Quick viewing(Text Mode)

Atmospheric Chemistry of CF3CF@CH2: Kinetics and Mechanisms of Gas-Phase Reactions with Cl Atoms, OH Radicals, and O3

Atmospheric Chemistry of CF3CF@CH2: Kinetics and Mechanisms of Gas-Phase Reactions with Cl Atoms, OH Radicals, and O3

Chemical Letters 439 (2007) 18–22 www.elsevier.com/locate/cplett

Atmospheric of CF3CF@CH2: Kinetics and mechanisms of gas-phase reactions with Cl , OH radicals, and O3

O.J. Nielsen a,*, M.S. Javadi a, M.P. Sulbaek Andersen a, M.D. Hurley b, T.J. Wallington b,*, R. Singh c

a Department of Chemistry, University of Copenhagen, Universitetsparken 5, DK-2100 Copenhagen, Denmark b Physical and Environmental Sciences Department, Ford Motor Company, Mail Drop SRL-3083, Dearborn, MI 48121, USA c Honeywell International Inc., 101 Columbia Road, Morristown, NJ 07962, USA

Received 31 January 2007; in final form 6 March 2007 Available online 21 March 2007

Abstract

11 Long path length FTIR- chamber techniques were used to determine k(Cl + CF3CF@CH2) = (7.03 ± 0.59) · 10 , 12 21 3 1 1 k(OH + CF3CF@CH2) = (1.05 ± 0.17) · 10 , and k(O3 +CF3CF@CH2) = (2.77 ± 0.21) · 10 cm s in 700 Torr of N2,N2/O2, or air diluent at 296 K. CF3CF@CH2 has an atmospheric lifetime of approximately 11 days and a global warming potential (100 yr time horizon) of four. CF3CF@CH2 has a negligible global warming potential and will not make any significant contribution to radiative forcing of change. 2007 Elsevier B.V. All rights reserved.

1. Introduction tion with and (iv) atmospheric implications. Results are reported herein. Recognition of the adverse environmental impact of chlorofluorocarbon (CFC) release into the 2. Experimental [1,2] has led to an international effort to replace these com- pounds with environmentally acceptable alternatives. Experiments were performed in a 140-liter Pyrex reactor Unsaturated fluorinated hydrocarbons are a class of com- interfaced to a Mattson Sirus 100 FTIR spectrometer [3]. pounds which have been developed to replace CFCs and The reactor was surrounded by 22 fluorescent blacklamps saturated hydrofluorocarbons in air conditioning units. (GE F15T8-BL), which were used to photochemically initi- Prior to their large-scale industrial use an assessment of ate the experiments. Chlorine atoms were produced by the atmospheric chemistry, and hence environmental photolysis of molecular chlorine. impact, of these compounds is needed. To address this need Cl2 þ hv ! Cl þ Cl ð1Þ the atmospheric chemistry of CF3CF@CH2 was investi- gated. Smog chamber/FTIR techniques were used to deter- OH radicals were produced by photolysis of CH3ONO in mine the following properties for this compound: (i) the presence of NO in air. kinetics of its reaction with chlorine atoms, (ii) kinetics of its reaction with hydroxyl radicals, (iii) kinetics of its reac- CH3ONO þ hv ! CH3O þ NO ð2Þ CH3O þ O2 ! HO2 þ HCHO ð3Þ

HO2 þ NO ! OH þ NO2 ð4Þ * Corresponding authors. E-mail addresses: [email protected] (O.J. Nielsen), [email protected] In the relative rate experiments the following reactions take (T.J. Wallington). place.

0009-2614/$ - see front matter 2007 Elsevier B.V. All rights reserved. doi:10.1016/j.cplett.2007.03.053 O.J. Nielsen et al. / Letters 439 (2007) 18–22 19

Cl þ Reactant ! products ð5Þ 3.5 Cl þ Reference ! products ð6Þ 3.0 OH þ Reactant ! products ð7Þ ) C H t

] 2 2 OH þ Reference ! products ð8Þ 2 2.5 It can be shown that CF=CH

  3 ½Reactant k ½Reference Ln t0 Reactant Ln t0 9 2.0

¼ ð Þ /[CF

½Reactant kReference ½Reference t0 t t ] 2 where [Reactant]t0, [Reactant]t, [Reference]t0, and [Refer- 1.5 C H ence]t are the of reactant and reference at 2 4 CF=CH times t0 and t, and kReactant and kReference are the rate 3 1.0 constants for the reactant and the reference. Plots of Ln[Reactant]t0/[Reactant]t) vs. Ln([Reference]t0/[Refer- Ln ([CF 0.5 ence]t) should be linear, pass through the origin, and have a slope of kReactant/kReference. The kinetics of the O3 reac- tion were studied using an absolute rate method in which 0.0 0.00.51.01.52.02.5 the pseudo first-order loss of CF3CF@CH2 was measured Ln ([Reference]t0/[Reference]t) in the presence of excess O3. O was produced from O via silent electrical discharge 3 2 Fig. 1. Decay of CF3CF@CH2 vs. C2H4 and C2H2 in the presence of Cl using a commercial O3 ozonizer. CH3ONO was synthesized atoms in 700 Torr of either air (open symbols) or N2 (filled symbols) at by the drop wise addition of concentrated sulfuric acid to a 296 ± 2 K. saturated solution of NaNO2 in . Other reagents were obtained from commercial sources. Experiments were to the data in Fig. 1 gives k10/k11 = 0.76 ± 0.04 and k10/ conducted in 700 Torr total pressure of N2,orN2/O2 dilu- k12 = 1.38 ± 0.06. 11 ent at 296 ± 1 K. Using k11 = (9.29 ± 0.51) · 10 [4] and k12 = (5.07 ± 11 Concentrations of reactants and products were moni- 0.34) · 10 [4] (700 Torr, 295 K) gives k10 = (7.06 ± tored by FTIR . IR spectra were derived from 0.54) · 1011 and (7.00 ±0.56) · 1011 cm3 molecule1 s1. 32 coadded interferograms with a spectral resolution of We choose to cite a final value which is the average of the 1 0.25 cm and an analytical path length of 27.1 m. To individual determinations together with error limits which check for unwanted loss of reactants and reference com- encompass the extremes of the determinations, hence 11 3 1 1 pounds via heterogeneous reactions, reaction mixtures k10 = (7.03 ± 0.59) · 10 cm molecule s . While there were left to stand in the chamber for 60 min. There was have been no previous studies of k10, we can compare our 10 no observable (<2%) loss of any of the reactants or prod- result with k(Cl + CH3CH@CH2) = 2.4 · 10 [5], k(Cl + 11 ucts in the present work. Unless stated otherwise, quoted CF3CH@CH2) = (9.07 ± 1.08) · 10 [6], k(Cl + 11 uncertainties are two standard deviations from least C4F9CH@CH2) = (8.9 ± 1.0) · 10 [7], k(Cl+C6F13CH@ 11 squares regressions. CH2) = (9.1 ± 1.0) · 10 [7],andk(Cl + CF3CF@ 11 3 1 1 CF2) = (2.7 ± 0.3) · 10 cm molecule s [8]. The 3. Results and discussion reaction of Cl atoms with propene proceeds via electro- philic addition to the >C@C< double bond. The presence @ 3.1. Kinetics of the Cl + CF3CF CH2 reaction of electron withdrawing fluorine substituents is expected to lead to decreased reactivity with Cl atoms. Consistent The rate of reaction (10) was measured relative to reac- with expectations, the reactivity of CF3CF@CH2 reported tions (11) and (12): here lies between those of CF3CH@CH2 and CF3CF@CF2 reported previously. Cl þ CF3CF@CH2 ! products ð10Þ

Cl þ C2H4 ! products ð11Þ 3.2. Kinetics of the OH + CF3CF@CH2 reaction Cl þ C2H2 ! products ð12Þ Reaction mixtures consisted of 19.1–26.2 mTorr of The rate of reaction (13) was measured relative to reac- tions (14) and (15): CF3CF@CH2, 104–133 mTorr Cl2, and either 4.33–

30.2 mTorr C2H4, or 2.35–8.5 mTorr C2H2, in 700 Torr OH þ CF3CF@CH2 ! products ð13Þ of air, or N , diluent. The observed loss of CF CF@CH 2 3 2 OH þ C H ! products ð14Þ vs. those of the reference compounds is plotted in Fig. 1. 2 4 As seen from Fig. 1, there was no discernable difference be- OH þ C2H2 ! products ð15Þ tween the results obtained in N2, or air, diluent. A linear Initial reaction mixtures consisted of 17.6–18.1 mTorr of least squares fit (unweighted, not forced through the origin) CF3CF@CH2, 110–200 mTorr CH3ONO, and 3.38 mTorr 20 O.J. Nielsen et al. / Chemical Physics Letters 439 (2007) 18–22

0.5 reactivity of CF3CF@CF2 appears to be anomalously high. A computational study of the reaction of OH radicals with CF3CF@CF2 would be of interest to shed further light on

) C H t 2 2 ] the mechanism of these reactions. 2 0.4

3.3. Absolute Rate Study of k(O3 +CF3CF@CH2) CF=CH 3 0.3 The kinetics of reaction (16) were studied by observing

/[CF @ t0 the decay of CF CF CH when exposed to ozone in the

] 3 2 2 reaction chamber. Reaction mixtures consisted of 14– 0.2 28 mTorr CF3CF@CH2, 30–46 mTorr cyclohexane, and

CF=CH 180–1890 mTorr O3 in 700 Torr of air diluent. Cyclohexane 3 was added to avoid potential problems associated with the C2H4 0.1 loss of CF3CF@CH2 via reaction with OH radicals formed

Ln ([CF in reaction (16). Variation of the [cyclohexane]/ [CF3CF@CH2] ratio over the range 1–3 had no discernable @ 0.0 effect on the observed decay of CF3CF CH2 suggesting 0.0 0.5 1.0 1.5 2.0 that loss via reaction with OH radicals is not a significant @ Ln ([Reference] /[Reference] ) complication. The loss of CF3CF CH2 followed pseudo t0 t first-order kinetics in all experiments (see insert in Fig. 3).

Fig. 2. Decay of CF3CF@CH2 vs. C2H4 and C2H2 in the presence of OH Fig. 3 shows a plot of the pseudo first-order loss of radicals in 700 Torr of air at 296 ± 2 K. CF3CF@CH2 vs. O3 . The line through the 21 3 1 1 data gives k16 = (2.77 ± 0.21) · 10 cm molecule s .

CF3CF@CH2 þ O3 ! products ð16Þ C2H4 or 3.09 mTorr C2H2 in 700 Torr total pressure of air diluent. Fig. 2 shows the loss of CF3CF@CH2 plotted ver- It is of interest to compare this result with the reported sus loss of the reference compounds. Linear least squares reactivity of ozone towards other fluoroalkenes and alk- analysis gives k13/k14 = 0.125 ± 0.007 and k13/k15 = enes. The reported rate constants for reactions of O3 with 1.21 ± 0.09. propene, 1-butene, 1-pentene , 1-hexene, 1-heptene, 1-oc- 12 Using k14 = (8.52 ± 1.28) · 10 [9] (atmospheric pres- tene, and 1-decene are indistinguishable and are approxi- 13 17 3 1 1 sure, 298 K) and k15 = (8.45 ± 0.85) · 10 [10] gives mately 1.0 · 10 cm molecule s [9]. The rate 12 12 3 @ k13 = (1.07 ± 0.17) · 10 and (1.02 ± 0.13) · 10 cm constants for reactions of O3 with CF3CF CF2 and 1 1 @ 22 molecule s . Indistinguishable values of k13 are CF3CH CH2 are (6.2 ± 1.5) · 10 [14] and obtained using the two different references. We choose to cite a final value which is the average of the individual 30 determinations together with error limits which encompass )

0 0.0 ] the extremes of the determinations, hence k13 = (1.05 ± 2 12 3 1 1 0.17) · 10 cm molecule s . 25 -0.1 CF=CH

It is of interest to compare our result with the reactivity 3 -0.2 of propene and fluorinated propenes reported in the litera- ]/[CF 2 ture. The reaction of OH radicals with propene proceeds ) 20 -1 -0.3

@ s

via electrophilic addition to the >C C< double bond with CF=CH -5 11 3 1 1 3 a rate constant of 2.6 · 10 cm molecule s in one -0.4

(10 15 0 50 100 150 200

atmosphere of air at 298 K [9]. Measurements of Ln([CF

1st Time (min) k k(OH + CF3CH@CH2) by Orkin et al. [11] and Sulbaek Andersen et al. [6] are in good agreement, taking an aver- 10 age from the two studies gives k(OH + CF3CH@CH2)= 1.45 · 1012 cm3 molecule1 s1. McIlroy and Tully [12], Dubey et al. [13], Orkin et al. [11], and Mashino et al. [8] 5 studied the reaction of OH radicals with CF3CF@CF2. The results at ambient from the four studies were in good agreement; the average from the studies is 0 12 3 1 1 0246 k(OH + CF3CH@CH2) = 2.4 · 10 cm molecule s . [O ] (1016 molecule cm-3 ) In contrast to Cl atoms, the reactivity of OH radicals with 3 @ @ @ CH3CH CH2,CF3CH CH2,CF3CF CH2, and Fig. 3. Pseudo first-order loss of CF CF@CH versus O concentration. @ 3 2 3 CF3CF CF2 does not follow the trend expected assuming The insert shows typical decay plots for CF3CF@CH2 when exposed to a simple electrophilic addition mechanism. Specifically, the 180 mTorr (circles), 585 mTorr (triangles), or 1890 mTorr (squares) of O3. O.J. Nielsen et al. / Chemical Physics Letters 439 (2007) 18–22 21

(3.5 ± 0.3) · 1019 cm3 molecule1 s1[6], respectively. The ) reactivity of fluorinated propenes towards ozone follows -1 4 the trend expected (CH3CH@CH2 >CF3CH@CH2 > CF3CF@CH2 >CF3CF@CF2) for reaction proceeding via @ 3 electrophilic addition of ozone to the >C C< double molecule 2 bond. In its reaction with O3,CF3CF@CH2 is less reactive than its non-fluorinated counterpart by a factor of 3600. cm -18 2 When compared to Cl atoms and OH radicals, O3 has the lowest reactivity and hence its rate of reaction with the compounds considered above is most sensitive to the 1 presence of the electron withdrawing fluorine substituents. Finally, it is worth noting that while reactions of O3,Cl, and OH proceed via electrophilic addition to the >C@C<

Cross Section (10 0 double bond there are differences in mechanism with O3 800 1000 1200 1400 1600 1800 2000 adding across the double bond and Cl atoms and OH rad- -1 icals adding to one of the carbon atoms. Wavenumber (cm )

Fig. 4. IR spectrum of CF3CF@CH2. 4. Atmospheric lifetime and global warming potential

CF CF@CH will not undergo photolysis [11] and is not 3 2 global warming potential, HGWP [20], for CF CF@CH expected to be removed effectively by either wet or dry 3 2 (relative to CFC-11) can then be estimated using the deposition. Cl atoms are not present in the atmosphere in expression: sufficient quantity to impact the lifetime of CF3CF@CH2.  @ @ Reaction with OH and O3 are expected to be loss IFCF3CF CH2 sCF3CF CH2 M CFC11 HGWPCF3CF@CH2 ¼ mechanisms for CF CF@CH . The value of k(OH + IF s M @ 3 2 CFC11 CFC11 CF3CF CH2 CF3CF@CH2) measured in the present work can be used 1 expðt=sCF3CF@CH2 Þ to provide an estimate of the atmospheric lifetime of 1 expðt=sCFC11Þ CF3CF@CH2. Using a global weighted-average OH con- 6 3 @ @ centration of 1.0 · 10 cm [15] leads to an esti- where IFCF3CF CH2 ,IFCFC11,MCF3CF CH2 ,MCFC11, s @ s mated lifetime of CF3CF@CH2 with respect to reaction CF3CF CH2 ,and CFC11 are the instantaneous forcings, with OH radicals of 11 days. In a similar fashion our value molecular weights, and atmospheric lifetimes of CF CF@CH and CFC-11, and t is the time horizon over of k(O3 +CF3CF@CH2) can be combined with the global 3 2 which the forcing is integrated. Using s(CF CF@CH )= background O3 concentration of approximately 35 ppb [16] 3 2 to provide an estimated lifetime with respect to reaction 11 days and sCFC11 = 45 years [21] we estimate that the @ 3 with ozone of 13 years. We conclude that the atmospheric HGWP of CF3CF CH2 relative to CFC-11 is 1.9 · 10 4 lifetime of CF3CF@CH2 is determined by its reaction with for a 20 yr horizon and 7.6 · 10 for a 100 yr time hori- OH and is approximately 11 days. The approximate nature zon, respectively. Relative to CO2, the GWP of CFC-11 of this lifetime estimate should be stressed; the average on 20 and 100 yr time horizons are 6300 and 4600 [21]. @ daily concentration of OH radicals varies significantly with Hence, relative to CO2, the GWP of CF3CF CH2 is both location and [17]. The quoted lifetime is a glo- approximately 12 for a 20 yr horizon and 4 for a 100 yr @ bal average, the local lifetimes could be significantly shorter time horizon, respectively. CF3CF CH2 has a negligible or longer. global warming potential and will not make any significant The IR spectrum of CF3CF@CH2 measured in the pres- contribution to radiative forcing of . ent work is shown in Fig. 4.CF3CF@CH2 has an inte- grated IR absorption cross section (800–2000 cm1)of Acknowledgements (1.63 ± 0.09) · 1016 cm molecule1. The quoted uncer- tainty (±5%) is comprised of the following components: O.J.N., M.S.J., and M.P.S.A. acknowledge financial sample concentration (±2%), path length (±1.5%), residual support from the Danish Natural Science Research Coun- baseline offset after subtraction of the background cil for the Copenhagen Center for Atmospheric Research (±0.5%), and spectrometer accuracy (±1%) [18]. There (CCAR). All statements, information, and data given here- are no literature IR data for CF3CF@CH2 to compare with in are presented without guaranty, warranty, or responsi- our result. bility of any kind, expressed or implied, for Honeywell Using the method outlined by Pinnock et al. [18], the IR International Inc. spectrum of CF3CF@CH2 shown in Fig. 4, and the IR spectrum of CFC-11 [19] we calculate instantaneous forc- References ings for CF3CF@CH2 and CFC-11 of 0.22 and 0.26 W m2 ppb1, respectively. Values of the halocarbon [1] M.J. Molina, F.S. Rowland, Nature 249 (1974) 810. 22 O.J. Nielsen et al. / Chemical Physics Letters 439 (2007) 18–22

[2] J.D. Farman, B.G. Gardiner, J.D. Shanklin, Nature 315 (1985) 207. [13] M.K. Dubey, T.F. Hanisco, P.O. Wennberg, J.G. Anderson, [3] T.J. Wallington, S.M. Japar, J. Atmos. Chem. 9 (1989) 399. Geophys. Res. Lett. 23 (1996) 321. [4] T.J. Wallington, J.M. Andino, I.M. Lorkovic, E.W. Kaiser, G. [14] G. Acerboni, J.A. Beukes, N.R. Jensen, J. Hjorth, G. Myhre, C.J. Marston, J. Phys. Chem. 94 (1990) 3644. Nielsen, J.K. Sundet, Atmos. Environ. 35 (2001) 4113. [5] R. Atkinson et al., Atmos. Chem. Phys. Discuss. 5 (2005) 6295. [15] R.G. Prinn et al., Science 292 (2001) 1882. [6] M.P. Sulbaek Andersen et al., J. Photochem. Photobiol. A: Chem. [16] B.J. Finlayson-Pitts, J.N. Pitts Jr., Chemistry of the Upper and Lower 176 (2005) 124. Atmosphere, Academic Press, London, 2000. [7] E. Ve´sine, V. Bossoutrot, A. Mellouki, G. Le Bras, J. Wenger, H. [17] G. Klecka et al., Evaluation of Persistence and Long-Range Trans- Sidebottom, J. Phys. Chem. A. 104 (2000) 8512. port of Organic Chemicals in the Environment, SETAC Press, [8] M. Mashino, Y. Ninomiya, M. Kawasaki, T.J. Wallington, M.D. Pensacola, 2000. Hurley, J. Phys. Chem. A. 104 (2000) 7255. [18] S. Pinnock, M.D. Hurley, K.P. Shine, T.J. Wallington, T.J. Smyth, J. [9] J.G. Calvert, R. Atkinson, J.A. Kerr, S. Madronich, G.K. Moortgat, Geophys. Res. 100 (1995) 23227. T.J. Wallington, G. Yarwood, The Mechanisms of Atmospheric [19] Y. Ninomiya, M. Kawasaki, A. Gushin, L.T. Molina, M. Molina, Oxidation of the , Oxford University Press, Oxford, 2000. T.J. Wallington, Environ. Sci. Technol. 34 (2000) 2973. [10] M. Sørensen, E.W. Kaiser, M.D. Hurley, T.J. Wallington, O.J. [20] D.A. Fisher, C.H. Hales, W. Wang, M.K.W. Ko, N.D. Sze, Nature Nielsen, Int. J. Chem. Kinet. 35 (2003) 191. 344 (1990) 513. [11] V. L Orkin, R.E. Huie, M.J. Kurylo, J. Phys. Chem. A. 101 (1997) [21] J.T. Houghton et al. (Eds.), Climate Change 2001: The Scientific 9118. Basis, Cambridge University Press, 2001. [12] A. McIlroy, F.P. Tully, J. Phys. Chem. 97 (1993) 610.