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以三羟甲基乙烷为原料, 通过脱水反应首先制得3-羟甲基-3'-甲基氧杂环丁烷(HMO). HMO再分别与丙烯腈和二缩三乙二醇单甲醚反应得到两个取代氧杂环丁烷单体3-(2-氰基乙氧基)甲基-和3-[甲氧基(三乙氧基)]甲基-3'-甲基氧杂环丁烷(HMOAN和HMOPEO). 再用阳离子开环聚合方法, 以BF 3\5乙醚作催化剂, 丁二醇为引发剂, 将两类单体共聚即可得到一系列不同组成的共聚物(PAP). 利用 1H NMR谱图计算了该共聚物中两种不同结构单元的比, 结果表明, 其与投料比基本吻合. GPC测得该共聚物的数均分子量范围为2 756~5 342, 分子量分布为1.26~1.83. DSC测试结果发现, 除在225~246 K之间有一个玻璃化转变温度之外, 在305~348 K之间还存在一个热转变温度. TGA测得共聚物的分解温度为573 K, 远高于目前广泛使用的液体电解质. 电导率测试结果表明, AN20的室温电导率可达到1.07×10 -5 S/cm, 353 K时电导率可达到2.79×10 -4 S/cm, 接近实用要求. 相似文献
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以三羟甲基乙烷为原料,通过脱水反应首先制得3-羟甲基-3′-甲基氧杂环丁烷(HMO).HMO再分别与丙烯腈和二缩三乙二醇单甲醚反应得到两个取代氧杂环丁烷单体3-(2-氰基乙氧基)甲基-和3-[甲氧基(三乙氧基)]甲基-3′-甲基氧杂环丁烷(HMOAN和HMOPEO).再用阳离子开环聚合方法,以BF3.乙醚作催化剂,丁二醇为引发剂,将两类单体共聚即可得到一系列不同组成的共聚物(PAP).利用1H NMR谱图计算了该共聚物中两种不同结构单元的比,结果表明,其与投料比基本吻合.GPC测得该共聚物的数均分子量范围为2 756~5 342,分子量分布为1.26~1.83.DSC测试结果发现,除在225~246 K之间有一个玻璃化转变温度之外,在305~348 K之间还存在一个热转变温度.TGA测得共聚物的分解温度为573 K,远高于目前广泛使用的液体电解质.电导率测试结果表明,AN20的室温电导率可达到1.07×10-5S/cm,353 K时电导率可达到2.79×10-4S/cm,接近实用要求. 相似文献
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近十几年来,N原子上带有保护基团的α,β脱氢氨基酸及其衍生物的新的合成方法,由于发现这类化合物存在于微生物、低等植物和海生动物体中而具有重要意义。另 相似文献
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3,3-二硝基氮杂环丁烷和1,1′-亚甲基-双(3,3-二硝基-1-氮杂环丁烷)的合成研究 总被引:2,自引:0,他引:2
3,3-二硝基氮杂环丁烷(DNAZ)的含能盐及衍生物是一类重要的高能量密度材料,因此DNAZ的合成和应用受到了密切关注.采用新的合成方法,以1-叔丁基-3,3-二硝基氮杂环丁烷为起始原料,以76.3%的总收率得到了DNAZ,然后以DNAZ为原料,与多聚甲醛反应,得到了1,1′-亚甲基-双(3,3-二硝基-1-氮杂环丁烷)(DNAZ-CH2-DNAZ).用红外和核磁共振光谱等对各化合物的结构进行了表征. 相似文献
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由2-乙氧羰基-3-硝基-1,1,1-三氟丁烷(1b)与异氰基乙酸乙酯发生Barton-Zard反应制备2-乙氧羰基-3-三氟甲基-4-甲基吡咯(1)的过程中,分别用K2CO3和乙醇代替有机碱1,8-二氮杂二环[5.4.0]十一碳-7-烯(DBU)和四氢呋喃溶剂,这种改进的Barton-Zard方法具有操作简便、试剂价廉易得、溶剂毒性低和产率更高等优点。 另外,在3-硝基-1,1,1-三氟-2-丁醇(1a)通过乙酰化反应转变为中间体1b的过程中,用沸腾温度下的甲苯溶液与乙酰氯代替浓硫酸催化下的酸酐反应体系;合成化合物1b的最优化的反应条件被确定为:乙酰氯与反应物1a之间的摩尔比为1.2∶1,反应时间为3~3.5 h。 又根据改进的卟啉合成法,在低温下用过量氢化铝锂还原吡咯1,将还原所得的尚未干燥或储存的粗产物α-羟甲基-三氟甲基-4-甲基吡咯(1c),立即在未经处理的三氯甲烷溶剂中,以三氟化硼·乙醚(BF3·OEt2)为催化剂进行四聚化反应,然后用2,3-二氯-5,6-二氰基-1,4-苯醌(DDQ)氧化,合成出含三氟甲基取代的卟啉衍生物2。 研究发现,由化合物1c制备产物2时,用BF3·OEt2取代p-TsOH作为催化剂,在确定的反应条件下,能够将产物2的收率由14%提高至50%。 相似文献
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Molecular dynamics computer simulation based on the Born-Mayer-Huggins potential function has been carried out to study the effects of duster size and temperature on the nucleation rate of sodium chloride dusters in the temperature range of 580 K to 630 K. Clusters with 256 and 500 NaCl molecules have been studied and the results have been compared with those obtained from 108 molecule dusters. The melting point (MP) of the clusters were observed to increase with the size of the clusters and can be well described by a linear equation MP =1107(37)-1229(23)N^-1/3(N is the number of molecules in the duster).The nucleation rate was found to decrease with increasing the duster size or temperature. Various nucleation theories have been used to interpret the nucleation rates obtained from this molecular dynamics simulation. It is possible to use a constant diffuse interface thickness to interpret the nucleation rate from the diffuse interface theory in the temperature range of this study. However, the interfacinl free energy estimated from classical nucleation theory and diffuse interface theory increases too fast with increasing the temperature while that from Gran-Gunton theory does not change with changing temperatures.The sizes of critical nuclei estimated from all the theories are smaller than those estimated from our simulations. 相似文献
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Molecular dynamics computer simulations have been carried out to study the effects of cluster size and temperature on the nucleation rate of rubidium chloride clusters in the temperature range of 500-650 K. Clusters with 256 and 500 RbCl molecules have been studied and the results are compared with those obtained from 108 molecule clusters. The melting point (MP) of the clusters was observed to increase with the size of the clusters and can be described by a linear equation MP=997-405 N−1/3, where N is the number of molecules in the cluster. The nucleation rate is found to decrease with increasing cluster size or increasing nucleation temperature. Both classical nucleation theory and diffuse interface theory are used to interpret our observed results. 相似文献
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YANG Wei-wei DI You-ying LI Jing KONG Yu-xia 《高等学校化学研究》2010,26(2):304-308
The crystal structure of ephedrine hydrochloride was determined by means of X-ray crystallography.The crystal system of the compound is monoclinic,and the space group is P21.Unit cell parameters are a=0.7308(6) nm,b=0.6124(5) nm,and c=1.2618(11) nm;α=90°,β=102°,and γ=90°;Z=2.Low-temperature heat capacities of the title compound were measured with an improved precision automated adiabatic calorimeter over a temperature range from 77 K to 396 K.A polynomial equation of the heat capacities as a function of temperature in the temperature region was fitted by the least-squares.Based on the fitted polynomial equation,the smoothed heat capacities and thermodynamic functions of the compound relative to the standard reference temperature 298.15 K were calculated and tabulated at the intervals of 5 K. 相似文献
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双核钴簇合物(C6H5C2R)Co2(CO)6的合成 总被引:1,自引:0,他引:1
羰基钴簇合物Co2(CO)8可用于有机合成的催化剂。但Co2(CO)8本身不稳定,易被氧化。因此,研究不向CO2簇合物的稳定性及其催化性能具有一定的意义。 相似文献
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CrystalStructureof3-hydroxyl-1,5-diazacycloheptaneDihydrobromideC_5H_(12)N_2O·2HBrLIUYong;XUEGuo-Ping;WUCheng-Tai(Departmentof?.. 相似文献
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SynthesisandCrystalStructureofSquarateComplex[CuLaSm(C_4O_4)_4(H_2O)_(16)]·2H_2O¥ShiJing-Min;YanShi-Ping;LiaoDai-Zheng;JiangZong... 相似文献
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1 INTRODUCTION Norfloxacin (0.16 g, 5 mmol) and PdCl2 (0.02 g) in methanol solution. The brown solution was filtered Norfloxacin (H-Norf = 1-ethyl-6-fluoro-1,4-dihy- and the filtrate was stood undisturbed. Single crys- dro-4-oxo-7-(1-piperazinyl)-3-quinoline carboxylic tals suitable for X-ray analysis were obtained by slow- acid), a quinolone type compound, is widely used as ly evaporating the methanol solvent at 20 ℃. an antibacterial drug which targets the bacterial type 2. 2 TGA an… 相似文献
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5-苯基-3,5-二乙氧基-2(5H)-呋喃酮的晶体结构 总被引:1,自引:0,他引:1
标题化合物C14H16O4的晶体结构用X-射线单晶衍射法测定。晶体属三斜晶系,P空间群,晶胞参数a =8.696(2), b=8.943(2) , c=9.379(2) ?, ( = 69.28(3), ( =76.67(3), ( =80.28(3)o, V=660.8(3) ? 3, Z=2, Mr=248.28, Dx=1.248 g/cm3, F(000)=264, μ(MoK()=0.0851 mm—1。晶体结构用直接法解出,经全矩阵最小二乘法对原子参数进行修正,最终的偏离因子为R=0.061, wR=0.089。标题化合物有2个环:呋喃酮环和苯环。由C(1),C(2),C(3),C(4),O(4)构成的五元呋喃酮环的5个原子较好地处于1个平面上,平均偏差为0.0078?。O(2),O(3) 两个原子与呋喃酮环共平面。呋喃酮环和苯环之间的两面角为79.39o。 相似文献
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铂单晶电极表面下不可逆反应动力学(III) 总被引:5,自引:0,他引:5
在本系列研究论文Ⅰ[1]和Ⅱ[2]报导的结果基础上,进一步发展动力学数据解析方法.通过改变反应体系的温度,首次获得甲酸在Pt(100),Pt(110),Pt(111)电极上直接氧化反应的表观活化Gibbs自由能(△G≠0).在实验选定的标准状态下,即0.0V/SCE、298.15K和1.013×105Pa下,来算得到。还发现传递系数β在实验温度范围(283.15~303.15K)不随温度变化,但随电极表面原子排列结构变化,大小次序与△G≠0的变化一致. 相似文献