多氟烯烃和炔烃的钯催化氢化

本文报道Pd/Al_2O_3(1%)催化剂催化氢化CF_3CCl=CClCF_3,CF_3CCI==CHCF_3和CF_3C=CCF_3等多氟烯烃和炔烃的结果。经1~H和(19)~F核磁共振、质谱、红外等分析,证明了用制备色谱分离后的氢化产物主要成份的结构。前二者的氢化产物中主要是CF_3CH_2CH_2CF_3和CF_3CH_2CHClCF_3的混合物,而CF_3C=CCF_3氢化后只生成CF_3CH_2CH_2CF_3。     

全氟和多氟烷基磺酸的研究 ⅩⅧ.由二氟甲磺酰氟的衍生物产生二氟卡宾的研究

前文报道HCF_2SO_2F(1)与某些亲核试剂反应时会产生:CF_2,HCF_2SO_3H和P_2O_5,POCl_3等作用时也会形成:CF_2.本文报道二氟甲磺酸和磺酰胺在不同条件下产生:CF_2的结果. 我们在研究CH_3O_2CCF_2SO_3R(R=C_6H_5,HCF_2CF_2CH_2)的脱甲氧羰基反应时发现在质子溶剂(如ROH)中进行时得到HCF_2SO_3R.若用LiCl在HMPA/THF中与它反应,并加     

铜参与的1,1,1-三氟-2,2-二氯乙烷及1,1,1-三氟-2,2,2-三氯乙烷与苯乙烯的加成反应研究

该反应为铜/联吡啶调控的CF_3CHCl_2及CF_3CCl_3对苯乙烯化合物的原子转移自由基加成反应.该反应通过添加联吡啶来增强铜的还原性,成功实现了CF_3CHCl_2和CF_3CCl_3较惰性C—Cl键的断裂,并与烯烃生成单一的自由基加成产物.     

全氟和多氟烷基磺酸的研究 ⅩⅦ.全氟烷磺酸二氟甲酯及其反应

和R_FSO_3CH_2R(1)及R_FSO_3CF_2R′_F(2)不同,R_FSO_3CF_2H(3)(RF=CF_3,3a;ICF_2CF_2OCF_2CF_2,3b;Cl_2CFCF_2OCF_2CF_2,3c;ClCF_2CF_2OCF_2CF_2,3d)和亲核试剂的反应较为复杂。除X-(X=F,Cl,I)及C_2H_5OH与3反应时只发生C—O键断裂外,其它试剂如RCO_2~-,C_6H_5S~-等既可进攻硫原子又可进攻碳原子,但以前者为主,碱性较强的试剂如RO~-还可夺取二氟甲基的氢原子而产生二氟卡宾,在3中由于甲基碳上存在两个氟原子,确实有着一定的屏蔽作用,因此阻碍了某些试剂对它的亲核进攻,但由于这个碳上还连有一个氢原子,所以这种屏蔽作用并不完全。     

氟磺酰基二氟乙酰氟,六氟环氧丙烷和六氟丙烯加成反应的研究

本文研究了FO_2SCF_2COF、HFPO和HFP在F~(?)催化下的三元加成反应。我们发现在反应开始时存在着一个反应速度增长的过程,这个过程的长短受溶剂的用量和反应温度的影响。 (CF_3)_2CFCOCF(CF_3)OCF_2CF_2SO_2F只有在5℃以上和乳化催化剂的存在下才生成。通过~(19)F NMR的研究,我们认为FO_2SCF_2COF、HFPO和HFP对于F~(?)的反应活性存在如下的顺序: FO_2SCF_2COF>HFPO>HFP     

CF_3I催化合成中氟夺取途径的密度泛涵理论研究

CF_3I在制冷剂、刻蚀剂、发泡剂、灭火剂以及有机氟工业等领域具有广泛的应用.在活性炭负载碱金属盐的催化下,以CHF_3和碘为原料,可直接合成CF_3I.CF_3及CF_4分别是该反应过程中重要的中间产物和副产物,而积碳则导致催化剂失活的重要原因.因此研究它们的产生机理具有重要意义.对此本文采用密度泛涵理论(DFT)方法进行了研究.结果表明:CF_2及CF_3可以对吸附于graphite(001)表面的CFCF_3进行多步氟夺取,最终得到CF_3、CF_4以及C_2自由基.以上氟夺取反应产生的C_2自由基也导致了实验中的积碳现象.上述反应机理与现有的实验数据相符.     

有机氟化学的新进展

本文综述氟有机化学的最新进展。论及:1.气溶胶直接氟化法,新的温和的氟化试剂——CH_3CO_2F,N-氟代二氢吡咯酮,R_F(?)(C_6H_5)CF_3SO_3(?)和喷雾干燥的KF。2.合成全氟烷基磺酸的新方法,如全氟烷基碘在金属活化下与SO_2在DMF中的反应,又如I(CF_2)_2O(CF_2)_2SO_2F与C_2F_4调聚和全氟卤代烷的亚磺化脱碘反应。3.惰性—CF_2—及—CF_3的新反应,如五氟一氯丙酮与KF的反应,多氯氟乙烷与硫酚钠的反应。4.具有生理活性的氟化物,如抗癌物fluorosesqisiloxane,杀虫剂29-fluorositosterol。     

氟氯烷烃与三氯化铝的反应

Park等从全氟丙烯与三氯化铝的反应产物中,分离出一系列氟氯烯烃,并指出该反应中全氟丙烯氟原子被氯原子取代的次序.CF_2ClCFClCF_2CFCl_2(1)与三氯化铝反应,仅得到CF_2ClCFClCF_2CCl_3,产率58％.我们研究了1及CFCl_2CF_2CFCl_2(2)分别与三氯化铝的反应.由1的反应得CF_     

全氟和多氟烷基磺酸的研究——ⅩⅤ.由α-氟砜基二氟甲基乙酸甲酯形成二氟卡宾和氟砜基二氟甲基阴离子

FO_2SCF_2CO_2CH_3(1)和许多亲核试剂作用时很容易发生脱羧甲基分解反应。例如X~-(Cl~-,Br~-,I~-)CNS~-,Et_3N,C_5H_5N等都可以进攻其甲基碳,接着消去CO_2,SO_2和F~-而产生:CF_2。在非水有机溶剂中,脱羧后极快地同时消去SO_2,F~-形成:CF_2;但在含水有机溶剂中,则先形成中间体FO_2SCF_2~-,它可被质子捕获生成HCF_2SO_2F(2)。大部分仍继续消除SO_2和F~-产生:CF_2。烷氧阴离子不能类似地将1分解,而是进攻1的硫原子得到相应的磺酸酯CH_3O_2CCF_2SO_2—Z(10)(Z=OCH_2CF_2CF_2H,OC_6H_5)。在无溶剂情况下,Et_2NH也能使1分解而形成:CF_2,还伴有少量进攻羧基碳的产物FO_2SCF_2CONEt_2(11)。     

多氟代烃类的反应 Ⅱ.氟氯烯烃与三氯化铝的反应

Park等曾报道全氟丙烯与三氯化铝在50-60℃下反应,分离出一系列取代反应产物,并阐明其分子中氟氯基团与三氯化铝反应时的稳定性次序。Haszeldine等做了2,3-二溴全氟丙烯在三溴化铝存在下的重排反应,并提出了相应的重排机理。本工作以CFCl_2CF_2CF=CF_2(1)为原料与三氯化铝反应,通过试验找到在极温和反应条件下(三氯化铝与1的摩尔比为0.5,10℃下反应3h)获得几乎定量的重排产物CF_3CF_2CF=CCl_2(3),这一反应可用在三氯化铝催化下,1分子内烯丙位氟原子在分子内完成两次1,3-转移,从而使双键发生连续的烯丙型转移来解释.     

Unimolecular rate constants, kinetic isotope effects and threshold energies for FH and FD elimination from CF3CHFCH3 and CF3CHFCD3

The combination of CF(3)CHF and CH(3) or CD(3) radicals was used to prepare vibrationally excited CF(3)CHFCH(3) or CF(3)CHFCD(3) molecules with 97 kcal mol(-1) of internal energy. The experimental unimolecular rate constants were 3.7 x 10(6) s(-1) for 2,3-FH elimination from CF(3)CHFCH(3) and 1.3 x 10(6) s(-1) for 2,3-DF elimination from CF(3)CHFCD(3). Unimolecular rate constants for 1,2-FH elimination reaction were approximately 230 and 98 times smaller for CF(3)CHFCH(3) and CF(3)CHFCD(3), respectively, than the corresponding rate constants for 2,3-FH elimination. Density functional theory (DFT) was used to calculate the structures and vibrational frequencies of the molecules and transition states; this information was subsequently employed for calculations of RRKM rate constants. Comparison of the experimental and calculated rate constants gave a threshold energy of 73 +/- 2 kcal mol(-1) for the 1,2-FH elimination process and 60.5 +/- 1.5 kcal mol(-1) for the 2,3-FH elimination reaction from CF(3)CHFCH(3). The calculated kinetic-isotope effects agree with the experimental results. The experimentally derived threshold energies for 1,2-FH and 2,3-FH elimination reactions from several fluoropropanes and fluorochloropropanes are summarized and compared to those from DFT calculations.     

Unimolecular elimination of HF and HCl from chemically activated CF3CFClCH2Cl

The unimolecular reactions of CF3CFClCH2Cl molecules formed with 87 kcal mol(-1) of vibrational energy by recombination of CF3CFCl and CH2Cl radicals at room temperature have been characterized by the chemical activation technique. The 2,3-ClH and 2,3-FH elimination reactions, which have rate constants of (2.5 +/- 0.8) x 10(4) and (0.38 +/- 0.11) x 10(4) s(-1), respectively, are the major reactions. The 2,3-FCl interchange reaction was not observed. The trans (or E)-isomers of CF3CFCHCl and CF3CClCHCl are favored over the cis (or Z)-isomers. Density functional theory at the B3PW91/6-31G(d',p') level was used to evaluate thermochemistry and structures of the molecule and transition states. This information was used to calculate statistical rate constants. Matching the calculated to the experimental rate constants for the trans-isomers gave threshold energies of 62 and 63 kcal mol(-1) for HCl and HF elimination, respectively. The threshold energy for FCl interchange must be 3-4 kcal mol(-1) higher than for HF elimination. The results for CF3CFClCH2Cl are compared to those from CF3CFClCH3; the remarkable reduction in rate constants for HCl and HF elimination upon substitution of one Cl atom for one H atom is a consequence of both a lower E and higher threshold energies for CF3CFClCH2Cl.     

Use of the ultraviolet absorption spectrum of CF2 to determine the spatially resolved absolute CF2 density, rotational temperature, and vibrational distribution in a plasma etching reactor

Broadband ultraviolet absorption spectroscopy has been used to determine CF(2) densities in a plasma etch reactor used for industrial wafer processing, using the CF(2) A (1)B(1)<--X (1)A(1) absorption spectrum. Attempts to fit the experimental spectra using previously published Franck-Condon factors gave poor results, and values for the higher vibrational levels of the A state [(0,v(2),0), with v(2) (')>6] from the ground state were missing; hence new values were calculated. These were computed for transitions between low-lying vibrational levels of CF(2) X (1)A(1) to vibrational levels of CF(2) A (1)B(1) (v(1) ('),v(2) ('),0) up to high values of the vibrational quantum numbers using high level ab initio calculations combined with an anharmonic Franck Condon factor method. The Franck Condon factors were used to determine the absorption cross sections of CF(2) at selected wavelengths, which in turn were used to calculate number densities from the experimental spectra. Number densities of CF(2) have been determined in different regions of the plasma, including the center of the plasma and outside the plasma volume, and CF(2) rotational temperatures and vibrational energy distributions were estimated. For absorption spectra obtained outside the confined plasma volume, the CF(2) density was determined as (0.39+/-0.08)x10(13) molecule cm(-3) and the vibrational and rotational temperatures were determined as 303 and 350 K, respectively. In the center of the plasma reactor, the CF(2) density is estimated as (3.0+/-0.6)x10(13) molecules cm(-3) with T(rot) approximately 500 K. The fitted vibrational distribution in the CF(2) ground state corresponds to two Boltzmann distributions with T(vib) approximately 300 and T(vib) approximately 1000 K, indicating that CF(2) molecules are initially produced highly vibrationally excited, but are partially relaxed in the plasma by collision.     

Unimolecular reactions in the CF3CH2Cl ↔ CF2ClCH2F system: isomerization by interchange of Cl and F atoms

The recombination of CF(2)Cl and CH(2)F radicals was used to prepare CF(2)ClCH(2)F* molecules with 93 ± 2 kcal mol(-1) of vibrational energy in a room temperature bath gas. The observed unimolecular reactions in order of relative importance were: (1) 1,2-ClH elimination to give CF(2)═CHF, (2) isomerization to CF(3)CH(2)Cl by the interchange of F and Cl atoms and (3) 1,2-FH elimination to give E- and Z-CFCl═CHF. Since the isomerization reaction is 12 kcal mol(-1) exothermic, the CF(3)CH(2)Cl* molecules have 105 kcal mol(-1) of internal energy and they can eliminate HF to give CF(2)═CHCl, decompose by rupture of the C-Cl bond, or isomerize back to CF(2)ClCH(2)F. These data, which provide experimental rate constants, are combined with previously published results for chemically activated CF(3)CH(2)Cl* formed by the recombination of CF(3) and CH(2)Cl radicals to provide a comprehensive view of the CF(3)CH(2)Cl* ? CF(2)ClCH(2)F* unimolecular reaction system. The experimental rate constants are matched to calculated statistical rate constants to assign threshold energies for the observed reactions. The models for the molecules and transition states needed for the rate constant calculations were obtained from electronic structures calculated from density functional theory. The previously proposed explanation for the formation of CF(2)═CHF in thermal and infrared multiphoton excitation studies of CF(3)CH(2)Cl, which was 2,2-HCl elimination from CF(3)CH(2)Cl followed by migration of the F atom in CF(3)CH, should be replaced by the Cl/F interchange reaction followed by a conventional 1,2-ClH elimination from CF(2)ClCH(2)F. The unimolecular reactions are augmented by free-radical chemistry initiated by reactions of Cl and F atoms in the thermal decomposition of CF(3)CH(2)Cl and CF(2)ClCH(2)F.     

Mechanistic study and kinetic properties of the CF3CHO + Cl reaction

Theoretical investigations have been carried out on the mechanism and kinetics for the reaction of CF 3 CHO + Cl using duallevel direct dynamics method. The potential energy surface information was obtained at the MCQCISD/3//MP2/cc-pVDZ level and the kinetic calculations were done using variational transition state theory with interpolated single-point energy (VTST-ISPE) approach. The calculated results show that the reaction proceeds primarily via the H-abstraction channel, while the Cl-addition channel is unfavorable due to the higher barriers. The improved canonical variational transition-state theory (ICVT) with the small-curvature tunneling correction (SCT) was used to calculate the rate constants. The theoretical rate constants at room temperature are in general agreement with the experimental values. A three-parameter rate constant expression was fitted over a wide temperature range of 200-2000 K.     

The infrared intensities and polar tensors of the fluorochloromethanes

The polar tensors of CF3Cl, CF2Cl2 and CFCl3 have been calculated using recent measurements of their gas phase infrared fundamental intensities. The polar tensors obtained for CF2Cl2 and CFCl3 are in very good agreement with those obtained previously since the more recent experimental intensity results are in good agreement with those reported earlier. For CF2Cl2 rhoC = +1.626, rhoF = -0.577 and rhoCl = -0.26e whereas rhoC = +1.369, 0.478 and rhoCl = 0.297e for CFCl3. However, two sets of significantly different mean dipole moment derivatives are obtained from the experimentally measured intensities of CF3Cl reported by two different laboratories. On the other hand, the differences in the mean derivatives of these two sets are not large enough so that results from electronegativity models, potential models for core ionization energies and quantum chemical calculations at the Moller-Plesset 2 and B3LYP density functional levels are sufficient to indicate which set is the correct one. As such average values of rhoC = +1.907+/-0.178e, rhoF = -0.590+/-0.056e and rhoCl = -0.139+/-0.013e obtained from both sets of polar tensor elements are recommended for the CF33Cl mean dipole moment derivatives.     

Unimolecular reactions of vibrationally excited CF2ClCHFCH3 and CF2ClCHFCD3: evidence for the 1,2-FCl interchange pathway

Chemically activated CF2ClCHFCH3 and CF2ClCHFCD3 molecules were prepared with 94 kcal mol-1 of vibrational energy by the recombination of CF2ClCHF and CH3(CD3) radicals at room temperature. The unimolecular reaction pathways were 2,3-FH(FD) elimination, 1,2-ClF interchange and 1,2-ClH elimination; the interchange produces CF3CHClCH3(CF3CHClCD3) with 105 kcal mol-1 of vibrational energy. Rate constants for CF2ClCHFCH3 [CF2ClCHFCD3] were (3.1+/-0.4)x10(6) s-1 [(1.0+/-0.1)x10(6) s-1] for 2,3-FH [FD] loss, (1.5+/-0.2)x10(6) s-1 [(8.3+/-0.9)x10(5) s-1] for 1,2-ClF interchange, and (8.2+/-1.0)x10(5) s-1 [(5.3+/-0.6)x10(5) s-1] for 1,2-ClH [DCl] loss. These correspond to branching fractions of 0.55+/-0.06 [0.43+/-0.04] for 2,3-FH [FD] loss, 0.29+/-0.03 [0.35+/-0.04] for 1,2-ClF interchange, and 0.16+/-0.02 [0.22+/-0.02] for 1,2-ClH [ClD] loss. Kinetic-isotope effects were 3.0+/-0.6 for 2,3-FH [FD] loss, 1.6+/-0.3 for 1,2-ClH loss, and 1.8+/-0.4 for 1,2-ClF interchange. The CF3CHClCH3 (CF3CHClCD3) molecules formed by 1,2-FCl interchange react by loss of HCl [DCl] with rate constants of (5.6+/-0.9)x10(7) s-1 [(2.1+/-0.4)x10(7)] s-1 for an isotope effect of 2.7+/-0.4. Density functional theory was employed to calculate vibrational frequencies and moments of inertia for the molecules and for the transition-state structures. These results were used with RRKM theory to assign threshold energies from comparison of computed and experimental unimolecular rate constants. The threshold energy for ClF interchange is 57.5 kcal mol-1, and those for HF and HCl channels are 2-5 kcal mol-1 higher. Experiments with vibrationally excited CF2ClCF2CF3, CF2ClCF2CF2Cl, and CF2ClCF2Cl, which did not show evidence for ClF interchange, also are reported.     

Preparation, crystallographic characterization and theoretical study of two isomers of C70(CF3)12

Two isomers of C70(CF3)12 have been isolated from a mixture obtained by trifluoromethylation of C70 with CF3I; their molecular structures determined by X-ray crystallography are in good agreement with the results of theoretical DFT calculations for the most stable C70(CF3)12 isomers.     

Time-dependent density functional approach for the calculation of inelastic x-ray scattering spectra of molecules

We apply time-dependent density functional theory to study the valence electron excitations of molecules and generalize the typically used time-propagation scheme and Casida's method to calculate the full wavevector dependent response function. This allows the computational study of dipole-forbidden valence electron transitions and the dispersion of spectral weight as a function of the wavevector. The method provides a novel analysis tool for spectroscopic methods such as inelastic x-ray scattering and electron energy loss spectroscopy. We present results for benzene and CF(3)Cl and make a comparison with experimental results.     

Adsorption of fluorinated ethers and alcohols on fresh and oxidized carbon overcoats for magnetic data storage

Temperature programmed desorption has been used to study the desorption kinetics and desorption energies of perfluorodiethylether, (CF3CF2)2O, and 2,2,2-trifluoroethanol, CF3CH2OH, adsorbed on fresh and oxidized hydrogenated amorphous carbon (a-CHx) films. (CF3CF2)2O and CF3CH2OH serve as models for the ether backbone and hydroxyl end-groups of Fomblin Zdol, the lubricant most commonly used to lubricate the surfaces of amorphous carbon overcoats on magnetic data storage hard disks. Our measurements clearly reveal, for the first time, the effects of surface oxidation on the adsorption of fluorocarbon lubricants such as Fomblin Zdol on a-CHx films. Oxidation of the a-CHx surface increases the desorption energy of CF3CH2OH but has no observable impact on the desorption energy of (CF3CF2)2O. These results support the suggestion that the alcohols interact with the surface via hydrogen bonding. From a practical perspective, these results imply that the oxidation of the fresh a-CHx film may serve as a means to control or tailor the a-CHx surface to optimize the properties of the lubricant-overcoat interface in hard disks.