2-甲基-4-羟基-6-苯基嘧啶和2-甲基-4-羟基-5-溴-6-苯基嘧啶的高效液相色谱法分离测定

采用ODS-C18色谱柱和紫外检测器,对2-甲基-4-羟基-6-苯基嘧啶和2-甲基-4-羟基-5-溴-6-苯基嘧啶的含量进行HPLC分离测定.以甲醇水=4555为流动相,紫外检测波长为237 nm,样品线性范围为0.001～0.1 mg/mL.2-甲基-4-羟基-6-苯基嘧啶的RSD为0.5%;2-甲基-4-羟基-5-溴-6-苯基嘧啶的RSD为1.0%.     

2-甲氧基-3-氟-4-碘吡啶的合成

2-甲氧基-3-氟-4-碘吡啶是一个重要的医药化工中间体,其合成路线未见文献报道。以2-甲氧基-3-氟-5-氯吡啶为起始原料,经氢解和碘代两步反应合成标题化合物,总收率62.8%,其结构经¹H NMR, ¹³C NMR和MS确证。     

3-甲基-1-戊烯-4-炔-3-醇的合成

以甲基乙烯酮为原料,用乙炔基格氏试剂对其加成,然后水解得到目标物3-甲基-1-戊烯-4-炔-3-醇。研究了温度对反应的影响,发现在25℃的反应温度下,目标化合物的气相色谱产率为50%,减压蒸馏纯化后收率为30%。目标产物用1HNMR、IR进行了表征。     

3-甲基-2-戊烯-4-炔醛的合成新方法

化合物3-甲基-2-戊烯-4-炔-1-醛两端均为活性官能团,在分子连接及成环反应中能够起到非常重要的作用,是合成轮烯酮[1-7],脱落酸[8]和二苯基二苯并环辛烯[9]等的重要中间体.     

4-甲基-苯磺酸-2-氧-2-[3-(5-芳基-[1,3,4]噁二唑-2-基)-硫脲]-乙基酯的合成及生物活性研究

合成了12个未见文献报道的4-甲基-苯磺酸2-氧-2-[3-(5-芳基-[1,3,4]噁二唑-2-基)-硫脲]-乙基酯, 其结构经元素分析、¹H NMR和IR确证. 初步活性测试结果表明: 部分化合物有较好的杀菌活性.     

水溶剂中反-2,3-环氧-1-苯基-3-(2′-硝基-5′-氯苯基)-1-丙酮的合成及产物的晶体结构

用 2-硝基-5-氯苯甲醛、氯代苯乙酮和氢氧化钠以三乙基苄基氯化铵作催化剂在水溶剂中反应可合成反-2,3-环氧-1-苯基-3-(2′-硝基-5′-氯苯基)-1-丙酮(C15H10ClNO4)。产物的结构通过单晶 X-射线衍射法确定,其晶体属于单斜晶系。空间群 P21/c, a = 9.942(1), b = 15.774(3), c =8.756(1) ?, β = 96.39(1)°, Mr = 303.69, Z = 4,V = 1364.6(3) ?3, Dc = 1.478 g/cm3, μ(MoKα) =0.295 mm–1, F(000) = 624, 最终的偏离因子为 R = 0.0336, wR = 0.0745。X-衍射分析表明, 该产物为反式异构体。     

2-甲基-1-(4-芳基噻唑-2-基)-苯并咪唑-6-甲酸乙酯的合成、表征及生物活性

以4-乙酰氨基苯甲酸乙酯为原料设计合成了14 种2-甲基-1-(4-芳基噻唑-2-基)-苯并咪唑-6-甲酸乙酯新化合物. 化合物结构经质谱、1H NMR、红外光谱和元素分析等确证, 并用单晶X射线衍射仪测定了化合物5a的晶体结构. 生物活性实验结果表明, 化合物5c(500 mg/L)对小麦白粉病菌抑制率达到95%; 化合物5e对辣椒疫霉病菌(25 mg/L)的抑制率为61.9%, 对油菜菌核病菌(500 mg/L) 抑制率高达97.2%; 化合物5k(25 mg/L) 对小麦赤霉病菌抑制率为55.1%.     

稳定烯醇结构3-氯-2-羟基-4-羰基-4-对甲苯基-2-丁烯酸乙酯的合成

以甲苯为起始原料,通过傅克-酰基化、Aldol反应合成了具有稳定烯醇结构的3-氯-2-羟基-4-羰基-4-对甲苯基-2-丁烯酸乙酯,反应过程生成了中间体3,3-二氯-2-羟基-4-羰基-4-对甲苯基丁酸乙酯,采用红外、核磁共振谱、HRMS产品进行了测定和结构表征。对反应机理进行了初步探讨。     

(±)-12-乙基-13-甲氧基-8,11,13-罗汉松三烯-7-酮和(±)-12-乙基-13-甲氧基-8,11,13-罗汉松三烯的全合成

以α-环柠檬醛(1)为A环合成子,以季盐(2)为C环合成子,经缩合及分子内环化反应得到关键中间体(5).为引入乙基,进行了Friedel-Crafts反应和脱氧反应等,共经7步反应得到了(±)-12-乙基-13-甲氧基-8,11,13-罗汉松三烯-7-酮[(±)-nimbonone](9)及(±)-12-乙基-13-甲氧基-8,11,13-罗汉松三烯(10).     

卤代-2-(3-甲基-5-取代-4H-1,2,4-三唑-4-基)-苯甲酸的合成

邻氮基苯甲酸;缩合反应;卤代-2-(3-甲基-5-取代-4H-1;2;4-三唑-4-基)-苯甲酸的合成     

Ab Initio Calculation of Room Temperature Ionic Liquid 1-Ethyl-3-Methyl-Imidazolium Chlorocuprate （I）

The Hartree-Fock method has been employed to investigate the electronic structures of EMIM^＋（1-ethyl-3-methyl-imidazolium^＋）, CuCl2^-, Cu2Cl3^-, CuCl3^2-, EMIM＋^-CuCl2^-, EMIM^＋-Cu2Cl3^-, and EMIM^＋-CuCl3^2- pairs. Full optimization and frequency analyses of EMIM^＋, CuCl2^-, Cu2Cl3^-, CuC13^-, eight initial EMIM^＋-CuCl2^-, six EMIM^＋-Cu2Cl3^-, and four EMIM^＋-CuCl3^2- geometries have been carried out using Gaussian-94 soft-package at 6-31＋G（d,p） basis set level for hydrogen, carbon, nitrogen, chlorine atoms and Hay-Wadt effective core potential for copper atom. The electronic structures of lowest energy of EMIM^＋-CuCl2^-, EMIM＋-Cu2Cl3^-, EMIM^＋-CuCl3^2-, single EMIM^＋, CuCl2^-, Cu2Cl3^-, and CuCl3^2- have been comparatively studied. The calculated results showed that EMIM^＋-CuCl2^- pair conformer of lowest energy was five ring parallel to Cl-Cu-Cl with 3.2A distance, EMIM^＋-CuCl3^2- pair conformer of lowest energy was five ring parallel to CuCl3^2-plane with 3.4A distance, and the optimized EMIM^＋-Cu2Cl3^- pair conformer of lowest energy was five ring perpendicular to Cl-Cu-Cl-Cu-Cl plane with 3.0A distance between the terminal Cl atoms and the 5-ring of EMIM^＋. The cohesion between cations and anions is brought about by C-H. C1 hydrogen bonds that are reinforced by charge assistance. The frequency analyses suggested that all stationary points are minimum because of no appearing of imaginary frequency. The assigned frequencies were in agreement with the experimental report. The low energy of interaction because of the bulkyasymmetry of EMIM＋ and the charge dispersion of cation and anion leads to the low melting point of the ionic liquids, EMIM^＋-CuCl2^-, EMIM^＋-Cu2Cl3^-, and EMIM^＋-CuCl3^2-. The interaction energy of EMIM^＋-CuCl2^-, EMIM^＋-Cu2Cl3^-, and EMIM^＋-CuCl3^2- is 309.0 kJ/mol, 316.8 kJ/mol, and 320.2 kJ/mol, respectively. The relationship of interaction energy via distance between cations and anions was also investigated by single point energy scan.     

Effect of anions on static orientational correlations, hydrogen bonds, and dynamics in ionic liquids: a simulational study

Three different ionic liquids are investigated via atomistic molecular dynamics simulations using the force field of Lopes and PAdua (J. Phys. Chem. B 2006, 110, 19586). In particular, the 1-ethyl-3-methylimidazolium cation EMIM+ is studied in the presence of three different anions, namely, chloride Cl-, tetrafluoroborate BF(4)(-), and bis((trifluoromethyl)sulfonyly)imide TF2N-. In the focus of the present study are the static distributions of anions and cations around a cation as a function of anion size. It is found that the preferred positions of the anions change from being close to the imidazolium hydrogens to being above and below the imidazolium rings. Lifetimes of hydrogen bonds are calculated and found to be of the same order of magnitude as those of pure liquid water and of some small primary alcohols. Three kinds of short-range cation-cation orderings are studied, among which the offset stacking dominates in all of the investigated ionic liquids. The offset stacking becomes weaker from [EMIM][Cl] to [EMIM][BF4] to [EMIM][TF2N]. Further investigation of the dynamical behavior reveals that cations in [EMIM][TF2N] have a slower tumbling motion compared with those in [EMIM][Cl] and [EMIM][BF4] and that pure diffusive behavior can be observed after 1.5 ns for all three systems at temperatures 90 K above the corresponding melting temperatures.     

DFT Study on the Structure of Ionic Liquid 1-Ethyl-3-methylimidazolium Hexafluorophosphate

1 INTRODUCTION Ionic compounds generally have high melting points and always exist in solid state since they are main- tained by electrovalent bonds. Ionic Liquids (ILs), which are liquids at or near ambient temperature, have been a class of ionic compounds extensively studied experimentally and theoretically in recent years[1, 2]. ILs consist exclusively of anions and ca- tions and do not contain any neutral molecule. They have many attractive properties, such as low vapor pressure, no…     

Ab Initio Calculation of Room Temperature Ionic Liquid 1-Ethyl-3-Methyl-Imidazolium Chlorocuprate (Ⅰ)

The Hartree-Fock method has been employed to investigate the electronic structures of EMIM (1-ethyl-3-methyl-imidazolium ), CuCl2-, Cu2Cl3-, CuCl32-, EMIM -CuCl2-, EMIM -Cu2Cl3-,and EMIM -CuCl32- pairs. Full optimization and frequency analyses of EMIM , CuCl2-, Cu2Cl3-, CuCl32-,eight initial EMIM -CuCl2-, six EMIM -Cu2Cl3-, and four EMIM -CuCl32- geometries have been carried out using Gaussian-94 soft-package at 6-31 G(d,p) basis set level for hydrogen, carbon, nitrogen, chlorine atoms and Hay-Wadt effective core potential for copper atom. The electronic structures of lowest energy of EMIM -CuCl2-, EMIM -Cu2Cl3-, EMIM -CuCl32-, single EMIM , CuCl2-, Cu2Cl3-, and CuCl32- have been comparatively studied. The calculated results showed that EMIM -CuCl2- pair conformer of lowest energy was five ring parallel to Cl-Cu-Cl with 3.2 (A) distance, EMIM -CuCl32- pair conformer of lowest energy was five ring parallel to CuCl32-plane with 3.4 (A) distance, and the optimized EMIM -Cu2Cl3- pair conformer of lowest energy was five ring perpendicular to Cl-Cu-Cl-Cu-Cl plane with 3.0 (A) distance between the terminal Cl atoms and the 5-ring of EMIM . The cohesion between cations and anions analyses suggested that all stationary points are minimum because of no appearing of imaginary frequency.The assigned frequencies were in agreement with the experimental report. The low energy of interaction because of the bulky asymmetry of EMIM and the charge dispersion of cation and anion leads to the low melting point of the ionic liquids, EMIM -CuCl2-, EMIM -Cu2Cl3-, and EMIM -CuCl32-. The interaction energy of EMIM -CuCl2-, EMIM -Cu2Cl3-, and EMIM -CuCl32- is 309.0 k J/mol, 316.8 k J/mol, and 320.2 k J/mol, respectively. The relationship of interaction energy via distance between cations and anions was also investigated by single point energy scan.     

Ab Initio Calculation of Room Temperature Ionic Liquid 1-Ethyl-3-Methyl-Imidazolium Chlorocuprate (Ⅰ)

The Hartree-Fock method has been employed to investigate the electronic structures of EMIM (1-ethyl-3-methyl-imidazolium ), CuCl2-, Cu2Cl3-, CuCl32-, EMIM -CuCl2-, EMIM -Cu2Cl3- , and EMIM -CuCl32- pairs. Full optimization and frequency analyses of EMIM , CuCl2-, Cu2Cl3-, CuCl32-, eight initial EMIM -CuCl2-, six EMIM -Cu2Cl3-, and four EMIM -CuCl32- geometries have been carried out using Gaussian-94 soft-package at 6-31 G(d,p) basis set level for hydrogen, carbon, nitrogen, chlorine atoms and Hay-Wadt effective core potential for copper atom. The electronic structures of lowest energy of EMIM -CuCl2-, EMIM -Cu2Cl3-, EMIM -CuCl32-, single EMIM , CuCl2-, Cu2Cl3-, and CuCl32- have been comparatively studied. The calculated results showed that EMIM -CuCl2- pair conformer of lowest energy was five ring parallel to Cl—Cu—Cl with 3.2 A distance, EMIM -CuCl32- pair conformer of lowest energy was five ring parallel to CuCl32-plane with 3.4 A distance, and the optimized EMIM -Cu2Cl3- pair conformer of lowest energy was five ring perpendicular to Cl—Cu—Cl—Cu—Cl plane with 3.0 (?) distance between the terminal Cl atoms and the 5-ring of EMIM . The cohesion between cations and anions is brought about by C—H…Cl hydrogen bonds that are reinforced by charge assistance. The frequency analyses suggested that all stationary points are minimum because of no appearing of imaginary frequency. The assigned frequencies were in agreement with the experimental report. The low energy of interaction because of the bulky asymmetry of EMIM and the charge dispersion of cation and anion leads to the low melting point of the ionic liquids, EMIM -CuCl2-, EMIM -Cu2Cl3-, and EMIM -CuCl32-. The interaction energy of EMIM -CuCl2-, EMIM -Cu2Cl3-, and EMIM -CuCl32- is 309.0 kJ/mol, 316.8 kJ/mol, and 320.2 kJ/mol, respectively. The relationship of interaction energy via distance between cations and anions was also investigated by single point energy scan.     

咪唑氟硼酸类离子液体熔点与分子内相互作用能的关系

运用密度泛函理论B3LYP方法及6-311++G(d,p)基组对11种咪唑氟硼酸离子液体进行了研究.选择相应化合物的离子体系{[XIM][BF4]n}(n-1)-(n=2,3)作为研究对象,即研究体系由一个烷基咪唑阳离子XIM+和2-3个BF4-阴离子构成,对其进行结构优化.在优化得到的最低能量构型的基础上计算了分子内阳离子与阴离子间的相互作用能,同时考虑了基组重叠误差的修正.结果表明所研究离子体系的离子间相互作用能与离子液体的实验熔点之间存在明确的线性关系,并且所得到的线性方程与氨基酸阳离子型离子液体中存在的线性关系相近.我们的工作为今后借助量子化学方法设计功能化离子液体提供了一定的理论基础.     

Molecular Structure,Vibrational Spectra,and Hydrogen Bonding of the Ionic Liquid 1‐Ethyl‐3‐methyl‐1H‐imidazolium Tetrafluoroborate

The IR and Raman spectra and conformations of the ionic liquid 1‐ethyl‐3‐methyl‐1H‐imidazolium tetrafluoroborate, [EMIM] [BF₄] ( 6 ), were analyzed within the framework of scaled quantum mechanics (SQM). It was shown that SQM successfully reproduced the spectra of the ionic liquid. The computations revealed that normal modes of the EMIM⁺?BF ion pair closely resemble those of the isolated ions EMIM⁺ and BF , except for the antisymmetric BF stretching vibrations of the anion, and the out‐of‐plane and stretching vibrations of the H? C(2) moiety of the cation. The most plausible explanation for the pronounced changes of the latter vibrations upon ion‐pair formation is the H‐bonding between H? C(2) and BF . However, these weak H‐bonds are of minor importance compared with the Coulomb interactions between the ions that keep them closely associated even in dilute CD₂Cl₂ solutions. According to the ‘gas‐phase’ computations, in these associates, the BF anion is positioned over the imidazolium ring of the EMIM⁺ cation and has short contacts not only with the H? C(2) of the latter, but also with a proton of the Me? N(3) group.     

Evidence for spin diffusion in a H,H-NOESY study of imidazolium tetrafluoroborate ionic liquids

The ionic liquids 1-ethyl-3-methylimidazolium tetrafluoroborate ([EMIM][BF4]) and 1-methyl-3-propylimidazolium tetrafluoroborate ([PMIM][BF4]) were studied by H,H-NOESY NMR using a cross-relaxation matrix analysis. Cross-peak intensities are seen to increase with increasing mixing time. Experimental and theoretical hydrogen-hydrogen distances are in agreement at short mixing times (50 ms). Mixing times longer than 50 ms result in an increasing contribution of spin diffusion that produces unrealistically short hydrogen-hydrogen distances. Gas-phase ab initio molecular structures are obtained using Hartree-Fock (HF) and density functional theory (B3LYP) methods at the 6311 + G(2d,p) basis set level. The hydrogen-hydrogen distances obtained from the theoretical structures are in reasonable agreement with those calculated from the cross-relaxation matrices.     

1-乙胺基-3-甲基咪唑四氟硼酸盐吸收CO_2的理论研究

采用密度泛函理论(DFT)对离子液体1-乙胺基-3-甲基咪唑四氟硼酸盐([NH2e-mim][BF4])吸收CO_2的反应机理进行了研究.在B3LYP/6-311++G(d,p)计算水平下,对离子液体[NH2e-mim][BF4]的结构及与CO_2反应的中间体、过渡态和产物进行了全优化,获得了优化结构的构型参数、振动频率和热力学数据.利用自然键轨道(NBO)分析了离子液体[NH2e-mim][BF4]和CO_2的自然电荷布居.计算结果表明,通过阳离子[NH2e-mim]+自偶解离产生的阳离子[NH3e-mim]2+能与阴离子[BF4]-结合形成更强的离子键.根据反应吉布斯自由能变(ΔG0—)和焓变(ΔH0—)的计算结果,判断离子液体[NH2e-mim][BF4]吸收CO_2按理论摩尔比2∶1分步进行反应,吸收过程中质子的转移需克服52.51 k J/mol的能垒.     

13C NMR relaxation rates in the ionic liquid 1-ethyl-3-methylimidazolium butanesulfonate

A new method of obtaining molecular reorientational dynamics from 13C spin-lattice relaxation data of aromatic carbons in viscous solutions is applied to 13C relaxation data of both the cation and anion in the ionic liquid, 1-ethyl-3-methylimidazolium butanesulfonate ([EMIM]BSO3). 13C pseudorotational correlation times are used to calculate corrected maximum NOE factors from a combined isotropic dipolar and nuclear Overhauser effect (NOE) equation. These corrected maximum NOE factors are then used to determine the dipolar relaxation rate part of the total relaxation rate for each aromatic 13C nucleus in the imidazolium ring. Rotational correlation times are compared with viscosity data and indicate several [EMIM]BSO3 phase changes over the temperature range from 278 to 328 K. Modifications of the Stokes-Einstein-Debye (SED) model are used to determine molecular radii for the 1-ethyl-3-methylimidazolium cation. The Hu-Zwanzig correction yields a cationic radius that compares favorably with a DFT gas-phase calculation, B3LYP/(6-311+G(2d,p)). Chemical shift anisotropy values, Deltasigma, are obtained for the ring and immediately adjacent methylene and methyl carbons in the imidazolium cation and for the three carbon atoms nearest to the sulfonate group in the anion.