5-氟尿嘧啶与牛血清白蛋白的相互作用

根据合理的假设和Langmuir结合理论, 在298.15 K下, 以等温滴定微量热(ITC)实验数据为依据, 应用非线性最小方差拟合方法确定了抗肿瘤药物配5-氟尿嘧啶(5-FU)与牛血清白蛋白(BSA)相互作用的热力学性质的改变. 研究结果表明, 牛血清白蛋白(BSA)与5-氟尿嘧啶相互作用存在两类结合位点. 第一类结合, N=(54.0 0.3), ⊿H⁰=(30.0±0.4) kJ·mol^-1 (吸热), ⊿S⁰=(196.0±2.6) J·mol-1·K-1(熵增), ⊿G⁰=(-28.4±0.3) kJ·mol^-1; 第二类结合, N=(77.0±0.4), ⊿H⁰=(-20.0±0.4) kJ·mol^-1 (放热), ⊿S⁰=(28.6±0.3) J·mol^-1·K^-1 (熵增), ⊿G⁰=(-28.5±0.2) kJ·mol^-1. 结合体系的圆二色谱(CD)分析结果说明, 抗肿瘤药物5-氟尿嘧啶与BSA的相互作用诱导蛋白质(BSA)二级结构单元的相对含量发生了一定程度的变化.     

荧光光谱法研究橙皮甙与牛血清白蛋白的相互作用

在pH7.40的Tris-HCl 缓冲体系中,采用荧光光谱技术研究了橙皮甙与牛血清白蛋白(BSA)的相互作用.随着温度升高,橙皮甙与BSA 的猝灭常数逐渐增加.实验表明:橙皮甙对BSA的荧光猝灭为动态猝灭过程.由热力学参数焓变(△H=70.71 kJ/mol)大于零和熵变[△S=316.29J/(mol·K)]大于零,...     

依诺沙星与牛血清白蛋白相互作用的荧光法研究

用荧光光谱法研究了新型氟喹诺酮药物依诺沙星与牛血清白蛋白的相互作用机制。求得它们在16℃和26℃温度下的结合常数分别为K1=9.0×103 和K2=1.73×103,结合位点数分别为n1=0.89和n2=0.74。根据不同温度时的结合常数 ,求得依诺沙星与牛血清白蛋白的热力学参数(26℃) :ΔHm= -51.44kJ/mol,ΔGm= -8.05kJ/mol,ΔSm= -0.145kJ/(mol·K)。根据F rster非辐射能量转移机制 ,测定了实验条件下依诺沙星与牛血清白蛋白相互结合时 ,能量给体 -受体间的作用距离(r=4.74nm)和能量转移效率(E=0.074) ,并用同步荧光技术考察了依诺沙星对牛血清白蛋白构象的影响。实验表明 ,依诺沙星与牛血清白蛋白分子间有较强的结合作用 ,且结合作用力主要是氢键和范德华作用力     

希夫碱钴配合物的吸氧热力学及其自氧化作用

本文合成了一个新的双Schiff碱钴配合物,并研究了该配合物在吡啶溶液中的吸氧过程热力学。在4—24℃范围内,吸氧摩尔比为1:1,吸氧过程热力学参数为:△H=-26.8(±0.5)kJ/mol,△S=-89.2(±1.8)J/mol·K。在30—45℃范围内,吸氧摩尔比为2:1,吸氧过程的热力学参数为:△H=-172.6(±9.14)kJ/mol,△S=-517.3(±29.4)J/mol·K。温度超过45℃,自氧化作用变得明显,配合物中苄羟基被氧化为醛基。提出了可能的氧化反应机理。     

荧光法研究盐酸拓扑替康、盐酸依利替康喜树碱类药物牛血清白蛋白的相互作用

用荧光光谱法、分光光度法研究了盐酸拓扑替康(Topotecan hydrochloride,简记为THC)与盐酸依利替康(Irinotecan hydrochloride,简记为IHC)两种喜树碱类药物与牛血清白蛋白(Bovine serum albumins,BSA)的相互结合反应.实验表明喜树碱类药物与牛血清白蛋白的相互结合作用为单一的静态猝灭过程,在溶液中二者以物质的量比11牢固结合,25℃时其结合反应的平衡常数K0分别为K0,THC=7.73×105 L·mol-1,K0,IHC=4.73×105 L·mol-1.根据F(o)rster非辐射能量转移机理,求算了给体(BSA)与受体(喜树碱类药物)间距离r和能量转移效率E分别为rTHC=3.75nm,rIHC=3.08 nm,ETHC=0.26,EIHC=0.51.并研究了五种离子对喜树碱类药物与BSA结合作用的影响,推测了二者之间的主要作用力为疏水作用和偶极-偶极相互作用.     

杂多酸盐K7[PTi2W10O40]·6H2O与牛血清白蛋白相互作用的研究

Under the imitated physiological condition of animal body, the interactions of heteropoly salt (PM-19) with bovine serum albumin (BSA) were investigated by fluorescence and absorption spectroscopy. It was shown that this compound had a quite strong ability to quench the fluorescence launching from BSA. After analyzing the fluorescence quenching data according to Stern-Volmer equation and Lineweaver-Burk double-reciprocal equation, we found that BSA had reacted with PM-19 and formed a certain new compound. The quenching belonged to static fluorescence quenching. According to Lineweaver-Burk equation, the forming constants of the compound (298 K: 2.68 × 10⁵ L·mol^-1; 304 K: 2.19 × 10⁵ L·mol^-1; 310 K: 1.82 × 105 L·mol^-1) and the thermodynamic parameters (ΔH=-24.72 kJ·mol^-1; ΔS=20.97 J·mol^-1·K^-1 / 20.92 J·mol^-1·K^-1/ 20.97 J·mol^-1·K^-1; ΔG=-30.97 kJ·mol^-1/ -31.08 kJ·mol^-1/-31.22kJ·mol^-1) at the corresponding temperatures were obtained. The latter shows that binding power between them is mainly electrostatic interaction. Based on F?rster′s non-radiation energy transfer mechanism, the binding locality (r=4.14 nm) was calculated between donor and accepter. The effect of PM-19 on the conformation of BSA was also analyzed by synchronous fluorescence spectroscopy.     

Cr(Ⅵ)与牛血清白蛋白的相互作用

采用荧光光谱、紫外光谱、CD光谱法研究了K2Cr2O7与牛血清白蛋白(BSA)的相互作用。实验结果表明,铬(Ⅵ)使BSA的紫外吸收降低,峰位红移,表明铬(Ⅵ)与BSA发生较强的相互作用;铬(Ⅵ)酸根离子与BSA形成基态复合物导致BSA内源荧光猝灭,猝灭机理主要为静态猝灭。测定了不同温度下该反应的热力学参数,ΔGθ0,ΔHθ和ΔSθ分别为-12.60kJ/mol和56.60J/(mol.k),表明上述作用过程是一个熵增加、自由能降低的自发分子间作用过程,铬(Ⅵ)酸根离子与BSA之间以静电作用力为主;非辐射能量转移机理确定了铬(Ⅵ)与牛血清白蛋白中色氨酸残基之间的距离r=2.85nm;同步荧光和CD光谱研究表明,铬(Ⅵ)使BSA的二级结构发生改变,α-螺旋含量降低,色氨酸残基所处微环境的极性减小。     

Cr（VI）与牛血清白蛋白的相互作用

采用荧光光谱、紫外光谱、CD光谱法研究了K2Cr2O7与牛血清白蛋白(BSA)的相互作用。实验结果表明, 铬(Ⅵ)使BSA的紫外吸收降低,峰位红移,表明铬(Ⅵ)与BSA发生较强的相互作用;铬(Ⅵ)酸根离子与BSA形成基态复合物导致BSA内源荧光猝灭,猝灭机理主要为静态猝灭。测定了不同温度下该反应的热力学参数,ΔGθ＜0,ΔHθ和ΔSθ分别为–12.60 kJ/mol 和 56.60 J/(mol·k), 表明上述作用过程是一个熵增加、自由能降低的自发分子间作用过程,铬(Ⅵ)酸根离子与BSA之间以静电作用力为主;非辐射能量转移机理确定了铬(Ⅵ)与牛血清白蛋白中色氨酸残基之间的距离 r＝2.85 nm;同步荧光和CD光谱研究表明,铬(Ⅵ)使BSA的二级结构发生改变,α–螺旋含量降低,色氨酸残基所处微环境的极性减小。     

疏水作用对光化学和光物理过程的影响 Ⅲ.长链β-萘甲酸烷基酯在簇集体中形成激基缔合物的热力学和动力学

在乙二醇-水(EG-H₂O)和二甲基亚砜-水(DMSO-H₂0)混合溶剂中,β-萘甲酸十二烷基酯和十六烷基酯很容易发生簇集.本文研究了簇集体中的β-萘甲酸酯在—40℃3到90℃温度范围内的稳态荧光光谱和时间分辨荧光光谱以及荧光偏振,测定了激基缔合物形成和解离的速度常数,求出激基缔合物形成的活化能,焓变和熵变分别为10.9±0.4kJ/mol,—16.7±0.4kJ/mol和—50±4J/mol·K。A₁₂和A₁₆簇集体分别在—20℃和5℃发生相变.测定了不同温度下簇集体内的微观粘度。     

光谱法研究诱惑红与牛血清白蛋白的相互作用

采用荧光光谱、紫外吸收光谱、同步荧光光谱和圆二色光谱研究了诱惑红(AR)与牛血清白蛋白(BSA)的相互作用;讨论了AR对BSA荧光的猝灭机理。荧光光谱与紫外吸收光谱表明,AR使BSA的荧光猝灭属于静态猝灭。根据热力学参数焓变(ΔH0)和熵变(ΔS0)可推断AR和BSA的相互作用力主要为静电引力。在298K,303K,308K温度下,两者间的结合常数分别为3.72×105,3.13×105,2.96×105L·mol-1,结合位点数为1.1。当AR与BSA的浓度比为1∶1时,两者间的结合距离为2.59nm。同步荧光光谱、三维荧光光谱和圆二色光谱研究结果表明,在结合过程中BSA的构象发生了变化。     

抗肿瘤药物5-氟尿嘧啶与人血清白蛋白相互作用的热力学研究

在298.15 K下,根据本结合过程的假设和Langmuir结合理论, 用等温滴定微量热和圆二色谱分析法研究了抗肿瘤药物5-氟尿嘧啶(5-FU)与人血清白蛋白(HSA)的相互作用. 研究结果表明, 蛋白质(HSA)与药物配体5-氟尿嘧啶的相互作用存在两类结合位点. 第一类结合, 结合位点数N＝71±0.1, 结合常数 K＝(1.46±0.016)×10⁵ L•mol^－1, 结合焓ΔH＝(39.61±0.220) kJ•mol^－1, 结合熵ΔS＝(231.68±0.025) J•mol^－1•K^－1, 结合自由能ΔG＝(－29.48±0.030) kJ•mol^－1. 结合过程为熵驱动过程, 疏水相互作用是过程的主要推动力;第二类结合, 结合位点数N＝140±0.2, 结合常数 K＝(1.49±0.032)×10⁵ L•mol^－1, 结合焓ΔH＝(－19.31±0.103) kJ•mol^－1, 结合熵ΔS＝(34.30±0.055) J•mol^－1•K^－1, 结合自由能ΔG＝(－29.53±0.041) kJ•mol^－1, 结合过程为焓-熵协同驱动过程, 氢键和静电相互作用是过程的主要推动力. 圆二色谱分析结果表明, 在两类结合过程中, 药物5-氟尿嘧啶(5-FU)的作用致使蛋白质(HSA)二级结构单元的相对含量发生了变化.     

Analysis of binding interaction between pegylated puerarin and bovine serum albumin by spectroscopic methods and dynamic light scattering

The interaction between bovine serum albumin (BSA) and pegylated puerarin (Pur) in aqueous solution was investigated by UV-Vis spectroscopy, fluorescence spectroscopy and circular dichroism spectra (CD), as well as dynamic light scattering (DLS). The fluorescence of BSA was strongly quenched by the binding of pegylated Pur to BSA. The binding constants and the number of binding sites of mPEG(5000)-Pur with BSA were 2.67±0.12 and 1.37±0.05 folds larger after pegylating, which were calculated from the data obtained from fluorescence quenching experiments. The enthalpy change (ΔH) and entropy change (ΔS) were calculated to be 4.09 kJ mol(-1) and 20.01 J mol(-1) K(-1), respectively, according to Van't Hoff equation, indicating that the hydrophobic force plays a main role in the binding interaction between pegylated Pur and BSA. In addition, the negative sign for Gibbs free energy change (ΔG) implies that the interaction process is spontaneous. Moreover, the results of synchronous fluorescence and CD spectra demonstrated that the microenvironment and the secondary conformation of BSA were changed. Comparing with Pur, all our data collected indicated that pegylated Pur interacted with BSA in the same way as that of Pur, but docked into the hydrophobic pocket of BSA with more accessibility and stronger binding force. DLS measurements showed monomethoxy polyethylene glycol (mPEG) have an effect on BSA conformation, and revealed that changes in BSA size might be due to increases in binding constant and the absolute values of ΔG after Pur pegylation.     

The thermodynamic properties of magnesium uranoborate

The standard enthalpy of formation of crystalline Mg(BUO₅)₂ at 298.15 K (?4347.5 ± 8.0 kJ/mol) was determined by reaction calorimetry. The heat capacity of magnesium uranoborate was studied by adiabatic vacuum calorimetry over the temperature range 8–330 K. The thermodynamic functions of the compound were calculated. The standard entropy and Gibbs energy of formation at 298.15 K were found to be ?903.0 ± 2.1 J/(mol K) and ?4078.5 ± 9.0 kJ/mol, respectively.     

The thermodynamic properties of magnesium uranoborate tetrahydrate

The standard enthalpy of formation of crystalline Mg(BUO₅)₂ · 4H₂O at 298.15 K (?5563 ± 10 kJ/mol) was determined by reaction calorimetry. The heat capacity of the compound was studied over the temperature range 8–340 K by adiabatic vacuum calorimetry, and its thermodynamic functions were calculated. The standard entropy and Gibbs function of formation at 298.15 K (?1692.2 ± 3.4 J/(mol K) and ?5059 ± 11 kJ/mol, respectively) were determined.     

The thermodynamic properties of calcium uranoborate

The standard enthalpy of formation of crystalline Ca(BUO₅)₂ at 298.15 K was determined by reaction calorimetry (?4491.0 ± 3.5 kJ/mol). The heat capacity of the substance was measured over the temperature range 7–304 K by adiabatic vacuum calorimetry, and its thermodynamic functions were calculated. The standard entropy and the Gibbs function of formation at 298.15 K were found to be ?887.1 ± 2.1 J/(mol K) and-4226.5 ± 4.0 kJ/mol, respectively. The standard thermodynamic functions of calcium uranoborate synthesis reactions were calculated and analyzed.     

The thermodynamic properties of Ba2SrUO6

The standard enthalpy of formation of crystalline Ba₂SrUO₆ at 298.15 K was determined by reaction calorimetry (-2940.0 ± 8.5 kJ/mol). The heat capacity of the compound was measured over the temperature range 8-330 K by adiabatic vacuum calorimetry. The thermodynamic functions of Ba₂SrUO₆ were calculated. The standard entropy (-558.6 ± 2.1 J/(mol K)) and Gibbs function of formation at 298.15 K (-2773.5 ± 9.0 kJ/mol) were determined.     

The thermodynamic properties of uranyl metaborate

The standard enthalpy of formation of crystalline UO₂(BO₂)₂ at 298.15 K was determined by reaction calorimetry (?2542.5 ± 3.5 kJ/mol). The heat capacity of this compound was measured over the temperature range 6–302 K by adiabatic vacuum calorimetry. The thermodynamic functions were calculated, including the standard entropy (502.8 ± 2.1 J/(mol K)) and Gibbs function of formation (?2392.5 ± 4.0 kJ/mol) at 298.15 K. The standard thermodynamic functions of reactions with the participation of uranyl metaborate were determined and analyzed.