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Theoretical investigations on mechanisms and kinetics of the CH3CFClO2· with ClO· reaction in the atmosphere


The singlet and triplet potential energy surfaces of the ClO• radical reaction with the CH3CFClO2• radical have been investigated at the CCSD(T)/cc-pVTZ level based on the optimized geometries at the B3LYP/6–311++G(d,p) level. On the singlet potential energy surfaces (PES), the possible reaction involves association-dissociation, direct H-abstraction and Nucleophilic Substitution 2 (SN2) mechanisms. On the triplet PES, SN2 displacement and direct H-abstraction reaction pathways have been investigated, which are less competitive compared with the reaction pathways on the singlet PES. The rate constants have been calculated at 10–10 to 1010 atm and 200–3,000 K by Rice–Ramsperger–Kassel–Marcus (RRKM) theory for the important product pathways. At 200–800 K, IM1 produced (CH3CFClOOOCl) by collisonal deactivation is dominant; at high temperatures, the production P1 (CH3CFO + ClOOCl) becomes dominate. The calculated rate constants for CH3CFClO2• + ClO• are good agreement with the available experimental value. The atmospheric lifetime of CH3CFClO2• in ClO• is around 3.27 h. TD-DFT computations imply that IM1 (CH3CFClOOOCl), IM2 (CH3CFClOOClO) and IM3 (CH3CFClOClO2) will photolyze under the sunlight.


ClO• radical is an active halogen species, and it is abundant in the atmosphere. It is of great atmospheric significance due to its ability to destroy ozone. ClO• plays a major role in the formation of the Antarctic “ozone hole”, through the following catalytic cycle1:

$$ \begin{gathered} {\text{ClO + ClO + M}} \to {\text{ClOOCl } + \text{ M}} \hfill \\ {\text{ClOOCl}} + hv \to {\text{Cl } + \text{ ClOO}} \hfill \\ {\text{ClOO } + \text{ M}} \to {\text{Cl}} + {\text{O}}_{2} + {\text{M}} \hfill \\ {\text{2*(Cl + O}}_{3} \to {\text{ClO } + \text{ O}}_{{2}} ) \hfill \\ {\text{Net:2O}}_{3} + hv \to 3{\text{O}}_{2} \hfill \\ \end{gathered} $$

The production and photolysis for the dipolymer of ClO• (ClOOCl) are necessary for the chemistry in the above process. According to statistics, this cycle brought about 70% destruction of the Antarctic ozone2. However, recent studies have suggested that this gas-phase chemistry alone cannot account for ozone loss due to chlorine-catalyzed loss of ozone3.

The CH3CFClO2• radical is predicted to be produced by the photolysis of the CH3CFCl2 in the presence of excessive oxygen4

$$ \begin{gathered} {\text{CH}}_{3} {\text{CFCl}}_{2} + hv \to {\text{CH}}_{3} {\text{CFCl}} + {\text{Cl}} \hfill \\ {\text{CH}}_{3} {\text{CFCl}} + {\text{O}}_{2} \to {\text{CH}}_{3} {\text{CFClO}}_{2} \hfill \\ \end{gathered} $$

The possible degradation mechanism of the peroxy radicals includes self-reactions and reactions with radicals, i.e. •Cl, ClO• and NO4,5. In particular, the reaction of alkyl peroxide radical with ClO• is an interesting system, which has an important influence on stratospheric ozone chemistry and CH3CFCl2 oxidation chain. Previous research5 have estimated that the dominant products of the CH3CFClO2• + ClO• reaction are alkoxy chloride (CH3CFClOCl), oxygen molecule, alkoxy group (CH3CFClO) and chlorine peroxide (ClOO).

$$ \begin{gathered} {\text{CH}}_{3} {\text{CFClO}}_{2} + {\text{ClO}} \to {\text{CH}}_{3} {\text{CFClOCl}} + {\text{O}}_{2} \hfill \\ {\text{CH}}_{3} {\text{CFClO}}_{2} + {\text{ClO}} \to {\text{CH}}_{3} {\text{CFClO } + \text{ ClOO}} \hfill \\ \end{gathered} $$

Wu and Carr5 investigated the with CH3CFClO2• + ClO• reaction by UV flash photolysis and time-resolved mass spectrometry at 253–321 K and 4–60 Torr, and the rate constants were estimated to be (4.5 ± 1) × 10–12 cm3molecule-1 s-1 in the temperature range of these experiments. In this work, a detailed mechanism investigation of the CH3CFClO2• + ClO• reaction was performed by means of quantum chemical calculations. The rate constants of the dominant reaction pathways of the CH3CFClO2• + ClO• reaction were calculated by RRKM theory6, which has been employed to deal with the complex reactions successfully7,8,9,10,11,12.

Computational methods

All calculations in the present study were preformed using the GAUSSIAN09 program13. The geometries of some important intermediates and transition states (IM1, IM2, IM3, TS1, TS2, TS3, TS7 and TS10) were optimized with density functional theory (B3LYP14,15 and M06-2X16,17 functionals) with the same triple-§ 6–311++G(d,p) basis set. The other geometries on potential energy surfaces were calculated using the B3LYP/6–311++G(d,p) method. All stationary points were characterized by harmonic vibrational frequency analysis (the number of imaginary frequencies, NIMAG, 0 for minima and 1 for transition states). In addition, we calculated the intrinsic reaction coordinates (IRC)18,19 to verify the connectivity between transition state and the corresponding reactants or products. Based on the B3LYP optimized geometry structures, the time-dependent functional theory (TDDFT) theory with the DFT/B3LYP methods with 6–311++G(d,p) as basis set was used to obtain the vertical excitation energy (TV) of all the intermediates in the CH3CFClO2• + ClO• reaction. In order to obtain more reliable relative energy, single points energy calculations have been performed by the method of CCSD(T)20/cc-pVTZ using the functional B3LYP-D3(BJ).

Results and discussion

The optimized geometries of the intermediates and transition stats involved on the triplet and singlet PESs in the title reaction at the B3LYP/6–311++G(d,p) level are depicted in Fig. 1. The optimized geometries for the reactants and products are shown in Fig. 2, along with the available experimental values21. All possible pathways involved in the CH3CFClO2• + ClO• reaction are presented in Fig. 3. Table 1 summarizes ZPE corrections, relative energies, reaction enthalpies and Gibbs free energy. The harmonic vibrational frequencies, moment of inertia and the Z-matrix Cartesian coordinate of all species found on the PESs as supplementary materials are shown in Tables S1, S2, respectively. The frequencies of CH3CFO, CH3CClO, OClO, HOCl, ClO•, HO2, O3 and O2(3Σ) are in agreement with experimental data21. The energies obtained at CCSD(T)/cc-pVTZ//B3LYP/6–311++G(d,p) level are employed to the following discussion.

Figure 1

CH3CFClO2• with ClO• reaction: optimized B3LYP geometries of the intermediates and transition stats at B3LYP/6–311 +  + G(d,p) level. The values in bold are obtained at M06-2X/6–311 +  + G(d,p) level. Bond distances are given in Å.

Figure 2

CH3CFClO2• with ClO• reaction: optimized B3LYP geometries of the reactants and products. Angles are given in º, and bond distances are given in Å. The values in italics are experimental data from ref 21.

Figure 3

Potential energy surface obtained at CCSD(T)//B3LYP level for the CH3CFClO2• + ClO• reaction.

Table 1 Zero Point Energies (ZPE) and relative Energies (ΔE), relative enthalpies (ΔH) and Gibbs free energy (ΔG) for the species involved in the CH3FClO2• with ClO• reaction (energies in kcal/mol).

The formation of adducts on the singlet PES

The ClO• + CH3CFClO2• reaction initiated by the oxygen or chlorine atom of ClO• radical addition to the terminal-O atom of CH3CFClO2• without a barrier and produced the original adduct IM1 (CH3CFClOOOCl) or IM2 (CH3CFClOOClO) with exothermicity of 18.44 kcal/mol or 1.76 kcal/mol. The formed O–O and OCl bonds are 1.302 and 1.888 Å in IM1 and IM2, respectively. IM1 could isomerize to IM2 via a ClOO triangular structure TS1, in which the O–Cl bond that will be formed is 2.246 Å, while the distance of breaking O–O bond is 2.278 Å. TS1 lies 26.28 and 7.84 kcal/mol above IM1 and reactants, respectively. In addition, IM2 can isomerize to IM3 (CH3CFClOClO2) via the transition state TS2 with a barrier of 16.86 kcal/mol, in whch the –ClO group insert into the O–O bond between the terminal and the middle O atoms, and the O–O bond breakage simultaneously. The breaking O–O bond in the triangular structure TS2 is stretched to 2.216 Å and the forming O–Cl bond is 2.490 Å. The imaginary frequency of TS2 is 157i cm-1, involving the O–O and O–Cl bonds stretch vibrations simultaneously. In a word, three adducts IM1 (CH3CFClOOOCl), IM2 (CH3CFClOOClO) and IM3 (CH3CFClOClO2) are generated on the singlet PES with the energy of − 18.01, − 1.53 and − 11.42 kcal/mol, which could further dissociate to various products, and will be discussed as bellow.

The decomposition pathways from IM1 (CH3CFClOOOCl), IM2 (CH3CFClOOClO) and IM3 (CH3CFClOClO2)

Starting from IM1, the O–O bond decomposes and the Cl or F atom in –CFCl– group moves to the middle-O atom in the –OOO– skeleton synchronously resulting in P1 (CH3CFO + ClOOCl) or P2 (CH3CClO + FOOCl) via a ClCOO or FCOO four-numbered-ring transition state TS3 or TS4. The broken O–O and C–Cl bonds are about 1.970 and 2.302 Å in TS3, and the broken O–O and C-F bonds are 2.211 and 1.806 Å in TS4. The produced Cl–O bond in TS3 and F–O bond in TS4 are 2.614 and 2.094 Å, respectively. The barriers for these two decomposition channels are 26.97 and 54.38 kcal/mol, respectively. The IM1 → TS3 → P1 pathway is exothermic by 33.15 kcal/mol, and the IM1 → TS4 → P2 pathway is endothermic by 2.68 kcal/mol. The overall ΔG for these two decomposition channels are − 34.94 and 0.86 kcal/mol, indicating that the pathway via TS3 is practicable thermodynamically.

1,5-H migration from the –CH3 group to the middle-O atom in the –OOCl skeleton, associated with the O–O and O–Cl bonds fracturing through TS5 gives rise to P3 (cyc-CFClCH2O + HO2 + Cl). In TS5, the C–H bond (1.272 Å), O–O bond (2.657 Å) and the C–Cl bond (2.105 Å) are elongated by 0.183, 1.127 and 0.253 Å compared with those of in IM1 (1.089, 1.530 and 1.852 Å, respectively), and the formed O–H bond is 1.361 Å. Although the overall exothermicities of forming P3 (cyc-CFClCH2O + HO2 + •Cl) pathway is estimated to be 2.41 kcal/mol, the barrier for IM1 → TS5 → P3 is 48.40 kcal/mol. To any extent, the high barrier restrains the dissociation pathways from proceeding.

Besides the above three decomposition pathways from IM1 (CH3CFClOOOCl), the reaction resulting in P4 (CH3CFCl2 + O3) takes place by synchronously the migration of the terminal Cl atom to the carbon atom of –CFCl– group and breaking of the C–O bond through a COOOCl five-center structure TS6. The activation barrier of the IM1 → TS6 → P4 process is 75.81 kcal/mol. Apparently, this decomposition channel is not important to the overall reaction.

IM2 (CH3CFClOOClO) could take place decomposition into the end product P5 (CH3CFO + Cl2O2) or P6 (CH3CClO + FClO2) through five-center structure TS7 or TS8, respectively. These two decomposition channels involve the Cl atom or F atom of the –CFCl– group migrating to the chlorine atom of the –OOClO skeleton, accompanied by the O–O bond splitting, respectively. In TS7, the C–Cl bond (2.075 Å) and the O–O bond (2.024 Å) are elongated by 0.269 and 0.622 Å compared with the corresponding bond in IM2 (1.806 and 1.402 Å, respectively), and the formed Cl-Cl bond is 3.092 Å. In TS8, the C-F bond (1.764 Å) and the O–O bond (2.234 Å) are elongated by 0.402 and 0.832 Å, and the formed F-Cl bond is 2.375 Å. Vibrational frequency analysis of TS7 or TS8 reveal one imaginary frequency of 242i and 469i cm−1. The activation barriers for IM2 → TS7 → P5 and IM2 → TS8 → P6 are 13.17 and 30.71 kcal/mol, and the relative energy of P5 and P6 are − 20.36 and − 5.98 kcal/mol. Therefore, the pathway of leading to P5 (CH3CFO + Cl2O2) has priority over the formation of P6 (CH3CClO + FClO2) pathway.

Additionally, IM2 (CH3CFClOOClO) could decompose to P7 (CH3CFClOCl + O2 (1Δg)) via COOClO five-center structure TS9 with the barrier of 47.29 kcal/mol. In TS9, the terminal-O atom shifts to the carbon atom of the –CFCl- group, associated with the breakage of C–O and Cl–O bonds. Though the ΔH and ΔG for this channel are − 20.07 and − 18.49 kcal/mol, this dissociation pathway is unfavorable due to the high barrier height.

IM3 (CH3CFClOClO2) could involve 1,4-Cl shift and O-Cl bond breaking producing P8 (CH3CFO + ClOClO) via TS10, or may take 1,4-F-shift and O-Cl bond breaking resulting in P9 (CH3CClO + FOClO) via TS11. The decomposition barriers for IM3 → TS10 → P8 and IM3 → TS11 → P9 are 19.05 and 46.67 kcal/mol, respectively. The loose ClCOClO and FCOClO five-membered ring in TS10 and TS11 are nonplanar. The migrating chlorine is away from the origin-C atom of 2.167 Å, and 2.674 Å away from the shifting terminus oxygen atom, and the O–Cl bond that will be disruption is as long as 2.266 Å. The vibrational mode of frequency of TS11 corresponds to O–Cl, C–F and O–F bonds stretch vibration, that is, r(O–Cl) = 2.451 Å, r(C–F) = 1.922 Å, and r(O–F) = 2.135 Å. The enthalpy of P8 and P9 are − 17.20 and 23.98 kcal/mol and the Gibbs free energy of P8 and P9 are − 19.17 and 22.15 kcal/mol, imply that IM3 → TS10 → P8 is exothermic and spontaneous, and IM3 → TS11 → P9 is endothermic and nonspontaneous.

Direct H-abstraction pathways on the singlet PES

One direct H-abstraction pathway is found for the CH3CFClO2• + ClO• reaction. One of the H atoms in CH3CFClO2• is abstracted by the O atom in ClO• via TS12 to form P10 (CH2CFClO2 + HOCl). The distance of the breaking C–H bond is 1,254 Å, and forming O–H bond is 1.312 Å. We can define a parameter which represents the reactant- or product-like character of the forming transition state. The L parameter could be computed with the expression22,23,24,25: \(L(C - {\text{H}}) = \frac{{\delta r\left( {{\text{C}} - {\text{H}}} \right)}}{{\delta r\left( {{\text{O}} - {\text{H}}} \right)}}\), where \(\delta r\left( {{\text{C}} - {\text{H}}} \right)\) and \(\delta r\left( {{\text{O}} - {\text{H}}} \right)\) are the corresponding bond distance variations between the TS12 structure and the reactant CH3CFClO2• for the C–H bond and between the TS12 structure and the product HOCl for the O–H bond. The L parameter denotes if a transition state structure is reactant-like (L < 1) or product-like (L > 1) and also quantifies the corresponding trend. The value of L parameter for TS12 is 0.47, indicating that TS12 is a reactant-like transition state. The barrier for CH3CFClO2• + ClO• → TS12 → P10 (CH2CFClO2 + HOCl) pathway is 12.05 kcal/mol, which may be important for the reaction.

The SN2 displacement pathways on the singlet PES

Beside the above addition/elimination and direct H-abstraction pathways, SN2 displacement reaction could occur through TS13 or TS14 with the O atom or the Cl atom of ClO• attacking the carbon atom of the –CFCl– group in CH3CFClO2•, accompanied by the O2 (1Δg) leaving away. In TS13 and TS14, the distance of the forming C–O and C–Cl bonds are 2.330 and 3.012 Å, and the breaking C–O bonds are stretched to 2.014 and 2.384 Å, respectively. The barriers for these two SN2 displacement reactions are rather high, 62.97 and 59.24 kcal/mol, making they are unimportant and could be excluded.

The pathways on the triplet PES

Many attempts failed to locate the intermediate on the triplet PES. Based on our results, three SN2 displacement and one direct H-abstraction channels were found. Figure 1 displays that surmounting T-TS1, T-TS2, T-TS3 and T-TS4, P12 (CH3CFClOCl + O2 (3∑)), P13 (CH3CFClO + OClO), P14 (CH3CFClOOCl + O(3P)) and P10 (CH2CFClO2 + HOCl) are produced, and the corresponding relative energy of the products is − 50.32, 9.14, 23.68 and 8.53 kcal/mol, respectively. The relative energy of T-TS1, T-TS2, T-TS3 and T-TS4, are 30.18, 41.25, 48.80 and 48.72 kcal/mol. It is suggested that the direct H-abstraction and all SN2 displacement channels on the triplet PES contribute less to the title reaction judging from the high barriers.


As discussed above, for the reaction pathways producing P1, P5 and P8 (Scheme 1), the reaction energy barriers are lower and the reactions are exothermic, so these reaction pathways are involved in the kinetics calculations. However, the reaction pathways producing P2, P3, P4, P5, P7, P9, P10, P11, P12, P13 and P14 with higher energy barrier are less competitive in energy, and their contribution to the total reaction is negligible.

Scheme 1

The primary reaction pathways for the CH3CFClO2• with ClO• reaction.

Temperature- or pressure-dependent rate constants for the important pathways (Scheme 1) of the CH3CFClO2• + ClO• reaction were computed at 200–3,000 K, 10–10–1010 atm utilizing RRKM theory. The kinetics calculations based on the optimized geometries, moment of inertia and frequencies obtained at B3LYP/6–311 +  + G(d,p) level, and the energies obtained at the CCSD(T)/cc-pVTZ level.

Steady-state assumption for all the excited (IMj) generates to the following expressions: for the second-order rate constants of diverse product pathways:

$$ k_{{\rm{IM1}}} (T,P) = \frac{{\alpha_{a} }}{h}\frac{{Q_{t}^{ \ne } Q_{r}^{ \ne } }}{{Q_{{\rm{CH}_{3} \rm{CFClO}_{\rm{2}} \bullet }} Q_{{\rm{ClO} \bullet_{{}} }} }}e^{{ - E_{a} /RT}} \times \int_{0}^{\infty } {\frac{\omega }{{X_{5} }}} N_{a} (E^{ \ne } )e^{{ - E^{ \ne } /RT}} dE^{ \ne } $$
$$ k_{{\rm{IM2}}} (T,P) = \frac{{\alpha_{a} }}{h}\frac{{Q_{t}^{ \ne } Q_{r}^{ \ne } }}{{Q_{{\rm{CH}_{3} \rm{CFClO}_{\rm{2}} \bullet }} Q_{{\rm{ClO} \bullet_{{}} }} }}e^{{ - E_{a} /RT}} \times \int_{0}^{\infty } {\frac{{\omega X_{3} }}{{X_{5} }}} N_{a} (E^{ \ne } )e^{{ - E^{ \ne } /RT}} dE^{ \ne } $$
$$ k_{{\rm{IM3}}} (T,P) = \frac{{\alpha_{a} }}{h}\frac{{Q_{t}^{ \ne } Q_{r}^{ \ne } }}{{Q_{{\rm{CH}_{3} \rm{CFClO}_{\rm{2}} \bullet }} Q_{{\rm{ClO} \bullet_{{}} }} }}e^{{ - E_{a} /RT}} \times \int_{0}^{\infty } {\frac{{\omega X_{{1}} X_{3} }}{{X_{5} }}} N_{a} (E^{ \ne } )e^{{ - E^{ \ne } /RT}} dE^{ \ne } $$
$$ k_{{\rm{P1}}} (T,P) = \frac{{\alpha_{a} }}{h}\frac{{Q_{t}^{ \ne } Q_{r}^{ \ne } }}{{Q_{{\rm{CH}_{3} \rm{CFClO}_{\rm{2}} \bullet }} Q_{{\rm{ClO} \bullet_{{}} }} }}e^{{ - E_{a} /RT}} \times \int_{0}^{\infty } {\frac{{k_{2} (E)}}{{X_{5} }}} N_{a} (E^{ \ne } )e^{{ - E^{ \ne } /RT}} dE^{ \ne } $$
$$ k_{{\rm{P2}}} (T,P) = \frac{{\alpha_{a} }}{h}\frac{{Q_{t}^{ \ne } Q_{r}^{ \ne } }}{{Q_{{\rm{CH}_{3} \rm{CFClO}_{\rm{2}} \bullet }} Q_{{\rm{ClO} \bullet_{{}} }} }}e^{{ - E_{a} /RT}} \times \int_{0}^{\infty } {\frac{{k_{7} (E)X_{{3}} }}{{X_{5} }}} N_{a} (E^{ \ne } )e^{{ - E^{ \ne } /RT}} dE^{ \ne } $$
$$ k_{{\rm{P8}}} (T,P) = \frac{{\alpha_{a} }}{h}\frac{{Q_{t}^{ \ne } Q_{r}^{ \ne } }}{{Q_{{\rm{CH}_{3} \rm{CFClO}_{\rm{2}} \bullet }} Q_{{\rm{ClO} \bullet_{{}} }} }}e^{{ - E_{a} /RT}} \times \int_{0}^{\infty } {\frac{{k_{8} (E)X_{1} X_{3} }}{{X_{5} }}} N_{a} (E^{ \ne } )e^{{ - E^{ \ne } /RT}} dE^{ \ne } $$

With the following definition:

$$ \begin{gathered} {\text{X}}_{{1}} = k_{{5}} \left( E \right)/(k_{{6}} \left( E \right) + k_{{8}} \left( E \right) + \omega ) \hfill \\ {\text{X}}_{{2}} = k_{{4}} \left( E \right) + k_{{5}} \left( E \right) + k_{{7}} \left( E \right) + \omega \hfill \\ {\text{X}}_{{3}} = k_{{3}} \left( E \right)/({\text{X}}_{{2}} - k_{{5}} \left( E \right)*{\text{X}}_{{1}} ) \hfill \\ {\text{X}}_{{4}} = k_{{1}} \left( E \right) + k_{{2}} \left( E \right) + k_{{3}} \left( E \right) + \omega \hfill \\ {\text{X}}_{{5}} = {\text{X}}_{{4}} - k_{{4}} \left( E \right)*{\text{X}}_{{3}} \hfill \\ \end{gathered} $$

The microcanonical rate constant is calculated using the RRKM theory as follows:

$$ k_{i} (E) = \alpha_{i} C_{i} N_{i} (E_{i}^{ \ne } )/h\rho_{j} (E_{j} ) $$

In the above equations, \(\alpha_{\alpha }\) is the statistical factor for the reaction path a, and αi is the statistical factor (degeneracy) for the ith reaction path; Ea is the energy barrier for the reaction step a. \(Q_{{\rm{ClO} \bullet }}\) and \(Q_{{\rm{CH}_{3} \rm{CFClO}_{\rm{2}} \bullet }}\) are the total partition function of ClO• and CH3CFClO2•, respectively; \(Q_{t}^{ \ne }\) and \(Q_{r}^{ \ne }\) are the translational and rotational partition functions of entrance transition state, respectively; \(N_{a} \left( {E^{ \ne } } \right)\) is the number of state for the association transition state with excess energy \(E^{ \ne }\) above the association barrier. \(k_{i} \left( E \right)\) is the energy-specific rate constant for the ith channel and Ci is the ratio of the overall rotational partition function of the TSi and IMj; \(N_{i} \left( {E_{i}^{ \ne } } \right)\) is the number of states at the energy above the barrier height for transition state i; \(\rho_{j} \left( {E_{j} } \right)\) is the density of states at energy Ej of the intermediate. The density of states and the number of states are calculated using the extended Beyer–Swinehart algorithm.

The rate constants of IM1 (CH3CFClOOOCl), IM2 (CH3CFClOOClO) and IM3 (CH3CFClOClO2) collisional stabilization channels, and those for the P1 (CH3CFO + ClOOCl), P5 (CH3CFO + Cl2O2) and P8 (CH3CFO + ClOClO) channels (denoted as kIM1, kIM2, kIM3, kP1, kP5 and kP8) and the total rate coefficient (ktot = kIM1 + kIM2 + kIM3 + kP1 + kP5 + kP8) at 200–3,000 K, 12 torr N2 are presented in Fig. 4. ktot appears to reduce firstly and then increase with the temperature increasing. Meanwhile, ktot was in accord with the experimental data (e.g. ktot = 4.50 × 10–12 cm3 molecule−1 s−1 vs. ktot(exp) = 3.84 × 10–12 cm3 molecule-1 s-1 at 253 K). The branching ratios are listed Fig. 5. The generation of IM1 (CH3CFClOOOCl) is dominated at 200–800 K, and with the production of the P1 (CH3CFO + ClOOCl) becoming predominant quickly with the rise of temperature. The P5 (CH3CFO + Cl2O2) or P8 (CH3CFO + ClOClO) product pathway generating from the IM2 (CH3CFClOOClO) or IM3 (CH3CFClOClO2) and the collisional stabilization of the IM2 (CH3CFClOOClO) and IM3 (CFCl2CH2OClO2) almost don’t occur.

Figure 4

taken from Ref 5.

Temperature dependence of the total and individual rate coefficients for the CH3CFClO2• + ClO• reaction at 200–3,000 K at 12 Torr of N2. The experimental data are

Figure 5

Branching ratios of the primary routes for the CH3CFClO2• + ClO• reaction at 12 Torr of N2.

The rate constants for formation of individual products and total rate constants of the CH3CFClO2• + ClO• reaction at 200–3,000 K and 10–10–1010 atm are shown in Fig. 6. As seen from the figure, kP1, kP5, kP8, kIM1, kIM2 and kIM3 for the formation of IM1 (10–10–1010 atm), IM2 (10–10–102 atm) and IM3 (10–10–102 atm) by collisional deactivation is strongly pressure dependent with a pattern opposite to that of the decomposition processes and IM2 (104–1010 atm) and IM3 (104–1010 atm) by collisional deactivation because of the competitive effect of the stabilization vs decomposition as alluded to above. kIM1, kIM2 and kIM3 become smaller and less competitive at lower pressure; at pressure over 1 atm, kIM1 is approaching the high pressure limit at T ≤ 1,000 K. In addition, kIM1 displays negative dependence on temperature at 200–3,000 K owing to the reduction of collision inactivation rate, except at high-pressure limit pressure. The rate constants kP1, kP5 and kP8 for the dissociation reactions display positive dependence on temperature and negative pressure dependent. At low temperatures and high pressures, kP1 become insignificantly small. ktot reflects positive pressure dependent. The high-pressure limit rate constants monotone increase firstly and then reduce monotonously with the temperatures increase, with a model contrary to the collisionless limit pressure, which may due to competition between addition and decomposition reaction.

Figure 6

Forecasted rate coefficients for the total reaction and each individual product pathway of the CH3CFClO2• + ClO• reaction at 200–3,000 K and 10–10-1010 atm.

The branching ratios of the individual product pathways of the CH3CFClO2• + ClO• reaction at low-pressure limit (10–10 atm), atmospheric pressure (1 atm) and high-pressure limit pressure (1010 atm) are presented in Fig. 7. Six product channels dominant noticeably—the competitive deactivation and decomposition producing IM1, IM2, IM3, P1, P5 and P8, respectively. At high-pressure limit pressure, the formation of the stabilization product, IM1 (CH3CFClOOOCl) dominants the reaction at 200–3,000 K. At low-pressure limit and atmospheric pressure, the production of P1 (CH3CFO + ClOOCl) dominates the reaction at T ≥ 300 K and T ≥ 1,000 K, respectively; conversely at low temperatures, the collision inactivation of IM1 (CH3CFClOOOCl) dominants the reaction.

Figure 7

Forecasted branching ratios for the CH3CFClO2• with ClO• reaction at low-pressure limit pressure, atmospheric pressure and high-pressure limit pressure.

The three-parameter Arrhenius equations for the rate constants of generation of IM1 (CH3CFClOOOCl) (kIM1) and P1 (CH3CFO + ClOOCl) (kP1) at low-pressure limit, 1 atm and high-pressure limit N2 can be represented by:

$$ k_{{\rm{IM1}}}^{0} \left( {\rm{CH}_{\rm{3}} \rm{CFClOOOCl}} \right)/\left( {\rm{cm}^{\rm{3}} \rm{molecule}^{{\rm{ - 1}}} \rm{s}^{{\rm{ - 1}}} } \right) = {\text{ 6}}.{\text{12}} \times {\text{1}}0^{{ - {\text{2}}0}} T^{{ - 0.{\text{95}}}} {\text{exp}}\left( {{\text{1653}}.{\text{76}}/T} \right)~({\text{2}}00 \le T \le {\text{3}}000{\text{ K}}) $$
$$ k_{{\rm{P1}}}^{0} \left( {\rm{CH}_{\rm{3}} \rm{CFO + ClOOCl}} \right)/\left( {\rm{cm}^{\rm{3}} \rm{molecule}^{{\rm{ - 1}}} \rm{s}^{{\rm{ - 1}}} } \right) = {\text{ 9}}.{\text{2}}0 \times {\text{1}}0^{{ - {\text{23}}}} T^{{0.{\text{3}}0}} {\text{exp}}\left( { - {\text{6665}}.{\text{7}}/T} \right)~~~~~~({\text{2}}00 \le T \le {\text{3}}000{\text{ K}}) $$
$$ k_{{\rm{IM1}}}^{{}} \left( {\rm{CH}_{\rm{3}} \rm{CFClOOOCl}} \right)/\left( {\rm{cm}^{\rm{3}} \rm{molecule}^{{\rm{ - 1}}} \rm{s}^{{\rm{ - 1}}} } \right) = {\text{ 1}}.{\text{92}} \times {\text{1}}0^{{ - {\text{9}}}} T^{{ - {\text{1}}.{\text{22}}}} {\text{exp}}\left( {{\text{436}}.{\text{86}}/T} \right)~~~~~~~({\text{2}}00 \le T \le {\text{3}}000{\text{ K}}) $$
$$ k_{{\rm{P1}}}^{{}} \left( {\rm{CH}_{\rm{3}} \rm{CFO + ClOOCl}} \right)/\left( {\rm{cm}^{\rm{3}} \rm{molecule}^{{\rm{ - 1}}} \rm{s}^{{\rm{ - 1}}} } \right) = {\text{ 4}}.{\text{19}} \times {\text{1}}0^{{ - {\text{13}}}} T^{{0.{\text{39}}}} {\text{exp}}\left( { - {\text{6454}}.{\text{79}}/T} \right)~~~~~({\text{2}}00 \le T \le {\text{3}}000{\text{ K}}) $$
$$ \begin{gathered} k_{{\rm{IM1}}}^{\infty } \left( {\rm{CH}_{\rm{3}} \rm{CFClOOOCl}} \right)/\left( {\rm{cm}^{\rm{3}} \rm{molecule}^{{\rm{ - 1}}} \rm{s}^{{\rm{ - 1}}} } \right) = {\text{ 2}}.{\text{86}} \times {\text{1}}0^{{ - {\text{16}}}} T^{{{\text{1}}.{\text{84}}}} {\text{exp}}\left( { - {\text{425}}.{\text{41}}/T} \right)~~~~~~({\text{2}}00 \le T \le {\text{18}}00{\text{ K}}) \hfill \\ = {\text{ 3}}.{\text{38}} \times {\text{1}}0^{{ - {\text{6}}}} T^{{ - {\text{1}}.{\text{21}}}} {\text{exp}}\left( { - {\text{811}}.{\text{52}}/T} \right)~~~~~({\text{18}}00 < T \le {\text{3}}000{\text{ K}}) \hfill \\ \end{gathered} $$

$$ k_{{\rm{P1}}}^{\infty } \left( {\rm{CH}_{\rm{3}} \rm{CFO + ClOOCl}} \right)/\left( {\rm{cm}^{\rm{3}} \rm{molecule}^{{\rm{ - 1}}} \rm{s}^{{\rm{ - 1}}} } \right) = {\text{ 3}}.{\text{15}} \times {\text{1}}0^{{ - {\text{13}}}} T^{{ - 0.{\text{42}}}} {\text{exp}}\left( { - {\text{9664}}.{\text{7}}/T} \right)~~~~~({\text{2}}00 \le T \le {\text{3}}000{\text{ K}}) $$


Atmospheric lifetimes of CH3CFClO2

The atmospheric lifetime of CH3CFClO2• can be deduced by means of the following formula:\(\tau = \frac{{1}}{{k\left[ {\rm{ClO}} \right]}}\). The calculated average daytime atmospheric concentrations of chlorine monoxide radical (ClO•) are 1 × 107 molecules per cm3 26, and kClO = 8.49 × 10–12 molecules per cm3 at 298 K 760 Torr was considered. The atmospheric lifetime of CH3CFClO2• is approximately 3.27 h, which suggests that ClO-initiated reaction of CH3CFClO2• plays an important role in some special areas and the marine boundary layer.

Vertical excitation energy of IM1 (CH3CFClOOOCl), IM2 (CH3CFClOOClO) and IM3 (CH3CFClOClO2)

The photo-oxidation of compounds containing chlorine is significant for Cl atmospheric chemistry. As source of Cl, the photolysis might influence the stratosphere and troposphere. In order to get new insights of photolytic stability of the chlorinated compounds, the vertical excitation energy (TV) of the first five excited states for IM1 (CH3CFClOOOCl), IM2 (CH3CFClOOClO) and IM3 (CH3CFClOClO2) were calculated by employing TDDFT method based on the B3LYP/6–311 +  + G(d,p) optimized geometries, and the calculation results including wavelength (λ), excitation energy (TV) and oscillator strength (f) are listed in Table 2. Compounds will be considered to photolyze if TV value is smaller than 4.13 eV or wavelength is longer than 300 nm. From Table 2 it is seen that the TV (wavelength) value of the first two excited states of IM1 (CH3CFClOOOCl) are 2.95 eV (420.0 nm), 3.96 eV (313.4 nm) and the oscillator strength are 0.0001, 0.0001, and the second excited states of IM2 (CH3CFClOOClO) is 3.65 eV (339.70 nm) and the oscillator strength is 0.0007, indicating the possibility of photolysis of IM1 (CH3CFClOOOCl) and IM2 (CH3CFClOOClO) under the sunlight. As for IM3 (CH3CFClOClO2), TV value and oscillator strength the first three excited states take values of 3.28 eV (378.2 nm), 3.78 eV (327.7 nm) 4.10 eV (302.6 nm) and 0.0029, 0.0742, 0.0007, respectively, implying the photolysis is feasible under the sunlight, which might be one source of Cl-containing species in the atmosphere.

Table 2 The excitation energy TV (in eV), oscillator strength f (in atomic units) and wavelength λ (in nm) of the first five excited states of IM1 (CH3CFClOOOCl), IM2 (CH3CFClOOClO) and IM3 (CH3CFClOClO2) at the TD-B3LYP level of theory.


The reaction mechanisms, kinetics, and products distribution for the CH3CFClO2• + ClO• reaction in atmosphere were investigated by using the CCSD(T)//B3LYP method. Addition–elimination, direct H-abstraction and SN2 displacement mechanisms are located on the singlet PES, and direct H-abstraction and SN2 displacement mechanisms are located on the triplet PES. The result suggests that major product is P1 (CH3CFO + ClOOCl) on the singlet PES produced by the addition–elimination reaction, which proceeds the addition of the O in ClO to the terminal-O atom in CH3CFClO2• and then the ClOOCl-elimination forming the products. Owing to the higher barrier heights, other products contribute less to the title reaction. The rate constants and branch ratio of products are estimated by means of RRKM theory at extensive temperature and pressure range. The rate constants at 200–3,000 K show stronger temperature dependence. The stabilization of the adduct IM1 (CH3CFClOOOCl) is dominant at 200–800 K, while the generation of P1 (CH3CFO + ClOOCl) is the primary channel at high temperature. The lifetime of CH3CFClO2• in the presence of ClO• was predicted to 3.27 h. IM1 (CH3CFClOOOCl), IM2 (CH3CFClOOClO) and IM3 (CH3CFClOClO2) will photolyze under the sunlight.


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This work was supported by the Natural Science Foundations of China (No. 21707062).

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The conception and design of computations: Y.Z. The execution and analysis of calculations: Y.Z. and B.H. Paper writing: Y.Z. B.H. and Y.S. All authors have reviewed the manuscript.

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Correspondence to Yunju Zhang.

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Zhang, Y., He, B. & Sun, Y. Theoretical investigations on mechanisms and kinetics of the CH3CFClO2· with ClO· reaction in the atmosphere. Sci Rep 10, 11078 (2020).

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