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Laboratory Studies of VUV CH 4 Photolysis and Reactions of the Resulting Radicals Robin Shannon, Mark Blitz, Mike Pilling, Dwayne Heard, Paul Seakins University of Leeds, UK
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Background to Leeds Leeds has long background in Laboratory Reaction Kinetics with applications to: – Combustion – Pyrolysis – Atmospheric Chemistry Additionally field work on OH and HO 2 detection (spectroscopic) and hydrocarbons (chromatography) Development of large models (MCM) Theory on pressure dependent reactions New STFC grant on methane photolysis and benzene formation on Titan
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Outline 1.Methane Photolysis – Previous work – Possible approaches 2.Reactions of 1 CH 2 – Rare gas collisions – Reaction vs relaxation 3.Reactions of CH 4.Recent studies with Laval expansion system (Heard)
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1. Methane Photolysis Gans et al. PCCP Front cover
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CH 4 Photolysis – Background Product Channels: CH 3 + H 1 CH 2 + H 2 3 CH 2 + 2H CH + H + H 2 Smith and Nash, Icarus, 2006
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CH 4 Photolysis – Previous Work C Gans et al. PCCP 2011
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CH 4 Photolysis – Previous Work ReferenceGans et al. Park et al. Mordaunt et al. Heck et al. Brownswo rd et al. Wang et al. Lodriguito et al. Method Direct determination of CH 2 and CH 3 Simultaneous photolysis and detection of H atoms by LIF ToF H atom kinetic energy spectroscopy Photofragmen t imaging Photolysis and H atom detection (vuvLIF) at Lyman α Determination of H and molecular products Trajectory calculations Date2011 200819931996199720002009 λ/nm118.2121.6 121.6 nm H atom 105-115 nm H 2 121.6118.2 and 121.6121.6 CH 3 + H 0.26 ±0.040.42 ± 0.050.31 ± 0.050.490.66-0.29 ± 0.070.39 ± 0.03 CH 2 (a 1 A 1 ) + H 2 0.17 ± 0.050.48 ± 0.050.6900.22-0.59 ± 0.100.50 ± 0.06 CH 2 (X 3 B 1 ) + 2H 0.48 ± 0.060.03 ± 0.08-0--0.066 ± 0.0120.10 ± 0.02 CH + H + H 2 0.090.07-0.510.11-0.068 ± 0.0130.02 ± 0.01 Total H1.31 ± 0.130.55 ± 0.170.31 ± 0.051.0 ± 0.5 0.47 ± 0.110.47 ± 0.100.60 ± 0.10 Total H 2 0.26 ± 0.050.55 ± 0.050.690.51 0.65 ± 0.100.51 ± 0.06 Summary of Previous Results
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CH 4 Photolysis – Possible approaches Repeat of Gans et al. approach (synchrotron photolysis source?) Direct detection of CH via laser induced fluorescence Enhanced end product analysis studies – Excimer lamps (e.g. 126 nm) as strong sources (>50 mW cm -2 ) – Chemical conversion ( 3 CH 2 particularly difficult to detect via optical spectroscopy) – Use of PTR-MS for sensitive end-product analysis, H 3 O + + RH → RH + + H 2 O (soft ionization)
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2. 1 CH 2 Reactions – Temperature Dependence
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Importance of 1 CH 2 reactions Wilson and Atreya, JGR 108, E2 5014, 2003
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1 CH 2 + rare gas 1 CH 2 + RG → 3 CH 2 + RG Gannon et al. JCP 132 2010
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Temperature Dependence of 1 CH 2 removal by C 2 H 2 Gannon et al. JPCA 114 2010 Monitor removal of 1 CH 2 by LIF 1 CH 2 + C 2 H 2 → C 3 H 3 + H 1 CH 2 + C 2 H 2 + M → C 3 H 4 + M 1 CH 2 + C 2 H 2 → 3 CH 2 + C 2 H 2 Monitor calibrated production of H by LIF
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Product Temperature Dependence Temperature k k overall k relaxation reaction relaxation
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H Atom Yields 1 CH 2 + ΓHΓH 195 K250 K298 K398 K498 K C2H2C2H2 0.28 ± 0.110.53 ± 0.150.88 ± 0.091.1 ± 0.161.1 ± 0.42 C2H4C2H4 0.35 ± 0.090.51 ± 0.130.71 ± 0.080.86 ± 0.161.08 ± 0.19 Relaxation increases with decreasing temperature Opposite of rare gas behaviour Relaxation will be more important for planetary atmospheres – more focus on 3 CH 2 chemistry ?
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PES showing surface crossing Crossing is below entrance channel Gannon et al. Faraday Discussions 147 2010 (Glowacki and Harvey, Bristol)
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3. CH Reactions
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CH Chemistry Reactivity very high – capable of reacting with N 2 Important intermediate for increasing carbon number CH + CH 4 → H + C 2 H 4 Single channel so useful calibration reaction More usually several open channels CH + CH 3 OH → HCHO + CH 3 CH + CH 3 OH → H + CH 3 CHO
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4. Product Studies from Laval Reactor (Blitz, Shannon and Heard)
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Low temperature kinetics of abstraction Reactions OH + CH 3 COCH 3 → H 2 O + CH 2 COCH 3 Barrier, so activated process – what is happening at low T? Shannon et al. PCCP 16 2014
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Product Formation OH + CH 3 OH → CH 3 O + H 2 O Shannon et al. Nature Chem. 5 2013
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5. Summary CH 4 photolysis yields are important Currently uncertainty on CH 4 photochemistry New experiments to be undertaken as part of STFC project building on expertise in atmospheric and combustion studies 1 CH 2 chemistry shows interesting T dependence, not always taken into account in models. More focus on 3 CH 2 ? Acceleration in loss rates at low temperatures associated with chemical reaction. Further experiments in Laval systems in progress
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Reagent and product time profiles 1 CH 2 H
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Experimental Generate 1 CH 2 by pulsed photolysis of ketene Monitor removal of 1 CH 2 by LIF 1 CH 2 + C 2 H 2 → C 3 H 3 + H 1 CH 2 + C 2 H 2 + M → C 3 H 4 + M 1 CH 2 + C 2 H 2 → 3 CH 2 + C 2 H 2 Monitor calibrated production of H by LIF
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Master Equation Calculations MESMER (Master Equation Solver for Multi Energy-well Reactions) A + B k Ri k ji k ij k Pj source term n j (E) n i ) Products (infinite sink) E i En)( E j En)( K(E)’s calculated from RRKM theory. Energy transfer calculated an exponential down model ~150 - 450cm -1
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Master Equation Results Modelling shows no stabilization below 50 Torr Balance of reaction is relaxation Experimental Pressure
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Experimental James Lockhart
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Flash Photolysis LIF Detection C Gas mixing manifold MFC N 2 C2H2C2H2 (CH 3 ) 3 COOH O2O2 Reaction Cell Exhaust Line / Needle valve Rotary Pump Gas mixture flows in towards the cell Photolysis laser pulse 248 nm Rhodamine 6G Dye Laser Nd: YAG Laser Probe Laser Pulse 282 nm Photodiode PMT Boxcar Averager Excimer Laser
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k = (7.59 ± 0.31) 10 -11 s -1 cm -3 Gas phase oxidation will compete with aerosol uptake Onel, L; Blitz, M. A; Seakins, P. W J.Phys.Chem.Lett 2012, 3, 853−856 II - OH + MEA (monoethanolamine) OH uptake ? PM
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II - Recycling OH with Excess Oxygen OH Decay in N 2 Zero OH Yield 100% OH Yield Experimental OH Yield
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MESMER Master Equation Solver for Multi Energy-well Reactions MESMER 3.0 Released 24 th Feb 2014. Contact Robin Shannon (R.Shannon@leeds.ac.uk) for more information.R.Shannon@leeds.ac.uk
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