不同热管工质对热管冷却反应堆堆芯物理参数的影响与分析

热管冷却反应堆采用非能动传热技术,热响应速度快,可避免堆芯单点失效,具有功率密度大、寿命长、环境适应性强、工作性能稳定等特点,是目前空间核反应堆研究的热点。本文基于清华大学开发的反应堆蒙特卡洛中子输运程序RMC (Reactor Monte Carlo code),以美国爱荷华国家实验室(Idaho National Laboratory, INL)设计的热管冷却反应堆INL Design A为研究对象,选取3种热管工质开展热管冷却反应堆堆芯物理计算。计算结果表明：锂热管工质不仅拥有很好的热物性参数,并且使用锂热管工质的热管冷却反应堆缓发中子有效份额最大、中子能谱较硬、燃耗反应性损失最小、增殖性能最佳,有利于热管冷却反应堆堆芯小型化与长寿命。因此,推荐锂为热管冷却反应堆的热管工质。     

基于PSO磁悬浮球系统自适应灰预测控制

目的 针对磁悬浮球系统非线性不稳定和滞后性的问题,提出一种基于粒子群优化的自适应灰色预测 PID (Proportion Integration Differentiation)复合控制策略。 方法 通过在 PID 控制模块的反馈环中引入具有等维新息特征的灰色预测器,对系统误差进行及时反馈修正,以提高控制系统的响应速度和鲁棒性;同时,融合粒子群智能算 法对控制器参数迭代优化,以提高控制系统控制精度和抗干扰能力;最后,在 MATLAB / Simulink 环境下搭建仿真 平台进行对比实验。 结果 验证基于粒子群优化的自适应灰预测控制系统模型的超调量、峰值时间、调节时间显著 改善。 结论 证实该策略可以有效抑制系统滞后性,具有良好的稳定性和鲁棒性。     

图的一种加权邻接矩阵谱半径和能量的界

图G的一种加权邻接矩阵记为A_db(G)=(a^db_ij)_n×n,若顶点v_i和顶点v_j相邻,则$a_{i j}^{d b}=\frac{d_{i}+d_{j}}{d_{i} d_{j}}$, 反之a^db_ij=0.给出图G的加权谱半径的上下界,并在此基础上给出加权谱半径的Nordhaus-Gaddum-type关系.得到了图G的加权能量的几个上下界,并在此基础上给出加权能量的Nordhaus-Gaddum-type关系.     

悬浮预热器中的换热分析

本文通过分析悬浮预热器的传热机理,讨论了颗粒的加速过程和换热时间对分散和换热的影响,论述了分散不良引起的“准短路”对分散、换热及能量损失的影响,并指出可以通过温熵图计算不可逆损失。     

夫伦克耳激子的运动

本文从晶格模型出发,同时考虑周期场和电子-声子相互作用对激子能态的影响。夫伦克耳激子在晶格中运动有两种不同方式:在低温区,是能带传递;在高温区,是跳跃过程。     

Energy flow and community structure in freshwater ecosystems

The goal of this article is twofold: 1) It aims at providing an overview on some major results obtained from energy flow studies in individuals, populations, and communities, and 2) it will also focus on major mechanisms explaining community structures. The basis for any biological community to survive and establish a certain population density is on the one hand energy fixation by primary producers together with adequate nutrient supply and the transfer of energy between trophic levels (bottom-up effect). On the other hand, predator pressures may strongly control prey population densities one or more trophic levels below (top-down effect). Other interpopulation effects include competition, chemical interactions and evolutionary genetic processes, which further interact and result in the specific structuring of any community with respect to species composition and population sizes.     

2,3-二羟基哌嗪与几种氨基化合物的缩合反应研究

由乙二胺与乙二醛的缩合物２,３－二羟基哌嗪,分别与甲酰胺、脲和乙二胺反应,制得２,４,７,９,１１,１４－六氮杂三环［８,４,０,０３,８］十四烷六盐酸盐四水合物（１）,２,５,７,９－四氮杂双环［４,３,０］壬－８－酮二盐酸盐－水合物（２）和２,５,７,１０－四氮杂双环［４,４,０］癸烷（３）。化合物１为未见文献报道的新化合物。化合物２的合成工艺条件优化后,反应得率与文献［１］相比有一定提高。化合物３的合成,由于将反应分为低温和高温两个缩合阶段,使反应得率提高到７７．５％。     

大立体角多参数电离室

因重离子核物理研究工作研究,研制成功灵敏区深庶３５ｃｍ的大立体角多参数电离室,可同 量信号△Ｅ、Ｅ和位置信号Ｘ、Ｙ等多项参数。     

The v-v energy transfer of highly vibrationally excited states (I)

The relaxation of the highly vibrationally excited CO (v = 1–8) by CO₂ is studied by timeresolved Fourier transform infrared emission spectroscopy (TR FTIR). 193 nm laser photolysis of the mixture of CHBr₃ with O₂ generates the highly vibrationally excited CO(v) molecules. TR FTIR records the intense infrared emission of CO(v→v-1). The vibrational populations of each level of CO(v) have been determined by the method of spectral simulation. Based on the evolution of the time resolved populations and the differential method, 8 energy transfer rate constants of CO(v = 1–8) to CO₂ molecules areobtained: (5.7±0.1), (5.9±0.1), (5.2±0.2), (3.4±0.2), (2.4±0.3), (2.2±0.4), (2.0±0.4) and (1.8±0.6) (10¹⁴ cm³ · molecule⁻¹ · s⁻¹), respectively. A two-channel energy transfer model can explain the feature of the quenching of CO(v) by CO². For the lower vibrational states of CO, the vibrational energy transfers preferentially to the u³ mode of CO² For the higher levels, the major quenching channel changes to the vibrational energy exchange between CO(v→v-1) and the u¹ mode of CO².     

The v-v energy transfer of highly vibrationally excited states (II)

The vibrational energy transfer from highly vibrationally excited CO to H₂O molecules is studied by time-resolved Fourier transform infrared emission spectroscopy (TR FTIR). Following the 193 nm laser photolysis of CHBr₃ and O₂ the secondary reactions generate CO(v). The infrared emission of CO(v → v−1) is detected by TR FTIR. The excitation of H₂O molecules is not observed. By the method of the spectral simulation and the differential technique, 8 rate constants for CO(v)/H₂O system are obtained: (1.7 ±0.1), (3.4 ±0.2), (6.2 ±0.4), (8.0 ±1.0), (9.0 ±2.0), (12 ±3), (16 ±4) and (18 ±7) (10¹³cm³ · molecule^-1· s^-1). At least two reasons lead to the efficient energy transfer. One is the contributions of the rotational energy to the vibational energy defect and the other is the result of the complex collision. With the SSH andab initio calculations, the quenching mechanism of CO(v) by H₂O is suggested.