三氧化铀-三氧化钍系烧结三氧化铀-三氧化钍系烧结体研究(第1报)

敏之 佐多, 雷作 清浦
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引用次数: 1

摘要

已知铀-钍体系的化学计量组成形成一系列连续的固溶体,作为核陶瓷燃料,其性能仅在氧化电阻性、耐火性和钍作为繁殖材料的实用性方面优于铀。该系统中富钍部分的烧结体从1956- 1957年开始在美国阿贡国家实验室进行了研究,并进行了反应堆试验,即将应用于动力堆的燃料材料。作者已经发表了该体系富铀部分的抗氧化性和烧结结果。本文研究了它们在空气中的烧结和化学计量成分的还原。原料是由铀和钍的混合硝酸溶液中加入氨溶液,在空气中烧制得到的重铀酸铵和氢氧化钍共沉淀混合物的产物。在混合硝酸盐溶液中加入氢氧化铵后pH值的变化如图1所示,用热重天平对共沉淀物在空气中的煅烧过程进行了跟踪,结果如图2所示。煅烧粉末在800℃空气中2小时的密度和Blain值。进行了测量,并进行了x射线衍射测试。由图3可知,由于在U3O8和固溶体的混合相中阻碍了晶体的生长,含10-30% ThO2的粉末的晶粒尺寸非常小。随着钍的加入,铀中U3O8相的含量降低,萤石型固溶体的含量增加。U3O8相在含钍量大于60%的组合物中消失,仅形成固溶体。将在800℃空气中煅烧的粉末以3吨/cm2的速度压成直径约10mm的球团,在空气中烧结,用CO气体还原。结果如图4所示,含10%、20%和30%钍的压块在1400℃下烧结良好,含50%钍的压块在1500℃下烧结良好。烧结温度越高,CO气体将烧结球团还原为化学计量成分的效果越理想,但含th2低于10%的试样出现了裂纹,如表1所示。由于煅烧后的粉末中含有30%的ThO2,由于粉末太细而无法压制,因此尝试将煅烧温度提高到1000℃。这些样品在1000℃煅烧时烧结效果良好(表2)。相反,含有50% ThO2的粉末在1400℃很难烧结,但使用600℃煅烧的粉末可以烧结(表3)。富铀样品在空气中烧结时,铀组分的挥发存在一些缺陷,并伴有还原步骤的较大尺寸变化。因此,在中性气氛下烧结,然后在1300°-1400°C进行氢还原。这些烧结性能在氮气气氛和二氧化碳气氛中没有明显的差异,并证实了化学计量成分为70-30和50-50的样品在1400℃烧结时可以获得良好的结果。烧结过程将在下面的文章中报道。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
酸化ウラン-酸化トリウム系の焼結酸化ウラン-酸化トリウム系焼結体の研究 (第1報)
It is known that stoichiometric compositions of the urania-thoria system form a series of continuous solid solutions having some better properties as a nuclear ceramic fuel than urania only in oxidation resistivity, refractoriness, and usefulness of thoria as breeding materials. The sintered bodies of thoria-rich portion in the system have been studied since 1956-7 in Argonne National Laboratory, and subjected to the reactor tests, and going to be applied to fuel materials of power reactor.The authors have already published the results on the oxidation resistance and the sintering of the urania-rich portion of this system. This paper is concerned with their sinterings in air and reductions to stoichiometric compositions.The starting materials were the products of firing in air the coprecipitated mixtures of ammonium diuranate and thorium hydroxide obtained from mixed nitrate solutions of uranium and thorium by adding ammonia solution. The variation of pH by adding ammonium hydroxide to the mixed nitrate solution is shown in Fig. 1, and the calcination processes of the coprecipitates in air were traced by means of the thermogravimetric balance, with the results as given in Fig. 2. The tapped densities and Blain values of the calcinated powders in air at 800°C for 2 hrs. were measured, and also subjected to X-ray diffraction test. The results shown in Fig. 3 indicate that the grain size of he powders of containing 10-30% ThO2 are very small because of the hindrance of the crystal growth in the mixed phase of U3O8 and solid solution. The content of U3O8 phase has decreased and that of solid solution of fluorite type has increased as thorias were added to urania. U3O8 phase has disappered in the compositions containing thoria more than 60 weight%, forming only the solid solutions.The powders calcinated in air at 800°C were pressed at 3tons/cm2 to pellets of about 10mm in diameter, and sintered in air and reduced by CO gas. The results are given in Fig. 4 which show that the compacts containing 10, 20, and 30 wt.% of thoria have perfectly sintered at 1400°C, and those with 50% of thoria at 1500°C. The reduction of sintered pellets to stoichiometric composition by CO gas could be made more perfectly at higher sintering temperature, but the specimens containing less than 10% of ThO2 have cracked, as given in Table 1.The calcinated powder containing ThO2 30% was too fine to be pressed, and therefore the raising of calcination temperature up to 1000°C was tried. The sintering of these specimens showed a good results with the powder calcinated at 1000°C (Table 2). On the contrary the powders containing ThO2 50% was difficult to sinter at 1400°C, but this was possible by using the powder calcinated at 600°C (Table 3).The sintering in air of the uranium-rich specimens showed some faults of the volatilization of uranium component accompanying a large dimengional change at the reducing step. Therefore, the sinterings in neutral atomosphere, followed by hydrogen reduction were made at 1300°-1400°C. These sintering properties showed no particular differences between the atomosphere of nitrogen and carbon dioxide, and it was confirmed that good results may be obtained when the samples of 70-30 and 50-50 stoichiometric composition are sintered at 1400°C. The sintering processes will be reported in a following paper.
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