微量热法研究漆酶和3,4,5—三羟基苯甲酸的反应

用ＬＫＢ－２１０７型微量热系统，在不同的温度（ｐＨ＝７．４）的条件下，测定了３，４，５－三羟基苯甲酸与漆酶反应的摩尔反应焓，米氏常数，反应速率常数，漆酶的活性并计算了结合能，活化自由能，活化能和活化熵等。在此基础上，应用过渡态理论，从能量变化的角度，对其催化过程进行了分析，由活化熵（△Ｓ＾≠Ｔ〈０）得出酶－底物过渡态的结构较酶－底物复合物更为有序的结论。     

微量热法研究单底物酶促反应的热力学和动力学性质及过渡态的分析

用LKB-2107型微量热系统, 测定了漆酶催化氧化3, 4-二羟基苯甲醛、邻甲氧基酚、邻苯三酚、3, 4, 5-三羟基苯甲酸反应的热谱图, 利用热谱图计算了米氏常数(Km)、反应速率常数(k2)和热力学参数(ΔrHm, ΔG0, ΔT^≠, Ea, ΔST^≠)。并应用过渡态理论对其催化过程进行了分析。结果表明: 稳定过渡态结构有利于酶促反应, 酶-底物在反应物时相互作用仅仅是降低酶的催化效率。提出两种可能提高酶催化效率的方法。由活化熵(ΔST)<0得出酶-底物在过渡态的结构较酶-底物复合物的结构更为有序。     

壳聚糖-g-N-羧甲基-2-硫代-4,5-2H咪唑啉酮-多壁碳纳米管复合物固定漆酶基化学传感器的性能

通过壳聚糖-g-N-羧甲基-2-硫代-4,5-2H咪唑啉酮(CTS-g-N-CSIDZ)非共价功能化多壁碳纳米管(MWCNTs)的方式制备固定漆酶载体,该复合物载体主要通过物理吸附和漆酶活性中心与载体上配体之间的配位作用来固定漆酶,较大程度地保持了游离漆酶活性位原始构象.将固定了漆酶的复合物附着在裸玻碳电极上便构筑了复合物固定漆酶修饰玻碳电极.在以分光光度法测定了这种复合物载体对漆酶的担载量、固定漆酶比活力、稳定性、重复使用性及其催化2,6-二甲氧基苯酚(DMP)氧化动力学参数的基础上,还对基于此种复合物固定漆酶修饰玻碳电极作为化学传感器(以DMP作为底物)的性能进行了研究.结果表明,该复合物具有较高的固酶担载量(81.7 mg/g)和固定漆酶比活力(1.33 U/mg);而作为电化学传感器的复合物固定漆酶修饰玻碳电极对底物DMP具有较高的亲和力(对DMP的米氏常数KM是0.0918 mmol/L),较高的灵敏度( 3680 mA· L/mol),较低的检测限(3.3×10-4 mmol/L),较高的响应选择性,良好的重现性、重复使用性和长期稳定性.这种漆酶基电极有望用作电流型特定结构的酚类传感器.     

漆酶与酚类模式底物的结合及反应活性的理论研究

通过生物信息学分析、分子动力学模拟及量子化学计算,对21种邻对位取代酚类模式底物与漆酶的结合能力以及反应活性进行了探讨.生物信息学结构比对分析发现漆酶的活性口袋含有Asp/Glu206,Asn/His208,Asn264,Gly392和His458等保守的氨基酸残基(氨基酸残基编号以Trametes versicolor漆酶为例,PDB:1KYA);采用MM-GBSA方法计算了21种酚类模式底物与T.versicolor漆酶的结合自由能.分子力学计算结果表明,漆酶与底物的结合力主要来自Asp206和Asn264等残基与底物分子形成的分子间氢键,并且Phe265残基和酚类底物的芳香环形成π-π相互作用.量子化学计算表明,芳环上取代基的推拉电子效应显著影响协同电子转移的底物去质子化过程,其中推电子能力较强的—NH2,—OH,—OCH3和—CH CHCH3等基团能够明显增强酚羟基反应活性,而吸电子的—CONH2和—Cl则具有相反的效应.     

漆酶活化碱木质素的磺甲基化反应活性研究

采用漆酶对碱木质素进行活化预处理,并对活化碱木质素进行磺甲基化改性,揭示了漆酶活化对碱木质素磺甲基化反应活性影响的作用机理.采用顶空气相色谱、红外光谱、凝胶渗透色谱、核磁共振等研究了漆酶活化碱木质素的结构特征,结果表明,漆酶对碱木质素既有聚合作用又有解聚作用,分子量变化不大,多分散性增加;漆酶活化使得碱木质素发生脱甲基作用,酚羟基含量增大,紫丁香基含量减低;另外,漆酶可氧化酚羟基变成苯氧自由基使碱木质素聚合.采用分子模拟对漆酶活化碱木质素的电子云密度进行了计算,结果表明脱甲基作用增大了木质素苯环上的电子云密度,有利于磺甲基化反应的进行.采用电位滴定测试磺甲基化产物的磺化度来表征其反应活性的大小,结果表明漆酶活化磺甲基化碱木质素的磺化度提高了35%,且对二氧化钛悬浮体系的分散性能得到明显提高.     

贝壳状革耳菌漆酶酶活测定方法分析

酶活测定方法中所用的反应底物、反应条件以及酶活单位定义对漆酶酶活的测定结果有很大的影响。在对贝壳状革耳菌 (Panusconchatus)漆酶酶活测定方法的研究中发现 ,该酶与 2 ,2’ -连氮 -双 ( 3-乙基并噻- 6 -磺酸 ) (ABTS)反应的最适pH值为 3.0 ,而与紫丁香醛连氮、2 ,6-二甲氧基苯酚和邻甲联苯胺反应的最适pH值均为 4.0。上述底物与Panusconchatus漆酶反应的Km (米氏常数 )分别为 0 .0 1 1 6(mmol·L) - 1 ,1 4.1 0 95 (mmol·L) - 1 ,0 .1 0 1 1 (mmol·L) - 1 ,0 .1 41 5 (mmol·L) - 1 。该酶与ABTS、2 ,6-二甲氧基苯酚和邻甲联苯胺反应均表现为零级反应 ,而与紫丁香醛连氮反应时只在一定范围的酶浓度以及反应时间内才表现为零级反应。     

CH3SH与NO2的反应机理及动力学

在G3B3, CCSD(T)/6-311＋＋G(d,p)//B3LYP/6-311＋＋G(d,p)水平上详细研究了CH3SH与基态NO2的微观反应机理. 在B3LYP/6-311＋＋G(d,p)水平得到了反应势能面上所有反应物、过渡态和产物的优化构型, 通过振动频率分析和内禀反应坐标(IRC)跟踪验证了过渡态与反应物和产物的连接关系. 在CCSD(T)/6-311＋＋G(d,p)和G3B3水平计算了各物种的能量, 得到了反应势能面. 利用经典过渡态理论(TST)与变分过渡态理论(CVT)并结合小曲率隧道效应模型(SCT), 分别计算了在200～3000 K温度范围内的速率常数kTST, kCVT和kCVT/SCT. 研究结果表明, 该反应体系共存在5个反应通道, 其中N进攻巯基上H原子生成CH3S＋HNO2的通道活化势垒较低, 为主要反应通道. 动力学数据也表明, 该通道在200～3000 K计算温度范围内占绝对优势, 拟合得到的速率常数表达式为k1CVT/SCT＝1.93×10－16T0.21exp(－558.2/T) cm3&;#8226;molecule－1&;#8226;s－1.     

CH3NO2和CH3自由基吸氢反应途径和变分速率常数计算

采用MP2(full)/6-311G(d, p)从头算方法,优化了硝基甲烷和甲基自由基吸氢反应的过渡态结构,经QCISD(T)方法进行能量校正,得出该反应的正逆向反应的活化位垒分别是58.21 kJ•mol－1和67.17 kJ•mol－1.沿IRC分析指出该反应是氢转移协同反应,而且在反应途径上存在一个引导反应进行的振动模式,这一反应模式引导反应进行的区间在反应坐标S的-0.9～1.0(amu)1/2bohr之间;在温度为800～2600 K范围内,运用改进的变分过渡态理论(ICVT),计算了该反应的速率常数,并与实验类比所得的速率常数随温度的变化趋势进行了比较.     

人工设计逆醛缩酶RA95.5-8F催化β-羟基酮C—C裂解的理论研究

采用量子力学与分子力学组合(QM/MM)方法对人工设计逆醛缩酶RA95.5-8F催化β-羟基酮化合物裂解反应的机理进行了研究. 结果表明, 裂解反应主要包括赖氨酸Lys1083对底物的亲核进攻、 Schiff碱形成、 烯胺水解及C—N断裂等过程, C—N键裂解生成丙酮为整个反应的决速步骤, 能垒为106.27 kJ/mol; 活性中心的赖氨酸Lys1083、 酪氨酸Tyr1051、 天冬酰胺Asn1110和酪氨酸Tyr1180构成一个催化四联体, Lys1083通过与底物形成席夫碱对底物进行活化, Tyr1051作为催化酸碱参与质子转移过程, 催化四联体的氢键网络有利于反应过渡态的稳定并使R-构型的底物更容易结合在活性位点, 导致RA95.5-8F对R构型底物具有高的选择性和催化活性.     

漆树漆酶的催化氧化作用 (ⅹⅢ)──Fe~(2+)离子对漆酶催化氧化反应的影响()

以５,６－二溴－２,３－二氰基氢醌为底物,在ｐＨ４．５０条件下,用分光光度法考察了ＦｅＳＯ４对漆树漆酶催化氧化反应的影响．结果表明,在本文实验条件下ＳＯ２－４离子对酶促反应的影响基本可以忽略,而Ｆｅ２＋离子对漆酶的催化氧化反应则有明显的竞争性抑制作用．研究证实,Ｆｅ２＋离子的抑制作用是通过它还原酶促反应的产物半醌自由基阴离子来实现的     

Synthesis,crystal structure and thermal behavior of 4-amino-3,5-dinitropyrazole copper salt

A novel energetic combustion catalyst, 4-amino-3,S-dinitropyrazole copper salt （[Cu（adnp）2（H2O）2]）, was synthesized in a yield of 93.6% for the first time. The single crystal of [Cu（adnp）2（H2O）2] was determined by single crystal X-ray diffraction. It crystallizes in a triclinic system, space group p^-1 with crystal parameters a = 5.541（3） A, b = 7.926（4） A, c = 10.231（5） A,β = 101.372（8）°, V = 398.3（3） A3, Z = 1, μ = 1.467 mm^-1, F（0 0 0） = 243, and Dc = 2.000 g cm^-3. The thermal behavior and non-isothermal decomposition reaction kinetics of [Cu（adnp）2（H2O）2] were studied by means of different heating rate differential scanning calorimetry （DSC）. The kinetic equation of major exothermic decomposition reaction for [Cu（adnp）2（H2O）2] was obtained. The entropy of activation （△S≠）, enthalpy of activation （△H≠）, free energy of activation （△G≠）, the self-accelerating decomposition temperature （TSADT） and the critical temperature of thermal explosion （Tb） are 59.42 j mol^-1 K^-1, 169.5 kJ mol^-1, 1141.26 kJ mol ^-1 457.3 K and 468.1 K, respectively.     

Low-temperature Heat Capacity and Standard Thermodynamic Functions of D-Galactose and Galactitol

The heat capacities of D-galactose and galactitol were measured on a quantum design physical property measurement system(PPMS) over a temperature range of 1.9―300 K, and the experimental data were fitted to a function of T using a series of theoretical and empirical models in appropriate temperature ranges. The fit results were used to calculate thermodynamic function values,C_p,m^θ,Δ₀^TS_m^θ, and Δ₀^TH_m^θfrom 0 K to 300 K. The standard molar heat capacity, entropy and enthalpy values of D-galactose and galactitol at 298.15 K and 0.1 MPa were determined to be C_p,m^θ =(227.96±2.28) and (239.50±2.40) J·K^-1·mol^-1,S_m^θ= (211.22±2.11) and (230.82±2.30) J·K^-1·mol^-1 and = H_m^θ (33.95±0.34) and (36.57± 0.37) kJ/mol, respectively.     

Synthesis and Thermal Behavior of 1,8-Dihydroxy- 4,5-dinitroanthraquinone Manganese Salt

A novel energetic combustion catalyst, 1,8-dihydroxy-4,5-dinitroanthraquinone manganese salt （DHDNEMn）, was synthesized by virtue of the metathesis reaction in a yield of 91%, and its structure was characterized by IR, element analysis and differential scanning calorimetry（DSC）. The thermal decomposition reaction kinetics was studied by means of different heating rate DSC. The results show that the apparent activation energy and pre-exponential factor of the exothermic decomposition reaction of DHDNEMn obtained by Kissinger＇s method are 162.3 kJ/mol and 1011.8 s^-1, respectively. The kinetic equation of major exothermic decomposition reaction of DHDNEMn is dα/dT= 10^118/β 2/5（1-α）[-ln（1-α）[-ln（1-α）]^3/5 exp（-1.623×10^5/RT）. The entropy of activation（△S^≠）, enthalpy of activation（△H^≠） and free energy of activation（A△G^≠） of the first thermal decomposition are -24.49 J·mol^-1·K^-1, 185.20 kJ/mol and 199.29 kJ/mol（T=575.5 K）, respectively. The self-accelerating decomposition temperature（TSADT） and critical temperature of thermal explosion（Tb） are 562.9 and 580.0 K, respectively. The above-mentioned information on the thermal behavior is quite useful for analyzing and evaluating the stability and thermal safety of DHDNEMn.     

Synthesis and Thermal Properties of Three Energetic Ion Salts of 3,6-Bis[(1H-1,2,3,4-tetrazol-5-yl)-amino]-1,2,4,5-tetrazine

Three energetic ion salts of 3,6-bis[(1H-1,2,3,4-tetrazol-5-yl)-amino]-1,2,4,5-tetrazine(BTATz), namely, methylamine salt(compound 1), ethylenediamine salt(compound 2), and diethylamine salt(compound 3), were synthesized and characterized by elemental analysis, Fourier transform infrared spectrometry, NMR spectroscopy, and ^13C NMR spectroscopy. The crystal structure of compound 1 was determined by single-crystal X-ray crystallography, and structural analysis revealed that it belonged to the monoclinic system with P21/c space group. In addition, the thermal behavior of the three compounds was studied by differential scanning calorimetry and thermogravimetry techniques. The thermal decomposition peak temperatures of the compounds were 574.89, 545.60, and 606.72 K, indicating that the three ion salts exhibited good thermal stability. Tlie kinetic mechanism equations of the main decomposition process and the entropy of activation(△S^≠), enthalpy of activation(△H^≠), and Gibbs free energy of activation(△G^≠) of the three compounds were also obtained. Moreover, the thermal safety of the compounds was evaluated by the values of the self^accelerated decomposition temperature(Tsadt)5 thermal ignition temperature(TTIT), and critical temperature of thermal explosion(7b). The results showed that all the compounds demonstrated good thermal safety, and the thermal safety of compound 3 was better than that of the others.     

Thermal Kinetics and Decomposition Mechanism of 1-Amino-1,2,3-triazolium Nitrate

The thermal decomposition kinetics of 1-amino-l,2,3-triazolium nitrate（ATZ-NO3） was investigated by non-isothermal TG-DTG at various heating rates（2,5,10,15 and 20 ℃/min）.The results show that the thermal decomposition of ATZ-NO3 consists of two stages corresponding to the losing of nitrate anion,substituent group and the splitting of triazole ring respectively.The kinetic triplets of the two stages were described by a three-step method.First,the differential Kissinger and intergral Ozawa methods were used to calculate the apparent activation energies（E） and pre-exponential factors（A） of the two decomposition stages.Second,two calculation methods（intergral （S）atava-（S）esták and differential Achar methods） were used to obtain several probable decomposition mechanism functions.Third,three judgment methods（average,double-extrapolation and Popescu methods） were used to confirm the most probable decomposition mechanism functions.Both reaction models of the two stages were randominto-nucleation and random-growth mechanisms with n=3/2 for the first stage and n=1/3,m=3 for the second stage.The kinetic equations for the two decomposition stages of ATZ-NO3 may be expressed as da/dt=1013.60·e-128970/RT（1-α）[-1n（1-α）]-1/2 and da/dt=1011.41·e-117370/RT（1-α）[-1n（1-α）]-2/3.The thermodynamic parameters including Gibbs free energy of activation（△G≠）,entropy of activation（△S≠） and enthalpy of activation（△H≠）,for the thermal decomposition reaction were also derived.     

Electrochemistry of CeCl3 in Molten LiCl-KCl Eutectic

The electrochemical properties of CeCl3, dissolved in LiCI-KCI eutectic melt, were investigated by electrochemical techniques, such as cyclic voltammetry and square wave voltammetry on Mo electrode. It was shown that Ce（Ⅲ） is reduced to Ce（0） based on a three-step mechanism. In a temperature range of 833-923 K, the diffusion coefficient of Ce（Ⅲ） is lgDceoH）=-2.49-1704/T determined by means of the Berzins-Delahay equation with two different expressions under reversible and irreversible conditions. The apparent standard potential of a Ce（Ⅲ）/Ce（0） redox system is ECE^3＋0^＊/Ce^0 =3.551＋0.0006132T（K） vs. Cl2/Cl^-. Some thermochemical properties of CeCl3 solutions were also derived from the electrochemical measurements, such as the enthalpy, entropy, Gibbs free energies and the activity coefficients of Ce（Ⅲ）. The Gibbs free energy of a dilute solution of CeCl3 in this system was determined to be △G^0CeCl3/（kJ·mol^-1）=-1027.9＋0.178T（K） And the activity coefficients, γCeCl3 , range between （7.78-9.14）×10^-3. Furthermore, the standard rate constant of kinetic reaction was calculated to be （4.94-9.72）× 10^-3 cmZ/s and the reaction was regarded as a quasi-reversible reaction under the present experimental conditions at 833 K.     

Denatured Thermodynamics of Proteins in Weak Cation－exchange Chromatography

The thermostability of some proteins in weak cation-exchange chromatography was investigated at 20—80 ℃. The results show that there is a fixed thermal denaturation transition temperature for each protein. The appearance of the thermal transition temperature indicates that the conformations of the proteins are de-stroyed seriously. The thermal behavior of the proteins in weak cation-exchange and hydrophobic interaction chromatographies were compared in a wide temperature range. It was found that the proteins have a higher thermostability in a weak cation-exchange chromatography system. The thermodynamic parameters (△H^0,△S^0) of those proteins were determined by means of Van′t t Hoff re|ationship(lnk′-1/T). According to stan-dard entropy change(△S^0) , the conformational change of the proteins was judged in the chromatographic pro-cess. The linear relationships between △H^0 and △S^0 can be used to evaluate “compensation temperature“ (β) at the protein denaturation and identify the identity of the protein retention mechanism in weak cation-ex-change chromatography.     

立方体纳米Cu2O吸附热力学及动力学的粒度效应研究

采用不同粒径的单一(100)晶面的立方体纳米Cu₂O作为模型材料, 研究了粒径和温度对其吸附动力学和吸附热力学性质的影响规律. 基于已建立的纳米材料吸附热力学和动力学理论, 推导出了单一(100)晶面立方体纳米Cu₂O材料的吸附热力学和吸附动力学性质与粒径之间的关系式. 实验结果与理论预测结果一致: 随着纳米Cu₂O粒径的减小, 吸附速率常数增大而吸附活化能和吸附指前因子减小; 标准摩尔吸附Gibbs自由能 Δ_a $G^{\rlap{-}0}_{m}$减小而标准吸附平衡常数ln $K^{\rlap{-}0}$、 标准摩尔吸附焓 Δ_a $H^{\rlap{-}0}_{m}$和标准摩尔吸附熵 Δ_a$S^{\rlap{-}0}_{m}$均增大, 且以上参数均与粒度的倒数具有较好的线性关系.     

Sorption of Am(Ⅲ) on Na-bentonite:Effect of pH,ionic strength,temperature and humic acid

Sorption of Am(Ⅲ) on Na-bentonite as a function of contact time,pH,ionic strength,humic acid(HA) and temperature was investigated under ambient conditions.The results showed that the sorption was strongly dependent on pH and ionic strength. Am(Ⅲ) sorption can be described well by pseudo-second-order model.The presence of HA takes a positive effect at low pH;but a negative influence under high pH range.Enthalpy,entropy and Gibbs free energy(i.e.,△H~0,△S~0 and△G~0) calculated from sorption isotherms suggested that sorption process of Am(Ⅲ) was spontaneous and endothermic.