cantilever beam (CB) specimens subjected to furnace cooling or water quenching after electrolytic charging with hydrogen. An acoustic emission sensor was used to detect the incubation time taken before the start of DHC. The shape of the notch tip changed from fatigue cracks to smooth cracks with its tip radius ranging from 0.1 to 0.15 mm. The DHC incubation time increased remarkably with the increased radius of the notch tip, which appeared more strikingly on the furnace-cooled CB specimens than on the water-quenched ones. However, both furnace-cooled and water-quenched CB specimens indicated little change in DHC velocity with the radius of the notch tip unless their notch tip exceeded 0.125 mm. These results demonstrate that the nucleation rate of hydrides at the notch tip determines the incubation time and the DHC velocity becomes constant after the concentration of hydrogen at the notch tip reaches terminal solid solubility for dissolution (TSSD), which agrees well with the Kim’s DHC model. A difference in the incubation time and the DHC velocity between the furnace-cooled and water-quenched specimens is attributed to the nucleation rate of reoriented hydrides at the notch tip and the resulting concentration gradient of hydrogen between the notch tip and the bulk region. 相似文献
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This paper reports the observed changes for equilibrium factors between 226Ra and 222Rn with sealing time of the samples. The samples include soil, raw coal, mineral water, cement, rock, etc. Especially the conceptions of "pre-equilibrium time" and "pre-equilibrium factor" have been put forward and methods of measuring and processing data have been given which can be used for rapidly reporting activity of 226Ra in samples with unknown equilibrium factor. It is definitely concluded that, using methods given in the paper, a test report will be completed in 3~7days, instead of one month, after receiving the sample whose activity is not lower than LLD of the spectrometer. 相似文献
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J.R. Coleman 《Nuclear Engineering and Design》2010,240(5):1028-1032
The multiple recycling of uranium in light-water reactors is evaluated to understand its sustainability in multiple recycling scenarios and to evaluate its impact on fuel design and the fuel cycle. Two recycling scenarios were evaluated. One involves the mixing of repU with natU prior to reenrichment. A second involves the mixing of repU with 19.9% EU to provide the new reactor fuel. The equilibrium concentrations of troublesome isotopes such as U-232 and U-236 are evaluated along with the required overenrichment of U-235. It was confirmed that a U-235 overenrichment factor of 0.28 applied to the U-236 concentration is sufficient to meet the cycle reactivity requirements and yields equilibrium enrichments of 5.06% and 5.52% for the two cycles, respectively. The impact on plutonium production and cycle reactivity is further evaluated to ensure the new fuel can meet the desired burnup requirements. Here, the plutonium production was found to be greater and the reactivity swing less in recycling scenarios with higher U-236 concentration. 相似文献
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In the present work, growth of cesium iodide aerosols in a mixture of steam and air (non-condensable) is investigated. The condensation rates are calculated including the Kelvin and solute effects. Particle growth to its equilibrium size, with and without energy conservation, is calculated for a range of particle size, temperature and surrounding relative humidity. The time required for the particles to grow to their equilibrium sizes is reported. Finally, the effect of particle growth on the removal of cesium iodide aerosols by gravitational sedimentation is presented. 相似文献
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高压直流电源是电离室等核辐射探测器的关键部件。针对需要3 kV左右高压的电离室,本文研制了0~3 kV连续可调的低噪声、高效率、小体积及高稳定性的高压直流电源。该高压直流电源系统采用线性与开关混合模式设计,兼顾了转换效率与低噪声。核心部分升压转换部分采用线性罗耶谐振电路与高频变压器实现,保证足够低的高压电源输出纹波。罗耶谐振电路的供电电源则由边沿时间控制型超低噪声开关稳压器LT1534提供,从而实现了混合模式高压直流电源的设计。高压直流电源输出部分采用二阶RC滤波电路进一步降低了输出电压的纹波。实测输出电压范围为0~3 kV,静态功耗为0.4 W,3 kV输出时纹波为16.55 mV,由此可知该电源可用于低噪声的核辐射探测器供电场合。 相似文献