盐酸三甲胺三氧化铬对二醇及肟的选择性氧化

前文曾报道盐酸三甲胺三氧化铬(TCC)的制备方法及对一些一元醇的氧化实验,结果发现TCC对一元醇的氧化有很好的选择性。本文在此基础上,用TCC在DMF中作了一些对二醇及肟的氧化实验,实验表明:TCC在DMF中只氧化二醇中的苄基型羟基而不氧化     

焙烧温度对 MnO2-CeO2/Zr0.25Ti0. 25Al0. 5O1.75 整体式催化剂 NH3 低温选择性催化还原 NO 性能的影响

 采用等体积浸渍法在不同温度下焙烧制备了一系列 MnO2-CeO2/Zr0.25Ti0.25Al0.5O1.75 整体式催化剂样品, 并用低温 N2 吸附-脱附、储氧量、X 射线衍射、X 射线光电子能谱和 NH3 程序升温脱附等对催化剂进行了表征, 考察了催化剂上 NH3 选择性催化还原 (SCR) NO 的活性. 结果表明, 随着焙烧温度的升高, 催化剂的比表面积和孔体积逐渐减小, 平均孔径逐渐增大, 储氧能力逐渐降低. 在 500~700 oC 焙烧时, 催化剂主要以无定形或微晶的形式存在; 在 500 oC 焙烧时, 催化剂表面 Mn 与载体之间的相互作用较强, 表面酸量最高, 有利于提高 SCR 活性. 尽管在 600 和 700 oC 焙烧的催化剂仍具有较高的 SCR 活性, 且表现出一定的抗 H2O 和 SO2 性能, 但活性有所下降. 800 oC 焙烧后催化剂的活性显著降低.     

良分散性磁性壳聚糖纳米粒子的制备及吸附性能研究

采用原位共沉淀法,在碱性条件下以环氧氯丙烷为交联剂,制备出了具有超顺磁性、分散性良好的磁性壳聚糖纳米粒子。用红外光谱仪(FTIR)、X射线衍射仪(XRD)、透射电子显微镜(TEM)、振动样品磁强计(VSM)对纳米粒子的组成、形貌和磁性能进行了表征。结果表明:用原位共沉淀法制备得到的磁性壳聚糖纳米粒子平均粒径约7nm,饱和磁化强度为73.5emu/g。与活性炭相比,磁性壳聚糖纳米粒子对偶氮染料具有很高的吸附容量和快速的吸附速率。     

十六烷基三甲基溴化铵逆胶束介质中邻氯代苯亚甲基丙二腈的化学发光测定

以十六烷基三甲基溴化烷 (CTMAB)在氯仿 环己烷为主体溶剂相中所形成的逆胶束介质 ,基于鲁米诺 H2 O2 化学发光体系对邻氯代苯亚甲基丙二腈 (CS)进行定量分析 ,详细研究了氯仿与环己烷的不同配比、R值 ([H2 O] [表面活性剂 ])、CTMAB浓度、pH值、鲁米诺浓度及H2 O2 浓度对化学发光强度的影响。CS的检测线性范围为 1× 10 - 5～ 5 .5× 10 - 3mol L ,检出限达 4× 10 - 6 mol L(S N =3) ,对水样及土样的回收率均在 90 %以上。     

氮、氩在5A^。分子筛上的低温吸附分离

测定了不同温度下氮、氩在5分子筛上的吸附等温线,其中三参数的Langmuir-Freundlich方程和Toth方程在不同温度下都能获得较好的拟合结果;计算了不同温度下氮、氩在5分子筛上吸附的亨利常数,获得了氮、氩选择性和温度的关系.测定了125K温度下氮、氩混合气体在5分子筛吸附柱上的穿透曲线.结果表明:最先流出的5L气体中含有约70%的氩,通过收集5L气体即可实现混合气体中氩的初步分离.     

新型三腈基呋喃衍生物光谱特性的研究

通过两步反应合成了一种带有新型电子给体的D-π-A型三腈基呋喃衍生物(DCDHF-2-V),并采用旋涂法制备出与聚甲基丙烯酸甲酯(PMMA)共混均匀的聚合物薄膜.采用UV1700紫外可见分光光度计和F-4500荧光分光光度计研究了该化合物在不同极性溶剂以及薄膜状态下的吸收光谱和荧光光谱特性.结果表明,在薄膜状态下化合物的吸收峰有一定蓝移,吸收带变宽.随溶液极性的增加,荧光光谱的最人峰值波长逐渐红移,分子的荧光量子产率以及斯托克斯位移也有较大变化.据此计算出DCDHF-2-V分子激发态与基态偶极矩之差为35.68×10-30C·m,并根据双能级模型确定了分子的二阶非线性极化率β随波长的变化情况,当激光基频波长为1064 nm时,β为3323.4×10-40m4/V.     

Simulation of radiation losses using non-coronal model on HL-2A

In this paper, the radiation losses of impurity on HL-2A have been simulated by assuming the profiles electron temperature and density and solving ionization rate equation under conditions of non-coronal radiation. The time required for an impurity species to establish equilibrium is proved to be sensitively dependent on the plasma electron temperature, and it is strongly correlated with the ionization state distribution during equilibrium establishment of impurity species. It is found from simulation results that the residence parameter plays an important role in the enhancement of radiation losses of plasma.     

并联谐振AC-link三相AC/AC变换器仿真研究

基于AC-Link技术的充电电源具有高效率、高功率密度等优点,可作为高功率微波系统的初级能源。针对三相AC/AC能量变换的需求,仿真研究了一种基于AC-Link并联谐振技术的三相AC/AC变换器。给出了并联谐振AC-link三相AC/AC变换器的拓扑结构;分析了控制原理;阐述了16模式的具体控制过程和软开关切换的实现方法;明确了开关切换时间的计算方法;搭建15 kW仿真平台分析了不同负载要求下的能量变换过程。结果表明: 该变换器可以实现固定输出的能量变换,并且输出电压、频率可调;输入/输出电流波形均为正弦,输入功率因数为1;控制方法正确有效,实现了软开关切换。     

Gamma-radiation effects in pure-silica-core photonic crystal fiber

We investigated the steady state gamma-ray radiation response of pure-silica-core photonic crystal fibers(PSC-PCFs)under an accumulated dose of 500 Gy and a dose rate of 2.38 Gy/min. The radiation-induced attenuation(RIA) spectra in the near-infrared region from 800 nm to 1700 nm were obtained. We find that the RIA at 1550 nm is related with hydroxyl(OH-) absorption defects in addition to the identified self-trapped hole(STH) defects. Moreover, it is proposed and demonstrated that reduced OH-absorption defects can decrease the RIA at 1550 nm. The RIA at 1550 nm has effectively declined from 27.7 d B/km to 3.0 dB/km through fabrication improvement. Preliminary explanations based on the unique fabrication processes were given to interpret the RIA characteristics of PSC-PCFs. The results show that the PSC-PCFs,which offer great advantages over conventional fibers, are promising and applicable to fiber sensors in harsh environments.     

Effect of λ/2 SiO_2 overcoat on the laser damage of HfO_2/SiO_2 high-reflector coatings

The effect of λ/2 SiO2 overcoat on the laser damage characteristics of HfO2/SiO2 high-reflector (HR) coatings is investigated with 1-on-l and N-on-1 laser damage test methods. The laser damage surface of 1-on-l is analyzed by a step analyzer. The surface morphologies show that laser damage makes the coating damaged area protrudent and rough for HR coating without λ/2 silica overcoat, but concave and smooth for HR coating with A/2 silica overcoat. The result of 10-on-l multi-pulse irradiation on the same point of the coating shows that there is an energy density stage on the damage curve. If the laser energy density is within the range of the stage, HfO2/SiO2 HR coatings with λ/2 silica overcoat will not be damaged more than 2 times for multi-shots, and the surface damages are very slight so that there is no impact on the coating performance. Another interesting result is that the energy density stage extends from the damage threshold to the point of about 3 times of threshold, which is similar to the