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1.
Rate constants for the gas‐phase reactions of hydroxyl radicals and chlorine atoms with a series of alcohols have been determined by using the relative method. The experiments were performed at 295 ± 2 K and at 1 atmospheric pressure. The obtained values of the rate constants in units of 10?12 cm3 molecule?1 s?1 are as follows:
Alcohol Rate Constants for OH with Rate Constants for Cl with
Propane Cyclohexane Propane Cyclohexane
Ethyl alcohol 3.40 ± 0.25 103 ± 4 96 ± 7
n‐Propyl alcohol 5.47 ± 0.44 153 ± 13 147 ± 11
Isopropyl alcohol 5.31 ± 0.39 73.5 ± 3.7 82.7 ± 7.4
n‐Butyl alcohol 8.66 ± 0.66 211 ± 11 223 ± 10
Isobutyl alcohol 9.08 ± 0.35 9.59 ± 0.45 182 ± 4 196 ± 11
tert‐Butyl alcohol 1.11 ± 0.07 31.5 ± 2.4 34.1 ± 2.5
n‐Pentyl alcohol 12.2 ± 1.0 12.4 ± 0.5 257 ± 25 258 ± 12
Isopentyl alcohol 13.8 ± 0.5 13.2 ± 1.1 237 ± 7 235 ± 9
The above relative rate constants are based on the values (in units of 10?12 cm3 molecule?1 s?1) of k(OH + propane) = 1.08, k(OH + cyclohexane) = 7.22, k(Cl + propane) = 131 and k(Cl + cyclohexane) = 307. The results are compared with previous determinations. © 2002 Wiley Periodicals, Inc. Int J Chem Kinet 35: 81–87, 2003  相似文献   

2.
Rate constants for the gas phase reactions of hydroxyl radicals and chlorine atoms with a number of ethers have been determined at 300 ± 3 K and at a total pressure of 1 atmosphere. Both OH radical and chlorine atom rate constants were determined using a relative rate technique. Values for the rate constants obtained are as follows.
compound kOH×1012(cm3 molecule?1 s?1) kC1×1011(cm3 molecule?1 s?1)
Hexane 5.53 ± 1.55
2-Chloro ethyl methyl ether 4.92 ± 1.09 14.4 ± 5.0
2,2-Dichloro ethyl methyl ether 2.37 ± 0.50 4.4 ± 1.6
2-Bromo ethyl methyl ether 6.94 ± 1.38 16.3 ± 5.4
2-Chloro,1,1,1-trifluoro ethyl ethyl ether <0.3 0.30 ± 0.10
Isoflurane <0.3 <0.1
Enflurane <0.3 <0.1
Di-i-propyl ether 11.08 ± 2.26 16.3 ± 5.4
Diethyl ether 25.8 ± 4.4
The above relative rate constants are based on the values of k(OH + pentane)=[3.94 ± 0.98]×10?12 and k(OH + diethyl ether)=[13.6 ± 2.26] × 10?12 cm3 molecule?1 s?1 in the case of the hydroxyl reactions. In the case of the chlorine atom reactions, the above rate constants are based on values of k(Cl + ethane)=[5.84 ± 0.88] × 10?11 and k(Cl + diethyl ether)=[25.4 ± 8.05] × 10?11 cm3 molecule?1 s?1. The quoted errors include ±2σ from a least squares analysis of our slopes plus the uncertainty associated with the reference rate constants. Atmospheric lifetimes calculated with respect to reaction with OH radicals are based on a tropospheric OH radical concentration of (7.7 ± 1.4) × 105 radicals cm?3, and lifetimes with respect to reaction with Cl atoms are based on a tropospheric Cl atom concentration of 1 × 103 atoms cm?3. Observed trends in the relative rates of reaction of hydroxyl radicals and chlorine atoms with the ethers studied is discussed. The significance of the calculated tropospheric lifetimes is also reviewed. © 1993 John Wiley & Sons, Inc.  相似文献   

3.
The kinetics of chlorine atom abstraction from the chloroethanes (EClH) 1,1,2-C2Cl3H3, 1,1-C2Cl2H4, and 1,2-C2Cl2H4 by radiolytically generated cyclohexyl radicals was studied in the liquid phase by a competitive method. The chlorine atom abstraction data were put on an absolute basis by comparing the rates of the metathetical reactions with the known rate of addition of cyclohexyl radicals to C2Cl4. The following Arrhenius parameters were obtained:
E(EClH)- Temperature
A(ECLH) E(CCl4) log A(EClH) E(EClH) Range
log
EClH A(C2Cl4) (kcal/mol) (1.mol·sec) (kcal/mol) (°C)
CHCL2CH2Cl 0.03 ± 0.08 3.87 ± 0.17 8.98 ± 0.14 11.17 ± 0.27 150 – 250
CHCL2CH3 0.13 ± 0.13 4.63 ± 0.27 8.18 ± 0.19 11.93 ± 0.37 130 – 250
CHCL2CH2Cl 0.50 ± 0.17 7.57 ± 0.35 9.18 ± 0.23 14.87 ± 0.45 150 – 250
The error limits are the standard deviations from least mean square Arrhenius plots. The α and ß activation effects on the kinetics of Cl atom abstraction from chloroalkanes are discussed. From the linear relation between the relative reactivities of cyclohexyl radicals toward the XCCl3 and XCHCl2 series, ECl(c-C6H11· + CHCl2CHCl2) = 10.2 ± 1 kcal/mol and ECl(c-C6H11· + CHCl22CCl3) = 9.7 ± 1 kcal is derived.  相似文献   

4.
The reactions (R = CF3, C2F5, and i,-C3F7) have been studied competitively in the gas phase over the range of 27–231°C. The following Arrhenius parameters were obtained:
log A,(cm3/mol · s) E,(kJ/mol)
R = CF3 13.99 ± 0.21 17.1 ± 2.0
R = C2F5 13.97 ± 0.20 11.5 ± 2.0
R = i,-C3F7 14.18 ± 0.20 10.2 ± 2.0
The above data lead to bond dissociation energies D(R-I) which are compared with previous published results. The following values are recommended: D,(CF3-I) = 224, D,(C2F5-I) = 219, and D,(i,-C3F7-I) = 215 kJ/mol.  相似文献   

5.
We present a kinetic study of atomic potassium in its electronic ground state, K(42S½), generated in the “single-shot mode” by pulsed irradiation at elevated temperatures and monitored by time-resolved atomic resonance absorption spectroscopy using the Rydberg doublet at λ = 404 nm (K[52PJ]←K[42S½]). Profiles for the decay of atomic potassium in the presence of various halogenated reactants were recorded at different temperatures, yielding the following Arrhenius parameters (kR = A exp(?E/RT), errors 1σ):
R A/10?10 cm3 molecule?1s?1 E/kJ mol?1 Temp. Range
CH3F 1.93+1.1?0.7 59±3.3 822–922 K
C2H5F 1.40+2.5?0.9 62±6.6 694–807 K
C6H5F 2.0+1.6?0.9 41±3.9 705–812 K
CH3Br 1.7+0.3?0.2 15.9±1.2 798–903 K
HCl 5.6+3.5?2.1 34.7±3.5 828–902 K
HBr 1.9+0.3?0.3 34±1.2 836–925 K
A limited body of data is reported for k(K + C2H5Br) = 3.6 × 10?11 cm3 molecule?1 s?1 for the temperature range 704–733 K. These results for atomic potassium constitute a new body of absolute rate data which are compared with some previous results for reactions of atomic potassium with other reactants, and for reactions of atomic sodium, also determined by time-resolved atomic resonance absorption spectroscopy. The data for HCl and HBr are finally compared with early estimates reported using diffusion flames.  相似文献   

6.
We present a kinetic study of the reaction of ground state silicon atoms with halogenated unsaturated organic compounds (R). Si(33PJ) was generated by the repetitive pulsed irradiation of SiCl4 in the presence of excess helium buffer gas and the reactant R in a slow flow system, kinetically equivalent to a static system. The ground state atom was monitored by time-resolved atomic resonance absorption spectroscopy at λ = 252 nm [Si(43PJ) ← Si(33PJ)] on time scales by which the optically metastable tates,Si(31D2) and Si(31S0) had relaxed to the 3P state, using signal averaging methods. Computerized fitting of the resulting atomic decay traces in the presence of the various reactants, R, yielded the following new body of absolute second-order rate constants (kR, T = 300 K, errors = 2sigma;):
R kR/cm3 molecule?1 s?1
C2F4 1.6 ± 0.2 × 10?10
C2Cl4 9.9 ± 1.7 × 10?10
CH2CF2 4.0 ± 0.6 × 10?10
CHClCCl2 7.0 ± 1.1 × 10?10
CF3CH? CH2 4.6 ± 0.5 × 10?10
C6H6 4.4 ± 1.0 times; 10?10
C6F6 4.4 ± 0.6 × 10?10
C6HF5 4.6 ± 1.3 × 10?10
C6H2F4 3.9 ± 0.8 × 10?10
C6F5—CF3 5.1 ± 0.6 × 10?10
These data are compared, where appropriate, with analogous data for unsaturated hydrocarbon organic compounds. They are also discussed within the general context of nuclear recoil measurements involving 31Si.  相似文献   

7.
The kinetics of reactions involving halogen atom abstraction from haloalkanes by methyl radicals have been studied in the gas phase. Arrhenius parameters for halogen atom transfer were determined relative to those for methyl radical combination:
RX log10A2(L/mol · s) E2(kcal/mol)
CFCl3 8.3 ± 0.2 10.7 ± 0.4
CF3CCl3 7.9 ± 0.3 9.7 ± 0.6
CF2Cl2 9.1 ± 0.4 11.3 ± 0.7
CF3Cl 8.8 ± 0.5 11.8 ± 1.0
CF3CF2Cl 8.3 ± 0.3 10.9 ± 0.7
CF3Br 8.6 ± 0.2 9.3 ± 0.5
CF3I 8.1 ± 0.1 4.3 ± 0.2
CH3CH2I 8.9 ± 0.3 7.4 ± 0.6
The rate data obtained are used to provide information on the importance of polar effects for halogen abstraction processes.  相似文献   

8.
Singlet molecular oxygen, O2(1Σ), is one of the important intermediate species in the atmospheres of Earth, Mars, and Venus. To elucidate the chemistry of this excited molecular oxygen, a series of kinetic measurements have been undertaken using the flow-discharge/optical-emission technique. By monitoring the characteristic emission (762 nm for 1Σ), the quenching rates for several important molecules have been obtained at room temperature. The following table summarizes measurements.
Quencher Rate Constants (cm3/s)
CH2 (4.6 ± 0.5) × 10?13
H2 (7.0 ± 0.3) × 10?13
N2 (1.7 ± 0.1) × 10?15
Cl2 (4.5 ± 0.8) × 10?16
CO (4.5 ± 0.5) × 10?15
O3 (2.2 ± 0.3) × 10?11
2,3 DBM-2 (6.0 ± 0.1) × 10?13
The error limits represent one standard deviation. The systematic error is estimated to be about 15%. For CO2 and O3 molecules, the quenching rate constants were also measured in the temperature range of 245–362 K. In both reactions, negligible temperature dependences (with the activation energy less than 0.6 kcal/mole) were observed.  相似文献   

9.
The reactions of some perfluoroalkyl radicals with carbon tetrachloride have been studied using the photolysis of the corresponding perfluoroalkyl iodide as the free radical source. The Arrhenius parameters, based on the value of 2.3 × 1013 cm3 mol?1 s?1 for the self-combination rate constant of all radicals are:
Reaction log(A/cm3 mol?1 s?1) E/kcal mol?1
CF3 + CCl4 12.8 11.3
C2F5 + CCl4 12.8 11.6
n-C3F7 + CCl4 12.9 12.0

Citing Literature

Volume 16 , Issue 11 November 1984

Pages 1351-1356  相似文献   


10.
A kinetic investigation is described of the reaction of ground state atomic carbon, C(2p2(3PJ)), monitored by time-resolved atomic resonance absorption spectroscopy, with a wide range of halogenated olefins and aromatic compounds. Atomic carbon was generated by the repetitive pulsed irradiation (λ > ca. 160 nm) of C3O2 in the presence of excess helium buffer gas and the added reactant gases in a slow flow system, kinetically equivalent to a static system. C(23PJ) was then monitored photoelectrically by time-resolved atomic resonance absorption in the vacuum ultra-violet (λ = 166 nm, 33PJ ← 23PJ) with direct computer interfacing for data capture and analysis. The following absolute second-order rate constants for the reactions of C(23PJ) with the following reactants are reported:
Reactant kR/cm3 molecule?1 s?1 (300 K)
C2F4 (1.9 ± 0.1) × 10?10
C2Cl4 (10.6 ± 0.5) × 10?10
CH2CF2 (4.3 ± 0.2) × 10?10
CHClCCl2 (7.9 ± 0.4) × 10?10
C6H6 (4.8 ± 0.3) × 10?10
C6F6 (4.9 ± 0.3) × 10?10
C6HF5 (5.0 ± 0.3) × 10?10
C6H2F4 (4.4 ± 0.2) × 10?10
C6H5—CH3 (5.5 ± 0.3) × 10?10
C6F5—CF3 (5.4 ± 0.3) × 10?10
These results, constituting the first reported body of absolute rate data for reactions of ground state carbon with these reactants, are compared with the analogous body of absolute rate data for atomic silicon in its Si(3p2(3PJ)) ground state, also determined hitherto by time-resolved atomic resonance absorption spectroscopy and demonstrating similar kinetic behavior. © 1993 John Wiley & Sons, Inc.  相似文献   

11.
The relative hydroxyl radical reaction rate constants from the simulated atmospheric oxidation of selected acetates and other esters have been measured. Reactions were carried out at 297 ± 2 K in 100-liter FEP Teflon®-film bags. The OH radicals were generated from the photolysis of methyl nitrite in pure air. Using a rate constant of 2.63 × 10?11 cm3 molecule?1 s?1 for the reaction of OH radicals with propene, the principal reference organic compound, the rate constants (×1012 cm3 molecule?1 s?1) obtained for the acetates and esters used in this study are:
n–propyl acetate 3.42 ± 0.87
n–butyl acetate 5.71 ± 0.94
n–pentyl acetate 7.53 ± 0.48
2–ethoxyethyl acetate 10.56 ± 1.31
2–ethoxyethyl isobutyrate 13.56 ± 2.32
2–ethoxyethyl methacrylate 27.22 ± 2.06
4–pentene-1-yl acetate 43.40 ± 3.85
3–Ethoxyacrylic acid ethyl ester 33.30 ± 1.22
Error limits represent 2σ from linear least-squares analysis of data. A linear correlation was observed for a plot of the measured relative rate constants vs. the number of CH2 groups per molecule of the following acetates: methyl acetate, ethyl acetate, n-propyl acetate, butyl acetate, and pentyl acetate. © 1993 John Wiley & Sons, Inc.  相似文献   

12.
Internationally distributed organic and inorganic oxygen isotopic reference materials have been calibrated by six laboratories carrying out more than 5300 measurements using a variety of high‐temperature conversion techniques (HTC) a in an evaluation sponsored by the International Union of Pure and Applied Chemistry (IUPAC). To aid in the calibration of these reference materials, which span more than 125‰, an artificially enriched reference water (δ18O of +78.91‰) and two barium sulfates (one depleted and one enriched in 18O) were prepared and calibrated relative to VSMOW2 b and SLAP reference waters. These materials were used to calibrate the other isotopic reference materials in this study, which yielded:
Reference material δ18O and estimated combined uncertainty c
IAEA‐602 benzoic acid +71.28 ± 0.36‰
USGS35 sodium nitrate +56.81 ± 0.31‰
IAEA‐NO‐3 potassium nitrate +25.32 ± 0.29‰
IAEA‐601 benzoic acid +23.14 ± 0.19‰
IAEA‐SO‐5 barium sulfate +12.13 ± 0.33‰
NBS 127 barium sulfate +8.59 ± 0.26‰
VSMOW2 water 0‰
IAEA‐600 caffeine ?3.48 ± 0.53‰
IAEA‐SO‐6 barium sulfate ?11.35 ± 0.31‰
USGS34 potassium nitrate ?27.78 ± 0.37‰
SLAP water ?55.5‰
The seemingly large estimated combined uncertainties arise from differences in instrumentation and methodology and difficulty in accounting for all measurement bias. They are composed of the 3‐fold standard errors directly calculated from the measurements and provision for systematic errors discussed in this paper. A primary conclusion of this study is that nitrate samples analyzed for δ18O should be analyzed with internationally distributed isotopic nitrates, and likewise for sulfates and organics. Authors reporting relative differences of oxygen‐isotope ratios (δ18O) of nitrates, sulfates, or organic material should explicitly state in their reports the δ18O values of two or more internationally distributed nitrates (USGS34, IAEA‐NO‐3, and USGS35), sulfates (IAEA‐SO‐5, IAEA‐SO‐6, and NBS 127), or organic material (IAEA‐601 benzoic acid, IAEA‐602 benzoic acid, and IAEA‐600 caffeine), as appropriate to the material being analyzed, had these reference materials been analyzed with unknowns. This procedure ensures that readers will be able to normalize the δ18O values at a later time should it become necessary. The high‐temperature reduction technique for analyzing δ18O and δ2H is not as widely applicable as the well‐established combustion technique for carbon and nitrogen stable isotope determination. To obtain the most reliable stable isotope data, materials should be treated in an identical fashion; within the same sequence of analyses, samples should be compared with working reference materials that are as similar in nature and in isotopic composition as feasible. Copyright © 2009 John Wiley & Sons, Ltd.  相似文献   

13.
The reactions have been studied by a mass-balance method involving the photolysis of small amounts of biacetyl in the presence of a large excess of isobutane containing a small proportion of the unsaturated substrate. The following Arrhenius parameters have been derived:
Temperature
E log A range
Reaction (kcal/mol) (1./mol·sec) (°K)
?H3 + C2H4 → ?3H7 7.3 ± 1.0 8.32 ± 0.5 350 – 500
?H3 + C2H2 → ?3H5 7.7 ± 1.5 8.79 ± 0.8 379 – 487
?H3 + C6H6 → C7H9 7.6 ± 1.0 8.79 ± 0.5 372 – 484
The results for methyl addition to ethylene are based on previous determinations by other techniques as well as the present studies. The results for methyl addition to acetylene and benzene are derived solely from the present experiments and are calculated relative to a rate constant of log k2(l./mol·sec) = 7.42 - (7.1/θ) for the reference reaction (2), ·H3 + (CH3)3CH → CH4 + ·4H9.  相似文献   

14.
The following Arrhenius parameters have been determined for the hydrogen-abstraction reactions: R + (CH3)4Si → RH + (CH3)3SiCH3
R Temp. (°K) E (kcal/mole) Log A (mole?1 cc sec?1) Log k(400°K) (mole?1 cc sec?1)
CF3 330–433 7.23 ± 0.09 11.90 ± 0.05 7.95
CH3 396–476 10.23 ± 0.36 11.55 ± 0.18 5.68
CD3 396–496 10.36 ± 0.12 11.84 ± 0.06 6.20
C2H5 423–522 11.40 ± 0.48 11.88 ± 0.22 5.68
The activation energies are in keeping with the strengths of the bonds formed during the reaction. By comparison with the activation energies for the analogous reactions of neopentane it is estimated that D((CH3)3SiCH2? H) ? 97 kcal/mole. The A factors for the above series of reactions fall within the range predicted by transition-state theory for this type of process and the validity of previous results of Kerr, Slater, and Young is seriously in doubt.  相似文献   

15.
The overall photobromination reactions have been studied using a competitive technique. Relative Arrhenius parameters were obtained for the rate-determining step These were placed on an absolute basis using previous-absolute values of A and E for RFI=CF3I. The activation energies were used to calculate bond dissociation energies D(R? I) with the following results:
RF? E16 D(RF?I)(kcal/mole)
CF3I a a E16 from [1]
10.8 52.6
C2F5I 8.8 50.6
n-C3F7I 7.4 49.2
i-C3F7I 7.5 49.2
n-C4F9I 6.7 48.4
  • a E16 from [1]
The D(RI) are compared with related D(R? I) and it is concluded that for a given alkyl group RH and the corresponding perfuloroalkyl group RF, D(RI) > D(RI) whereas it has previously been found that D(RX;) < D(RX) where X is not iodine.  相似文献   

16.
The gas phase photolysis of CCl4 in the presence of several alkanes has been used to obtain Arrhenius parameters for the abstraction of hydrogen atoms by the CCl3 radical: The following log k4 values were obtained:
RH log k4
c-C5H10,
n-C6H14
2,3-Dimethylbutane
c-C7H14
Methylcyclohexane
c-C8H16
The results are compared to those for CH3 and CF3 radicals.  相似文献   

17.
Four analogues of LH-RH modified in position 5 have been synthesized using either classical procedures or the solid phase method. The gonadotropin-releasing activities were determined by radioimmunological measurements of LH and FSH in vivo and in vitro and the immunoreactivities by a specific LH-RH radioimmunoassay (RIA). The following relative potencies and immunoractivities were found:
in vivo in vitro Immuno-reactivity
LH-RH: 100 % 100 % 100 %
[Tyr(Me)5] -LH-RH: 8.6% 6.0% 40.0%
[Phe5] -LH-RH: 42.5% 27.5% 17.0%
[Cha5]
  • a Abbreviations were used according to [37]; Cha = cyclohexyl-L-alanine.
  • -LH-RH: 22.4% 27.8% 10.0%
    [Gly5] -LH-RH: 0.1% 0.5% 0.7%

    Citing Literature

    Volume 57 , Issue 7 6 November 1974

    Pages 2131-2139  相似文献   


    18.
    Competitive studies of the reactions of ground-state oxygen atoms, generated by mercury-photosensitized decomposition of nitrous oxide, have been carried out with ethylene and all the fluoroethylenes using 2-(trifluoromethyl)-propene as reference compound. From measurements at 25°C and 150°C relative rate constants have been determined and used to calculate the Arrhenius parameters shown in the following table:
    Olefin ΔERef ΔE
    CH2? CH2 1.10 ?1.18 (1.0) (0)
    CH2? CHF 1.03 0.84 0.94 2.02
    CH2? CF2 0.71 1.49 0.65 2.67
    CHF? CHF (cis-) 1.23 1.92 1.12 3.10
    CHF? CHF (trans-) 1.40 0.79 1.27 1.97
    CF2? CHF 1.06 0.00 0.96 1.22
    CF2? CF2 0.86 ?3.22 0.78 ?2.04
    • a ΔERef = Eolefin ? E2TFMP and ΔE = Eolefin ? E. Units are kJ/mole.
    The results are compared with corresponding data for other atoms and radicals, and discussed in terms of the electronic changes produced in the double bond by fluorine substitution, and in relation to the nature of the transition state.  相似文献   

    19.
    The photolysis of 1,1,3,3-tetrafluoroacetone has been reinvestigated as a source of CHF2 radicals at temperatures up to 578°K, and the following rate constant ratio was determined for the reactions
  • 1 θ= 2.303 RT in kcal/mole.
  • 1,1-Difluoro- and 1,1,3,3-tetrafluoroacetone were photolyzed in the presence of tetramethylsilane, and Arrhenius parameters were measured for the hydrogen abstraction reactions: R + Me4Si → RH + Me3SiCH2
    R T(°K) E (kcal/mole) log A (mole?1cc sec?1) log k (500°K) (mole?1cc sec?1)
    CH2F 473–586 12.00 ± 0.30 11.68 ± 0.12 6.44
    CHF2 416–526 10.18 ± 0.33 11.65 ± 0.15 7.21
    By comparing with previous data on the CH3 and CF3 reactions, the activation energies were interpreted in terms of the enthalpy changes for the reactions and a polar effect operative between the attacking fluoromethyl radicals and the substrate which tends to reduce the activation energy progressively as the fluorine content of the radical increases. This polar effect, which decreases the activation energy for hydrogen abstraction from SiMe4 along the series CH3, CH2F, CHF2, and CF3, is in marked contrast to the polar repulsion between the fluorinated radicals and SiHCl3 which was tentatively proposed to explain the increase in activation energy observed in the same series of reactions with SiHCl3.  相似文献   

    20.
    The photolyses of 1,3-difluoro- and 1,1,3,3-tetrafluoroacetone have been reinvestigated as sources of fluoromethyl radicals, and the following rate constant ratios were determined
  • 1 θ= 2.303 RT in kcal/mole.
  • The results are in substantial agreement with the original investigations. The photolyses of the fluoroacetones were used as sources of CH2F and CHF2 radicals, and the following Arrhenius parameters were obtained for the hydrogen abstraction reactions R + SiHCl3 → RH + SiCl3:
    R T(°K) E (kcal/mole) log A (mole?1 cc sec?1) log k (400°K) (mole?1 cc sec?1)
    CH2F 335–443 6.06 ± 0.15 10.79 ± 0.08 7.48 CHF2
    CHF2 334–442 6.82 ± 0.09 11.32 ± 0.05 7.59
    The rates of reactions of CH2F and CHF2 radicals toward hydrogen abstraction from SiHCl3 are an order of magnitude lower than the corresponding rates for the CH3, C2H5, and CF3 radicals as a result of increased activation energies for the CH2F and CHF2 reactions. The interpretation of the results is hindered by a lack of accurate thermochemical data on the radicals. The activation energies, as they stand, can be rationalized in terms of a polar repulsion between SiHCl3 and the radicals, increasing regularly and leading to a progressive increase in activation energy with increasing fluorine substitution in the radical. This interpretation is consistent with the estimates D(CH2F? H) ∝ D(CHF2? H) ∝ 97 kcal/mole. On the other hand, there is some indication, from the spread of A-factors in the series of fluoromethyl radicals reacting with SiHCl3, that internal compensation of Arrhenius parameters is occurring in some of the reactions; and when this is taken into account, the interpretation of activation energies is more difficult.  相似文献   

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