高机械灵敏度悬空导电薄膜的制备方法研究

微机电系统中的悬空薄膜的制备技术是微结构制备的关键技术之一.研究了周边固支方形薄膜的机械灵敏度及通过浓硼扩散自停止腐蚀法制备高灵敏度悬空导电薄膜.实验结果表明,当扩散温度为1 175℃,扩散时间为3h,去除硼硅玻璃后四甲基氢氧化铵(TMAH)腐蚀液中腐蚀7.5h,可得到厚度为3μm,边长为5 mm,方块电阻为1.12 Ω/sq,致密均匀的悬空导电薄膜.给出了详细的制备工艺;针对扩散过程中出现的硼硅玻璃等问题,给出了切实可行的解决办法.     

硼氢化物(BHn)(n=1~5)稳定性与红外光谱

采用密度泛函(DFT)中的B3P86方法,结合Dunning的相关一致基组cc-PVTZ,优化计算硼氢化物(BHn)(n=1～5)可能的几何构型,得出最稳定构型的几何参数、电子结构和红外光谱等性质参数,给出了最稳定结构的总能量(ET)、结合能(EBT)、平均结合能(Eav)、电离势(EIP)、能隙(Eg)、费米能级(EF)和氢原子差分吸附能(Bdiff)等.结果表明硼氢化物基态稳定结构的电子态分别为:n为奇数为单重态1∑和1 A,n为偶数为双重态2A;由于B原子属于缺电子原子,能与等电子原子H化合,通过氢端或桥键形成氢化物,本文优化计算发现,硼氢化物最稳定的构型都存在氢端或桥键,且n为奇数的氢化物的氢端或桥键作用比相邻偶数的氢化物强.最后计算了硼氢化物最稳定结构的红外光谱、平均结合能、电离势、能隙和费米能级等动力学电子特性,分析得出(BHn)(n=1～5)氢化物中BH3的电离势和能隙最大,说明该氢化物最稳定,氢原子差分吸附能也最大.     

硼酰化镍的合成及应用研究

本文研究了以碳酸镍合成硼酰化镍的新方法。系统地研究了各种因素对合成硼酰化镍的影响,找到了较优的合成条件。以2—乙基己酸和硼酸三丁酯为有机原料合成的硼酰化镍,可用作橡胶—金属粘合促进剂。     

热处理对B1500HS钢激光拼焊板力学性能的影响

利用单轴拉伸试验机、扫描电子显微镜、能量色散谱仪、光学显微镜、维氏硬度仪等研究了热处理前后B1500HS钢激光拼焊板的淬火性能.结果表明:热处理前B1500HS钢拼焊板焊缝强度远高于母材区,硬度分布极不均匀;热处理后,B1500HS钢拼焊板的元素分布几乎没有变化,整体强度有了大幅的提高,但塑性下降程度较大,其中横向塑性最差,经维氏硬度测试,发现焊缝至母材区的硬度过渡平滑.硬度值平滑过渡使得应力和应变分布更加均匀,保证了母材和焊缝力学性能的良好连续性,可以显著提高B1500HS钢拼焊板的成形性能.     

硼钢板相比例控制试验方法及试验参数的确定

车身用硼钢板的机械性能实际取决于微观组织的相比例,而不同的相比例是由保温温度、保温时间等试验参数决定的,若要获得材料预期的相比例,需研究试验参数与相比例的关系.利用高温相变仪在降温速率30℃·s-1的工况下研究了不同保温温度下材料的相比例,并结合经验公式给出了硼钢板相比例控制的关键参数及相比例控制方法,可为工程实际中获取固定相比例的微观组织提供理论参考.     

Superior machinability of steel enhanced with BN and MnS particles

The strategy that replacing part of MnS with BN was proposed in order to decrease the sulfur content in sulfur based free-cutting steel. The effects of BN and MnS inclusions on the microstructure and machinability of the steel were systematically investigated. The results show that most of the BN and MnS inclusions exist individually in the steel and only a small amount of them are in a composite state forming either isolated particles or clusters of particles. In the case of multi-phased steel, the theoretical calculation predicts that the volume of large BN particles should be 0.7 times of the volume of large MnS particles. The machinability of this type of BN and MnS alloy steel over a wide range of cutting speeds ranging from a low speed appropriate for drilling to a high speed appropriate for turning is confirmed as being equal to or superior to that of an MnS reference steel, even though the sulfur content in the composite steel is only half that of the MnS steel. The aptitude for cutting effect of 240 ppm nitrogen and 115 ppm boron in the composite steel is demonstrated to be equivalent or even better than 1000 ppm sulfur in MnS free-cutting steel.     

微量硼对高纯铁硫合金沿晶断裂和硫沿晶偏析的影响

利用俄歇能谱微区分析、低温拉伸试验和ＳＥＭ断口观察,研究了微量硼在高纯铁－６×１０－５(质量分数)硫合金中的沿晶偏析及其对硫沿晶偏析和硫偏析引起的低温沿晶断裂的影响·结果表明,硼能强烈地沿铁晶界偏析,显著降低硫的沿晶偏析倾向,抑制低温沿晶断裂·文中还讨论了硼影响的机理·     

高温热处理PAN基CF时硼的促进石墨化作用

研究了热处理温度,Ｈ３ＢＯ３溶液质量浓度和ＣＦ在Ｈ３ＢＯ３溶液中的浸泡时间等因素对ＰＡＮ基ＣＦ力学性能和电学性能的影响。并通过考察加和未添加Ｈ２ＢＯ３的ＣＦ分别经高温石墨化热处理后在结构和性能上的差异,对硼在ＰＡＮ基ＣＦ高温热处理时的促进石墨化作用进行了初步探讨。     

14 MeV中子防护体设计的MCNP模拟

用富氢材料防护产额为108个/s的D T中子发生器, 当富氢材料厚度大于76 cm时, 其中子辐射剂量低于0.025 mSv/h. 为降低防护体厚度, 用铜和含硼聚乙烯组成的双层材料作为14 MeV中子防护体. Monte Carlo(MCNP)计算结果表明, 若中子辐射剂量小于0.025 mSv/h, 则双层材料的最小厚度为52 cm, 硼的质量分数为1.00%, 铜和含硼聚乙烯的厚度分别为37 cm和15 cm.     

Titanium effect on the microstructure and properties of laminated high boron steel plates

High-boron steel is an important material used for thermal neutron shielding. The appropriate amount of added boron must be determined because excessive boron may deteriorate the steel's workability. A uniform microstructure can be formed by adding titanium to boron steel. In this study, casting and hot rolling were used to fabricate laminated high-boron steel plates whose cores contained 2.25wt% boron and 0wt%-7.9wt% titanium. The effects of titanium content and hot-rolling and heat-treatment processes on the microstructure and properties of the laminated plates were studied. The results indicated that the optimum titanium content was 5.7wt% when the boron content was 2.25wt%, and that the best overall properties were obtained after heat treatment at 1100℃ for 4 h. The tensile strength, yield strength, and elongation at the specified temperature and holding time were as high as 526.88 MPa, 219.36 MPa, and 29%, respectively.