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891.
基于液晶调制器调制的实时测温系统   总被引:1,自引:0,他引:1  
分析了一种基于基尔霍夫定律的钽酸锂(LiTaO3)热释电探测器作为接收元件的实时测温系统中,机械式调制盘对测量精度影响,提出了改变机械式调制盘对测量精度的影响的方法;介绍了液晶调制器的结构、对辐射调制的原理以及在使用过程中的优点。设计了利用液晶调制器替代机械调制器的钽酸锂热释电实时测温系统。结果表明,利用液晶调制器改进后的测温系统在给定的温度范围中,测量精度均有明显的改善,符合测量要求。  相似文献   
892.
脉冲激光在液体中激发的声波特性研究   总被引:1,自引:0,他引:1  
理论上分析了脉冲激光在液体中产生的声波波阵面随光声源形状的变化,以及不同激发机制下光声脉冲波形的差别,并从实验中得出了脉冲CO2激光光声脉冲频谱特性.结果表明光声波波阵面为球面或柱面,热弹机制激发双极性的光声脉冲,汽化机制激发单极性的光声脉冲,CO2脉冲激光在水中激发的声波频谱峰值主要在100 kHz以下.通过选择光声源的形状和激发机制可以获得所需的光声信号.  相似文献   
893.
电吸附技术的应用与研究   总被引:8,自引:0,他引:8  
陈榕  胡熙恩 《化学进展》2006,18(1):80-86
本文综述了活性炭、活性炭纤维、炭气凝胶及活性氧化铝等材料的电吸附/脱附技术的研究进展。主要介绍了其在去除水中无机和有机污染物方面的应用,并对今后的研究方向提出了建议。  相似文献   
894.
微孔配位聚合物作为新型储氢材料的研究   总被引:6,自引:0,他引:6  
杨勇  沈泓滢  邢航  潘毅  白俊峰 《化学进展》2006,18(5):648-656
微孔配位聚合物性质独特、结构多样,具有广泛的应用前景,它已成为近几年来一个热门的研究领域。本文简要介绍该类化合物作为一种新型的储氢材料,在合成、结构和储氢性能方面的研究进展。  相似文献   
895.
Si(001)-(2×2×1):H表面O2吸附的密度泛函理论研究   总被引:1,自引:0,他引:1  
A novel model was developed to theoretically evaluate the O2 adsorption on H-terminated Si(001)-(2*2*1) surface. The periodic boundary condition, the ultrasoft pseudopotentials technique based on density functional theory (DFT) with generalized gradient approximation (GGA) functional were applied in our ab initio calculations. By analyzing bonding energy on site, the favourable adsorption site was determined. The calculations also predicted that the adsorption products should be Si=O and H2O. This theoretical study supported the reaction mechanism provided by Kovalev et al. The results were also a base for further investigation of some more complex systems such as the oxidation on porous silicon surface.  相似文献   
896.
陶瓷基钛掺杂硅胶块体吸附剂研究   总被引:5,自引:0,他引:5  
以陶瓷纤维纸为基材, 顺次经水玻璃、酸性硫酸氧钛溶液浸渍共沉淀制得新型蜂窝状陶瓷基钛掺杂硅胶块体吸附剂. FTIR谱在波数954 cm-1附近的特征吸收峰表明钛掺杂硅胶中存在Si-O-Ti键; XRD谱显示掺杂材料为无定型非晶相材料; SEM显示钛掺杂硅胶粒子较好地分散在陶瓷纤维表面及其空隙中; 用EDS及XPS揭示了材料的组成和钛原子含量, 根据钛掺杂前后XPS中Si2p, O1s, Ti2p 3/2电子结合能变化以及29Si MAS NMR中硅原子化学位移差异, 进一步表明钛原子替代硅原子进入了四面体骨架; BET分析显示掺杂材料以中孔为主. 与硅胶相比, 由于钛掺杂, 其比表面积、孔容增大, 吸附性能、耐热性能增强.  相似文献   
897.
苯及其含氮等电子体化合物的结构和性质的理论研究   总被引:9,自引:1,他引:8  
梁晓琴  蒲雪梅  舒远杰  田安民 《化学学报》2006,64(20):2057-2064
采用密度泛函理论的B3LYP方法在aug-cc-pvDZ基组上研究了13种苯及其含氮等电子体化合物的分子结构、 能量和异构体相对稳定性, 重点考察了含氮量对化合物含能性质的影响. 结果表明: 随着氮原子数增加分子的总能量降低, 且存在很好的线性相关性. 采用G3方法对分子的生成热进行了计算, 结果显示随着分子中氮原子个数增加, 各含氮等电子体化合物的生成热将增大, 其中六嗪、五嗪的生成热较大, 它们成为含能材料的潜力较大. 对各异构体分析显示, 氮原子位置与总能量和生成热的关系均为: (邻)间位<(邻)对位<邻位. 此外, 通过NBO方法分析了分子的超共轭作用和立体排斥能对异构体稳定性的影响, 结果表明超共轭作用是影响各异构体构型相对稳定性的主要因素.  相似文献   
898.
The conversion efficiency of stimulated Raman scattering (SRS) in CH4 is studied by using a single longitudinal mode second-harmonic Nd:YAG laser (532 nm, linewidth 0.003 cm-1, pulse-width (FWHM) 6.5 ns).Due to the heat release from vibrationally excited particles, SRS processes often suffer from the thermal defocusing effect (TDE). In view of 6.5 ns laser pulse width is much shorter than the vibrational relaxation time of CH4 molecules, TDE can only affect the SRS processes afterwards. In the cases of low laser repetition, TDE will be not serious, because it will be removed by the thermal diffusion in Raman medium before the next pulse arrives. At the laser repetition rate 2 Hz, CH4 pressure 1.1 MPa and pump laser energy 95 m J, the quantum conversion efficiency of backward first-Stokes (BS1) has attained 73%. This represents the highest first-stokes conversion efficiency in CH4. Furthermore, due to the relaxation oscillation, the BS1pulses are narrowed to about 1.2 ns. As a result, the BS1 peak power turns out to be 2.7 times that of the pump. Its beam quality is also much better and is only slightly affected by TDE. This reason is that BS1 represents a wave-front-reversed replica of the pump beam, which can compensate the thermal distortions in Raman amplify process. Under the same conditions, but pump laser repetition rate as 10 Hz, the conversion efficiency of BS1 goes down to 36% due to TDE. From this study, we expect that a well-behaved 630 nm Raman laser may be designed by using a closed CH4/He circulating-cooling system, which may have some important applications.  相似文献   
899.
The adsorption and the growth of ZnO on α-Al2O3(0001) surface at various temperatures were theoretically calculated by using a plane wave pseudopotentials (USP) method based on density functional theory.The average adsorption energy of ZnO at 400, 600 and 800 ℃ is 4.16±0.08, 4.25±0.11 and 4.05±0.23 eV respectively. Temperature has a remarkable effect on the structure of the surface and the interface of ZnO/α-Al2O3(0001). It is found that the Zn-hexagonal symmetry deflexion does not appear during the adsorption growth of ZnO at 400 ℃, and that the ZnO10-10 is parallel with the 10-10 of the α-Al2O3(0001), which is favorable for forming ZnO film with the Zn-terminated surface. It is observed from simulation that there are two kinds of surface structures in the adsorption of ZnO at 600 ℃: one is the ZnO surface that has the Zn-terminated structure, and whose 10-10 parallels the 10-10 of the substrate surface, and the other is the ZnO10-10 //sapphire 11-10 with the O-terminated surface. The energy barrier of the phase transition between these two different surface structures is about 1.6 eV, and the latter is more stable. Therefore,the suitable temperature for the thin film growth of ZnO on sapphire is about 600 ℃, and it facilitates the formation of wurtzite structure containing Zn-O-Zn-O-Zn-O double-layers as a growth unit-cell. At 600 ℃, the average bond length of Zn-O is 0.190±0.01 nm, and the ELF value indicates that the bond of (substrate)-O-Zn-O has a distinct covalent character, whereas the (Zn)O-Al (substrate) shows a clear character of ionic bond. However, at a temperature of 800 ℃, the dissociation of Al and O atoms on the surface of the α-Al2O3(0001) leads to a disordered surface and interface structure. Thus, the Zn-hexagonal symmetry structure of the ZnO film is not observed under this condition  相似文献   
900.
The interaction of atomic oxygen with the clean Cu(100) surface has been studied by means of cluster and periodic slab models density functional theory in the present paper. The Cu(4,9,4) cluster and a three-layer slab with c(2×2) structure are used to model the perfect Cu(100) surface. Three possible adsorption sites,top, bridge and hollow site, were considered in the calculations. The predicted results show that the hollow site is the prefer site for atomic oxygen adsorbed on Cu(100) surface energetically. This is in good agreement with the experiment. The calculated binding energies are respective 2.014, 3.154 and 3.942 eV for top, bridge and hollow sites at mPW1PW91/LanL2dz level for the cluster model. The geometry of Cu(100) surface has also been optimized theoretically with various density functional methods and the results show that the prediction from the B3PW91/LanL2dz and mPW1PW91/LanL2dz reproduce the experimental observation.The frontier molecular orbitals and partial density of states analysis show that the electron transfer from the d orbital of substrate to the p orbital of the surface oxygen atom.  相似文献   
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