Status: this preprint was under review for the journal ACP but the revision was not accepted.
Modelling the chemistry and transport of bromoform within a sea breeze driven convective system during the SHIVA Campaign
P. D. Hamer,V. Marécal,R. Hossaini,M. Pirre,N. Warwick,M. Chipperfield,A. A. Samah,N. Harris,A. Robinson,B. Quack,A. Engel,K. Krüger,E. Atlas,K. Subramaniam,D. Oram,Emma C. Leedham Elvidge,G. Mills,K. Pfeilsticker,S. Sala,T. Keber,H. Bönisch,L. K. Peng,M. S. M. Nadzir,P. T. Lim,A. Mujahid,A. Anton,H. Schlager,V. Catoire,G. Krysztofiak,S. Fühlbrügge,M. Dorf,and W. T. Sturges
Abstract. We carry out a case study of the transport and chemistry of bromoform and its product gases (PGs) in a sea breeze driven convective episode on 19 November 2011 along the North West coast of Borneo during the "Stratospheric ozone: Halogen Impacts in a Varying Atmosphere" (SHIVA) campaign. We use ground based, ship, aircraft and balloon sonde observations made during the campaign, and a 3-D regional online transport and chemistry model capable of resolving clouds and convection explicitly that includes detailed bromine chemistry. The model simulates the temperature, wind speed, wind direction fairly well for the most part, and adequately captures the convection location, timing, and intensity. The simulated transport of bromoform from the boundary layer up to 12 km compares well to aircraft observations to support our conclusions. The model makes several predictions regarding bromine transport from the boundary layer to the level of convective detrainment (11 to 12 km). First, the majority of bromine undergoes this transport as bromoform. Second, insoluble organic bromine carbonyl species are transported to between 11 and 12 km, but only form a small proportion of the transported bromine. Third, soluble bromine species, which include bromine organic peroxides, hydrobromic acid (HBr), and hypobromous acid (HOBr), are washed out efficiently within the core of the convective column. Fourth, insoluble inorganic bromine species (principally Br2) are not washed out of the convective column, but are also not transported to the altitude of detrainment in large quantities. We expect that Br2 will make a larger relative contribution to the total vertical transport of bromine atoms in scenarios with higher CHBr3 mixing ratios in the boundary layer, which have been observed in other regions. Finally, given the highly detailed description of the chemistry, transport and washout of bromine compounds within our simulations, we make a series of recommendations about the physical and chemical processes that should be represented in 3-D chemical transport models (CTMs) and chemistry climate models (CCMs), which are the primary theoretical means of estimating the contribution made by CHBr3 and other very short-lived substances (VSLS) to the stratospheric bromine budget.
Received: 31 May 2013 – Discussion started: 07 Aug 2013
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P. D. Hamer,V. Marécal,R. Hossaini,M. Pirre,N. Warwick,M. Chipperfield,A. A. Samah,N. Harris,A. Robinson,B. Quack,A. Engel,K. Krüger,E. Atlas,K. Subramaniam,D. Oram,Emma C. Leedham Elvidge,G. Mills,K. Pfeilsticker,S. Sala,T. Keber,H. Bönisch,L. K. Peng,M. S. M. Nadzir,P. T. Lim,A. Mujahid,A. Anton,H. Schlager,V. Catoire,G. Krysztofiak,S. Fühlbrügge,M. Dorf,and W. T. Sturges
P. D. Hamer,V. Marécal,R. Hossaini,M. Pirre,N. Warwick,M. Chipperfield,A. A. Samah,N. Harris,A. Robinson,B. Quack,A. Engel,K. Krüger,E. Atlas,K. Subramaniam,D. Oram,Emma C. Leedham Elvidge,G. Mills,K. Pfeilsticker,S. Sala,T. Keber,H. Bönisch,L. K. Peng,M. S. M. Nadzir,P. T. Lim,A. Mujahid,A. Anton,H. Schlager,V. Catoire,G. Krysztofiak,S. Fühlbrügge,M. Dorf,and W. T. Sturges
P. D. Hamer,V. Marécal,R. Hossaini,M. Pirre,N. Warwick,M. Chipperfield,A. A. Samah,N. Harris,A. Robinson,B. Quack,A. Engel,K. Krüger,E. Atlas,K. Subramaniam,D. Oram,Emma C. Leedham Elvidge,G. Mills,K. Pfeilsticker,S. Sala,T. Keber,H. Bönisch,L. K. Peng,M. S. M. Nadzir,P. T. Lim,A. Mujahid,A. Anton,H. Schlager,V. Catoire,G. Krysztofiak,S. Fühlbrügge,M. Dorf,and W. T. Sturges
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Institute of Atmospheric and Environmental Science, Dept. of Experimental AtmosphericResearch, J. W. Goethe-University Frankfurt am Main, Germany
L. K. Peng
Malaysian Meteorological Department, Ketua Stesen GAW Lembah Danum, Jabatan Meteorologi Malaysia, Cawangan Sabah, Lapangan Terbang Wakuba Tawau, Peti Surat 60109, 91011 Tawau, Sabah, Malaysia
M. S. M. Nadzir
School of Environmental and Natural Resource Sciences, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, 43600 Bangi, Selangor, Malaysia
P. T. Lim
Department of Aquatic Science, Universiti Malaysia Sarawak, 94300 Kota Samarahan, Sarawak Malaysia
A. Mujahid
Department of Aquatic Science, Universiti Malaysia Sarawak, 94300 Kota Samarahan, Sarawak Malaysia
A. Anton
Borneo Marine Research Institute, Universiti Malaysia Sabah, Jalan UMS, 88400 Kota Kinabalu, Sabah, Malaysia
H. Schlager
Deutsches Zentrum für Luft- und Raumfahrt (DLR), Institut für Physik der Atmosphäre, Atmosphärische Spurenstoffe, Münchner Straße 20, 82234 Oberpfaffenhofen-Wessling, Germany