基于运行模式切换的多能源系统的混合控制

为了实现具有高度灵活性的智能控制策略,以提高多能源系统的稳定性、安全性和自愈能力,文中提出了基于分布式能源运行模式切换的分层混合智能控制。对应于系统的混合动态行为,分层混合控制由上层的离散控制策略、下层的本地连续控制器和它们之间的相互作用组成。上层离散控制策略主要负责切换操作模式,以增强遭遇重大干扰时的安全性和自愈能力。下层连续控制的目的是调节各被控单元的动态稳定性,以获得满意的性能。通过仿真实例验证了该混合控制方法的有效性。     

开孔泡沫金属动态力学性能及能量特性

泡沫金属材料在防护吸能领域有着重要的应用前景,深入研究泡沫金属及其相关结构的冲击力学性能十分必要。通过Φ50 mm的分离式霍普金森杆(split Hopkinson pressure bar, SHPB)装置对开孔泡沫金属Fe、Ni、Fe-Ni合金(50 mm×10 mm)进行动态冲击试验。试验分析了应变和应变率对其力学性能及吸能特性的影响,通过对其峰值应力、波动应力、理想吸能效率等参数的对比分析多种冲击速度下不同泡沫金属材料的抗压强度与吸能性,为建筑、航天等工程的使用提供理论基础。研究结果表明：高冲击速度下峰值应力增大且Fe-Ni合金抗压强度最高,不同材料泡沫金属均存在波动应力且压密阶段时间各不相同。应变率介于600～1 150时泡沫金属Ni吸能性最优,该区间外Fe-Ni合金更优。当应变率大于1 000时,Fe-Ni合金理想吸能效率增幅较大,相较于700时提高了48%、为最优理想吸能材料。     

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.