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Detection of IO in the MBL using an open-path CRDS

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1 Detection of IO in the MBL using an open-path CRDS
June 25th, 2009 64th International Symposium on Molecular Spectroscopy Detection of IO in the MBL using an open-path CRDS *Ryuichi Wada, Joe M. Beames and Andrew J. Orr-Ewing University of Bristol, UK * Present address: Nagoya University, Japan

2 Overview Introduction Experimental set-up
Experiments in the laboratory Field observation Conclusions

3 Iodine monoxide (IO) I IO OIO Aerosol Ocean I2 CH2I2 CH3I Source
Atmospheric Iodine cycle O3 n IO h I2 CH2I2 CH3I I IO OIO Aerosol NO2 HO2 IONO2 HOI Aerosol Aerosol Deposition Ocean IO is important radical to understand the chemistry in the marine boundary layer (MBL).

4 Current observation of IO
First observation of [IO] (Mace Head, Ireland) Observation technique [IO] = ppt (1ppt=1/ ) ~ 20 km Differential Optical Absorption Spectroscopy (DOAS) U. Platt and co-workers, Nature, 397, 572, 1999 DOAS is the only technique for observation of IO. All observed [IO] were up to ~ 10 ppt.

5 There is no technique to measure inhomogeneous IO.
Disagreement with model and observation A model for MBL prediction of [IO] = ~100 pptv A. Ravishankara et al. Atmos. Chem. Phys., 4, 19, 2004 Possible interpretation Inhomo- geneous IO spot DOAS observed average concentration in light path (~ 10 ppt) Inhomogeneous sources of IO possibly exist (~ 100 ppt) Light path There is no technique to measure inhomogeneous IO.

6 Cavity ring down spectroscopy
It =e-kt Time /ms Intensity /arb. units It =e-k0t ∆k = k–k0 With absorbers ∆k=c[X]σX Without absorbers k: Ring-down decay rate c: Speed of light σX: Cross-section of X High sensitivity Optical path length ~ 10 km Compactness Point measurement CRDS has a possibly to detect inhomogenious IO radicals.

7 Experimental set-up Reaction N2O + hn(193nm)→ N2 + O(1D)
YAG-Dye laser (~435 nm) Excimer laser (193 nm) N2O/CF3I/Ar Reaction N2O + hn(193nm)→ N2 + O(1D) O(1D) + Ar → O(3P) CF3I + O(3P) → IO + CF3 Digitiser / PC

8 IO spectra IO A2P3/2 - X2P3/2 (3,0) Simulation Rotational structure
Experiment P R Simulation spectrum: A.Orr-Ewing et al., J. Chem. Soc. Faraday Trans., 94, 2681, 1998

9 Absorption cross-section of IO (3,0)
Experimental Model Calculation Numerical integration method [CF3I]int and [N2O]int k [IO] Reaction kinetics of IO N2O hn = N O(1D) O(1D) M = O(3P) + M CF3I O(3P) = IO CF3 IO IO = Products Wavelength σ=5.9×10-17 cm2 molecule-1 M.Kawasaki et al., J. Phys. Chem. A, 107, 6381, 2003 Time-dependent concentration of IO radicals

10 Result : time-dependent concentration of IO radicals
▪ Experimental Model calculation IO + IO → Product [IO] is good agreement between experiment and model.

11 Simulate the absorption cross-section IO A2P3/2 - X2P3/2 (3,0)
Resolution 0.2 cm-1 24 cm-1 Kawasaki et al., J. Phys. Chem. A, 2003 5.9 ± 0.6 3.1±0.4 Harwood et al., J. Phys. Chem. A, 1997 - 2.7±0.4 convolution Unit: cm2 molecule-1 Simulated spectrum Resolution: cm-1 - 24 cm-1

12 Open-path CRD spectrometer
Detector YAG-Dye laser system HR mirror Optical table Sampling Air Electronics Wheel & Vibration isolator

13 Field observation in Roscoff
High tide Low tide Extensive Seaweed beds are exposed.

14 Measurements method Total accumulation time for one data point: 30 s
Bandhead IO 6 Total accumulation time for one data point: 30 s 4 / cm2 molecule-1 Cross-section of IO 2 Baseline 22944 22948 22952 22956 Wavenumber /cm-1 NO2 NO2 has absorption in the measurement wavenumbers. 6 /10-19 cm2 molecule-1 Cross-section of NO2 / cm2 molecule-1 4 Same value of cross-sections 2 No interferences of NO2 22944 22948 22952 22956 Wavenumber /cm-1

15 Observation results 25th September 2006
Fine & cloudy day ● Mixing ratio of IO ○ Minimum detectable limit Wind High [IO] radicals were successfully detected. The concentrations have inverse-trend with tidal heights.

16 Conclusions An open-path CRD spectrometer was designed and constructed for atmospheric IO radicals. The cross-section of IO was tested by both of kinetic measurement and model simulation. 3. The open-path CRD spectrometer had been deployed in the field campaign and successfully detected high concentration of IO radicals.

17 Acknowledgements Professor Andrew J. Orr-Ewing
Dr Gordon McFiggans and observation team in RHaMBLe projects Professor Yutaka Matsumi Funding: EPSRC STE research lab in Nagoya University


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