Molecular Dynamic Simulation on the Absorbing Process of Isolating and Coating of α-olefin Drag Reducing Polymer

The absorbing process in isolating and coating process of α-olefin drag reducing polymer was studied by molecular dynamic simulation method, on basis of coating theory of α-olefin drag reducing polymer particles with polyurethane as coating material. The distributions of sodium laurate, sodium dodecyl sulfate, and sodium dodecyl benzene sulfonate on the surface of α-olefin drag reducing polymer particles were almost the same, but the bending degrees of them were obviously different. The bending degree of SLA molecules was greater than those of the other two surfactant molecules. Simulation results of absorbing and accu-mulating structure showed that, though hydrophobic properties of surfactant molecules were almost the same, water density around long chain sulfonate sodium was bigger than that around alkyl sulfate sodium. This property goes against useful absorbing and accumulating on the surface of α-olefin drag reducing polymer particles; simulation results of interactions of different surfactant and multiple hydroxyl compounds on surface of particles showed that, interactions of different surfactant and one kind of multiple hydroxyl compound were similar to those of one kind of surfactant and different multiple hydroxyl compounds. These two contrast types of interactions also exhibited the differences of absorbing distribution and closing degrees to surface of particles. The sequence of closing degrees was derived from sim-ulation; control step of addition polymerization interaction in coating process was absorbing mass transfer process, so the more closed to surface of particle the multiple hydroxyl com-pounds were, the easier interactions with isocyanate were. Simulation results represented the compatibility relationship between surfactant and multiple hydroxyl compounds. The isolating and coating processes of α-olefin drag reducing polymer were further understood on molecule and atom level through above simulation research, and based on the simulation, a referenced theoretical basis was provided for practical optimal selection and experimental preparation of α-olefin drag reducing polymer particles suspension isolation agent.     

环境与生物样品中铝测定的吸光光度和荧光光度分析方法进展

本文评述了九十年代以来环境与生物样品分析中测铝的吸光光度和荧光光度分析方法的进展。对不同的方法进行了详尽的比较和讨论     

CuX／bpy催化体系中甲基丙烯酸甲酯的原子转移自由基聚合

讨论了以α－溴代丙酸乙酯（ＥＰＮ－Ｂｒ）为引发剂、卤化亚铜（ＣｕＸ）／联二吡啶（ｂｐｙ）为催化剂，８０℃下，甲基丙烯酸甲酯（ＭＭＡ）地不同溶剂中的原子转移自由基聚合（ＡＴＲＰ）反应。通过对催化剂ＣｕＢｒ或ＣｕＣｌ及几种溶剂的考察，发现在８０℃下ＥＰＮ－Ｂｒ／ＣｕＢｒ／ｂｐｙ能有效控制丙烯酸甲酯（ＭＡ）的本体ＡＴＲＰ反应，但并不能很好地控制ＭＭＡ在ＥＡｃ中的聚合反应为一可控聚合过程，引发效率为０．８     

番红花红O-Mn2+-H2O2光度法测定茶叶的抗氧化性

在硫酸介质中,Mn2 -H2O2体系产生的羟自由基可以迅速氧化番红花红O,使其颜色变浅。实验证明,茶叶提取液具有可清除溶液中的羟自由基的功能,从而使番红花红O溶液的褪色程度降低。根据溶液吸光度的这一变化,可建立一种测定茶叶对羟自由基清除率的新方法。将本法用于8种茶叶的抗氧化性的测定,结果满意。     

质谱技术研究儿茶素及儿茶素-锗多聚体特性

采用HPLC-ESI-Q-TOF和MALD I-TOF质谱技术分析儿茶素组成与结构,发现儿茶素中的表没食子儿茶素没食子酸酯(EGCG)具有多聚体特性。有机化学法合成EGCG-Ge4 化合物,并经HPLC进一步分离纯化。红外光谱和质谱技术分析并证实EGCG不仅能形成多聚体,而且还能络合金属锗(包括其他金属离子),成为EGCG-Ge4 和EGCG-Ge4 多聚体。EGCG-Ge4 抑制肺癌细胞生长速率明显高于EGCG,其提高幅度约为30%~40%左右。     

在线氧化分光光度法测定铁的价态

1 引言铁的价态影响着铁在生态系统中的迁移性、生物可利用性以及毒性.本研究基于Fe3+与钛铁试剂在酸性条件下生成蓝紫色络合物的反应原理,建立了顺序注射在线氧化测定铁的价态的光度分析方法.     

固相萃取-石墨炉原子吸收法光谱分析铝合金中痕量铍的研究

建立了固相萃取-石墨炉原子吸收光谱法测定铝合金中铍的方法。利用偶氮砷酸类试剂7-(2′-胂酸基-5′-羧酸)苯偶氮-8-羟基喹啉-5-磺酸(H2L)与Be2+形成螯合物,该螯合物可用C18固相萃取柱富集,而Al3+则不被保留。采用石墨炉原子吸收光谱法(GF-AAS)测定C18柱洗脱液中的Be2+的螯合物,从而实现铝合金中铍的分离检测。最佳实验条件为:采用pH=3.0的5%H2L水溶液螯合Be2+,水相上柱,用2mL体积比为50%的甲醇/水溶液作为洗脱液。结果表明:经过C18柱固相萃取可以去除Al3+的干扰,Be2+的测定范围为0.05～16μg/L,检出限为0.025μg/L,加标回收率为92%～108%。应用该法于铝合金标样中铍的测定,结果与认定值相符。     

淀粉基荧光微球的制备及其布洛芬包载和释药性能

以淀粉为原料,用乙酸酐酰化后,将异硫氰酸荧光素（FITC）接枝到淀粉醋酸酯大分子链上,以自组装的方法制备出包载布洛芬的淀粉基荧光微球,同时考察了淀粉基荧光纳米微球对布洛芬的控制释放性能。 荧光淀粉酯的用量、布洛芬的加入量及丙酮与水的体积比可影响载药微球的包封率和药物释放速度。 研究结果表明,当荧光淀粉酯用量为200 mg、布洛芬的量为60 mg、水和丙酮体积分别为50和20 mL时所合成的载药微球包封率最高,为69.5%,其药物体外释放也最快,48 h可释放62.7%。 用扫描电子显微镜和激光共聚焦显微镜(CLSM)对包药微球的体外释放过程进行了表征。     

pH值、盐浓度敏感性两性聚电解质微球的合成及性质

以丙烯酰胺(AM)、丙烯酰氧乙基三甲基氯化铵(DAC)和甲基丙烯酸(MAA)为单体,在乙醇介质中制备出对pH值、盐浓度双敏感的两性聚电解质微球。 采用透射电子显微镜(TEM)和红外光谱(IR)方法对其形貌和结构进行了表征。 研究了聚电解质微球在不同pH值溶液及NaCl、CaCl2盐溶液中粒径的变化情况。研究结果表明,第二步中反应制备的微球粒径为1 177 nm,多分散指数(PDI)为0.181;相比第一步反应制备的微球(d=764 nm;PDI=0.069)其粒径明显增大,PDI数值略有增加。当溶液pH＜4.3时,微球的粒径随溶液pH值的减小而逐渐增加;当pH＞4.3时,微球的粒径随溶液pH值的变大逐渐增加;pH=4.3时,微球的粒径具有最小值。盐溶液的pH值接近等电点时,在单价态NaCl溶液中,两性聚电解质微球表现出典型反聚电解质效应;而在多价态CaCl2溶液中,其粒径先增长再逐渐下降。