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1.
硝基磺酚C光度法测定蛋白质的研究   总被引:19,自引:0,他引:19  
蛋白质的定量分析是生化研究、临床化验和食品检验等领域经常涉及的内容.以有机小分子作光谱探针测定蛋白质,如甲基橙[1,2]、考马斯亮蓝G-250[3]、溴酚蓝[4]、溴甲酚绿[5]和偶氮胂Ⅲ[6]等已得到研究.  相似文献   

2.
β-二酮络合物已获得广泛而深入的研究,Ce(Ⅳ)的β-二酮类络合物的研究也有报导[1-3].但是,关于Ce(Ⅳ)的β-二酮与其它混合配体络合物的研究至今未见报导.我们以(NH4)2Ce(NO3)6为起始物质,经由双-(三苯基氧化膦)硝酸铈(Ⅳ)中间络合物在混合溶剂中与DBM反应制得该化合物.通过紫外、红外光谱以及1HNMR谱等研究,对该络合物的性质进行了讨论.  相似文献   

3.
表面增强拉曼散射(SERS)自1974年被Fleischmann等[1]发现以来,日益受到人们的重视.通过SERS谱图分析,可以获得物质结构及其与基体作用的信息.由于SERS可使拉曼信号增强105~106[2],并且在某些情况下银胶还能使表面吸附质的荧光猝灭[3,4], SERS常用来检测一些普通拉曼光谱难以检测的样品和考察界面络合物的形成.  相似文献   

4.
稀土的乙酰丙酮络合物的研究已有80多年的历史。三价稀土离子与乙酰丙酮形成络合物的稳定常数早巳系统地测定过[1]。但是,二价稀土离子,例如铕(Ⅱ)与乙酰丙酮形成络合物的稳定常数未见报道。本文叙述试用pH法测定乙酰丙酮铕(Ⅱ)的稳定常数。  相似文献   

5.
由于温度的大幅度变化,分子的某些吸收带的强度将会产生明显的改变,但关于分子的红外吸收光谱与温度关系的研究尚少.在有机锂络合物的红外光谱研究中,我们发现邻甲氧基苯酚锂络合物显示了与其他锂络合物明显不同的特性[1,2],在改变温度过程中,这种不同结构效应的特性更加明显.为此我们从+100~-130℃的较宽温度变化区域内,测定了它的变温红外光谱.  相似文献   

6.
混合配体络合物是络合物溶液化学研究中一个十分活跃的领域,有关镉的混合配体有色络合物见诸文献者不多[1]。作者曾以光度法研究了镉(Ⅱ)-邻二氮菲(phen)-溴苯三酚红(BPR)三元体系中形成络合物的组成及有关光学特性[2]。  相似文献   

7.
鉴于钼化合物在催化方面的应用以及生物体内各种钼酶的存在[1],过去我们曾合成了一些钼的含硫配位体络合物[2-4]。这里我们报道一些双环戊二烯基二硫代氨基甲酸钼(Ⅳ)络合物和异核金属络合物的合成方法及性质的研究。  相似文献   

8.
焦磷酸络锰三价离子引发淀粉-丙烯酰胺的接枝共聚合   总被引:2,自引:0,他引:2  
将带有极性基团的乙烯类单体通过化学接枝到淀粉或纤维素之类的天然多糖上,可作为絮凝剂、脱除剂和粘接剂[1~3],近来已发展为高吸水性材料和石油分离剂[4]。用Ce4+引发乙烯类单体接枝到淀粉和纤维素类已有报道[5]。Rayonier用Mn3+的焦磷酸盐络合物引发接枝乙烯类单体至纤维素及其衍生物上[6];Cenita等用Mn3+引发MMA、AN接枝淀粉[7]。本文以焦磷酸络锰离子(Mn3+)作引发剂、丙烯酰胺(AM)为单体、淀粉为接枝基体进行接枝共聚,这一工作目前在国内外尚未见报道。  相似文献   

9.
方块菁染料在有机光导材料[1,2]、有机太阳能存储[2,3]、光记录[4、有机光盘中红外吸收器[4]以及光纤识别功能薄膜等领域中有着广泛应用前景.  相似文献   

10.
Shur等[1]曾对若干金属有机络合物如Cp2TiAr2的固氮作用进行了早朗研究。  相似文献   

11.
稀土乙酰丙酮络合物的激光拉曼和红外光谱(Ⅰ)   总被引:2,自引:2,他引:0  
本文测定了15个一水稀土乙酰丙酮络合物的激光拉曼和红外光谱,在401、415cm~(-1)附近的拉曼谱带对不同稀土离子表现敏感,它们随原子序数变化呈现“四分组”效应,这是第一次在振动光谱中观察到的镧系递变规律。该系列络合物的振动频率变化亦符合镧系“斜W”效应的规律,这些特征规律为确认401、415cm-1附近谱带为M-O拉伸振动提供了最好的证据。实验结果同时可用于讨论M-O键的性质。  相似文献   

12.
稀土乙酰丙酮络合物的拉曼光谱(Ⅱ)   总被引:2,自引:0,他引:2  
本文从拉曼光谱观察水合分子对无水、一水、三水稀土乙酰丙酮络合物的金属-氧(M-O)拉伸振动带的影响,发现无水络合物在400cm-1附近只有一个振动带,一水络合物在400和415cm-1附近有两个强度不等的振动带,它们的M-O振动频率随原子序数变化都呈“四分组”效应,而三水络合物400cm-1附近带变形,且随轻、重稀土而异,从而干扰了镧系变化规律,没有系统的“四分组”效应。由于一水络合物415cm-1附近带随脱水而消失,吸水而复现的可逆实验事实,修正了前文对415cm-1附近带的指定,而归属于(M-O)H2。络合物M-O拉伸带随水合分子变化反映灵敏,出现特征带形。  相似文献   

13.
The absorption spectra of 4f electron transitions of the complexes of neodymium and erbium with 8-hydroxyquinoline-5-sulphonic acid in the presence of diethylamine and ethanol have been measured by normal and third-derivative spectrophotometry. Their molar absorptivities are 70.7 l.mol~(-1).cm~(-1) for Nd and 62.5 l.mol~(-1).cm~(-1) for Er. They are 7.6 times and 14.9 times greater than those of corresponding chlorides, respectively. Use of the third-derivative spectra both eliminates the interference of Ce(Ⅳ) and increases the sensitivity for Nd and Er. Beer,s Law was obeyed from 0-10 ug/ml of Nd and Er. The method has been applied to the determination of neodymium and erbium in rare earth mixtures.  相似文献   

14.
研究了乙酰丙酮-meso-四-(对-甲氧基)苯基卟啉及其Sm、Gd、Tb、Dy、Ho、Er、Tm、Yb、Lu配合物在3600~225cm-1范围的付立叶变换红外光声光谱,对主要谱带进行了经验归属。结果表明,由于四-(对-甲氧基)苯基卟啉与稀土金属离子配位,削弱了乙酰丙酮环上的M-O键的伸缩振动,使此谱带向低波数移动。配合物中PN-H伸缩振动谱带消失,出现M-N伸缩振动与卟啉环变形振动等的复合振动。  相似文献   

15.
应用光谱减法研究了二甲基甲酰胺(DMF)和二甲基乙酰胺(DMA)水化作用所引起的红外光谱变化,由于羰基和水分子形成氨键的水化作用,含水DMF和DMA的羰基伸缩振动向低波数移动,根据含水DMF和DMA中红外指纹区及远红外区某些谱带的变化,水化作用似乎也表现为酰胺基上具有孤对电子的氮原子与水分子形成氢键。DMF和DMA的水化作用使水峰向高波数移动。  相似文献   

16.
The new organic-inorganic compound, [C_6H_7N_2O_2]_3TeCl_5·2Cl was synthesized and its structure was determined at room temperature in the triclinic system (P~-1) with the following parameters: a = 10.5330(11) ?, b = 10.6663(11) ?, c = 15.9751(16)?, α = 82.090(2)°, β = 71.193(2)°, γ = 68.284(2)°and Z = 2. The final cycle of refinement led to R = 0.057 and Rw = 0.149. The crystal structure was stabilized by an extensive network of N--H···Cl and non-classical C--H···Cl hydrogen bonds between the cation and the anionic group. Several thermal analysis techniques such as thermogravimetric analysis, differential scanning calorimetric analysis and evolved gas analysis were used. We used isoconversional kinetics methods to determine the kinetics parameters. We observe that the decomposition of [C_6H_7N_2O_2]_3TeCl_5·2Cl entails the formation hydrochloric acid of nitroaniline as volatiles. The infrared spectra were recorded in the4000–400 cm~(-1)frequency region. The Raman spectra were recorded in the external region of the anionic sublattice vibration 50–1500 cm~(-1). The optical band gap was calculated from the UV-Vis absorbance spectra using classical Tauc relation which was found to be 3.12 and 3.67 eV.  相似文献   

17.
钴与铬天青S、溴化羟十二烷基三甲铵在吡啶的水溶液中可发生灵敏的显色反应,但吡啶作用的机理未论及,且吡啶气味恶臭,不便于应用.为了探讨吡啶在钴多元络合物形成中的增稳作用以及寻找其它含氮中性配位体代替吡啶,对Co(Ⅱ)与CAS,吡啶(Py)及其衍生物(α-氨基吡啶α-AP、5-氯-α-氨基吡啶5-Cl-α-AP),阳离子表面活性剂(CSF)体系进行了系统的研究.  相似文献   

18.
采用理论与实验相结合的方法对稀土多金属氧酸盐的发光性质进行探究。首先,通过常规水溶液法合成了一系列稀土多金属氧簇Na9LnW10O36 (Ln3+=Sm3+、Eu3+、Tb3+、Dy3+);其次,利用粉末X射线衍射、红外光谱、拉曼光谱对簇合物的结构进行表征;最后,利用紫外-可见光谱、荧光光谱对簇合物的光学性质进行考查。通过系统性的实验使学生对稀土簇合物的结构表征以及发光性质有全面、深刻的认识。  相似文献   

19.
Vibrational spectroscopy is a powerful tool for studying the microstructure of liquids, and anatomizing the nature of the vibrational spectrum (VS) is promising for investigating changes in the properties of liquid structures under external conditions. In this study, molecular dynamics (MD) simulations have been performed to explore changes in the VS of 1-ethyl-3-methylimidazolium hexafluorophosphate ([Emim][PF6]) ionic liquid (IL) under an external electric field (EEF) ranging from 0 to 10 V·nm-1 at 350 K. First, the vibrational spectra for [Emim][PF6] IL as well as its cation and anion are separately obtained, and the peaks are strictly assigned. The results demonstrate that the VS calculated by MD simulation can well reproduce the main characteristic peaks in the experimentally measured spectrum. Then, the vibrational spectra of the IL under various EEFs from 0 to 10 V·nm-1 are investigated, and the intrinsic origin of the changes in the vibrational bands (VBs) at 50, 183, 3196, and 3396 cm-1 is analyzed. Our simulation results indicate that the intensities of the VBs at 50 and 183 cm-1 are enhanced. In addition, the VB at 50 cm-1 is redshifted by about 16 cm-1 as the EEF is varied from 0 to 2 V·nm-1, and the redshift wavenumber increases to 33 cm-1 as the EEF is increased to 3 V·nm-1 and beyond. However, the intensities of the VBs at 3196 and 3396 cm-1 show an obvious decrease. Meanwhile, the VB at 3396 cm-1 is redshifted by about 16 cm-1 when the EEF increases to 3 V·nm-1, and the redshift increases to 33 cm-1 with an increase in the EEF beyond 4 V·nm-1. The intensity of the VB at 50 cm-1 increases because of the increase in the total dipole moment of each anion and cation (from 4.34 to 5.46 D), and the redshift is attributed to the decrease in the average interaction energy per ion pair (from -378.7 to -298.0 kJ·mol-1) with increasing EEF. The intensity of the VB at 183 cm-1 increases on account of the more consistent orientations for cations in the system with increasing EEF. The VB at 3196 cm-1 weakens visibly because a greater number of hydrogen atoms appear around the carbon atoms on the methyl/ethyl side chains and the vibrations of the corresponding carbon-hydrogen bonds are suppressed under the action of the EEF. Furthermore, the intensity of the VB at 3396 cm-1 decreases due to the decrease in the intermolecular +C-H···F- hydrogen bonds (HBs), while the relaxation effect that is beneficial for the formation of HBs simultaneously exists in the system under the varying EEF, thus causing a redshift of the VB at 3396 cm-1.  相似文献   

20.
The IR studies on Ru surfaces have revealed important information such as disposition of nitogen[1-3] and adsorption site of H[3-4]. Most of Ru-based catalysts, however, were supported on oxides. In our experiments, Ru was supported on carbon nanotubes and this catalyst has high activity for ammonia synthesis. The experiment was carried out on Nicolet 740 FTIR. The catalyst surface was detected during the processed of temperature-programmed adsorption of N2 and H2) respectively, from 298 K to 773 K. The FTIR spectra of adsorbed H2 and N2 are shown on Fig.l. At 298 K two peaks assigned to adsorbed hydrogen atoms were observed at 2124 and 1564 cm-1. At 673 K, these two peaks shift to 2089 and 1475 cm-1, respectively, and another peak appeared at 1775 cm-1. The peaks at 2124 and 2089 cm-1 can be assigned to the model of H right on top of Ru, and 1564 and 1475 cm-1 may be due to the bridging H. The peak at 1775 cm-1, which can only be observed at high temperature, may be twin-type H. Nitrogen molecularly adsorbed was observed at 1893 cm-1 (298 K) and 1856 cm-1 (673 K) and they can be assigned to liner N2 on top site.  相似文献   

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