增塑剂对PVA碱性聚合物电解质电化学性能的影响

通过溶解―铸膜法制备聚乙烯醇(PVA)-KOH-H2O碱性聚合物电解质膜。向聚合物中添加增塑剂丙三醇(GROL)和碳酸丙烯酯(PC)来提高离子电导率。X射线晶体衍射分析(XRD)结果表明,添加增塑剂未改变聚合物的物相结构,薄膜仍主要为不定形态。差示扫描热分析(DSC)结果显示,添加增塑剂后聚合物电解质膜的玻璃化转变温度降低,促进了电解质膜向不定形态转变。电解质膜室温离子电导率随增塑剂添加而增大,增塑剂超过一定量后离子电导率开始下降。PC对提高离子电导率的作用优于GROL。循环伏安测试结果显示,电解质膜的电化学稳定性窗口随增塑剂的添加而有所变窄,但仍显示了较好的电化学稳定性。     

Measurements of saturated basic and acidic rock electrical conductivities at lower crustal temperatures and high pressures

Abstract

Laboratory measurements of the electrical conductivity of brine saturated acidic and metabasic rocks were done at confining pressures up to 0.2 GPa, high pore pressures and temperatures of 900°C. Acidic rocks showed conductivities insufficient to explain the lower crustal high conductivity layer. Basic rocks, however, showed conductivities consistent with the high conductivity layer at those temperatures that the layer is thought to possess.     

The influence of SiCp oxidized on the interface layer and thermal conductivity of SiCp/Al composites

In this work, oxidation of silicon carbide particles (SiCp) at elevated temperature and its influence on the interface layer and thermal conductivity of SiCp/ZL101 composites prepared using pressure infiltration process were investigated respectively. It is found that initial temperature for the oxidation of SiCp is about 850?°C, and that the oxidation increment of SiCp and the thickness of SiO₂ layer increase with the increase in pre-oxidation temperature and time, when the oxidized temperature exceeds 1100?°C, or the duration time exceeds 2?h at 1100?°C, a small amount of ablation will take place on the SiCp, as well as the oxidized layer has some loss. The formation of SiO₂ layer can provide certain interface reactions with interface layers (3.1–6.36?μm), and the higher the thickness of SiO₂ layer, the thicker the interface layer in SiCp/Al composites. However, the thickness of SiO₂ layer is more than 5.9?μm, which is not benefit for the formation of interface layer. With the increase in the thickness of interface layer, thermal conductivity declines, but is not linear.     

微纳米电子器件散热过程中的物理问题

微纳米电子器件的散热问题是目前制约半导体工业发展的重要瓶颈。将电子器件工作时产生的热量传输到封装外壳后再耗散到环境中去需要好几个步骤,每个步骤需要不同的方法,其中有些步骤涉及到了固体中的界面热传导问题和高性能导热材料。文章先介绍了近期关于微纳米尺度器件散热问题中碰到的热传导问题在理论和实验两方面的研究进展。在热传导理论和计算方法方面,作者讨论了傅里叶定律在微纳米尺度的适用性,介绍了玻尔兹曼方程、分子动力学模拟和格林函数方法。在热传导实验方面,介绍了用扫描热显微镜测量样品表面温度和用超快激光反射法测量薄膜材料的热导率及其界面热阻。然后介绍了界面热传导问题,包括界面热阻的计算以及电子—声子相互作用对界面热阻的影响。最后作者介绍了关于高性能导热材料方面的最新进展,包括碳基导热材料、晶格结构类似于石墨烯的氮化硼材料、高分子有机材料以及界面热阻材料。     

微纳器件热传导中的基础物理问题

纳米功能器件中的温度控制已经成为世界各国迫切需要解决的关键技术。在文章中,作者简单回顾了纳米器件发展的历程和现状;以碳纳米管和石墨烯为例,重点介绍了纳米尺度热传导研究中的一些基础物理问题,以及近年来该领域中一些热点研究方向和新奇物理效应。同时,还讨论了影响纳米材料热传导性质的主要物理机制。研究这些系统本身的热传导特性,不仅对于深入理解纳米尺度能量输运的基本物理原理具有重要意义,而且与微纳电子器件的未来发展密切相关,具有广阔深远的应用前景。     

Solid Sampling Pyrolysis Adsorption-Desorption Thermal Conductivity Method for Rapid and Simultaneous Detection of N and S in Seafood

In this work, a rapid method for the simultaneous determination of N and S in seafood was established based on a solid sampling absorption-desorption system coupled with a thermal conductivity detector. This setup mainly includes a solid sampling system, a gas line unit for controlling high-purity oxygen and helium, a combustion and reduction furnace, a purification column system for moisture, halogen, SO₂, and CO₂, and a thermal conductivity detector. After two stages of purging with 20 s of He sweeping (250 mL/min), N₂ residue in the sample-containing chamber can be reduced to <0.01% to improve the device’s analytical sensitivity and precision. Herein, 100 s of heating at 900 °C was chosen as the optimized decomposition condition. After the generated SO₂, H₂O, and CO₂ were absorbed by the adsorption column in turn, the purification process executed the vaporization of the N-containing analyte, and then N₂ was detected by the thermal conductivity cell for the quantification of N. Subsequently, the adsorbed SO₂ was released after heating the SO₂ adsorption column and then transported to the thermal conductivity cell for the detection and quantification of S. After the instrumental optimization, the linear range was 2.0–100 mg and the correlation coefficient (R) was more than 0.999. The limit of detection (LOD) for N was 0.66 μg and the R was less than 4.0%, while the recovery rate ranged from 95.33 to 102.8%. At the same time, the LOD for S was 2.29 μg and the R was less than 6.0%, while the recovery rate ranged from 92.26 to 105.5%. The method was validated using certified reference materials (CRMs) and the measured N and S concentrations agreed with the certified values. The method indicated good accuracy and precision for the simultaneous detection of N and S in seafood samples. The total time of analysis was less than 6 min without the sample preparation process, fulfilling the fast detection of N and S in seafood. The establishment of this method filled the blank space in the area of the simultaneous and rapid determination of N and S in aquatic product solids. Thus, it provided technical support effectively to the requirements of risk assessment and detection in cases where supervision inspection was time-dependent.     

相对论速调管放大器杂模振荡的抑制

研究了相对论速调管放大器（RKA）输入腔和中间腔之间的高阶杂模振荡问题。通过模式分析得知杂模在谐振腔内为TM11模式,而在漂移管中表现为TE11模式,针对该模式能在漂移管中传输的特性,利用漂移管内壁涂覆吸波材料吸收杂模功率的方法进行抑制。通过3维粒子模拟程序,分析了吸波材料的电导率及涂覆长度对抑制杂模增长率的影响。利用模拟分析得到的结果,对漂移管中涂覆吸波材料的RKA输入腔及中间腔结构进行了3维模拟研究,结果显示:合适的吸波材料的引入能够很好地抑制RKA输入腔和中间腔之间的杂模振荡。     

微型金柱腔中原位成型制备微孔泡沫

报道了在μm量级圆柱状金柱腔中原位成型制备微孔泡沫的方法。在直径400 μm、长度700 μm、壁厚20 μm、两端开口的金柱腔中原位成型成功制备出密度为50 mg·cm-3、蜂窝直径不超过1 μm的多元丙烯酸酯聚合物微孔泡沫。干燥过程中泡沫没有明显收缩,在柱腔中填充紧密,无需后续机械加工。     

液态泡沫结构及其稳定性

液态泡沫由大量气泡密集堆积在少量的表面活性剂溶液中形成, 是具有高度自组织结构的典型的软物质. 文章从泡沫物理学角度简要介绍了液态泡沫的结构特征和稳定性方面的研究.     

泡沫物理学史拾萃

人们对泡沫习以为常,却很难理解它的奇特性质,比如几乎完全由空气组成的泡沫,既能像固体一样发生弹性形变,又能像流体一样发生流动,这正是泡沫物理学的研究内容之一.泡沫物理是一门古老的学科,早在19世纪中下叶,气泡和泡沫结构静力学的描述已经完美,之后没有大的发展,直到1990年前后,随着流体力学、微观显像技术和计算技术等学科的发展,以及受材料科学和工业生产的需求,泡沫物理研究再次活跃起来.文章第一作者曾跟随英国皇家学会院士Denis Weaire从事泡沫物理研究多年,在他的演讲和个人收藏中,文章作者积累了一些材料,在此基础上,又仔细查阅了相关文献,整理成此文,它基本概括了泡沫结构静力学发展历程中的重要事件.