富氮杂环配位超分子化合物的合成、结构及光谱特征

以2,6-二(5-甲基-1H-吡唑-3-基)吡啶(简写为H2L)为第一配体,以均苯四甲酸和乙酸为第二配体,合成了2个新的配位超分子化合物[Ni(H2L)2]·(Me O-H2BTA)2(1)和Mn(H2L)(Ac)2(2)(H4BTA∶均苯四甲酸,HAc∶乙酸),并由元素分析、红外光谱、紫外-可见光谱以及X射线单晶衍射等对其进行了表征,分析了其光谱及结构特征。晶体结构分析表明,化合物1属于正交晶系,Pbcn空间群,a=0.95747(8)nm,b=1.99273(13)nm,c=2.50175(13)nm,α=90°,β=90°,γ=90°,V=4.773 3(6)nm3,Z=4;化合物2属于单斜晶系,Cc空间群,a=1.11300(13)nm,b=2.0239(2)nm,c=0.97308(12)nm,α=90°,β=118.555(16)°,γ=90°,V=1.9253(4)nm3,Z=4。     

K_2CdSnS_4的溶剂热合成与晶体结构(英文)

利用溶剂热法合成了层状硫代锡(Ⅲ)酸镉(Ⅱ)化合物K2CdSnS4。单晶X-射线衍射分析结果表明,化合物属单斜晶系,C2/c空间群,a=1.102 1(5)nm,b=1.103 0(5)nm,c=1.515 1(10)nm,α=90°,β=100.416(12)°,γ=90°,V=1.811 4(17)nm3,Z=8,Dc=3.209 g·cm-3,Mr=437.60,μ=6.853 mm-1,F(000)=1 600,λ=0.071 073 nm,R=0.104 2,wR=0.200 8。该化合物由类金刚烷[Cd2Sn2S10]8-结构单元互相连接形成层状结构。紫外-可见漫反射光谱研究表明,化合物为半导体,带隙为2.2 eV。     

硝酸钍氧化膦取代杯芳烃配合物的合成与结构

合成了一种硝酸钍与氧化膦取代杯芳烃衍生物的配合物 ,[L·Th(OH2 ) (NO3 ) 2 ] [Th(NO3 ) 6]·CH3 CN {L =四 (亚甲基二苯基氧化膦 )杯 [4 ]芳烃 }.通过元素分析和红外光谱对配合物进行了表征 .用X射线单晶衍射法测定了其晶体结构 .晶体属三斜晶系 ,P 1空间群 ,晶胞参数a =1 990 ( 7)nm ,b =2 2 17( 8)nm ,c =2 890 ( 10 )nm ;α =10 4 92 ( 12 )° ,β =10 0 76( 14 )° ,γ =93 13 ( 10 )° ,Z =4;V =12 0 3 3 ( 7)nm3 ,R1=0 0 90 1,wR2 =0 190 7.此配合物由配阳离子和配阴离子构成 .配阳离子中 ,1个Th4+ 与杯芳烃中的 4个磷氧键上的氧原子 ,2个双齿配位的硝酸根中的 4个氧原子 ,以及 1个水分子的氧原子配位 ,构成 1个九配位的单帽四方反棱柱体 ;配阴离子中 ,1个Th4+ 与 6个双齿配位的硝酸根离子配位     

一维Z形链状吡啶三唑-Zn(Ⅱ)化合物的合成、晶体结构及荧光性能

通过水热法成功合成了一例一维"Z"形链状结构的化合物[(4,3′-Hbpt)_2Zn(adp)]_n(1)(4,3′-Hbpt=3-(4-吡啶基)-5-(3-吡啶基)-1-H-1,2,4-三唑;adp=己二酸离子)),并通过X射线单晶衍射、元素分析、X射线粉末衍射和荧光光谱等方法对该化合物进行了结构表征和性质研究.X射线单晶衍射分析表明,化合物1属于单斜晶系,C2/c空间群,晶胞参数为a=1.938 8 nm,b=0.877 6 nm,c=1.844 1 nm,α=90°,β=109.1°,γ=90°,V=2.965 0 nm~3,D_c=1.470 g/cm~3,Z=4,F(000)=1 352,GOOF=0.957.在化合物1中,Zn~(2+)离子通过己二酸桥接形成一维"Z"形链状结构.此外,通过荧光光谱对化合物1的荧光性质进行了研究.     

一种新型吡啶鎓盐的合成、结构及光学性质（英文）

通过吡啶盐与3,4-二甲氧基苯甲醛在甲醇中反应,得到高氯酸4-[(3',4'-二甲氧基)苯乙烯基]-N-甲基吡啶鎓,分子式为C_(16)H_(18)ClNO_6。化合物的结构通过红外、元素分析、氢谱、电喷雾质谱和X-单晶衍射仪进行分析与表征。结果表明,该化合物属正交晶系,空间群Pbca,晶胞参数a=13. 5897(11) nm,b=13. 9126(11) nm,c=17. 3485(14) nm,α=90°,β=90°,γ=90°,M_r=355. 76,V=3280. 0(5) nm~3,Z=8,F(000)=1488,D_c=1. 181g/cm~3,μ=0. 265mm~(-1)。同时还研究了该化合物的光学性质。     

一种新型双缩合螺吡喃的合成、表征及晶体结构

以过量吲哚啉和5-硝基水杨醛为原料合成了4-(2-亚甲基-1-乙基-3,3-二甲基吲哚啉-2'-基)-6-硝基-1'-乙基-3',3'-二甲基-螺[3,4-二氢-2H-l-苯并吡喃-2,2'-吲哚啉],通过核磁共振、红外光谱、元素分析对其结构进行了表征.同时利用X单晶衍射仪测定了该化合物的结构,结果表明:晶体属单斜晶系,空间群P21/n,a=1.2476(3)nm,b=1.1939(2)nm,c=2.0317(4)nm,α=90°,β=107.45(3)°,γ=90°,Dc=1.205g/cm3,μ=0.077mm-1,F(000)=1120,V=2.8871(10)nm3,Z=4.     

N-对三氟甲基苯基-α-氨基烷基膦酸酯的合成、晶体结构及生物活性

采用活性基团拼接法将氟原子引入α-氨基烷基膦酸酯中,合成了一系列含氟芳基α-氨基烷基膦酸酯类新化合物,结构经元素分析,IR,1H NMR及MS确认.对所合成的化合物进行了抑制烟草花叶病毒(TMV)田间生物测试,结果表明,该类化合物具有良好的抑制TMV活性,其中4d化合物在0.0005%浓度下对烟草花叶病毒(TMV)防效达到了67.03%.就此对4d化合物作了单晶培养,并就晶体结构进行了X衍射分析.结构表明4d化合物分子属单斜晶系,空间群P21/c.晶胞参数a=1.1957(5)nm,b=1.0664(5)nm,c=1.5943(7)nm,α=90°,β=97.623(8)°,γ=90°,V=2.0150(15)nm3,Z=4.Dc=1.336 Mg/m3,μ=0.189nm-1,F(000)=840.     

超声辐射下2-氨基-7-甲基-4-芳基-5-氧代-4-H,5H吡喃并[4,3-b]吡喃-3-腈的“一锅法”合成

以芳醛、丙二腈与6-甲基-4-羟基-2-吡喃酮为原料,醋酸酐为溶剂,超声辐射下一步合成了2-氨基-7-甲基-4-芳基-5-氧代-4H, 5H-吡喃并[4,3-b]吡喃-3-腈系列产物.产率达72%～83%.产物结构经红外光谱、核磁共振和元素分析测试技术表征.其中化合物4e的结构经单晶X射线衍射进一步确证,单晶体属单斜晶系,空间群C2/c,晶胞参数:A=2.14917(7)nm, b=0.82498(2)nm, c=1.79137(6)nm, α=90°, β=112.104(2)°, γ=90°, Mr=314.72, V=2.94254(16)nm3, Z=8, Dc=1.421kg/m3, F(000)=1296, R=0.0495, wR=0.0878.     

基于2,5-二甲基苯-1,4-二亚甲基二膦酸的钴、镍同构化合物的水热合成及晶体结构(英文)

在水热条件下,利用2,5-二甲基苯-1,4-二亚甲基二膦酸(H4L)与CoCl2·6H2O或NiSO4·6H2O反应得到2个同构的过渡金属有机膦酸化合物,[Co(H2O)4(H2L)]n(1),[Ni(H2O)4(H2L)]n(2),并用元素分析、红外光谱、粉末及单晶X-射线等方法对其进行了表征。晶体结构分析表明:化合物1和2都属于三斜晶系,空间群为P1,化合物1的晶胞参数为a=0.497 0(2)nm,b=0.711 3(3)nm,c=1.177 8(5)nm,α=97.779(7)°,β=92.103(7)°,γ=107.217(6)°,V=0.3927(3)nm3,Z=2;化合物2的晶胞参数为a=0.494 35(19)nm,b=0.708 9(3)nm,c=1.172 6(5)nm,α=97.919(6)°,β=92.130(6)°,γ=107.441(5)°,V=0.387 0(3)nm3,Z=2。金属离子采取了八面体构型,6个配位氧原子分别来自2个反式构型的H2L配体和4个配位水分子。每1个金属离子与2个反式构型的H2L配体配位形成了一维线型链状结构。这2个化合物最终通过O-H…O氢键作用形成了三维结构。此外,对2个化合物的热稳定性也进行了研究。     

含吡唑基的1,5-苯并硫氮杂衍生物的合成及晶体结构

以1-苯基-3-甲基-5-苯氧基-吡唑-4-甲醛和1-苯基-3-甲基-5-对甲苯氧基-吡唑-4-甲醛为原料,在碱性条件下与苯乙酮(取代苯乙酮)发生羟醛缩合,合成出10种新型含吡唑基的查尔酮;再用此查尔酮与邻氨基硫酚在冰醋酸中反应,合成了10种新的1,5-苯并硫氮杂,化合物的结构经元素分析、IR和1HNMR确认,同时测定了化合物6c的晶体结构.化合物6c属单斜晶系(Monoclinic),空间群P2(1)/n,晶胞参数a=1.1793(2)nm,b=1.1907(2)nm,c=1.8726(4)nm,α=90°,β=104.71(3)°,γ=90°,M=522.04,V=2.5432(9)nm3,D=1.363Mg/m3,Z=4,F(000)=1088.     

Wetting of a drop on a sphere

In this work, the equilibrium morphology of a drop on a sphere is analyzed as a function of the contact angle and drop volume experimentally and with analytical effective interfacial energy calculations. Experimentally, a drop on a sphere geometry is realized in an oil bath by placing a water drop on a sphere coated with a dielectric, of which the radii of curvature are comparable with that of the drop. Electrowetting (EW) is used to change the contact angle of the water drop on the sphere. To validate the applicability of EW and the Lippman-Young equation on nonflat surfaces, we systematically investigate the response of the contact angle to the applied voltage (EW response) for various drop volumes and compared the results with the case of a planar surface. The effective interfacial energy of two competing morphologies, namely, the spherically symmetric "completely engulfing" and "partially engulfing" morphologies are calculated analytically. The analytical calculations are then compared to the experimental results to confirm which morphology is energetically more favored for a given contact angle and drop volume. Our findings indicate that the "partially engulfing" morphology is always the energetically more favorable morphology.     

Synthesis of a tetraazacyclotetradecadiene and a pentaazacyclotetradecatriene

Useful procedures for preparing a novel tetraazacyclotetradecadiene and a pentaazacyclotetradecatriene are reported. J. Heterocyclic Chem., 14, 1097 (1977)     

Rearrangement of a pyranone to a benzothiazole

The conversion of 2-chloromethyl-5-methoxy-4H-pyran-4-one to 2-amino-5-hydroxy-6-methoxybenzothiazole hydrochloride under mild reaction conditions has been observed. The synthesis of the identical benzothiazole by an alternate unequivocal method is also reported.     

Local pressure tensor of a simple fluid in a conelike cage of a solid

Asymptotic formulas are derived for distribution functions and components of the pressure tensor for a Van der Waals fluid in a conelike cage of a solid. The formulas describe the local behavior of the fluid far from the vertex of the cone and at rather large distances from solid walls. It is shown that, due to the symmetry of the system, three diagonal components and one off-diagonal component of the pressure tensor differ from zero. The effect of the deviation of conelike pore walls from a cylindrical shape on the appearance of a noticeable contribution to the local characteristics of the fluid in the pore is estimated.     

Thermal properties of a disc-like compound benzene-hexa-n-pentanoate: a precursor of a discotic mesogen

The heat capacity of a disk-like compound, benzene-hexa-n-pentanoate (BH5), a precursor of a discotic mesogen, has been measured by adiabatic calorimetry between 13 and 390 K. BH5 showed four different crystalline phases, but no liquid crystalline phase. Molar entropy and transition entropies were determined and compared with those of other homologues (BH6, BH7, and BH8). An odd-even effect with respect to the number of carbon atoms in the alkyl chain was observed for the cumulative entropies of the phase transitions occurring in the solid state. This effect is discussed by comparing with data for the n-alkanes. The molar entropies of the crystalline state, especially below 250 K, exhibited a peculiar 'pairing effect' between BH(2m- 1) and BH(2m), where m is an integer.     

Thermal properties of a disc-like compound benzene-hexa-n-pentanoate: a precursor of a discotic mesogen

The heat capacity of a disk-like compound, benzene-hexa-n-pentanoate (BH5), a precursor of a discotic mesogen, has been measured by adiabatic calorimetry between 13 and 390 K. BH5 showed four different crystalline phases, but no liquid crystalline phase. Molar entropy and transition entropies were determined and compared with those of other homologues (BH6, BH7, and BH8). An odd-even effect with respect to the number of carbon atoms in the alkyl chain was observed for the cumulative entropies of the phase transitions occurring in the solid state. This effect is discussed by comparing with data for the n-alkanes. The molar entropies of the crystalline state, especially below 250 K, exhibited a peculiar 'pairing effect' between BH(2m- 1) and BH(2m), where m is an integer.