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1. 中国科学院上海应用物理研究所 嘉定园区,上海,201800
2. 中国科学院核辐射与核能技术重点实验室,上海,201800
[ "作者简介:周金豪,男,1986年出生,2010年于华东理工大学获硕士学位,主要从事核燃料干法分离技术研究" ]
纸质出版日期:2015-07-10
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周金豪, 孙 波, 佘长锋, 等. 熔盐冷冻壁形成及控制实验研究[J]. 核技术, 2015,38(7):070602
ZHOU Jinhao, SUN Bo, SHE Changfeng, et al. Experimental research on the formation and controlling of molten salt frozen-wall[J]. Nuclear techniques, 2015, 38(7): 070602
周金豪, 孙 波, 佘长锋, 等. 熔盐冷冻壁形成及控制实验研究[J]. 核技术, 2015,38(7):070602 DOI: 10.11889/j.0253-3219.2015.hjs.38.070602.
ZHOU Jinhao, SUN Bo, SHE Changfeng, et al. Experimental research on the formation and controlling of molten salt frozen-wall[J]. Nuclear techniques, 2015, 38(7): 070602 DOI: 10.11889/j.0253-3219.2015.hjs.38.070602.
乏燃料干法后处理中高温熔盐化学工艺过程中存在设备腐蚀问题,以凝固盐层作为容器保护内衬的熔盐冷冻壁技术被认为是一种可行的解决方式。为开展该技术研究,自行研制并搭建了一套硝酸盐(40.0-7.0-53.0wt%NaNO2-NaNO3-KNO3)冷冻壁技术研究实验装置。该装置上熔盐运行温度150?250 oC,熔盐最大流量500 L?h?1,循环导热油运行温度5?120 oC,导热油流量1.5?15 m3?h?1。目前在该装置上开展了冷冻壁静态形成及平衡维持等工艺研究,实验中采用容器外壁循环导热油冷却换热实现冷冻壁的形成及维持,并试验了冷冻壁技术在熔盐静态工况下应用的工艺条件。冷冻壁形成平均速率可控制在0.2?0.5 mm?min?1。在冷冻壁静态形成过程中,随厚度增大,热交换量逐渐减小,同时冷冻壁层温差逐渐增大,并均呈衰减趋势变化;处于平衡维持状态时,径向温度分布、热流量及冷冻壁厚度均保持稳定,熔盐发热功率即为平衡状态时的热流量,其大小同时与外壁导热油的冷却热流量相等;实验还获得了较理想的静态应用工艺操作条件,为氟化物熔盐冷冻壁的研究及应用积累了经验。
Background: As corrosion of processing equipment from the high aggressive reagent is a serious problem during the pyroprocessing
the molten salt frozen-wall is proposed as an option for protecting the metallic walls from corrosion by a layer of frozen salt. Purpose: In order to study this means of corrosion protection
the research on the formation and controlling of molten salt frozen-wall was carried out. Methods: Nitrate molten salt (melt point: 142 oC) was used as the research medium and heat transfer oil was adopted as coolant. An experimental platform for the research of molten salt frozen-wall was built
which contains an up-flow tapered test tank covered with heat exchange jacket. The frozen-wall was formed and maintained by controlling the internally heating and the cooling of outer part of the test tank. The thickness of frozen wall was directly measured by caliper and also figured out by the measured temperatures. Results: The operation temperature of molten salt ranges from 150 oC to 250 oC; the maximum flowrate of molten salt is 500 L?h?1; the operation temperature of heat transfer oil ranges from 5 oC to 120 oC; and the flowrate of oil ranges from 1.5 m3?h?1 to 15 m3?h?1. Under the expected operating conditions
a layer of frozen can be easily and predictably deposited and maintained on surfaces contacted by the salt. The molten salt frozen-wall was adherent and stable. The average formation rate ranges from 0.2 mm?min?1 to 0.5 mm?min?1. The heat flow decreases with the thickness increasing during the process of formation
at the same time temperature difference through frozen-wall layer gradually increased
and the change trends are all damped. The frozen-wall could reach static equilibrium by controlling the heat transfer rate. When frozen-wall is in a state of balance
the temperature gradient and the thickness of frozen-wall are constant; the decay heat of fission produces simulated by heating rod is equal to the heat flow through frozen-wall layer
and is also equal to the cooling power of heat transfer oil. We also simulated the real application scenarios to test the operation parameters and get some good results. Conclusion: All the research results would be helpful for the developing of fluoride molten salt frozen-wall technology. Abstract
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