Vertical uplift resistance of two closely spaced horizontal strip anchors embedded in cohesive-frictional weightless medium

The vertical uplift resistance of two closely spaced horizontal strip plate anchors has been investigated by using lower and upper bound theorems of the limit analysis in combination with finite elements and linear optimization. The interference effect on uplift resistance of the two anchors is evaluated in terms of a nondimensional efficiency factor (eta(c)). The variation of eta(c) with changes in the clear spacing (S) between the two anchors has been established for different combinations of embedment ratio (H/B) and angle of internal friction of the soil (phi). An interference of the anchors leads to a continuous reduction in uplift resistance with a decrease in spacing between the anchors. The uplift resistance becomes a minimum when the two anchors are placed next to each other without any gap. The critical spacing (S-cr) between the two anchors required to eliminate the interference effect increases with an increase in the values of both H/B and phi. The value of S-cr was found to lie approximately in the range 0.65B-1.5B with H/B = 1 and 11B-14B with H/B = 7 for phi varying from 0 degrees to 30 degrees.

Structural investigation of resorcinol based symmetrical banana mesogens by XRD, NMR and polarization measurements

Synthesis and structural characterization of two novel symmetrical banana mesogens built from resorcinol with seven phenyl rings linked by ester and imine with a terminal dodecyl/dodecyloxy chain has been carried out. Density functional theory (DFT) has been employed for obtaining the geometry optimized structures, the dipole moments and C-13 NMR chemical shifts. The HOPM and DSC studies revealed enantiotropic B-2 and B-7 phases for the dodecyl and dodecyloxy homologs respectively. The powder X-ray studies of both the mesogens indicate the presence of layer ordering. The polarization measurements reveal an anti-ferroelectric switching for the B-2 phase of the dodecyl homolog whose structure has been identified as SmCSPA. The B-7 phase of the dodecyloxy homolog was found to be non-switchable. High resolution C-13 NMR study of the dodecyl homolog in its mesophase has been carried out. C-13-H-1 dipolar couplings obtained from the 2-dimensional separated local field spectroscopy experiment were used to obtain the orientational order parameters of the different segments of the mesogen. Very large C-13-H-1 dipolar couplings observed for the carbons of the central phenyl ring (9.7-12.3 kHz) in comparison to the dipolar couplings of those of the side arm phenyl rings (less than 3 kHz) are a direct consequence of the ordering in the banana phase and the shape of the molecule. From the ratio of the local order parameter values, the bent-angle of the mesogen could be determined in a straight forward manner to be 120.5 degrees.

塑性大应变微结构力学

《塑性大应变微结构力学》涉及以下三部分内容：小应变塑性力学；大应变分析；微结构力学分析及其应用。书中既论述有关的数学、力学基础知识，又介绍了学科前沿的研究成果。

第三版前言
第二版前言
第一版前言
第一部分小应变塑性力学
第一章直角坐标系中的向量和张量
1.1直角坐标与单位向量
1.2微积分运算中的公式
1.3坐标变换
1.4Descartes张量张量代数和张量演算
1.5两种张量表示方法的说明
练习
参考文献
第二章微小变形下的应力张量和应变张量
2.1一点上的应力
2.2一点上的应变
2.3平衡方程
2.4协调条件
练习
参考文献
第三章屈服准则和塑性理论
3.1屈服
3.2塑性理论中的公设
3.3流动理论
3.4比例加载下的形变理论
3.5塑性计算的示范
练习
参考文献
第四章塑性力学的发展
4.1基于塑性耗散能的本构形式
4.2近似蠕变分析-比应力-应变曲线方法
4.3机动硬化模型
4.4角点理论
4.5相关的和非相关的流动法则
参考文献
第二部分大应变分析
第五章一般坐标系中的张量及其各类时间导数
5.1一般坐标系中的基量
5.2坐标变换张量及协变导数
5.3坐标系统
5.4变换时间导数的Oldroyd方程
练习
参考文献
第六章应变张量应力张量和它们的变化率
6.1应变张量
6.2各类应变率张量
6.3应力张量
6.4应力张量的各种变化率
练习
参考文献
第七章在有限变形下平衡的变分原理及分叉理论
7.1固体的弹性超弹性和亚弹性
7.2变分原理及应力与应变的共轭关系
7.3平衡的稳定性和分叉准则
7.4Lagrange和逐级更新Lagrange系统中平衡和分叉的增量型变分原理
7.5大应变本构方程及数值计算步骤
练习
参考文献
第三部分微结构力学及其应用
第八章确定材料的总体力学行为与其微结构参数之间的
关系
8.1"自洽"原则
8.2塑性力学中的内变量
8.3用计算机模拟方法确定内变量
练习
参考文献
第九章空洞的分析
9.1空洞的萌生和扩展的试验
9.2单级空洞效应的理论模型
9.3两级空洞效应的理论模型
9.4空洞化材料的宏观响应与力学和几何微观参数之间的关系
9.5基于微结构研究成果所设立的连续介质本构模型和失效准则
9.6空洞化损伤的三维分析及探讨应变加载模态影响的方法
9.7应变加载模态对空洞化损伤材料力学性能的影响及其与次级空洞间的交互作用
参考文献
第十章剪切带状分叉
10.1材料分叉的原理
10.2平面应变条件下的局部化剪切带
10.3材料非均匀性或初始缺陷的影响
10.4轴对称加载下的局部化轴对称剪切带
10.5局部化曲线剪切带
10.6局部化剪切带的三维解
10.7平面应变条件下扩散型剪切带的一维分析
10.8平面应变条件下扩散型剪切带的二维分析
参考文献
第十一章空洞和分叉的分析在金属板材成型中应用
11.1平面应力模型中空洞扩展效应
11.2分叉分析
11.3双相钢薄板成型实验与数值分析的比较
11.4单向加载条件下平板的材料分叉
参考文献
第十二章韧性断裂
12.1塑性可膨胀本构方程的论证
12.2确定本构参数
12.3韧性断裂的计算
12.4韧姓断裂的实验
参考文献
附录A弹性力学基本方程
A.1广义Hooke定律
A.2平面问题
A.3轴对称问题
A.4弹性力学解的可叠加性和惟一性
A.5St.Venant原理
练习
参考文献
附录B弹性力学变分原理及解法
B.1应变能和应变余能
B.2虚位移和虚功原理
B.3最小势能原理
B.4最小余能原理
B.5两个变分原理的关系
B.6双变量广义变分原理
B.7基于变分原理的直接解法
练习
参考文献

三种萝藦科植物中C21甾类成分的研究

　　本实验对三种萝藦科植物通光散(Marsdenia tenacissima)、黑水藤（Biondia insignis Tsiang）和徐长卿（Cynanchum Paniculatum）中的C21甾体化合物进行了研究。从通光散藤茎乙酸乙酯提取物的水解产物中，分离得到两类八个C21甾类甙元。经光谱鉴定，它们的结构分别为11α-O-(2-甲基)-丁酰基-12β-O-顺芷酰通光藤甙元乙（1），11α-O-乙酰基-12β-O-乙酰基通光藤甙元乙（2），11α-O-（2-甲基）-丁酰基-12β-O-乙酰基通光藤甙元乙(3), 11α-O-苯甲酰基-12β-O-乙酰基通光藤甙元乙(4)， 11α-O-顺芷酰基-12β-O-乙酰基通光藤甙元乙（5）11α-O-顺芷酰基-12β-O-顺芷酰基通光藤甙元乙（6），12β-O-乙酰基通光藤甙元甲（7）和12β-O-顺芷酰基通光藤甙元甲（8）。其中，化合物2和8为新化合物。从黑水藤乙醇提取物的水解产物中，分离得到了两个C21甾体化合物。经1D、2D NMR技术鉴定，分别为（3β，14β，15β，17β）-3, 14-二羟基-15，16-裂-孕甾-5-烯-15-醛-16-半缩醛-20-酮（1）和白前甙元C（2）。其中1为15，16-裂环的新骨架类型的C21甾体化合物，命名为黑水藤甙元甲。从采购于昆明、浙江、湖南三地药材市场的徐长卿的根及根茎中，分离得到了18个化合物（其中昆明徐长卿6个，浙江徐长卿9个，湖南徐长卿3个）。经光谱数据分析，这些化合物被鉴定为：cynapanoside-C (1), cynapanoside-A (2), 白前甙元B 3-O-β-D-磁嘛吡喃糖甙(3)，白前甙元C 3-O-β-D-葡萄吡喃糖基-(1 → 4)-α-L-2-脱氧洋地黄吡喃糖基-（1 → 4）-β-D-洋地黄吡喃糖基-（1 → 4）-β-D-夹竹吡喃糖甙（4），白前甙元C3-O-β-D-葡萄吡喃糖基-(1 → 4)-α-D-夹竹桃吡喃糖基-(1 → 4)-β-D-洋地黄吡喃糖基-(1 → 4)-β-D-夹竹桃吡喃糖甙（5），白前甙元C 3-O-β-D-葡萄吡喃糖基-（1 → 4）-β-D-葡萄吡喃糖基-（1 → 4）-α-D-夹竹桃吡喃糖基-（1 → 4）-β-D-洋地黄吡喃糖基-（1 → 4）-β-D-夹竹桃吡喃糖甙（6），cynatratoside-B (7)，cynatratoside-C (8);glaucoside A(9)，新白薇甙元B 3-O-β-L-磁嘛吡喃糖基-（1 → 4）-β-D-洋黄吡喃糖基-（1 → 4）-β-D-夹竹桃吡喃糖甙（10），白前甙元 A 3-O-α-L-磁嘛吡喃糖基-（1 → 4）-β-D-洋地黄吡喃糖基-（1 → 4）-β-D-磁嘛吡喃糖甙（11），白前甙元 B 3-O-α-L-磁糖基吡喃糖基-(1 → 4)-β-D-磁嘛吡喃糖基-(1 → 4)-β-D-磁嘛吡喃糖甙(12)，白前甙元D 3-O-α-L-磁嘛吡喃糖基（1 → 4）-β-D-洋地黄吡喃糖基-（1 → 4）-β-D-磁嘛吡喃糖甙（13），白前甙元 C 3-O-β-D-葡萄吡喃糖基-（1 → 4）-β-D-葡萄吡喃糖基-（1 → 4）-α-L-2-脱氧洋地黄吡喃糖基-（1 → 4）-β-D-磁嘛吡喃糖基-（1 → 4）-β-D-夹竹桃吡喃糖甙（14），白前甙元 C 3-O-β-D-葡萄吡喃糖基-（1 → 4）-β-D-葡萄吡喃糖基-（1 → 4）-α-L-磁嘛吡喃糖基-（1 → 4）-β-D-洋地黄吡喃糖基-（1 → 4）-β-D-夹竹桃吡喃糖甙（15），白前甙元 B 3-O-α-D-夹竹桃吡喃糖基-(1 → 4)-β-D-洋地黄吡喃糖基-（1 → 4）-β-D-磁嘛吡喃糖甙（16），白前甙元 D 3-O-α-D-夹竹桃吡喃糖基-(1 → 4)-β-D-洋地黄吡喃糖基-(1 → 4)-β-D-磁嘛吡喃糖甙(17)，白前甙元月B 3-O-α-L-磁嘛吡喃糖基-(1 → 4)-β-D-洋地黄吡喃糖基-(1 → 4)-β-D-磁嘛吡喃糖甙（18）。其中，化合物3-6，10-18为新化合物，10的甙元为一个新甙元，命名为新白薇甙无B。

Isolation and characterization of miscellaneous terpenoids of Schisandra chinensis

Two new bisnortriterpenoids with 18-norschiartane skeleton, wuweizidilactones G (1) and H (2), four new highly oxygenated nortriterpenoids based on a schisanartane skeleton, schindilactones D-G (3-6), a pre-schisanartane skeleton, pre-schisanartanin B (7)

扁担塘两种底栖动物的周年生产量

研究了1996年4月至1997年3月间扁担塘两种底栖动物———幽蚊和圆扁螺的周年生产量,采用体长频率法测算的生产量分别是:幽蚊周年生产量湿质量为0.1419g·m-2·a-1,干质量为0.0114g·m-2·a-1,P/B系数为1.8;圆扁螺的周年生产量带壳湿质量为1.6266g·m-2·a-1,去壳干质量为0.0732g·m-2·a-1,P/B系数为7.1.但与国外数据相比,这些结果比较适中,说明扁担塘并不是幽蚊和圆扁螺的最适生长环境.

铜的多元复合物组成、结构和电学性质的研究

本论文包括三个部分的内容，第一部分研究了Y-Ba-Cu-O材料中，钙、钾、氟离子的掺入对材料结构和电、磁学性质的影响。1、在Y_(1-x)Ca_xBa_2Cu_3O_(7-y)系列中，当x ≤ 0.15时，钙离子进入了YBa_2Cu_3O_(7-y)晶格中钇离子的位置，使晶胞参数略为增大，但没有引起正交 → 四方相变。钙离子渗入导致123相中Cu~(3+)含量上升，同时材料的监界超导转变温度下降。因此，Cu~(3+)含旱管高可能是对超导电性不利的。由于钇离子位置紧邻着Cu(2)-O平面而与Cu(1)-O链相隔较远。因此，钇离子被钙离子替代时主要影响了Cu(2)-O平面的性质。少量钙离子的渗入即明显影响材料的超导电性，这说明Cu(2)-O平面的性质与超导电性密切相关，并可能起着关键的作用。2、在Y(Ba_(1-x)Ca_x)_2Cu_3O_y系的研究中，当x = 1，YCa_2Cu_3O_y是一个单一的化合物，文献未见报道，本文研究了它的结构，电学性质与热学性质，确定它的结构属正交晶系，a = 5.286 A、b = 7.636 A、c = 9.286 A。热分析表明YCa_2Cu_3O_y在1080 ℃分解，分解前于380 ℃ 和608 ℃出殃失氧现象。这个化合物是黑色n型半导体。室温电阻率1.2 * 10~5Ω·cm。与热分析中的失氧温度相对应，lnρ-1/T曲线上在370 ℃、620 ℃ 出现两个转折点。3、在Y-Ba-Cu-O材料中渗入钾离子能细化材料晶粒，降低超导转变宽度，提高零电阻温度，但由于KOH、K_2CO_3等强吸湿性杂质的存在也降低了材料的稳定性。4、在Y-Ba-Cu-O材料中间时掺入钾和氟离子时，材料的超导电性的变化与仅掺钾时相似。这种变化可能主要是钾离子的影响造成的。第二部分中，我们研究了Ca-Sr-Ca-O系的相图和新化合物Sr_3Cu_5O_(8+x)、CaSrCu_3O_(5+x)的结构和电学性质。在第三部分中，广泛研究了组成为Bi_tSr_vCa_wCu_zO_y超导材料的制备，结构和超导电性。铋系超导材料的形成貌与YBa_2Cu_3O_y材料有较大差异，前者是片状层叠的晶粒堆积而成，后者是球状小颗粒堆积而成的。我们合成的材料最高起始转变温度124K，最高零电阻温度112K，与国际上已达到的最高Tc值一致。Jc值达到131A/cm~2。

三面压缩进气道三维激波相干研究

三面压缩式高超声速进气道在侧压式进气道的基础上加入顶面压缩，理论上具有的更短的压缩距离，从而有利于超声速飞行器的整体设计。该进气道不同于传统的顶压式进气道和侧压式进气道，由于其压缩激波在竖直和水平方向都存在，因此出现三维空间的激波相交和反射，造成流场复杂度大大增加，而其也直接影响了进气道设计构型与波系的相对位置关系及进气道性能。\newline 三面压缩进气道由于顶板与侧板两个方向压缩，在顶板与侧板相交线附近区域，激波并不是简单的二维平面激波结构。顶压激波和侧压激波相交后，在波型上产生了明显的变化。在角区的激波相干后的波系结构：顶板激波与侧壁激波相交后，都变得不再连续，即在相互"穿越"的过程中发生了"断裂"，出现了过渡的桥波2。然而对该相干结构的认识目前也仅限于此，其流动的特征,对进气道性能的影响以及如何规划三面压缩进气道设计构型都还需要深入的探索。忽略激波边界层干扰，专注于激波相干现象本身，对于这种三维激波相干结构开展了无黏数值分析研究，探索了其关键影响因素，理论分析了其相干特征。\newline 本文分析认为角区波系可分成$A$，$B$，$C$，$D$，$E$5个部分，$A$为未经激波压缩的区域；$B$为只经过顶压激波3压缩的区域：$C$为只经过侧压激波1压缩的区域；$D$为经过顶压激波3和侧压激波1共同压缩的区域；$E$为过桥波2压缩的区域。对于顶压激波来说，$B$区域的气体与$D$区域的气体参数并不相同，因为$D$区域的气体还经过了侧压激波的压缩，因此在相同的气流转角下，$D$区域的顶板激波角大于$B$区域的顶板激波角，所以顶压激波在穿越侧压激波后发生了"断裂"，7的位置高于3的位置；同理，侧压激波穿越顶压激波后，4的位置也会向对称面移动，侧压激波也发生"断裂"。基于以上物理模型，应用二维激波关系，探索性给出的三维激波相干位置的无黏近似计算方法。\newline 数值研究进一步发现相干结构产生的桥波区域为低总压区，对进气道总压恢复系数不利。

中药蜘蛛香的化学成分研究及以羧甲基魔芋葡苷聚糖-壳聚糖为细胞膜的天冬酰胺酶人工细胞研究

本论文由三章组成。第一章介绍了中药蜘蛛香的化学成分的研究成果，第二章为羧甲基魔芋葡苷聚糖-壳聚糖为细胞膜的天冬酰胺酶人工细胞的研究，第三章综述了人工细胞在生物医学领域的应用。 第一章报道了中药蜘蛛香（Valeriana wallichii）根部乙醇提取物的化学成分，采用正、反相硅胶层析等分离方法和MS、NMR等多种波谱手段，从中共分离鉴定出17个化合物，分别为缬草素(valtrate，1)，valechlorine（2），homobadrinal（3），baldrinal（4），乙酰缬草素(acevaltrate 5)，valeriotetrate C（6），valeriotetrate B（7），对羟基苯乙酮(4'-hydroxy-acetophenone 8)，7-hydroxy valtrate（9），8-methylvalepotriate（10），1,5-dihydroxy-3,8-epoxyvalechlorine A（11），二氢缬草素(didrovaltrate 12)，胡萝卜苷（13），橙皮苷 (hesperidin 14)，prinsepiol-4-O-β-D-glucopyranoside（15），longiflorone（16），乙基糖苷（17）。其中化合物6、7、10、和11为新化合物，化合物9、15、16为首次从该植物中得到。新化合物11为含有氯原子的刚性骨架环烯醚萜，并且确定了其绝对构型。 第二章报道了以羧甲基魔芋葡苷聚糖（CKGM）和壳聚糖（CS）为膜的固定化L-天冬酰胺酶人工细胞研究成果。利用羧甲基魔芋葡苷聚糖和壳聚糖两种生物相容性很好的天然多糖之间的静电吸引力，在非常温和的条件下制备成具有半透过性膜的人工细胞，将治疗儿童急性成淋巴细胞性白血病(ALL)的药物L-天冬酰胺酶包裹在内。通过考察温度和pH对人工细胞的影响,结果表明以CKGM- CS为膜的L-天冬酰胺酶人工细胞对温度和pH的稳定性和耐受性均高于自由酶，说明CKGM-CS对酶具有保护作用，而且小分子底物和产物可以自由进出膜内外，而包裹在膜内的生物大分子则不能泄露出来。 第三章综述了微囊化人工细胞的研究进展。 This dissertation consists of three parts. In the first part, the chemical constituents from the root of Valeriana wallichii were reported. In the second part, preparation and characteristics of L-Asparaginase Artificial cell were reported. The third part is a review on progress of microcapsule artificial cell. The first chapter is about the isolation and identification of the chemical constituents from the root of V. wallichii. Seventeen compounds were isolated from the ethanol extract of roots of V. wallichii through repeated column chromatography on normal and reversed phase silica gel. By the spectroscopic and chemical evidence, their structures were elucidated as valtrate (1), valechlorine (2), homobadrinal (3), baldrinal (4), acevaltrate (5), valeriotetrate C (6), valeriotetrate B (7), 4'-hydroxy-acetophenone (8), 7-hydroxy valtrate (9), 8-methylvalepotriate (10), 1,5-dihydroxy-3,8-epoxyvalechlorine A (11), didrovaltrate (12), daucosterol (13), hesperidin (14), prinsepiol-4-O-β-D-glucopyranoside (15), longiflorone (16), and ethyl glucoside (17). Among them, 6, 7, 10, and 11 are new compounds. 15, 16 and 9 were isolated from this plant for the first time. The absolute configuration of compound 11, an unusual iridoid bearing a C-10 chlor-group and an oxo-bridge connecting C-3 and C-8 resulting in a rigid skeleton, was confirmed. The second chapter is about the semi-permeable microcapsule of carboxymethyl konjac glucomannan-chitosan for L-asparaginase immobilization. Carboxymethyl konjac glucomannan-chitosan (CKGM-CS) microcapsules, which have good biocompatibility, prepared under very mild conditions via polyelectrostatic complexation, were used for immobilize L-asparaginase-a kind of drug for acute lymphoblastic leukemia (ALL). The activity and stability under different temperature and pH of the enzyme loaded-microcapsules were studied. The results indicated the immobilized enzyme has better stability and activity contrasting to the native enzyme. The study illustrates that the L-asparaginase could be protected in CKGM-CS microcapsules, the substrate and product could pass through the system freely.

Self-assembly of diblock copolymer mixtures in confined states: A Monte Carlo study

The self-assembly of diblock copolymer mixtures (A-b-B/A-b-C or A-b-B/B-b-C mixtures) subjected to cylindrical confinement (two-dimensional confinement) was investigated using a Monte Carlo method. In this study, the boundary surfaces were configured to attract blocks A but repel blocks B and C. Relative to the structures of the individual components, the self-assembled structures of mixtures of the diblock copolymers were more complex and interesting. Under cylindrical confinement, with varying cylinder diameters and interaction energies between the boundary surfaces and the blocks, we observed a variety of interesting morphologies. Upon decreasing the cylinder's diameter, the self-assembled structures of the A(15)B(15)/A(15)C(15) mixtures changed from double-helix/cylinder structures (blocks B and C formed double helices, whereas blocks A formed the outer barrel and inner core) to stacked disk/cylinder structures (blocks B and C formed the stacked disk core, blocks A formed the outer cylindrical barrel), whereas the self-assembled structures of the A(15)B(7)/B7C15 mixtures changed from concentric cylindrical barrel structures to screw/cylinder structures (blocks C formed an inside core winding with helical stripes, whereas blocks A and B formed the outer cylindrical barrels) and then finally to the stacked disk/cylinder structures.

Structure and liquid crystalline properties of 5-[(4 '-heptoxy-4-biphenylyl)carbonyloxy]-1-pentyne

The crystal structure and liquid crystalline properties of a biphenyl-containing acetylene, [5-[(4'-heptoxy-4- biphenylyl) carbonyloxy]-1-pentyne (A3EO7) were investigated by electron crystallography, X-ray diffraction, polarizing optical microscopy, differential scanning calorimetry, transmission electron microscopy, and atomic force microscopy. A3EO7 crystals obtained from a toluene solution adopts a monoclinic P112/m space group with unit cell parameters of a = 6.25 Angstrom, b = 7.82 Angstrom, c = 46.70 Angstrom and gamma = 96.7degrees, as determined using electron diffraction. Upon cooling from the isotropic phase, A3EO7 exhibits a smectic A phase in the temperature range 72.4 - 53.6degreesC. Further lowering of the temperature results in the formation of a smectic C phase which exhibits a strong tendency towards crystallization.

Syntheses and crystal structures of [Mn(H2O)(4)(bpy)]L center dot 4H(2)O, [Mn(H2O)(4)(bpy)]L ' center dot 4H(2)O (H2L = SUCCINIC ACID, H2L ' = FUMARIC ACID)

Reactions of freshly prepared M(OH)(2-2x)(CO3)(x) (.) yH(2)O (M = Mn, Zn) and 4,4'-bipyridine (bpy) with succinic acid (H2L) or famaric acid (H2L') in CH3OH-H2O afforded [Mn(H2O)(4)(bpy)]L (.) 4H(2)O, 1, [Mn(H2O)(4)(bpy)]L' (.) 4H(2)O, 2 and [Zn(H2O)(4)(bpy)]L (.) 4H(2)O, 3. The three coordination polymers are isostructural and consist of (1)(infinity)[M(H2O)(4)(bpy)(2/2)](2+) cationic chains, crystal H2O molecules and dicarboxylate anions (succinate or fumarate anions). Within the chains, the metal atoms are each octahedrally coordinated by four aqua oxygen atoms and two pyridyl nitrogen atoms from two 4,4'-bipyridine ligands. The crystal H2O molecules are hydrogen bonded to dicarboxylate anions to form ribbon-like anionic chains. The cationic and anionic chains are interconnected via hyqrogen bonds to generate a 3D network. Crystal data: 1 triclinic, P (1) over bar, a = 7.235(1), b = 7.749(2), c = 10.020(2) Angstrom, alpha = 79.95(3), beta = 88.79(3), gamma = 71.39(3)degrees, V = 523.9(2) Angstrom(3) and D-cal = 1.494 g cm(-3) for Z = 1; 2 triclinic, P (1) over bar, a = 7.127(1), b = 7.800(2), c = 9.945(2) Angstrom, alpha = 80.26(3), beta = 87.86(3), gamma = 72.69(3)degrees, V = 520.2(2) Angstrom(3) and D-cal = 1.498 g cm(-3) for Z = 1; 3 triclinic, P (1) over bar, a = 7.189(1), b = 7.764(2), c = 9.843(2) Angstrom, alpha = 79.16(3), beta = 87.80(3), gamma = 71.29(3)degrees, V = 510.9(2) Angstrom(3) and D-cal = 1.559 g cm(-3) for Z = 1.

Crystal structure of 11-{[(4 '-heptoxy-4-biphenylyl) carbonyl]oxy}-1-undecyne

The crystal structure of 11-{[(4'-heptoxy-4-biphenylyl) carbonyl] oxy}-1-undecyne (A9EO7), an acetylene with a biphenyl mesogenic moiety, was studied by combination of electron diffraction (ED), wide-angle X-ray diffraction (WAXD), and molecular simulation of ED pattern and molecular packing. A9EO7 was found to adopt an orthorhombic P2(1)2(1)2 space group with cell parameters of a = 5.78 Angstrom, b = 7.46 Angstrom, and c = 63.26 Angstrom, for which molecular packing calculations were conducted to elucidate the molecular conformation. Its crystal morphology was observed using a transmission electron microscope (TEM) and an atom force microscope (AFM). A9EO7 crystal grew to form step like morphology. Crystallization behavior of A9EO7 in magnetic field was examined. Induced by magnetic field A9EO7 could crystallize in such a way that its molecular long axis was parallel to the substrate.

Structure, electric and magnetic properties of new compounds CdYMWO7 (M = Cr and Mn)

Two new compounds with the formula of CdYMWO7 (M = Cr, Mn) were prepared by solid state reaction. They crystallized with orthorhombic structure with the cell parameters of a = 11.7200 Angstrom, b = 7.1779 Angstrom, c = 6.9805 Angstrom (CdYCrWO7), and a = 11.7960 Angstrom, b = 6.1737 Angstrom, c = 7.6530 Angstrom (CdYMnWO7). These compounds are insulators with high resistivities at room temperature. The temperature dependence of the magnetic susceptibility of CdYMWO7 (M = Cr and Mn) show Curie-Weiss Law's behaviors from 80 to 300 K. The magnetic moments at room temperature fit very well with those corresponding to Cr3+ and Mn3+ ions. This suggests that both Cr and Mn ions exist in + 3 oxidation state in CdYMWO7 compounds. (C) 1998 Elsevier Science Ltd. All rights reserved.