COBALD measurements of aerosol backscatter in the ASM: , and outlook on the StratoClim WP2 field campaign (2016)

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COBALD measurements of aerosol backscatter in the ASM: 2013-2015, and outlook on the StratoClim WP2 field campaign (2016) S. Brunamonti, F.G. Wienhold, B. Luo and T. Peter Institute for Atmospheric and Climate Science (IAC), ETH Zürich, Switzerland Workshop on dynamics, transport and chemistry of the UTLS Asian monsoon Foothills Laboratory, National Center for Atmospheric Research (NCAR), 9 March 2016, Boulder CO

COBALD Compact Optical Backscatter Aerosol Detector COBALD is a light-weight aerosol backscattering detector at two wavelengths (blue = 455 nm, red = 940 nm) for balloon measurements, developed at ETH Zürich. Despite meant for high cloud research, COBALD can provide valuable information for the analysis of the Asian tropopause aerosol layer (ATAL) [Vernier et al., 2015]. Vernier et al., 2015 2/20

Backscatter ratio (BSR) of ATAL vs. Cirrus clouds CI = RedBSR 1 BlueBSR 1 Cirrus (15 km) BlueBSR 2-3 RedBSR > 10 CI 10 ATAL (16-17 km) BlueBSR 1.1 RedBSR 1.4 CI 5-6 Cloud-filtering criterion CI < 7 & RedBSR < 2.5 (as in Vernier et al., 2015) 3/20

Outline 1. Overview of COBALD soundings in the ASM 2013-2015 2. Optical modeling: constraining particle number densities in ATAL from the COBALD measurements 3. Outlook on StratoClim 2016: campaign sites and strategy 4/20

COBALD in the ASM region: 2013-2015 5/20

COBALD in the ASM region: 2013-2016 5/20

Lhasa 2013 18 soundings Vernier et al., 2015 Pressure binning: 47 levels between 16-260 hpa (ECWMF L137). 6/20

COBALD in the ASM region: 2013-2015 7/20

COBALD in the ASM region: 2013-2015 8/20

COBALD in the ASM region: 2013-2015 8/20

COBALD in the ASM region: 2013-2015 8/20

9/20

Optical modeling Method Using a Mie scattering optical model, BlueBSR and Color Index can be calculated by prescribing a lognormal size distribution (i.e. mode radius, sigma, number density): For a single-mode size distribution, CI is independent of number density and therefore it can be used as an «indicator» of particle size. BlueBSR = BlueBSR r, σ, N CI = RedBSR 1 BlueBSR 1 = CI r, σ Kunming 2014, 80-150 hpa 10/20

Optical modeling Method Using a Mie scattering optical model, BlueBSR and Color Index can be calculated by prescribing a lognormal size distribution (i.e. mode radius, sigma, number density): Step 1: constrain mode radius and sigma using CI from measurements BlueBSR = BlueBSR r, σ, N CI = RedBSR 1 BlueBSR 1 = CI r, σ Kunming 2014, 80-150 hpa Step 2: apply BlueBSR constraint calculate number density of each possible solution 10/20

Optical modeling Method Using a Mie scattering optical model, BlueBSR and Color Index can be calculated by prescribing a lognormal size distribution (i.e. mode radius, sigma, number density): Step 1: constrain mode radius and sigma using CI from measurements BlueBSR = BlueBSR r, σ, N CI = RedBSR 1 BlueBSR 1 = CI r, σ Kunming 2014, 80-150 hpa Step 2: apply BlueBSR constraint calculate number density of each possible solution 10/20

Optical modeling ATAL vs. Stratospheric aerosols Kunming 2014 Stratospheric aerosols Assuming mode radius 70 nm Sigma 1.85 Number density 10 cm -3 Consistent with literature (e.g. Hamill et al., 1997). ATAL (80-150 hpa) Assuming mode radius 50 nm Sigma 1.6 Number density 500 cm -3 Factor of 5 higher than the background concentration by the SCOUT-O3 campaign (Borrmann et al., 2010) 11/20

SCOUT-O3: Background UTLS aerosols Aircraft measurements of submicron (> 6 nm) particle concentration at the Southern Indian UTLS (20 N) during November-December 2005. Borrmann et al., ACP, 2010 12/20

Optical modeling Single vs. bimodal size distribution Background Bimodal distribution Calculated as single lognormal distribution after subtracting the BSR from a "background mode" defined as: Mode radius = 30 nm Sigma = 1.6 Number density = 100 cm -3 13/20

Optical modeling Single vs. bimodal size distribution Background Solution 1 More background particles Solution 2 Larger background particles Solution 3 Background + larger particles 14/20

StratoClim WP2 field campaign, summer 2016 Within the StratoClim project, ETH Zürich together with the Indian Institute of Tropical Metereology (IITM) will perform: 25x night-time launches with: COBALD / CFH / ECC / RS41 5-10x day-time launches with payload: CFH / RS41 / RS92 from two stations in India, simultaneously with the Geophysica-M55 aircraft campaign (approx. 18 Jul - 18 Aug 2016) Campaign stations: Nainital, northern India 79.45 E, 29.40 N Nagpur, central India 79.08 E, 21.15 N Ploeger et al., ACP [2015] 15/20

ECMWF analysis (0.15 x0.15 ) Jul-Aug 2015: Temperature 16/20

ECMWF analysis (0.15 x0.15 ) Jul-Aug 2015: Ice saturation 17/20

ECMWF analysis (0.15 x0.15 ) Jul-Aug 2015: H 2 O mixing ratio 18/20

ECMWF analysis (0.15 x0.15 ) Jul-Aug 2015: Ice water content 19/20

StratoClim 2016 field campaign: summary Nainital (79 E, 29 N) More likely inside the transport barrier [Ploeger et al., 2015] and the conduit [Bergman et al., 2013]. Warmer UTLS, lower ice saturations at the cold-point tropopause. Enhanced water vapour and aerosols (ATAL) at the UTLS. Nagpur (79 E, 21 N) More likely outside the transport barrier [Ploeger et al., 2015] and the conduit [Bergman et al., 2013]. Colder UTLS, higher ice saturations at the cold-point tropopause. More cirrus clouds, more dehydration, less water vapour in the LS. Draft campaign strategy: Nainital: 15 night-time + 5 day-time launches, between approx. 18 Jul -18 Aug Nagpur: 10 night-time launches, during the Geophysica in-situ flights (01-20 Aug) 20/20