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密度锁内无扰动时稳态温度场分析
引用本文:于沛,阎昌琪,谷海峰,陈薇.密度锁内无扰动时稳态温度场分析[J].核动力工程,2010,31(1).
作者姓名:于沛  阎昌琪  谷海峰  陈薇
作者单位:哈尔滨工程大学核科学与技术学院,哈尔滨,150001
基金项目:国家自然科学基金资助项目 
摘    要:实验模拟了密度锁内无扰动时稳态温度场分布。结果发现,稳态温度分布曲线上存在一个温度分层结束点;它是导热层与恒温层的分界,只有当温度分层结束点在密度锁内才能有效地抑制传热。应用半无限大平板导热模型、一维等截面直肋稳态导热模型和Fluent流体计算软件对无扰动时稳态温度场分布进行了理论计算。结果表明,半无限大平板导热模型是计算密度锁内无扰动时稳态温度场分布和温度分层结束点位置的最佳方法。

关 键 词:密度锁  无扰动  温度分布  导热层  恒温层  温度分层结束点

Analysis on Temperature Distribution in Density Lock on Steady State without Disturbance
YU Pei,YAN Chang-qi,GU Hai-feng,CHEN Wei.Analysis on Temperature Distribution in Density Lock on Steady State without Disturbance[J].Nuclear Power Engineering,2010,31(1).
Authors:YU Pei  YAN Chang-qi  GU Hai-feng  CHEN Wei
Abstract:Temperature distribution on steady state without disturbance in density lock is simulated ex-perimentally in this paper, and the temperature stratification end point is discovered on the temperature curve on steady state. It separated the heat conduction layer and homoiothermy layer. Only when the temperature stratification end point is in the density lock, heat can be restrained effectually. The temperature field is simulated with three methods. The first one is a method of semi-infinite flat-panel heat conduction, the second one is a method of one dimensional steady state conduction in constant cross-section straight-fin, and the last one is calculated using Fluent calculation software. The results indicated that the method of semi-infinite flat-panel heat conduction is the best one to calculate the distribution of temperature and location of temperature stratification end point.
Keywords:Density lock  Without disturbance  Distribution of temperature  Heat conduction layer  Homoiothermy layer  Temperature stratification end point
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