等温滴定量热法和荧光滴定法研究十二烷基硫酸钠与纤维素酶的结合

用等温滴定量热法和荧光滴定法研究了阴离子型去垢剂十二烷基硫酸钠（SDS ）与绿色木霉纤维素酶相互作用的热力学，SDS结合纤维素酶的亲和力较弱，为较 小的放热反应，并伴随着一定程度的熵增，为焓和熵共同驱动的反应，而且存在着 显著的焓-熵补偿作用。该结合过程的摩尔恒压热容为较大的负值（-186 J·mol~ (-1)·K~(-1)），这表明疏水相互作用是形成复合物的主要作用力，SDS的加入使 纤维素酶的内源荧光发生猝灭，同时导致该蛋白荧光光谱最大发射峰位的红移和酶 活力的部分丧失，这表明SDS与纤维素酶的相互作用既包含结合反应也包含SDS诱导 该蛋白部分去折叠的过程。     

时间分辨荧光技术与荧光寿命测量

介绍了时间分辨荧光技术与荧光寿命的测量方法、意义及应用。     

差示扫描量热法测定食用油脂的热氧化稳定性及氧化寿命

利用差示扫描量热法（DSC）测定了四种食用花生油的热氧化稳定性,用Ozawa法和Kissinger法计算了四种食用花生油热氧化反应的动力学参数,推算了不同温度下的氧化寿命。     

荧光素钠荧光寿命的测定

通过测定不同温度下荧光素钠溶液的荧光偏振度和粘度,根据Ｐｅｒｒｉｎ公式测定荧光素钠的荧光寿命。在ＰＨ值为８．５,溶液浓度为１．６＊１０＾－５ｍｏｌ／Ｌ的条件下,测得荧光素钠的荧光寿命为３．４ｎｓ,Ｐ〈０．２,测定方法的准确度较高。     

以腐植酸为对象开展稳态和时间分辨荧光实验教学

腐植酸是天然有机质的重要组成部分,其结构复杂且具有多种荧光发射特征。我们结合目前环境科学领域腐植酸或其他天然有机质的研究重点,利用腐植酸开展稳态和时间分辨荧光综合实验教学。本实验可以使学生全面掌握分子荧光分析中拉曼散射、激发光能量对荧光发射影响、荧光寿命和内滤效应等知识。     

CaWO4荧光体的微波热法合成和光致发光

本文报道微波热法合成 Ca WO4荧光体 ,X射线粉末衍射分析确证为四方晶系 ,Ca WO4:Pb0 .0 1 荧光体最大激发波长 λex=2 66.0 nm,最大发射波长 λem=450 .0 nm,在 2 54nm激发下 ,色坐标 x=0 .1 66,y=0 .1 2 4 ,与市售同类荧光体比较 ,相对发光亮度 86% ,荧光体中心粒径 D50 为9.1 8μm,体积比表面 SV 为 81 93 1 / cm。     

微量量热法研究淀粉酶催化反应

酶催化水解反应;热动力学;微量量热法研究淀粉酶催化反应     

量热法研究氯化铒与甘氨酸配合物的标准生成焓

量热法测定;量热法研究氯化铒与甘氨酸配合物的标准生成焓     

溶解量热法测三氧化钼标准生成焓

用溶解量热法,以KIO_4和KOH组成的弱碱性溶液为量热溶剂,设计3个不同的热化学循环,用RD-1型热导式自动量热计测定了MoO_3的标准生成焓,并推荐其值为ΔH_(t(moO_3))~0(298.15K)=-765.0±6.8kJ·mol~(-1)。     

伯胺N1923氯仿萃取盐酸和磷酸振荡反应的量热法研究

萃取振荡反应;微量量热法;伯胺N1923氯仿萃取盐酸和磷酸振荡反应的量热法研究     

Counterion and composition effects on discotic nematic lyotropic liquid crystals II. Ion exchange and molecular dynamics

The static fluorescence quenching of pyrene by bromide, at the interface of mixed TTAC/TTAB discotic nematic lyotropic liquid crystals, allowed an estimation of the equilibrium constant for the exchange of chloride by bromide. The affinity of the interface for bromide is much higher than for chloride (K(Br-/Cl-) = 13.2). For a molecular level understanding of the experimental results of this and the preceding paper, 20 ns molecular dynamics (MD) simulations were calculated for samples with TTAB/TTAC molar percent ratios 100/0 (A), 50/50 (B) and 0/100 (C). The increment in the concentration of chloride induces a wider distribution of ammonium headgroups along the axis normal to the bilayer surface, increasing the width of the interface. The charge density profile of simulation B shows that the concentration of bromide is higher than the concentration of chloride in the vicinity the ammonium headgroups. The short range contribution to the electrostatic energy from the ammonium-ammonium repulsion is 291.7 kJ/mol for TTAC and 195.6 kJ/mol for TTAB, and the short range ammonium-halide interaction is -6166 kJ/mol for TTAC and -6607 kJ/mol for TTAB, from simulations A and C, respectively. These results are in agreement with a more neutralized TTAB interface. Consistently, the electric dipole moments of water are significantly more aligned with the larger electric field of the TTAB interface.     

一个新型钌(Ⅱ)配合物的合成、表征与DNA的键合及溶剂变色性质

合成和表征了1个新的钌(Ⅱ)配合物[Ru(bpy)₂(dpapz)](ClO₄)₂,其中bpy=2,2'-联吡啶,dpapz=联吡啶并[3,2-a:2,'3-'c]-6-氮杂-吩嗪.通过紫外可见光谱、荧光光谱、与溴化乙锭的竞争键合实验和粘度测量研究了该配合物与小牛胸腺DNA的键合性质,并研究了该配合物的紫外可见光谱和荧光光谱的溶剂变色性质.结果表明,该配合物是具有键合常数Kb=6.9×10⁵L/mol(50mmol/LNaCl)的DNA嵌入键合试剂和优良的荧光溶剂传感分子.     

吲哚咪唑基钌(Ⅱ)联吡啶配合物与酵母RNA的相互作用

通过紫外-可见光谱和荧光光谱滴定、稳态荧光猝灭和溴化乙啶竞争键合实验研究了Ru(Ⅱ)配合物[Ru(bpy)(H₂iip)₂](ClO₄)₂{bpy=2,2′-联吡啶, H₂iip=2-(吲哚-3-基)-咪唑[4,5-f][1,10]-邻菲罗啉}的酵母RNA键合性质. 结果表明, 二者键合模式为嵌入键合, 其键合常数为7.09×10⁶ L/mol, 比小牛胸腺DNA的键合常数大, 且比同类配合物[Ru(bpy)₂(H₂iip)](ClO₄)₂的酵母RNA键合常数大.     

The experimental and theoretical QM/MM study of interaction of chloridazon herbicide with ds-DNA

We report a multispectroscopic, voltammetric and theoretical hybrid of QM/MM study of the interaction between double-stranded DNA containing both adenine-thymine and guanine-cytosine alternating sequences and chloridazon (CHL) herbicide. The electrochemical behavior of CHL was studied by cyclic voltammetry on HMDE, and the interaction of ds-DNA with CHL was investigated by both cathodic differential pulse voltammetry (CDPV) at a hanging mercury drop electrode (HMDE) and anodic differential pulse voltammetry (ADPV) at a glassy carbon electrode (GCE). The constant bonding of CHL-DNA complex that was obtained by UV/vis, CDPV and ADPV was 2.1×10(4), 5.1×10(4) and 2.6×10(4), respectively. The competition fluorescence studies revealed that the CHL quenches the fluorescence of DNA-ethidium bromide complex significantly and the apparent Stern-Volmer quenching constant has been estimated to be 1.71×10(4). Thermal denaturation study of DNA with CHL revealed the ΔTm of 8.0±0.2°C. Thermodynamic parameters, i.e., enthalpy (ΔH), entropy (ΔS°), and Gibbs free energy (ΔG) were 98.45 kJ mol(-1), 406.3 J mol(-1) and -22.627 kJ mol(-1), respectively. The ONIOM, based on the hybridization of QM/MM (DFT, 6.31++G(d,p)/UFF) methodology, was also performed using Gaussian 2003 package. The results revealed that the interaction is base sequence dependent, and the CHL has more interaction with ds-DNA via the GC base sequence. The results revealed that CHL may have an interaction with ds-DNA via the intercalation mode.     

Quadruplex-to-duplex transition of G-rich oligonucleotides probed by cationic water-soluble conjugated polyelectrolytes

G-quartet DNA converts to duplex form in the presence of its complementary strand. This conformational change can be detected in real time by a homogeneous assay method based on the signal amplification of conjugated polyelectrolytes and the specific interaction of intercalating dyes with double-stranded DNA (dsDNA). The probe solution contains a cationic, conjugated polymer (CCP), G-quadruplex labeled with a fluorescein at the 5'-terminus (G-quadruplex-Fl), and ethidium bromide (EB). The addition of a complementary target results in the transition from G-quadruplex to duplex (dsDNA-Fl) and EB intercalation within the duplex structure. Excitation of the CCP leads to energy transfer from CCP to dsDNA-Fl (FRET-1) and then energy transfer from dsDNA-Fl to EB (FRET-2). Increasing the number of mismatched bases discourages dsDNA formation, which is detected in the assay.     

电子转移反应O~2+O~2^.^-→O~2^.^-+O~2的从头算研究

利用abinitio方法,在UHF,UMP2及不同基组3-21G,6-31G^*,6-311+G^*和UMP2(full)/6-311+G^*水平上,研究了O~2/O~2^.^-自交换电子转移反应。优化了电子转移前后反应物和产物的结构,研究了体系能量的变化,计算了自交换电子转移反应的内重组能。对UHF方法和UMP2方法的计算结果进行了比较,并与实验结果进行了对照。结果表明UHF方法由于没有考虑组态相互作用,计算结果存在较大偏差,UMP2(full)/6-311+G^*水平上的计算结果与实验值吻合较好。在UMP2(full)/6-311+G^*水平上计算了气相自交换电子转移反应速率常数。在优化了电子转移复合物结构的基础上考虑了溶剂效应的影响,计算了水溶液中的溶剂重组能。研究结果表明O~2/O~2^.^-体系电子转移反应的活化能主要来源于溶剂重组能的贡献。最后计算了该反应在水溶液中的反应速率常数。理论计算结果与实验值吻合得很好。     

3-羰基吡唑质子转移过程的理论研究

采用密度泛函B3LYP／6—311G^＊＊方法,对3-羰基吡唑几何构型进行了全自由度优化,获得了它们的几何结构和电子结构．计算并考察了3-羰基吡唑的两种构象即syn和anti构象的稳定性以及3-羰基吡唑进行结构互变的质子转移过程的四种可能途径：（a）分子内质子转移;（b）水助质子转移;（C）同种二聚体双质子转移;（d）异种二聚体双质子转移．计算结果表明3-羰基吡唑的syn构象中N2-H型的稳定性大于N1-H型,进行质子转移时途径（C）所需要的活化能最小（52．78kJ／mol）,途径（a）所需要的活化能最大（200．59kJ／mol）;3,羰基吡唑的。anti构象中N1-H型的稳定性大于N2-H型,进行质子转移时途径（d）所需要的活化能最小（61．09kJ／mol）,途径（a）所需要的活化能最大（204．15kJ／mol）．     

3,6-二羟基哒嗪质子转移过程的理论研究

为了探索3,6-二羟基哒嗪分子醇式和酮式结构互变异构化的反应机理,本研究组采用DFT B3LYP/6-311+G(d)方法对标题化合物异构化反应的势能面进行了研究,在探讨各种可能的反应途径中,发现至少有34种异构体和43种过渡态.结果表明,6-羟基-3(2H)-哒嗪酮不论是单体,与水形成配合物,还是二聚体,比其相对应的异构体能量低,表明在通常情况下是以6-羟基-3(2H)-哒嗪酮形式稳定存在的,这与前人通过实验数据对互变异构体的比率进行预测的结果是一致的;在考察的可能反应途径中,直接进行的分子内质子转移过程需要的活化能为142.2 kJ·mol^-1,水助催化时,反应活化能为41.3 kJ·mol^-1,考虑溶剂效应后,其活化能为59.2 kJ·mol^-1,二聚体双质子转移的活化能为16.8 kJ·mol^-1,二聚体双质子转移所需活化能最低,在室温下就可以进行.由此可见氢键在降低反应活化能方面起着重要的作用.     

FLUORESCENCE ENERGY TRANSFER BETWEEN DIMETHYLDIAZAPEROPYRENIUM DICATION AND ETHIDIUM INTERCALATED IN POLY d(A-T)

Dimethyldiazaperopyrenium is one of the largest known DNA intercalators. Fluorescence energy transfer occurred between dimethyldiazaperopyrenium (donor) and ethidium (acceptor) when these dyes were bound to a double-stranded polynucleotide such as poly d(A-T). The addition of increasing amounts of ethidium bromide led to a marked shortening of the fluorescence lifetime of the donor, whereas the excited state of the acceptor was progressively populated via energy transfer from the donor. Critical Förster distance between these two chromophores was calculated to be 3.8 nm. The observed transfer efficiency was lower than that calculated on the basis of this critical distance and a statistical distribution of bound drugs. These results are discussed taking into account the conformational change induced by intercalation of dimethyldiazaperopyrenium in the double-stranded polynucleotide.     

Sticking of CO to crystalline and amorphous ice surfaces

We present results of classical trajectory calculations on the sticking of hyperthermal CO to the basal plane (0001) face of crystalline ice Ih and to the surface of amorphous ice Ia. The calculations were performed for normal incidence at a surface temperature Ts = 90 K for ice Ia, and at Ts = 90 and 150 K for ice Ih. For both surfaces, the sticking probability can be fitted to a simple exponentially decaying function of the incidence energy, Ei: Ps = 1.0e(-Ei(kJ/mol)/90(kJ/mol)) at Ts = 90 K. The energy transfer from the impinging molecule to the crystalline and the amorphous surface is found to be quite efficient, in agreement with the results of molecular beam experiments on the scattering of the similar molecule, N2, from crystalline and amorphous ice. However, the energy transfer is less efficient for amorphous than for crystalline ice. Our calculations predict that the sticking probability decreases with Ts for CO scattering from crystalline ice, as the energy transfer from the impinging molecule to the warmer surfaces becomes less efficient. At high Ei (up to 193 kJ/mol), no surface penetration occurs in the case of crystalline ice. However, for CO colliding with the amorphous surface, a penetrating trajectory was observed to occur into a large water pore. The molecular dynamics calculations predict that the average potential energy of CO adsorbed to ice Ih is -10.1 +/- 0.2 and -8.4 +/- 0.2 kJ/mol for CO adsorbed to ice Ia. These values are in agreement with previous experimental and theoretical data. The distribution of the potential energy of CO adsorbed to ice Ia was found to be wider (with a standard deviation sigma of 2.4 kJ/mol) than that of CO interacting with ice Ih (sigma = 2.0 kJ/mol). In collisions with ice Ia, the CO molecules scatter at larger angles and over a wider distribution of angles than in collisions with ice Ih.