甲烷在Mo/HZRP-1催化剂上无氧脱氢芳构化反应Ⅰ.Mo/HZRP-1催化剂的催化性能和积炭行为

用高 硅含磷五 员环 沸 石 分子 筛（ 商 品 代号 Ｈ Ｚ Ｒ Ｐ１） 作 为 载体 ，制 备 了 Ｍｏ／ Ｈ Ｚ Ｒ Ｐ１ 催化剂． 与 Ｍｏ／ Ｈ Ｚ Ｓ Ｍ５ 相比， Ｍｏ／ Ｈ Ｚ Ｒ Ｐ１ 对 甲烷无 氧脱氢芳 构化反 应也表现 出较好的 催化 性能 ． 实验过程 中，在反 应气中添 加 Ｎ２ 作 为内标 物，给出包 括甲烷 在 Ｍｏ／ Ｈ Ｚ Ｒ Ｐ１ 上 的结焦量 、转化率 及各产物选 择性在内 的总碳 物料平衡 计算结果 ． 考 察了不同 Ｍｏ 担 载量对催 化剂性 能和 积炭 行为 的影响； 重点考察 了不同 温度焙烧 后２０ ％ Ｍｏ／ Ｈ Ｚ Ｒ Ｐ１ 催化剂 的性能和 积炭行 为． 在 反应的初 始阶段 ，６ ％ Ｍｏ／ Ｈ Ｚ Ｒ Ｐ１ 表 现出 很 高 的 活 性： 反 应 进 行 ３０ ｍｉｎ 时， 甲 烷 转 化 率 为 １１ ％ ， 芳 烃 选 择 性 达８１ ％ ， 而催化 剂的结焦 选择性 仅为１２ ％ ． Ｂ Ｅ Ｔ， Ｎ Ｈ３ Ｔ Ｐ Ｄ 和 催 化反 应等 表 征结 果表 明： Ｍｏ 物种的数量 和状态， 分子筛的 酸强度和 酸量以 及分子筛 的孔道 结构是 决定 甲烷 无氧 脱氢 芳构 化反 应性能和积 炭行为 的关键因 素．     

Ph_3P/Mo~Ⅵ体系对吡啶-N-氧化物的脱氧反应

近年来,吡啶-N-氧化物在吡啶衍生物的合成中,日见重要。由于吡啶环上氮原子的电子效应,使吡啶环上的亲电取代反应较难发生,但将吡啶转变成其N-氧化物后,就改变了吡啶环上的电荷密度,使亲电反应能顺利地在2、     

Synthesis and Structure of a New Dinuclear Molybdenum(Ⅰ)Compound with Cyclohexanthiolate Ligand,[Mo_2(SC_6H_(11)_2(CO)_8]

<正>Molybdenum( I )-compound [Mo2(SC6H11)2(CO)8] 1, crystallizes in monoclinic, space group P21/c with a = 9.5863(9), b = 9.4469(9), c = 13.869(1) A, β = 99.697(2)°, V= 1238.1(2) A3, Z = 2,DC= 1.734 g/cm3, μ = 12.23 cm-1 and F(000) = 644. The finalR = 0.0455 and wR = 0.1159 for 1590 observed reflections with I> 2σ(I). 1 possesses a rhombic bimetallic core MoS2Mo with the Mo-Mo bond length of 2.975(1) and Mo-S of 2.485(2) A.     

Two molybdenum (VI) monophosphates with a tunnel structure: AMoO2PO4 (A=Cs, Tl) and structural relationships in the series

Two new molybdenum (VI) monophosphates CsMoO₂PO₄ and TlMoO₂PO₄ have been synthesized by solid state chemistry. Their structure were determined from single crystal X-ray diffraction studies. The frameworks MoO₂PO₄ delimit tunnels in which are located the univalent cations. Structural relationships between the different monophosphates of the AMoO₂PO₄ series with A = Ag, Na, K, Tl, Cs, are presented in which two kinds of frameworks appear owing to the size of the univalent cations.     

地质环境中微量元素与人类心血管疾病

介绍了地质环境中三种微量元素硒，铜，钼的分布特点及与人类心血管疾病的关系。     

In-situ TEM observation of the evolution of helium bubbles in Mo during He+ irradiation and post-irradiation annealing

The evolution of helium bubbles in purity Mo was investigated by in-situ transmission electron microscopy (TEM) during 30 keV He⁺ irradiation (at 673 K and 1173 K) and post-irradiation annealing (after 30 keV He⁺ irradiation with the fluence of 5.74×10¹⁶ He⁺/cm² at 673 K). Both He⁺ irradiation and subsequently annealing induced the initiation, aggregation, and growth of helium bubbles. Temperature had a significant effect on the initiation and evolution of helium bubbles. The higher the irradiation temperature was, the larger the bubble size at the same irradiation fluence would be. At 1173 K irradiation, helium bubbles nucleated and grew preferentially at grain boundaries and showed super large size, which would induce the formation of microcracks. At the same time, the geometry of helium bubbles changed from sphericity to polyhedron. The polyhedral bubbles preferred to grow in the shape bounded by {100} planes. After statistical analysis of the characteristic parameters of helium bubbles, the functions between the average size, number density of helium bubbles, swelling rate and irradiation damage were obtained. Meanwhile, an empirical formula for calculating the size of helium bubbles during the annealing was also provided.     

ChemInform Abstract: From 1∞ [(UO2)2O(MoO4)4]6‐ to 1∞ [(UO2)2(MoO4)3(MoO5)] 6‐ Infinite Chains in A6U2Mo4O21 (A: Na,K, Rb,Cs) Compounds: Synthesis and Crystal Structure of Cs6 [(UO2)2(MoO4)3(MoO5)] .

Single crystals of the title compound are obtained from a melt of U₃O₈, MoO₃, and excess Cs₂CO₃ (Pt crucible, 950 °C, 12 h, cooling rate 5 °C/h).