凹坑板式空气预热器的传热特性及多目标优化

以全焊接型凹坑板式空气预热器为对象,基于最优设计试验方案,运用Workbench Fluent软件数值模拟凹坑板片特征结构参数对传热流阻性能的影响。基于参数敏感度分析,得到单因素作用下对传热流阻性能的影响程度为凹坑的纵向间距>长轴>横向间距>深度。基于响应曲面法分析,得到多因素协同作用时,凹坑之间的结构参数横纵距对性能影响比凹坑自身的结构参数深径比大。基于遗传算法以摩擦因子f最小、努塞尔数Nu与综合换热因子J_F最大为优化目标,得到给定范围内的3组较优结构组合。     

IRS辅助的MISO-SWIPT安全速率最大化算法

为增强系统的稳定性,基于智能反射面（intelligent reflection surface,IRS）辅助安全通信,为用户采用功率分配架构的无线携能传输（simultaneous wireless information and power transfer,SWIPT）技术以提高用户安全速率并降低用户的能量消耗,建立了系统安全速率最大化的目标函数模型;考虑IRS相移约束、基站最大发射功率、功率分配比率约束和用户最低能量采集约束,提出了一种基于交替优化的安全速率最大化算法。利用连续凸近似算法,将目标函数转化为凸的形式;采用交替优化,对耦合变量进行解耦处理;提出一种波束赋形算法以实现安全速率最大化。仿真表明,提出的算法能够有效提升IRS辅助的SWIPT系统的安全速率,至少比其他算法提高了2.63bps/Hz。     

等衰落轨道角动量索引调制系统的信道容量性能分析

射频轨道角动量(orbital angular momentum,OAM)提供了一种可以在同一载波频率物理信道上复用一组正交模式以提高信道容量的方法。现有研究大多专注于信道容量提升,对系统复杂度的研究相对较少。在基于均匀圆形阵列(uniform circular array,UCA)的OAM通信系统中,发射机需要完成大量调制运算以生成OAM信号。于是,提出了一种等衰落轨道角动量索引调制(equal fading orbital angular momentum index modulation,EOAM-IM)方案,其中,IM有效降低了OAM调制运算复杂度,且等衰落发射机也保证了不同模式OAM子信道传输增益。此外,还详细推导了所提EOAM-IM方案的系统信道容量。仿真结果表明,所提EOAM-IM方案能以更低的调制复杂度获得比传统OAM方案更高的信道容量。     

溶剂萃取柠檬酸的传质研究

研究了用三辛胺溶剂分别从纯溶液和发酵液中萃取柠檬酸过程的传质规律与液滴粒径,无因次柱高及有机相配比对传质系数的影响,建立了液滴自由上升阶段的传质模型,并用以关联实验结果。     

2-(1-萘甲基)-3(2-四氢呋喃基)丙酸N,N-二乙氨基乙酯草酸盐的新法合成

改进２－（１－萘甲基）－３－（２－四氢呋喃基）丙酸Ｎ,Ｎ－二乙氨基乙酯草酸盐（Ⅵ）合成方法．方法在１－氯甲基萘和四氢糠基丙二酸二乙酯（Ⅰ）的烷基化反应中使用ＮａＨ／ＤＭＦ为催化剂;在２－（１－萘甲基）－３－（２－四氢呋喃基）丙酸（Ⅳ）与２－氯乙基－Ｎ,Ｎ－二乙基胺的酯化反应中加入相转移催化剂;在２－（１－萘甲基）－３－（２－四氢呋基）丙酸Ｎ,Ｎ二乙氨基乙酯（Ⅴ）与草酸成盐中,直接使用二水合草酸替代脱水草酸．结果烷基化反应产率提高到７５％,反应时间缩短到２ｈ;酯化反应产率从文献报道的７２％提高到９２％;二水合草酸成盐效果与脱水草酸相同．结论该方法较已有的合成方法产率有较大提高且操作简便,有较好的工业化前景．     

静电像管均方根半径的计算及像质评价

探讨在电子光学成像系统中像评定的一种途径。方法,从静电这像差均方根理论出发,追迹计算大量空间轨迹的落点及系统均根半径,并由此衍算成弦财制传递函数。     

谐振腔镜对高斯光束远场发散角的影响

利用变换矩阵和ＡＢＣＤ定律讨论了激光谐振空对高我束的变换,推导出高斯光束参数通过光腔输出镜的变换公式。并对热透镜腔,光束远场发散角等问题进行了讨论。     

坐标动量几率相关分布的辛普森法研究

用辛普森法研究了不同体系的粒子在动量空间和坐标空间的几率分布的相关性及坐标和动量的分布宽度之积与宽度内所含几率的关系。     

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.