CHF<sub>3</sub> (HFC-23) and CF<sub>3</sub>CHO QuantumYields in the Pulsed Laser Photolysis of CF<sub>3</sub>CHO at 248,266, 281, and 308 nm

Ultraviolet (UV) photolysis of trifluoroacetaldehyde (CF<sub>3</sub>CHO), an atmospheric degradation product of anthropogenically emitted compounds, is a potential source of fluoroform (CHF<sub>3</sub>, HFC-23), which is a potent greenhouse gas. In this study, CF<sub>3</sub>CHO photolysis quantum yields, ϕ<sub>CF<sub>3</sub>CHO</sub>(λ, <i>P</i>), and CHF<sub>3</sub> product and quantum yields were measured following the pulsed laser photolysis of CF<sub>3</sub>CHO at 248, 266, 281, and 308 nm at total pressures between 100 and 678 Torr (N<sub>2</sub>/NO bath gas mixtures). Loss of CF<sub>3</sub>CHO was measured using Fourier transform infrared spectroscopy (FTIR), and the formation of CHF<sub>3</sub> was measured by FTIR (248, 266, and 281 nm) and off-line gas chromatography–mass spectrometry (GC/MS) (248, 266, and 308 nm). ϕ<sub>CF<sub>3</sub>CHO</sub>(248 nm, 650–678 Torr) and ϕ<sub>CF<sub>3</sub>CHO</sub>(266 nm, 650 Torr) were measured to be 1.03 ± 0.06 and 0.94 ± 0.06, respectively, i.e., near unity, using CBrF<sub>2</sub>CBrF<sub>2</sub> (Halon-2402) and CF<sub>3</sub>I as the actinometry references, respectively. The CHF<sub>3</sub> molar product yields at 248 and 266 nm were measured to be 0.348 ± 0.02 and 0.438 ± 0.015, respectively. CF<sub>3</sub>CHO quantum yields measured for 281 and 308 nm photolysis were found to be pressure-dependent over the 100 to 650 Torr (N<sub>2</sub>/NO) pressure range. A Stern–Volmer analysis of the CF<sub>3</sub>CHO quantum yield results yielded <i>k</i><sub>Q</sub>/<i>k</i><sub>D</sub> values of (3.25 ± 0.20) × 10<sup>–20</sup> cm<sup>3</sup> molecule<sup>–1</sup> at 281 nm and (1.91 ± 0.02) × 10<sup>–19</sup> cm<sup>3</sup> molecule<sup>–1</sup> at 308 nm, i.e., ϕ<sub>CF<sub>3</sub>CHO</sub>(281 nm, 650 Torr) = 0.54 ± 0.06 and (308 nm, 650 Torr) = 0.204 ± 0.028. The CHF<sub>3</sub> molar product yields obtained at 281 and 308 nm showed a weak decrease with increasing pressure with values of 0.105 ± 0.002 and (1.71 ± 0.70) × 10<sup>–3</sup> obtained at 650 Torr, respectively. All quoted measurement uncertainties are 2σ standard deviation. An evaluation of this photochemical source of CHF<sub>3</sub> following the atmospheric degradation of hydrofluorocarbons (HFCs), hydrochlorofluorocarbons (HCFCs), hydrofluoroolefins (HFOs), and hydrochlorofluoroolefins (HCFOs) that are observed in the present-day atmosphere is presented and the atmospheric implications discussed.

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Figshare
Published
2025-02-27
DOI
https://doi.org/10.1021/acsearthspacechem.4c00316.s001
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Atmospheric Ozone and Climate
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article

CHF3 (HFC-23) and CF3CHO QuantumYields in the Pulsed Laser Photolysis of CF3CHO at 248,266, 281, and 308 nm

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Atmospheric Ozone and Climate
article

CHF3 (HFC-23) and CF3CHO QuantumYields in the Pulsed Laser Photolysis of CF3CHO at 248,266, 281, and 308 nm

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Abstract

Ultraviolet (UV) photolysis of trifluoroacetaldehyde (CF<sub>3</sub>CHO), an atmospheric degradation product of anthropogenically emitted compounds, is a potential source of fluoroform (CHF<sub>3</sub>, HFC-23), which is a potent greenhouse gas. In this study, CF<sub>3</sub>CHO photolysis quantum yields, ϕ<sub>CF<sub>3</sub>CHO</sub>(λ, <i>P</i>), and CHF<sub>3</sub> product and quantum yields were measured following the pulsed laser photolysis of CF<sub>3</sub>CHO at 248, 266, 281, and 308 nm at total pressures between 100 and 678 Torr (N<sub>2</sub>/NO bath gas mixtures). Loss of CF<sub>3</sub>CHO was measured using Fourier transform infrared spectroscopy (FTIR), and the formation of CHF<sub>3</sub> was measured by FTIR (248, 266, and 281 nm) and off-line gas chromatography–mass spectrometry (GC/MS) (248, 266, and 308 nm). ϕ<sub>CF<sub>3</sub>CHO</sub>(248 nm, 650–678 Torr) and ϕ<sub>CF<sub>3</sub>CHO</sub>(266 nm, 650 Torr) were measured to be 1.03 ± 0.06 and 0.94 ± 0.06, respectively, i.e., near unity, using CBrF<sub>2</sub>CBrF<sub>2</sub> (Halon-2402) and CF<sub>3</sub>I as the actinometry references, respectively. The CHF<sub>3</sub> molar product yields at 248 and 266 nm were measured to be 0.348 ± 0.02 and 0.438 ± 0.015, respectively. CF<sub>3</sub>CHO quantum yields measured for 281 and 308 nm photolysis were found to be pressure-dependent over the 100 to 650 Torr (N<sub>2</sub>/NO) pressure range. A Stern–Volmer analysis of the CF<sub>3</sub>CHO quantum yield results yielded <i>k</i><sub>Q</sub>/<i>k</i><sub>D</sub> values of (3.25 ± 0.20) × 10<sup>–20</sup> cm<sup>3</sup> molecule<sup>–1</sup> at 281 nm and (1.91 ± 0.02) × 10<sup>–19</sup> cm<sup>3</sup> molecule<sup>–1</sup> at 308 nm, i.e., ϕ<sub>CF<sub>3</sub>CHO</sub>(281 nm, 650 Torr) = 0.54 ± 0.06 and (308 nm, 650 Torr) = 0.204 ± 0.028. The CHF<sub>3</sub> molar product yields obtained at 281 and 308 nm showed a weak decrease with increasing pressure with values of 0.105 ± 0.002 and (1.71 ± 0.70) × 10<sup>–3</sup> obtained at 650 Torr, respectively. All quoted measurement uncertainties are 2σ standard deviation. An evaluation of this photochemical source of CHF<sub>3</sub> following the atmospheric degradation of hydrofluorocarbons (HFCs), hydrochlorofluorocarbons (HCFCs), hydrofluoroolefins (HFOs), and hydrochlorofluoroolefins (HCFOs) that are observed in the present-day atmosphere is presented and the atmospheric implications discussed.

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CHF<sub>3</sub> (HFC-23) and CF<sub>3</sub>CHO QuantumYields in the Pulsed Laser Photolysis of CF<sub>3</sub>CHO at 248,266, 281, and 308 nm · Figshare (2025) | TGRS Research Map | TGRS