聚伊文思蓝修饰电极对多巴胺和抗坏血酸的电分离及同时测定

研究多巴胺(DA)和抗坏血酸(AA)在聚伊文思蓝(Evans Blue)修饰电极上的伏安行为,建立差示脉冲伏安测定法.在pH4.5磷酸盐缓冲液中,聚伊文思蓝修饰电极对DA和AA有显著的增敏和电分离作用.DA和AA氧化峰电流与浓度分别在1.0×10-6~3.0×10-5mol/L和5.0×10-6~1.05×10-4mol/L范围内呈良好的线性关系,检测限分别为2.5×10-7mol/L和3.0×10-7mol/L.当DA与AA共存时,由该修饰电极检测的二者氧化峰电位差达184 mV,故可同时测定DA和AA,并有效消除其它组分对DA测定的干扰,已用于实际样品中DA和AA含量的测定,结果令人满意.     

双嵌段共聚物混合体系形态结构及相变研究

用自洽平均场理论(SCMFT)研究了由两种不同双嵌段共聚物(diblock copolymer)组成的混合体系在纳米尺度下的自组装行为.有较高聚合度的纯diblock1熔体呈层状有序结构;有较低聚合度的纯diblock2熔体呈均匀(无序)相.SCMFT研究表明,在二者的混合体系中,当diblock1的体积分数在0·7~1·0之间时,混合体系呈现层状结构;而当diblock1的体积分数在0·4~0·6之间时,体系呈现六角排布的柱状结构.这一理论研究结论与近期报道的实验结果有较好的吻合.同时,通过混合体系单体密度分布曲线和嵌段的连接点分布曲线,从理论上分析了混合体系中单体分布的细节.     

固化剂对环氧树脂/聚砜共混物层状结构形成的影响

不同含量的聚砜(PSF)对环氧树脂(EP)/PSF共混物相结构有重要影响,通过对反应分相后的样品进行断面观察,发现一定PSF含量时,体系形成了层状结构.这种层状结构通常为3层,包括上下2个外层、由聚砜和环氧树脂的颗粒-基体结构组成,以及1个双连续结构形成的中间层.研究表明,这种层状结构由反应诱导相分离开始之初形成的双连续结构发展而来,由于反应和相分离的进一步发展热塑性树脂富集相的体积分数逐渐减小、以及组分间的动力学不对称而最终形成的.在一定PSF浓度范围内,不同温度固化样品时均得到了这种层状结构.改变固化剂类型,层状结构的形貌受到影响,当固化剂活性较高时,外层变薄中间层增厚.当组分间的相容性较好时,双连续结构甚至不能演化发展到层状结构.     

Ru~(3+)增敏的化学发光新体系测定呋塞米的研究

Ru~(3+)存在下,呋塞米能够大幅度增强三(1,10-菲咯啉)钌(Ⅱ)(Ru(phen)_3~(2+))-Ce(Ⅳ)体系的化学发光,且当体系中Ru~(3+)的浓度从0增至15μmol/L时,呋塞米对体系发光的增强值提高1个数量级,基于此,建立了高灵敏测定呋塞米的Ru(phen)_3~(2+)-Ce(Ⅳ)-Ru~(3+)体系化学发光方法。在优化实验条件下,该法测定呋塞米的线性范围为5. 0×10~(-9)~2. 0×10~(-6)mol/L,检出限为3. 8×10~(-9)mol/L。方法具有较高的分析灵敏度,将其应用于呋塞米片剂和呋塞米注射液的分析,结果满意。结合紫外光谱的研究结果,对化学发光反应机理进行了探讨。     

用刚果红分光光度法测定阳离子表面活性剂

在弱酸性的HCl-NaAc缓冲介质中,某些阳离子表面活性剂(CS)与刚果红(CR)反应,形成离子缔合物时,刚果红发生褪色作用,最大褪色波长分别在510nm(CR-溴化十六烷基吡啶(CPB)体系)、514nm(CR-十六烷基三甲基溴化铵(CTAB)体系)。在最大褪色波长处,CS的浓度在0~4.16×10-5mol.L-1(CPB体系)、0~3.18×10-5mol.L-1(CTAB体系)范围内遵守比尔定律,表观摩尔吸光系数为1.62×104L/(mol.cm)(CPB体系)、1.72×104L/(mol.cm)(CTAB体系),检出限为9.78×10-7mol.L-1(CPB体系)、1.04×10-6mol.L-1(CTAB体系)。方法具有较高的灵敏度和良好的选择性,用于水样中CS的测定,结果满意。     

L-苯丙氨酸衍生物与脂肪胺构筑双组分超分子凝胶

设计合成了系列单链L-苯丙氨酸衍生物,该系列衍生物单组分没有胶凝性能.选择脂肪胺作为配对物,与L-苯丙氨酸衍生物组成双组分体系后能够胶凝许多有机溶剂形成凝胶.流变学测试显示该凝胶体系弹性模量(G′)比粘性模量(G′′)约高一个数量级,有着很好的机械性能,并且呈现出典型的类固体的流变学行为.傅里叶变换红外(FT-IR)光谱、核磁共振(NMR)谱、小角X射线衍射(SAXS)和扫描电镜(SEM)结果表明,凝胶中胶凝剂分子形成纤维状或片层状的聚集体,羧基(―COOH)和氨基(―NH2)的酸碱作用、酰胺基团间(―CONH―)的氢键作用以及分子间范德华作用力是形成该凝胶的主要驱动力.凝胶中胶凝剂分子自组装形成具有周期性的层状有序结构,层状结构进一步组装形成纤维状聚集体,最终形成三维网状结构阻碍溶剂流动形成凝胶.     

毛细管电泳-安培法测定复方磺胺甲噁唑片中的有效成分

采用毛细管电泳-安培法(CE-AD)同时分离测定了磺胺甲噁唑(sulfamethoxazole,SMZ)、磺胺嘧啶(sulfadiazine,SD)和抗菌增效剂甲氧苄胺嘧啶(trimethoprim,TMP)3种常用磺胺类抗菌药物成分,考察了实验参数对分离、检测体系的影响。在优化实验条件下,以300μm碳圆盘电极作为工作电极,检测电位为1050mV(vs.SCE),在Na2B4O7(13mmol/L)-KH2PO4(18mmol/L)(pH5.8)的缓冲溶液中,分离电压18kV,进样6s,3组分在14min内可实现基线分离。上述3组分浓度分别在5×10-4~5×10-2、5×10-4~0.1和5×10-4~5×10-2g/L范围内与其峰电流强度呈线性关系,检出限达5.1×10-5~8.0×10-5g/L(S/N=3)。该方法已成功应用于复方磺胺甲噁唑片中抗菌活性成分的含量测定,结果令人满意。     

水介质中二甲基姜黄素脂质体对金属离子的荧光识别

通过薄膜分散法制备二甲基姜黄素(ASC-J9)脂质体,其粒径分布均匀且在水中的分散效果好,平均粒径为145. 7 nm,分散系数为0. 361。将ASC-J9脂质体作为水溶性的荧光探针,通过荧光猝灭法可选择性识别Fe~(3+)、Fe~(2+)及Cu~(2+)。经过条件筛选得到最佳荧光测试条件为:ASC-J9脂质体浓度为5. 0×10~(-5)mol/L,平衡时间5 min,测试温度25℃。由Job's曲线和荧光滴定结果判断该探针与Fe~(3+)和Cu~(2+)的络合比均为1∶1,与Fe~~(2+)的络合比为2∶1; Stern-Volmer方程判断该荧光猝灭类型为静态猝灭,结合常数分别为KFe(Ⅲ)=9. 63×10~4L/mol,KFe(Ⅱ)=3. 65×10~5L/mol,KCu(Ⅱ)=2. 32×10~5L/mol;该识别体系检测快速、灵敏度高,对Fe~(3+)、Fe~(2+)、Cu~(2+)的线性范围分别为:5. 0×10~(-7)~3. 0×10~(-5)、5. 0×10~(-7)~1. 75×10~(-5)、5. 0×10~(-7)~2. 5×10~(-5)mol/L,检出限分别为6. 41×10~(-7)、3. 28×10~(-7)、5. 08×10~(-7)mol/L。     

基于间苯二甲酰腙的荧光探针的合成及其接力识别Al3+和焦磷酸根

设计合成了一种基于2-羟基-1-萘甲醛和间苯二甲酰肼的简单高效的荧光探针L,其结构通过~1H NMR、~(13)C NMR和HRMS进行表征。在乙醇-水(1∶1)的体系中,L能够高选择性识别铝离子,表现出明显的荧光增强,并具有较低的检测限(5. 924×10~(-6)mol/L),二者结合比为1∶2。此外,原位生成的配合物L-2Al~(3+)可接力识别焦磷酸根(PPi),具有良好的选择性和灵敏度,检测限可达4. 756×10~(-5)mol/L。该荧光探针具有潜在的应用价值。     

层状液晶中水溶性超微粒子材料[Co(NH~3)~6]Cl~3的制备

利用溶剂在层状液晶中的渗透性和层状液晶中溶剂厚度的限定性, 在TritonX-100/C~10H~21OH/H~2O体系层状液晶中, 以4%Co(NH~3)~6]Cl~3水溶液组分水制备水溶性超微粒子材料[Co(NH~3)~6]Cl~3, 粒径约为3~6nm。     

纳米粒子驱动受限环境下两嵌段共聚物/均聚物混合体系的自组装行为

采用含时金兹堡-朗道理论(time-dependent ginzburg-landau theory,简称TDGL)方法研究了纳米粒子(nanoparticles,简称NPs)掺杂的两嵌段共聚物/均聚物(AB/C)共混体系在球形受限下的自组装行为.在不同球形受限条件下,两嵌段共聚物/均聚物共混体系形成了多种丰富的形貌,如双螺旋结构、单螺旋结构、层状结构和洋葱环状结构等.当在以上前3种体系中掺杂纳米粒子后,体系结构发生了很大的变化.详细研究了纳米粒子的浓度和浸润强度对以上结构的影响.研究结果表明,通过调控纳米粒子的浓度和浸润性质,该共混体系实现了双螺旋结构→层状结构,单螺旋结构→双螺旋结构,层状结构→单螺旋结构等多种取向序的转变.对于洋葱环状结构,纳米粒子的加入对体系这一结构的影响不大.     

PHOTOLESIONS AND BIOLOGICAL INACTIVATION OF PLASMID DNA ON 254 nm IRRADIATION AND COMPARISON WITH 193 nm LASER IRRADIATION

Plasmid pTZ18R and calf thymus DNA in aerated neutral aqueous solution were irradiated by continuous 254 nm light. The quantum yields are φ_ssb= 4.0 × 10^-5 and φ_dsb= 1.4 × 10^-6 for single- and double-strand break formation, respectively, φ_br= 2.3 × 10^-5 for base release, φ_dn= 2.1 × 10^-3 for destruction of nucleotides, and φ_icl×φ_lds× 1 × 10^-6 for interstrand cross-links and locally denatured sites, respectively. The presence of Tris-HCI/ ethylenediaminetetraacetic acid (10:1, pH 7.5) buffer strongly reduces φ_ssb, The corresponding φ values, obtained on employing pulsed 193 nm laser irradiation, are much larger than those using λ_irr, = 254 nm. This is ascribed to a contribution of chemical reactions induced by photoionization, which is absent for 254 nm irradiation. The quantum yields of inactivation of plasmid DNA (λ_irr= 254 nm) were measured by transformation of the Escherichia coli strains AB1157 (wild type), φ_ina(1157) = 1.6 × 10^-4, AB1886 (uvr^-), φ_ina(1886) = 4.2 × 10^-4, AB2463 (rec^-), φ_ina(2463) = 4.1 × 10^-4 and AB2480 (uvr^- rec^-), φ_ina(2480) = 3.1 × 10^-3. The quantum yields of inactivation of plasmid DNA are compared with those of the four E. coli strains (denoted as chromosomal DNA inactivation) obtained from the literature. The results for E. coli strain AB2480 show that the chromosomal DNA and the plasmid DNA are both inactivated by a single pyrimidine photodimer per genome. With the E. coli strain AB2463 inactivation of plasmid and chromosomal DNA is the same for the same total damage per genome and is ～ 10 times smaller than for AB2480. This is explained by photodimer repair in chromosomal and plasmid DNA and by the absence of dsb repair in both cases. In the repair wild-type strain AB1157, inactivation of the plasmid DNA is roughly 100 times higher than that of the chromosomal DNA. We postulate that a portion of this difference is due to repair of dsb by the recA system in chromosomal DNA and that such repair does not take place in the plasmid DNA. The biological results from 254 nm irradiation are compared with those from 193 nm laser irradiation.     

一种聚氧乙烯醚链三头季铵盐表面活性剂的合成

以五甲基二乙烯三胺（PMDETA）、脂肪醇聚氧乙烯醚（FAPOE）和环氧氯丙烷（ECP）为原料,分两步合成了一种含聚氧乙烯醚链三头季铵盐的表面活性剂。对反应影响因素、产物结构与部分性能进行了分析与表征。结果表明：第一步反应n（ECP）：n（FAPOE）为2．5～3：1,溶剂为正己烷,四丁基溴化铵作相转移催化剂,无水K2CO3作缚酸剂,时间6～8h。第二步反应n（中间体）：n（PMDETA）为3．5—4．0：1,溶剂为正丁醇,时间40-45h;溶剂与时间是主要影响因素。定性表征符合产物结构：定量表征n（Cl^-）：n（阳离子部分）为3．4：1,略高于理论值。产物的表面活性高,1．0×10^-4mol／L水溶液的表面张力可降至6．65mN／m。     

Phase behavior and interfacial properties of diblock copolymer-homopolymer ternary mixtures: Influence of volume fraction of copolymers and interaction energy

We use a Monte Carlo method to study the phase and interfacial behaviors of A-b-B diblocks in a blend of homopolymers, A and B, which are confined between two asymmetric hard and impenetrable walls. Our results show that, when the interaction strength is weak, the block copolymersare uniformly distributed in the ternary mixtures under considered concentrations. Under strong interaction strength, distribution region of the block copolymers changes from a single smooth interface to a curved interface or multi-layer interface in the ternary mixtures. Furthermore, our findings show that with increasing volume fraction of A-b-B diblock copolymer(фC), copolymer profiles broaden while фC≥ 0.4, a lamellar phase is formed and by further increasing фC, more thinner layers are observed. Moreover, the results show that, with the increase of фC, the phase interface first gradually transforms from plane to a curved surface rather than micelle or lamellar phase while with the increase of the interaction between A and B segments(ε_(AB)), the copolymer chains not only get stretched in the direction perpendicular to the interface, but also are oriented. The simulations also revealthat the difference between symmetric and asymmetric copolymers is negligible in statistics if the lengths of two blocksare comparable.     

2-氨基-5-(对二甲氨基)苯基-1,3,4-噻二唑: Hg2+的选择性荧光传感分子

设计合成了结构简单的分子内电荷转移荧光传感分子1,3,4-噻二唑类衍生物(1), 实现了水-乙醇(体积比1∶9)混合溶剂中Hg2+的荧光猝灭型选择性灵敏传感, 荧光猝灭常数达5.5×105 mol-1·L, Hg2+线性响应范围为5.0×10-6～5.0×10-5mol/L. 基于等摩尔连续变化法、红外光谱和核磁滴定实验结果提出了传感分子1与Hg2+的1∶1型结合模式, 其中1-位S原子和2-位胺N原子为Hg2+配位原子; 结合光谱变化讨论了Hg2+结合显著增强分子内电荷转移的荧光猝灭机理.     

非MAO的茂钛均相催化体系催化苯乙烯间规聚合——[Cp~*TiMe_3]/[Ph_3C]~+[B(C_6F_5)_4]~-催化体系

非ＭＡＯ的茂钛均相催化体系催化苯乙烯间规聚合———［ＣｐＴｉＭｅ３］／［Ｐｈ３Ｃ］＋［Ｂ（Ｃ６Ｆ５）４］－催化体系许光学林尚安（中山大学高分子研究所广州５１０２７５）关键词茂钛络合物，茂金属催化剂，苯乙烯，间规聚苯乙烯间规聚苯乙烯（ｓＰＳ）由于具...     

两种四噻吩并萘分子晶体电荷传输性质的理论研究

采用密度泛函理论(DFT)方法结合不相干的电荷跳跃模型和随机Monte Carlo模拟,研究了2种四噻吩并萘晶体(AT1和AT2)的分子结构、电子性质及电荷载流子传输参数,并预测了这2种晶体室温下空穴和电子迁移率的各向异性.结果表明标题化合物具有近似平面的刚性骨架结构,电荷传输过程中分子的结构弛豫相当小.基于绝热势能面法计算的AT1和AT2分子空穴/电子传输内重组能分别为9.300×10~(-2)/1.100×10~(-1)eV和1.020×10~(-1)/1.290×10~(-1) eV,外重组能分别为1.835×10~(-2)/1.711×10~(-2) eV和1.857×10~(-2)/1.747×10~(-2) eV.利用Monte Carlo随机模拟方法预测的2种分子晶体室温(300K)下空穴/电子迁移率平均值分别为4.976×10~(-3)/2.766×10~(-2) cm~2 V~(-1)s~(-1)和3.857×10~(-3)/1.478×10~(-2)cm~2 V~(-1)s~(-1).此外,迁移率的角度依赖性研究表明2种载流子在AT1和AT2晶体aob平面传输时表现出显著的各向异性,其最大值均沿着电荷传输积分最大的方向,为制备高性能场效应晶体管器件提供了参考.     

Solution self-assembly of the sophorolipid biosurfactant and its mixture with anionic surfactant sodium dodecyl benzene sulfonate

The self-assembly in aqueous solution of the acidic (AS) and lactonic (LS) forms of the sophorolipid biosurfactant, their mixtures, and their mixtures with anionic surfactant sodium dodecyl benzene sulfonate, LAS, has been studied using predominantly small-angle neutron scattering, SANS, at relatively low surfactant concentrations of <30 mM. The more hydrophobic lactonic sophorolipid forms small unilamellar vesicles at low surfactant concentrations, in the concentration range of 0.2 to 3 mM, and transforms via a larger unilamellar vesicle structure at 7 mM to a disordered dilute phase of tubules at higher concentrations, 10 to 30 mM. In marked contrast, the acidic sophorolipid is predominantly in the form of small globular micelles in the concentration range of 0.5 to 30 mM, with a lower concentration of larger, more planar aggregates (lamellar or vesicular) in coexistence. In mixtures of AS and LS, over the same concentration range, the micellar structure associated with the AS sophorolipid dominates the mixed-phase behavior. In mixtures of anionic surfactant LAS with the AS sophorolipid, the globular micellar structure dominates over the entire composition and concentration range studied. In contrast, mixtures of LAS with the LS sophorolipid exhibit a rich evolution in phase behavior with solution composition and concentration. At low surfactant concentrations, the small unilamellar vesicle structure present for LS-rich solution compositions evolves into a globular micelle structure as the solution becomes richer in LAS. At higher surfactant concentrations, the disordered lamellar structure present for LS-rich compositions transforms to small vesicle/lamellar coexistence, to lamellar/micellar coexistence, to micellar/lamellar coexistence, and ultimately to a pure micellar phase as the solution becomes richer in LAS. The AS sophorolipid surfactant exhibits self-assembly properties similar to those of most other weakly ionic or nonionic surfactants that have relatively large headgroups. However, the more hydrophobic nature of the lactonic sophorolipid results in a more complex and unusual evolution in phase behavior with concentration and with concentration and composition when mixed with anionic surfactant LAS.     

Flow-Injection Spectrophotometric Determination of Oxalate,Citrate and Tartrate Based on Photochemical Reactions

Abstract

A flow-injection configuration for the spectrophotometric determination of oxalate, citrate and tartrate is proposed. The procedure is based on the photochemical decomposition of the complexes formed between iron(III) and these anions. The iron(II) produced in the photochemical reactions was detected by measuring the absorbance after complexation with ferrozine (λ_max=562 nm). Linear calibration graphs were obtained over the concentration ranges 5.0 × 10^?6 - 1.0 × 10^?4 M, 8 × 10^?6 - 1.8 × 10^?4 M and 1.0 × 10^?6 - 2 × 10^?5 M for oxalate, citrate and tartrate, respectively. The relative standard deviations at the 1x10^?5 M concentration level were within the range 1.29 - 1.47 %. The sampling frequency was about 40 samples h^?1. The usefulness of the method was tested in the determination of oxalate in urine and spinach, of citrate in pharmaceuticals and soft drinks and of tartrate in pharmaceuticals. For the determination of oxalate in urine samples a prior separation of the analyte by precipitation with calcium chloride is recommended.     

Liquid crystalline dendrimer of the fifth generation: From lamellar to columnar structure in thermotropic mesophases

The structure of a liquid crystalline (LC) carbosilane dendrimer of the fifth generation bearing 128 terminal cyanobiphenyl mesogenic groups has been studied. This dendrimer was synthesized by a hydrosilylation reaction and then the cyanobiphenyl mesogenic groups were chemically linked to the dendritic matrix via a-OOC-(CH2)10-Si(CH3)2OSi(CH3)2-spacer. Structural studies carried out by polarizing optical microscopy, differential scanning calorimetry and X-ray diffraction methods revealed unusual phase behaviour. At room temperature the dendrimer forms a lamellar (smectic A) phase which develops in-plane ordering above 40C.This is due toa tendency to form columns ofmolecules which areprobably perpendicular to the layers. Above 121C the material transforms into another more disordered mesophase which is probably a disordered hexagonal columnar phase. The proposed structures and molecular packing in these different types of mesophase are discussed.