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利用布朗动力学方法研究了ACB三嵌段粒子的分级自组装过程.由第一级组装得到的结构作为第二级组装的初始构型,通过调控体系中补丁B部分的吸引强度和补丁粒子的浓度,研究了第二级组装过程中形成有序结构的影响因素.通过设计组装模型、组装规则和组装路线,得到了蜂巢状网络结构和金刚石状结构.结果表明,在较高的吸引强度和适当的浓度下,可以得到更多且更规整的蜂巢状结构;较高和较低的吸引强度和浓度都不利于金刚石状结构的形成. 相似文献
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将盐酸羟胺与聚丙烯腈(PAN)反应得到偕胺肟化聚丙烯腈(AOPAN)溶液,随后采用同轴静电纺丝技术,制备了以AOPAN为壳,PAN为芯的同轴纳米纤维(AOPAN@PAN).通过透射电子显微镜(TEM)、扫描电子显微镜(SEM)和红外光谱(FTIR)等对纤维的形貌、组成和力学性能进行了表征.结果表明,随着PAN用量的增加,AOPAN@PAN同轴纳米纤维的强度逐渐变大,当芯层与壳层质量比为1∶3时,纳米纤维的抗拉伸强度和断裂伸长率分别为3.677 MPa和18.03%;对Cu~(2+),Pb~(2+),CrO_4~(2-)和甲基橙(MO)的最大吸附量分别为135.1,151.2,120.48和43.45 mg/g;使水中Cu~(2+),Pb~(2+),CrO_4~(2-)和MO的浓度分别降低到0.17,0.03,0.06和0.91 mg/L. 相似文献
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硼在高压下具有复杂的结构和多样的物理性质,对其结构和性质的深入研究具有很重要的意义,一直引起理论和实验研究领域的关注。高压下进行电学性质测量是获得物质物理性质的有效手段,利用集成在金刚石对顶砧上的微电路,在高压下和两个不同温度范围内对β相硼进行了电导率测量,分析了导电机制随压力的变化规律。在0~28.1 GPa范围内,β相硼的电导率随着压力的增大是逐渐增大的,卸压后样品的电导率不能回到最初的状态,是一个不可逆的变化过程;由室温到423 K的范围内,β硼的电导率随着温度的不断增加有明显的上升趋势,并且随着压力的升高,电导率变化逐渐加快。此外,对样品在14.5 GPa和18.6 GPa压力下,用溅射到金刚石对顶砧上的氧化铝薄膜做绝热层,对样品进行了激光加热实验,最高温度达到2 224 K,电导率随着温度的上升而增大,结果显示,β相硼的电学特征仍然属于半导体的特征范围内。 相似文献
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In situ energy dispersive x-ray diffraction for natural marmatite (Zn0.76Fe0.23S) is performed up to 17. 7 GPa and 623 K. It is fit, ted by the Birch-Murnaghan equation of state (EOS) that Ko and α0 for marmatite are 85(3)GPa and 0.79(16)*10^-4 K^-1, respectively. Fe^2+ isomorphic replacing to Zn^2+ in natural crystal is responsible for high bulk modulus and thermal expansivity of marmatite. Temperature derivative of bulk modulus (OK/OT)p for marmatite is fitted to be -0.044(23) GPaK^-1. The unambiguous B3-B1 phase boundaries for marmatite are determined to be Pupper(GPa)= 15.50 - 0.016T(℃) and Plower (GPa)=9.94-0.012T(℃) at 300-623K. 相似文献
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High-Pressure Phase Transitions of Cubic Y_2O_3 under High Pressures by In-situ Synchrotron X-Ray Diffraction 下载免费PDF全文
High-pressure phase transitions of cubic Y_2O_3 are investigated using in situ synchrotron x-ray diffraction in a diamond anvil cell up to 36.3 GPa. The pressure-induced phase transitions of cubic Y_2O_3, which display apparent inconsistencies in previous studies, are verified to be from a cubic phase to a monoclinic phase and further to a hexagonal phase at 11.7 and 21.6 GPa, respectively. The hexagonal Y_2O_3 displays noticeable anisotropic compressibility due to its layered structure and it is stable up to the highest pressure in the present study. A third-order Birch–Murnaghan fit based on the observed pressure-volume data yields zero pressure bulk moduli of180(3), 196(7) and 177(7) GPa for cubic, monoclinic and hexagonal phases, respectively. 相似文献
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利用多体耗散粒子动力学(Multibody Dissipative Particle Dynamics, Multibody DPD)方法研究了在溶剂蒸发条件下, 嵌段共聚物在表面自组装形成薄膜的过程, 分别考虑了两嵌段共聚物和三嵌段共聚物及不同组成对薄膜形貌的影响. 模拟得到了无序状薄膜和层状薄膜, 并计算了这些薄膜的序参量和薄膜厚度随时间的演化. 结果表明, 嵌段共聚物的组成对薄膜厚度几乎没有影响, 当某种组分的链段很短时, 只能形成序参量较小的无序薄膜, 相反, 则可以得到序参量较大的层状薄膜. 相似文献
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The static equation of state (EOS) of tantalum (Ta) is determined by in situ energy-dispersive synchrotron powder x-ray diffraction in a diamond anvil cell (DAC) up to 133GPa. The body-centered-cubic (bcc) phase of Ta is found to be stable over the entire pressure range investigated. The bulk moduli and its first pressure derivative of Ta are constrained by fitting the determined pressure-volume data to Vinet form EOS: B0 =192.65±(3.08)GPa and B'0 =3.58±(0.11). For the sake of avoiding the affect of non-hydrostatic stress, argon is used as a pressure media. A careful checking of the stress state of the sample is presented simultaneously. 相似文献
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通过溶剂挥发法获得了准一维C70纳米/亚微米棒状晶体,直径为~500nm, 长度为~10μm,呈六方密堆(hcp)结构. 利用金刚石对顶砧(DAC)高压装置,采用同步辐射能量色散X光能量色散衍射方法(EDXD)和高压拉曼光谱,研究了压力对C70纳米/亚微米棒结构的影响, 实验中最高压力为26.1GPa. 结果表明, 在准静水压条件下,在23.3—26.1GPa压力范围内, hcp结构的C70纳米/亚微米棒发生了由hcp结构向非晶化的相变,相变压力比体材料高约5GPa, 该相变是不可逆相变, 而且该相变是由于C70在高压下笼状结构被破坏所导致的. 相似文献