Acridinium Ion Ionization at Elevated Temperatures and Pressures to 200 °C and 2000 bar

The temperature and pressure dependences of pK for acridine ion ionization were determined up to 200 °C and 2000 bar. The UV-Vis measurements at high temperatures and pressures were conducted in flow-through spectrophotometric cells. Two independent series of experiment were performed: one in a Ti–Pd cell with silica quartz windows for measurements in the ultraviolet region, and another in a Ti grade 5 cell with sapphire windows for use at higher pressures, which permitted measurements in the visible region. Combined chemometric and thermodynamic analyses of the UV-Vis spectrophotometric data were used to extract the ionization constants as well as the changes in molar volume ΔV° for acridine protonation as functions of temperature and pressure. Values of pK decrease from 5.52 to 3.74 with increasing temperature from 25 to 200 °C at saturated water-vapor pressure. The pressure dependence of acridinium ion ionization is small (e.g., pK=5.5 at 25 °C and 2000 bar) and is characterized by positive ΔV°≤1.2 cm³⋅mol⁻¹, which is not surprising for this type of isocoulombic reaction involving a large molecule.     

Force fields and assignments of the vibrational spectra of acridine and phenazine—an ab initio study

A complete set of force constants and their corresponding scale factors in non-redundant local coordinates were obtained by fitting the in-plane ab initio Hartree–Fock (HF) vibrational frequencies computed using 4-21G and 6-31G^** basis sets to the experimental ones. Using these force constants the potential energy distribution (PED) of the normal modes was obtained and based on the PED the earlier empirical assignments were either confirmed or reassigned for all the in-plane fundamentals. The force constants of acridine and phenazine are compared to those of anthracene to study the similarities and differences. Probable assignment is proposed for the out-of-plane fundamentals of acridine based on Durig's simple scaling of the local force constants.     

十二烷基苯磺酸钠胶束中吖啶橙与罗丹明6G间的能量转移机理研究

以吖啶橙(AO)与罗丹明6G(R6G)为例讨论了胶束介质中碱性荧光染料间相互作用的机理。在十二烷基苯磺酸钠水溶液中,吖啶橙与罗丹明6G染料分子间相互作用发生有效能量转移。在不同温度下,通过对能量转移体系研究,初步证明吖啶橙与罗丹明6G间发生能量转移引起吖啶橙的荧光猝灭为静态猝灭过程。通过热力学参数的计算,得出能量转移体系的结合力主要为静电引力。同时也对转移体系的能量转移效率,结合位点数和结合距离进行了计算。     

关于吖啶氮氧化物与烃、醇、酮等之间的光化夺氢反应中的自由基的研究

有关吖啶及其某些衍生物在亲核加成反应中生成的各种自由基或离子基,曾由J.W.Happ等人予以研究^[1],吖啶本身与某些化合物之间的光化夺氢反应也曾被研究过^[2],而吖啶氮氧化物及其衍生物与烃类等化合物之间的光化夺氢反应研究,则尚未见文献报导。我们用吖啶氮氧化物、9-氯代吖啶氮氧化物和9-氰基吖啶氮氧化物分别与包括环烯烃、芳烃、烷烃、醇及羰基化物在内的15种化合物进行光化学反应,用ESR技术检出了很强而又相当稳定的氮氧自由基信号。     

用模板法制备TiO2纳米线阵列膜及光催化性能的研究

用溶胶-凝胶技术在多孔阳极氧化铝模板的有序微孔内制备了高度取向的TiO2纳米线阵列膜光催化剂.用XRD,AFM和SEM等手段对样品进行了表征.结果表明,TiO2纳米线阵列膜晶型为锐钛矿,从AFM图像中可以看出TiO2纳米线线径分布均匀一致,取向性极好,直径与AAO模板的孔径大小一致.以其对吖啶橙的降解效果作为评价光催化活性的标准,与相同条件下制备的TiO2/玻璃膜相比,TiO2纳米线阵列膜具有很好的催化活性.     

荧光共振能量转移猝灭法测定加替沙星

在pH=7.00的Britton-Robinson (B-R)缓冲溶液,及十二烷基硫酸钠(SDS)介质中,吖啶橙(AO)-罗丹明 (RB)能够发生有效的能量转移,使RB荧光增强.加替沙星(Gatifloxacin, GTFX)的加入又使得RB的荧光猝灭,据此建立了测定加替沙星的新方法.将此方法用于加替沙星片剂和粉针剂的测定,结果满意.实验表明,该方法简单、快速、灵敏、准确.     

等色吸收荧光猝灭法快速测定食品中苏丹红Ⅰ

在乙醇介质中, 强荧光染料吖啶的荧光波长478 nm与苏丹红Ⅰ的吸收光波长480 nm十分接近, 由于等色性苏丹红Ⅰ能够有效吸收吖啶发出的荧光, 使吖啶在激发波长λex=410 nm、荧光波长λem=478 nm处荧光猝灭, 依此建立了荧光猝灭测定苏丹红Ⅰ的新方法. 该方法快速、简便, 其线性范围为3.72～37.2 mg/L, 方法检出限为1.1 mg/L. 用于辣椒、辣椒酱食品中痕量苏丹红Ⅰ的测定. 6次平行测定, 相对标准偏差为0.8%～2.7%, 加标回收率为89.5%～104.0%.     

纳米TiO2/碳化树脂复合催化剂的合成及其光催化性能研究

利用一种简单、快速的方法合成了纳米TiO₂/碳化树脂(B)复合催化剂,对其组成、结构、尺寸及其光催化性能进行了表征.结果表明,该复合材料为由碳、氢、氧和钛等4种元素组成的纳米材料,尺寸约30nm,其中Ti和O的堆积结构为锐钛矿型;在该复合材料中,B为具有活性基团和不同长度碳-碳共轭链的大分子,且与TiO₂之间存在着某种化学作用,复合材料所具有的特殊电子结构不仅使其能吸收紫外-可见区的全程光波,而且对光生电荷具有很高的分离能力,从而表现出较高的光催化活性.     

荧光染料吖啶红作测定蛋白质的生物探针——蛋白质的染料分析法新进展

简述染料结合分析法的发展过程,吖啶红染料自取和体系测定蛋白质的最佳试验条件和测定结果。阳离子荧光染料吖淀红及其自聚的二聚体的可平衡转化,形成自聚平衡体系,在表面活性剂十二烷基磺酸钠的存在下,蛋白质的定量加入可调节这一平衡,从而引起体系 荧光有规律的变化。方法线性范围宽、灵敏度高、反应速度快、准确度高 、抗干扰 能力强,是染料分析法定量测定蛋白质的最新方法之一。     

The Crystal and Molecular Structure of 9-(3-Pentyl)-3,4,6,7,9,10-hexahydro-1,8(2H,5H) -acridine-dione

The crystal structure of the title compound is described. The structure has two molecules in the asymmetric unit and it crystallizes in the orthorhombic space group Pca21 with Z = 8. The unit cell dimensions are a = 14.574(2), b = 8.924(1) and c = 24.704(10) Å, V = 3212.7(14) ų, D_calc = 1.188 gcm^-3. All the rings of the molecule A adopt sofa conformation. One of the outer rings of molecule B adopts distorted sofa while the other two rings adopt sofa conformation.