Elemental and water-insoluble organic carbon in Svalbard snow: a synthesis of observations during 2007-2018
←
→
Page content transcription
If your browser does not render page correctly, please read the page content below
Atmos. Chem. Phys., 21, 3035–3057, 2021 https://doi.org/10.5194/acp-21-3035-2021 © Author(s) 2021. This work is distributed under the Creative Commons Attribution 4.0 License. Elemental and water-insoluble organic carbon in Svalbard snow: a synthesis of observations during 2007–2018 Christian Zdanowicz1 , Jean-Charles Gallet2 , Mats P. Björkman3 , Catherine Larose4 , Thomas Schuler5 , Bartłomiej Luks6 , Krystyna Koziol7 , Andrea Spolaor8,9 , Elena Barbaro8,9 , Tõnu Martma10 , Ward van Pelt1 , Ulla Wideqvist11 , and Johan Ström11 1 Department of Earth Sciences, Uppsala University, 752 36 Uppsala, Sweden 2 Norwegian Polar Institute, 9296 Tromsø, Norway 3 Department of Earth Sciences, University of Gothenburg, 405 30 Gothenburg, Sweden 4 Environmental Microbial Genomics, École Centrale de Lyon, Université de Lyon, 69134 Ecully, France 5 Department of Geosciences, University of Oslo, 0316 Oslo, Norway 6 Institute of Geophysics, Polish Academy of Sciences, 01-452 Warsaw, Poland 7 Department of Analytical Chemistry, Gdańsk University of Technology, 80-233 Gdańsk, Poland 8 Institute of Polar Sciences, ISP-CNR, 30170 Venice Mestre, Italy 9 Department of Environmental Sciences, Informatics and Statistics, Ca’ Foscari University of Venice, 30172 Mestre, Italy 10 Department of Geology, Tallinn University of Technology, 19086 Tallinn, Estonia 11 Department of Environmental Science, Stockholm University, 106 91 Stockholm, Sweden Correspondence: Christian Zdanowicz (christian.zdanowicz@geo.uu.se) Received: 19 May 2020 – Discussion started: 16 June 2020 Revised: 4 January 2021 – Accepted: 7 January 2021 – Published: 1 March 2021 Abstract. Light-absorbing carbonaceous aerosols emitted by 2009), comparable surveys. Both LEC WIOC snow and Lsnow increased biomass or fossil fuel combustion can contribute to ampli- with elevation and snow accumulation, with dry deposi- fying Arctic climate warming by lowering the albedo of tion likely playing a minor role. Estimated area-averaged snow. The Svalbard archipelago, being near to Europe and snowpack loads across Svalbard were 1.1 mg EC m−2 and Russia, is particularly affected by these pollutants, and im- 38.3 mg WIOC m−2 for the 2015–2016 winter. An ∼ 11-year proved knowledge of their distribution in snow is needed long dataset of spring surface snow measurements from the to assess their impact. Here we present and synthesize new central Brøgger Peninsula was used to quantify the inter- data obtained on Svalbard between 2007 and 2018, compris- annual variability of EC and WIOC deposition in snow. In ing measurements of elemental (EC) and water-insoluble or- EC and C WIOC at Ny-Ålesund (50 m a.s.l.) most years, Csnow snow ganic carbon (WIOC) in snow from 37 separate sites. We were 2–5 times higher than on the nearby Austre Brøgger- used these data, combined with meteorological data and breen glacier (456 m a.s.l.), and the median EC/WIOC in Ny- snowpack modeling, to investigate the variability of EC and Ålesund was 6 times higher, suggesting a possible influence WIOC deposition in Svalbard snow across latitude, longi- of local EC emission from Ny-Ålesund. While no long-term EC ) tude, elevation and time. Overall, EC concentrations (Csnow trends between 2011 and 2018 were found, Csnow EC and C WIOC snow −1 ranged from < 1.0 to 266.6 ng g , while WIOC concen- showed synchronous variations at Ny-Ålesund and Austre WIOC ) ranged from < 1 to 9426 ng g−1 , with trations (Csnow Brøggerbreen. When compared with data from other circum- the highest values observed near Ny-Ålesund. Calculated Arctic sites obtained by comparable methods, the median snowpack loadings (LEC WIOC snow , Lsnow ) on glaciers surveyed in EC on Svalbard falls between that found in central Green- Csnow spring 2016 were 0.1 to 2.6 mg m−2 and 2 to 173 mg m−2 , re- land (lowest) and those in continental sectors of European EC and the LEC on those glaciers spectively. The median Csnow Arctic (northern Scandinavia, Russia and Siberia; highest), snow were close to or lower than those found in earlier (2007– Published by Copernicus Publications on behalf of the European Geosciences Union.
3036 C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow which is consistent with large-scale patterns of BC in snow tered from melted snow (Cavalli et al., 2010; see below). Fol- reported by surveys based on other methods. lowing Petzold et al. (2013), we designate the more refrac- tory mass fraction as elemental carbon (EC; see Table 1 for a list of abbreviations used in this paper). The more volatile fraction represents carbon that evolved primarily from water- 1 Introduction insoluble organic carbon (WIOC) but may also include some contributions from the oxidation of carbonate particles (car- Light-absorbing black carbon (BC) aerosols that are trans- bonatic carbon; CC). While the WIOC data are not the main ported to Arctic latitudes can lower the albedo of snow-/ice- focus of our study, they are also presented, as such data are covered surfaces on which they are deposited, thereby en- sparse for Arctic snow. We used our datasets in combination acting a positive feedback that amplifies climate warming with meteorological snowpack modeling to (i) describe the (Bond et al., 2013). The Svalbard archipelago, owing to its spatial distribution of EC and WIOC deposited on Svalbard proximity to the European and Russian mainland, is partic- glaciers, (ii) estimate their mass loading in the winter snow- ularly affected by BC emissions from fossil fuel combus- pack and how it relates to spatial variations in snow accu- tion (FF; heating, gas flaring, etc.) and biomass burning (BB; mulation, and (iii) describe the interannual variability of EC e.g., agricultural or forest fires). Source attribution using car- and WIOC concentration in snow on the Brøgger Peninsula bon isotopes and atmospheric transport modeling indicates between 2007 and 2018. Lastly, we place our findings in a that BC associated with pollution haze events at the Zeppelin broader pan-Arctic perspective by comparison with a compi- Observatory on Spitsbergen includes both BB and FF con- lation of published data obtained between 2002 and 2018 by tributions, the latter being proportionally more important in comparable methods. winter than summer (Winiger et al., 2015, 2019). Quantify- ing the impact of BC deposition on the Arctic surface albedo requires knowledge of its concentrations, spatial distribution 2 Material and methods and variability in snow and ice. These data may also serve to verify the efficacy of ongoing and future measures to curb 2.1 Field sampling emissions of short-lived climate forcing aerosols, such as BC that impacts the Arctic (AMAP, 2015; Stohl et al., 2015). 2.1.1 Spring 2016 glacier survey On Svalbard, reconnaissance surveys of BC in snow were carried out in 1984–1985 by Noone and Clark (1988) and Part of the dataset presented here was produced following a in 2007 by Doherty et al. (2010). This was followed in 2007– comprehensive, coordinated survey of the physical, chemi- 2009 by more detailed investigations of the distribution of cal and microbiological properties of the Svalbard seasonal BC across the archipelago (Forsström et al., 2009, 2013). Lo- snowpack carried out at the end of the 2015–2016 win- calized studies have also been carried out near Longyearbyen ter by individuals from multiple institutions (see Acknowl- (Aamaas et al., 2011; Khan et al., 2017) and Ny-Ålesund (Si- edgments). In total, 22 sites were sampled between 4 and hna et al., 2018; Jacobi et al., 2019). In addition, two ice cores 29 April 2016 on seven individual glaciers of Spitsbergen recovered from the Lomonosovfonna and Holtedahlfonna ice and Nordaustlandet (Fig. 1). Snowpits were sampled at three fields (Spitsbergen) have provided insights into longer-term different elevations in the upper, middle and lower reaches variations in BC deposition on Svalbard (Ruppel et al., 2014, of each glacier, the snow depth increasing with altitude (e.g., 2017; Osmont et al., 2018). Pramanik et al., 2019). In the text and figures, specific snow- Here we present and synthesize new observational data pit locations are identified by a letter and number code, e.g., which document the variability of BC in snow across Sval- HB3 as Hansbreen glacier, snowpit no. 3 (Table 2, with bard in terms of latitude, longitude, altitude and time. These additional details in Table S1 in the Supplement). Glacier data were gathered through field investigations conducted be- sites were targeted partly for logistical reasons (ease of ac- tween 2007 and 2018 on both Spitsbergen and Nordaust- cess by snowmobile), but also because sampling supraglacial landet (Fig. 1). The datasets were developed from surveys snow avoided the heterogeneities in snow properties that may carried out on glaciers of Svalbard in springs 2016 and 2017 arise from interactions with vegetation and/or different sub- and from an 11-year long program of snow sampling for strates (e.g., wet vs. dry tundra soils). In addition, the selected EC on the central Brøgger Peninsula on northwestern Spits- glacier sites were at elevations of 102 to 1193 m a.s.l., which bergen. The spring 2016 survey included some of the sites span ∼ 65 % of the maximum relief in Svalbard (1713 m; previously visited in 2007–2009 by Forsström et al. (2009, Fig. 2). 2013), thus allowing for comparisons after a ∼ decadal in- In advance of the field campaign, standardized protocols terval. All data presented in this study were obtained by the were developed for the measurement of important snow thermo-optical transmittance method (TOT), which quanti- physical properties (e.g., density, temperature) and the col- fies separately the more refractory and volatile carbon mass lection of samples for a variety of analyses, including EC, fractions present in water-insoluble, particulate material fil- WIOC, and stable oxygen isotope ratios (δ 18 O) in water. Atmos. Chem. Phys., 21, 3035–3057, 2021 https://doi.org/10.5194/acp-21-3035-2021
C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow 3037 Figure 1. Map of the Svalbard archipelago, showing the location of the snow sampling sites mentioned in this study (Table 2). Sampling sites on glaciers near Ny-Ålesund (framed area; sites ALB, MLB, ABG, VBG and EDB) are shown in an enlargement in Fig. S2. These protocols are documented in Gallet et al. (2018) and tify EC concentrations in snow (CsnowEC ) at depths where light details relevant for this paper summarized hereafter. Snow absorption by carbonaceous particles has the largest impact sampling was performed in snowpits excavated down to on snow albedo (Marks and King, 2013). The deeper sam- the hard, icy firn surface representing the previous year’s ples were used to estimate the total column mass loading late summer ablation surface (in the accumulation zone of of EC and WIOC (LEC WIOC snow , Lsnow ) in the seasonal snowpack. glaciers) or to the underlying bare ice surface (in the abla- EC WIOC ) in lay- Quantification of Csnow (and, concurrently, of Csnow tion zone). All snowpits were located well away from point ers from discrete snowfall events was not feasible, owing to sources of contamination (e.g., field camps), were accessed the large snow volume required to achieve a sufficient par- by foot from at least 100 m and personnel doing the sam- ticulate carbon mass for TOT analysis. All snow samples pling wore protective, non-particulating suits, gloves, and were double-bagged in sterile low-density polyethylene bags face masks, and employed pre-cleaned plastic or stainless and returned frozen to a location where they were subse- steel tools. The snow accumulation of each snowpit (hSWE , quently melted and filtered. Depending on logistics, this was in water equivalent; w.e.) was calculated from discrete den- done either at the Polish Polar Station Hornsund operated by sity measurements. After recording the physical properties the Polish Academy of Sciences or at the Norwegian Polar of snow strata, large-volume snow samples (∼ 5 L each) Institute (NPI) facilities in Ny-Ålesund (Sverdrup station), were collected from the top 5 cm of the snowpack, and, Longyearbyen (UNIS) or Tromsø. A total of 89 samples were where snowpack depth allowed for it, at 50 cm depth inter- obtained from all 22 glacier sites. vals beneath. The surface samples were collected to quan- https://doi.org/10.5194/acp-21-3035-2021 Atmos. Chem. Phys., 21, 3035–3057, 2021
3038 C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow Table 1. Main symbols and abbreviations used in this paper. The various terms for black carbon (BC, EC) are as defined in Petzold et al. (2013). Abbreviation Units Definition or symbol BC Black carbon: light-absorbing, refractory particulate carbon aerosols emitted by the incomplete combustion of organic fuels (biomass or fossil fuels). TOT Thermo-optical transmittance method used to analyze particulate carbon in snow EC Elemental carbon: refractory carbon fraction determined by TOT WIOC Water-insoluble organic carbon: volatile carbon fraction determined by TOT CC Carbonatic carbon released by oxidation of carbonate minerals EC Csnow ng g−1 Mass concentration of EC in snow determined by the TOT method WIOC Csnow ng g−1 Mass concentration of OC in snow determined by the TOT method EC C̃snow ng g−1 EC Median value of Csnow WIOC C̃snow ng g−1 OC Median value of Csnow LEC filt µg cm−2 Mass loading of EC on filters determined by the TOT method LWIOC filt µg cm−2 Mass loading of OC on filters determined by the TOT method hSWE cm Snow depth expressed in water equivalent LEC snow mg m−2 EC Mass loading of EC in the seasonal snowpack, based on measurements of Csnow LWIOC snow mg m−2 OC Mass loading of OC in the seasonal snowpack, based on measurements of Csnow PSAP Particle Soot Absorption Photometer Analysis of downscaled climatological fields from the Eu- alyzed in the same manner as those of the spring 2016 glacier ropean Centre for Medium-Range Weather Forecasts (ERA- survey. Interim; Dee et al., 2011) over Svalbard shows that surface temperatures in the 2015–2016 winter exceeded the 30-year 2.1.3 Surface snow monitoring (2007–2018), Brøgger climatological normals for the 1981–2010 period by 2 to Peninsula 6 ◦ C, with the largest anomalies observed in the northeast- ern part of the archipelago (Fig. S1a in the Supplement). To- Surface snow layers have been sampled for EC measure- tal winter precipitation also exceeded 1981–2010 normals by ments by NPI staff at several sites on Brøgger Peninsula be- 0.2 to 0.7 m w.e. over much of central and northern Spitsber- tween 2007 and 2018 (Fig. 1; see enlargement in Fig. S2 gen (Fig. S1b). These unusual conditions arose partly owing for details). The first of these sites is in the accumulation to an extreme winter warming and precipitation event asso- zone of the glacier Austre Brøggerbreen (ABG; 78.87◦ N, ciated with a southerly air intrusion over Spitsbergen that oc- 11.92◦ E; 456 m a.s.l.), which was accessed by snowmobile curred in late December 2015 (Binder et al., 2017; Kim et from Ny-Ålesund. The other sites are on the outskirts of al., 2017). The implications of these climatological circum- Ny-Ålesund, one ∼ 80 m southeast of NPI’s Sverdrup sta- stances for the interpretation of our snow survey data are dis- tion (78.92◦ N, 11.93◦ E; ∼ 50 m a.s.l.) and the other near the cussed later. Gruvebadet Atmospheric Laboratory (78.92◦ N, 11.89◦ E; ∼ 50 m a.s.l.). Sampling was carried out at approximately weekly intervals by the NPI permanent staff at Sverdrup 2.1.2 Spring 2017 glacier survey station, whenever their work schedule made it possible and when safe snowmobile driving conditions (e.g., proper visi- EC and C WIOC measurements We also report additional Csnow bility, firm surface) allowed access to Austre Brøggerbreen. snow in surface snow collected at 17 sites on five glaciers in north- Because of these restrictions, the snow samples could not al- western Spitsbergen (n = 26; see Table 2, with additional de- ways be collected immediately after snowfall events. Over tails in Table S2). These samples were collected by NPI staff the ∼ 11-year period considered, a total of 201 samples were during other field research activities but were handled and an- collected between February and June, 86 % of which were Atmos. Chem. Phys., 21, 3035–3057, 2021 https://doi.org/10.5194/acp-21-3035-2021
C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow 3039 Table 2. Snow sampling sites in Svalbard mentioned in this paper. Glacier site codes that include a number (e.g., KVG3) are those where samples were collected during the spring 2016 survey. The “x” symbols indicate whether samples were collected from surface layers (S) and/or in snowpits (P). A few samples from Austre Brøggerbreen (ABG) were collected below 456 m a.s.l. Further details on sampling sites are provided in Tables S1 and S2. Sampling site Coordinates Elev. S P Sampling site Coordinates Elev. S P Lat. N Long E (m a.s.l.) Lat. N Lon. E (m a.s.l.) Northwestern Spitsbergen Edithbreen (EBR) Kongsvegen (KVG) 11◦ 110 78◦ 510 625 X KVG3 13◦ 200 78◦ 450 672 X X 11◦ 450 78◦ 510 425 X KVG2 13◦ 090 78◦ 470 534 X X Ny Ålesund area 12◦ 580 78◦ 480 395 X Sverdrup 78◦ 550 11◦ 560 ∼ 50 X KVG1.5 12◦ 520 78◦ 490 326 X X Gruvebadet 78◦ 550 11◦ 540 ∼ 50 X KVG1 12◦ 460 78◦ 500 226 X X 12◦ 290 78◦ 520 3 X Central Spitsbergen Holtedahlfonna (HDF) Lomonosovfonna (LF) HDF3 12◦ 240 79◦ 080 1119 X X LF3 17◦ 260 78◦ 490 1193 X X HDF2 12◦ 320 79◦ 020 718 X X LF2 17◦ 090 78◦ 410 523 X X 78◦ 590 13◦ 280 642 X LF1 17◦ 050 78◦ 380 223 X X HDF1 13◦ 180 78◦ 560 570 X X Austre Brøggerbreen (ABG) Southern Spitsbergen 78◦ 520 11◦ 550 456 X Werenskioldbreen (WSB) Vestre Brøggerbreen (VBG) WSB3 15◦ 290 77◦ 060 528 X 78◦ 540 11◦ 400 450 X WSB2 15◦ 260 77◦ 040 413 X 78◦ 540 11◦ 400 355 X WSB1 15◦ 190 77◦ 050 166 X 78◦ 540 11◦ 410 300 X Hansbreen (HB) 78◦ 550 11◦ 440 139 X HB3 15◦ 290 77◦ 070 396 X X Austre Lovénbreen (ALB) HB2 15◦ 380 77◦ 050 275 X X ALB3 12◦ 110 78◦ 520 513 X X HB1 15◦ 380 77◦ 030 102 X X ALB2 12◦ 100 78◦ 530 340 X X ALB1 12◦ 080 78◦ 530 195 X X Nordaustlandet Midtre Lovénbreen (MLB) Austfonna (AF) 11◦ 590 78◦ 520 403 X AF3 24◦ 000 79◦ 500 785 X X 12◦ 020 78◦ 530 297 X AF2 22◦ 500 79◦ 460 507 X X 12◦ 040 78◦ 540 87 X AF1 22◦ 250 79◦ 440 336 X X taken in the spring months (March–May), April being the microfiber filters (Fig. S3). For the spring 2016 and 2017 most represented month (n = 44). Methods for field sam- glacier surveys, the large number of samples obtained, com- ple collection were the same as those described above for bined with the need to process samples at various field sta- the April 2016 survey. Sample collection was limited to the tions (to avoid risky transport), made use of microwave ovens top 5 cm of the snowpack (occasionally deeper). These data impractical. Instead, these samples were melted at room tem- provide long-term estimates of the interannual variability of perature inside their closed bags. Melting the 5 L samples EC and C WIOC in Svalbard against which results of the Csnow took ∼ 24–36 h, depending on the exact volume and density snow April 2016 survey (and others) can be compared. of the material. The meltwater was drained periodically and filtered as it was being produced; i.e., filtration was done in 2.2 EC and WIOC analyses steps, as the samples melted, so the total duration of melt- ing does not equate the time any water was left standing in 2.2.1 Laboratory procedures the bags. In the end, the bags were rinsed with Milli-Q wa- ter, the rinse water also filtered, and the added water volume The snow samples collected routinely by NPI staff near Ny- accounted for. Ålesund and on Austre Brøggerbreen were processed follow- All the filters produced from the snow samples were air- ing the protocol described in Forsström et al. (2009). Briefly, dried at room temperature overnight, stored in sterile petri snow was transferred into pre-cleaned, 1 L borosilicate glass dishes, and later sent to the Department of Environmental beakers and melted in a microwave oven. At 800 W power, Science of Stockholm University. There, EC/WIOC analysis the typical melting time was ∼ 10 min kg−1 . The meltwater was performed using a Sunset Laboratory carbon aerosol an- was then filtered through pre-ashed, 47 mm diameter quartz https://doi.org/10.5194/acp-21-3035-2021 Atmos. Chem. Phys., 21, 3035–3057, 2021
3040 C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow tained for filters prepared from diluted aqueous suspensions of NIST-2975 diesel soot or from chimney soot. For the measurements on our samples, a 1 × 1 cm2 square section was used from each filter to determine separately the particulate EC and WIOC mass density, or loading, on each filter (LEC WIOC ), from which their mass concentrations in filt , Lfilt EC snow (Csnow , Csnow WIOC ) were calculated based on the volume of meltwater filtered, following EC LEC filt Afilt Csnow = , (1) Vmeltwater LWIOC Afilt WIOC Csnow = filt , (2) Vmeltwater where Afilt is the total area of the filter on which particulate matter was collected and Vmeltwater the volume of meltwater filtered. Calculated values of CsnowEC and CsnowWIOC are reported in ng EC g −1 snow and ng WIOC g −1 snow, respectively. Blank filters (n = 6) had particulate carbon loadings below the limit of detection (LOD) of the carbon analyzer, so no blank correction was applied to the data. During the first three years of the NPI snow monitoring program in the Ny-Ålesund area and on the glacier Aus- tre Brøggerbreen, the filters had been analyzed on the car- bon aerosol analyzer using the NIOSH-5040 thermal proto- col (Birch, 2003). Subsequent inter-comparison studies es- Figure 2. Snow sampling sites visited during the spring 2016 tablished that this protocol gave values of LEC filt that were glacier survey, plotted with respect to elevation and glacier surface lower than those obtained by the EUSAAR-2 protocol by an hypsometry (black line; from James et al., 2012). Each circle corre- average factor of 2 (Cavalli et al., 2010). Therefore, and as sponds to a sampling location, and those on glaciers are labeled as in discussed earlier in Forsström et al. (2013), these data were Table 2 and color-coded per region (inset; from König et al., 2014). later corrected by this factor to homogenize the results with The grey arrows and symbols to the left of the hypsometric curve those obtained by the EUSAAR-2 protocol. Since WIOC is indicate elevations at which surface snow samples were collected hundreds of times more abundant than EC in snow, the cor- during the spring 2017 survey. Also shown are the minimum (win- ter) and maximum (summer) thicknesses of the planetary boundary rection has a negligible impact on those results, which were layer (PBL) in the maritime sector of the European Arctic, based on left uncorrected. ERA-40 reanalysis over 1969–2001 (Esau and Sorokina, 2009). 2.2.2 Methodological uncertainties Several factors can contribute to uncertainties in TOT anal- yses of filters produced from melted snow. While some of alyzer (Sunset Laboratory Inc., Forest Grove, USA), follow- these were previously investigated and quantified for EC ing the European Supersites for Atmospheric Aerosol Re- (as discussed below), they remain largely unquantified for search thermal evolution protocol (EUSAAR_2; Cavalli et WIOC. In the absence of such information, we have used the al., 2010). One benefit of this protocol is that it minimizes same estimates of uncertainties pertaining to EC for WIOC, biases in the EC-WIOC split that may be caused by charring but our confidence in the latter is lower. Some uncertainties in and pyrolysis of organic compounds on filters (e.g., Cheng EC quantification arise irrespective of particle composition. et al., 2014). On each day of measurements, filters prepared These include heterogeneous distribution of EC in the snow- with standard sucrose solutions were used to calibrate the in- pack, loss of particles to container walls, undercatch during strument for WIOC measurements (e.g., Pantedeliadis et al., filtration, and uneven loading of particles on the filters. The 2015). There is presently no corresponding, widely accepted EC in snow at the meter scale due to natural variability of Csnow standard for calibration of EC by thermo-optical analysis. snowpack heterogeneity (σsh ) was previously estimated by However, Svensson et al. (2018) showed, using the same in- Forsström et al. (2009) and by Svensson et al. (2013) in Arc- strument and with the same thermal protocol as used in our tic snow, and we therefore used their results here. The loss study, that predictable and reproducible results can be ob- of EC particles to glass container walls was experimentally Atmos. Chem. Phys., 21, 3035–3057, 2021 https://doi.org/10.5194/acp-21-3035-2021
C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow 3041 found by Forsström et al. (2009) to be negligible for stor- ganic carbon by oxide minerals, which may lead to EC un- age times < 48 h (in a sample containing ∼ 35 ng g−1 EC). derestimation, and (c) the formation of EC-dust aggregates, Here, we have assumed this to also be the case for the sam- which is more likely to occur in aged sub-surface snow than ples melted in bags, although we acknowledge that losses in relatively fresh surface snow (Wang et al., 2012; Lim et may occur, which would have a larger impact for samples al., 2014; Kuchiki et al., 2015). with very low EC content. We used results from Amaas et There are, to our knowledge, no reliable data on the min- al. (2011), Svensson et al. (2013) and Forsström et al. (2013) eral dust content in Svalbard snow, but various published to estimate the possible effect of filtration undercatch, since data on trace element analyses suggest typical values be- these studies used the same methods as our own and were tween a few tens of ppb (ng g−1 ) and a few ppm (µg kg−1 ) based on double filtration of real snow samples, rather than based on typical crustal proportions (Casey, 2012; Singh et on “standards” (e.g., diesel soot), which may have proper- al., 2015; Thomas et al., 2020). Carbonate minerals are only ties different than those of actual snow particulates (Torres a minor dust constituent in the wintertime aerosol over Sval- et al., 2014). The aforementioned studies gave estimates of bard and thus unlikely to contribute much to deposition in undercatch that ranged between 18 % and 35 %, with a me- snow (Weinbruch et al., 2012; Moroni et al, 2015). However, dian of 22 %. Undercatch mostly affects the smallest parti- carbonates outcrop in many areas of Svalbard (e.g., central cles, which contribute little to the total BC particle mass (Lim Spitsbergen, Brøgger Peninsula) are common constituents in et al., 2014). Furthermore, the aggregation of particles (BC some cryosols (4 % to 37 % mass; Szymański et al., 2015; alone or BC-dust) as snow ages likely modifies their initial Hanaka et al., 2019) and are found in cryoconites on at least size distribution (Schwarz et al., 2012; Svensson et al., 2018). some Spitsbergen glaciers (Hodson et al., 2010; Langford et The snow samples analyzed in our study were variously aged al., 2011). Wind-blown dust deflated from local soils or sed- and included relatively fresh, near-surface snow and subsur- iments is therefore a potential source of carbonates and other face snow layers which were affected by partial melting– mineral particles in Svalbard snow. refreezing during winter thaw events (a frequent occurrence The EUSAAR-2 protocol used in this study minimizes the on Svalbard). Since we could not quantify how these differ- effect of carbonate minerals by causing CC to evolve into ences would affect filtration efficiency, we opted not to apply CO2 during the He mode of TOT analysis, thus being de- any systematic undercatch corrections to our EC (and WIOC) tected as WIOC rather than EC (Cavalli et al., 2010). Since data. WIOC is hundreds of times more abundant than EC, the ef- The uncertainty in EC quantification arising from un- fect on the measured WIOC concentrations is comparatively even filter loading (σf ) was evaluated from paired measure- very small. Some authors have suggested pre-treatments to ments on separate 1 cm2 filter sections prepared from the remove carbonates on filters (e.g., Evangeliou et al., 2018), spring 2016 snow survey samples (n = 87). The coefficients but as discussed in Svensson et al. (2018), these treatments of variation (CVs) between paired measurements of both may actually raise more issues than they solve, and so they LEC WIOC were found to scale up with the particle filt and Lfilt were not applied in our study. Furthermore, some snow sam- mass density on the filters. Based on these results, the median ples that were collected early during the NPI snow moni- value for LEC WIOC ), with an interquar- filt was 19 % (8 % for Lfilt toring program near Ny-Ålesund were tested at Stockholm tile range of 7 % to 35 % (4 % to 19 % for LWIOC filt ). These University for the effect that carbonate removal by acid fu- estimates also account for the carbon analyzer’s precision, migation had on EC quantification by TOT, but the resulting which contributes to the observed spread of results. By com- changes in thermograms were judged to be too minor to jus- bining the various sources of uncertainty listed above, we es- tify applying this procedure routinely. timated a median coefficient of variation (CV) of ∼ 40 % for With regards to the effect of oxides, Lim et al. (2014) re- EC and C WIOC . both Csnow ported probable artifacts due to such minerals in TOT analy- snow ses of alpine snow samples containing 1–10 µg kg−1 of dust 2.2.3 EC and C WIOC Possible effects of dust in Csnow but did not give the magnitude of the associated errors in snow the measured EC and WIOC concentrations, nor did they A total of 31 snow filters obtained from seven glaciers sur- find any systematic correlation between dust amounts and the veyed in spring 2016 (35 % of samples) were found to have presence or absence of such artifacts in TOT thermograms. faint to pronounced yellow-pink or grey-brown coloration, Hence, at present, there are simply no firm grounds on which likely indicating the presence of k-feldspars and/or oxides to base any error estimates or corrections. This will require which are commonly found in cryoconites, although carbon- dedicated research, which is outside the scope of our paper. ates may also be present in these filters (see notes in the Sup- Concerning the effect of EC–dust aggregates, Wang et plement dataset). al. (2012) showed that in snow with > 20 ng g−1 EC, the for- The presence of mineral dust particles can lead to biases mation of aggregates can lead to underestimation of EC by in the separation of EC and WIOC by the thermo-optical the TOT method, unless samples are sonicated prior to fil- method, owing to several competing effects: (a) CO2 released tration (sonication, however, may increase filtration under- from CC and incorrectly detected as EC, (b) pyrolysis of or- catch). The largest underestimation found in that study, for https://doi.org/10.5194/acp-21-3035-2021 Atmos. Chem. Phys., 21, 3035–3057, 2021
3042 C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow a single sample, was 20 % (80 ng g−1 prior to sonication, 2.4 Supporting data 100 ng g−1 after). For EC < 20 ng g−1 (all other samples), the effect of sonication (hence, presumably, of aggregates) 2.4.1 Surface meteorological observations was negligible. In our own data, EC > 20 ng g−1 occurs in < 3 % of glacier samples, but in ∼ 30 % of snow samples Automated weather stations (AWS) were operated on from near Ny-Ålesund (Sverdrup and Gruvebadet sites). The six glaciers sampled during the April 2016 survey (Table S3). glacier snow samples that produced colored filters were typ- These stations were situated close to the estimated equilib- ically found in layers near the base of snowpits, suggesting rium line altitude (ELA) of the glaciers and provided hourly windblown dust dispersion and deposition in the summer or recordings of air temperature and ultrasonic soundings of autumn when the ground is only partially snow-covered. In snow surface height changes that were used to interpret 11 of the colored filters, the measured LEC filt was noticeably snowpit stratigraphic data, in particular the timing of snow lower than in filters from snow layers immediately above, accumulation and of snowmelt events. Data from the AWSs and in six filters the LEC filt was < LOD. This might be due to were supplemented with records from Longyearbyen and the the effect of dust on TOT measurements, but it is presently airport in Ny-Ålesund obtained from the Norwegian Mete- impossible to confirm. orological Institute and from the Polish Polar Station Horn- sund (77.00◦ N, 15.11◦ E; 9 m a.s.l.). 2.2.4 Calculation of EC and WIOC loadings 2.4.2 Snowpack modeling For the snowpits excavated on glaciers in spring 2016, we computed mass loadings of EC (LEC WIOC snow ) and WIOC (Lsnow ) Owing to the scarcity of direct precipitation measurements in the seasonal snowpack following across Svalbard, reconstructing the snowpack accumulation 2 history is challenging, and estimates from snowpits, probing and radar can only fill some of the spatial and temporal gaps. X LEC snow = EC Csnow ρi zi , (3) i=1 i This difficulty can be partly circumvented by using the output Xn of a snowpack model forced with meteorological observa- LWIOC snow = WIOC Csnow ρi z i , (4) tions (e.g., Jacobi et al., 2019). In this study, we use a coupled i i=1 energy balance–snow model (van Pelt et al., 2012), which has recently been employed to investigate glacier and snow where LEC WIOC −2 snow and Lsnow are in mg m , ρi is the mean den- conditions across Svalbard (van Pelt et al., 2019). The model −3 sity of snow layer i in kg m , zi is its thickness in meters, includes subroutines for the surface energy balance as well as and n is the number of discrete layers. For samples which internal snowpack processes (e.g., densification, melt–freeze EC < 1 ng g−1 , we assigned a value of 0.5 ng g−1 yielded Csnow events), which makes it possible to simulate the evolution (half the LOD) in order to compute snowpack loadings (see of the seasonal snowpack (thickness and internal structure) below). An estimated error on individual density measure- for individual 1 × 1 km grid cells over Svalbard. The snow ments (σρ ) of ±6 % was used (Conger and McClung, 2009; model routine simulates subsurface density, temperature and Proksch et al., 2016), and the meter-scale variability of snow water content while accounting for vertical water transport, layer density at spatial scales of 1 to 100 m2 was assumed liquid water storage, refreezing and runoff (Marchenko et al., to be on the order of 5 %, following Koenig et al. (2016). 2017; Van Pelt et al., 2019). Fresh snow density is described EC and C WIOC with these er- Combining uncertainties in Csnow snow by a temperature- and wind-dependent function (Van Kamp- rors yields a median CV of ∼ 30 % for LEC WIOC snow and Lsnow enhout et al., 2017), while snow densification is the sum of (n = 22 snowpits). destructive metamorphism, compaction by overburden pres- sure and compaction by drifting snow (Vionnet et al., 2012). 2.3 Determination of δ 18 O in snow meltwater Snow scouring and redistribution by wind is not accounted The stable isotope ratio of oxygen (18 O : 16 O) in melted for, however. Layered snow properties are modeled with a snowpit samples collected in April 2016 was used to detect vertical resolution of 1 cm. The performance of the model evidence of warming events associated with large autumn or was estimated by Van Pelt et al. (2012) by comparing the winter snowfalls, which could help to interpret the LEC predicted winter surface mass balance bw with the water- snow and LOC data. The measurements were made at the Institute of equivalent snow accumulation (hSWE ) measured over a net- snow Geology of Tallinn’s University of Technology, Estonia, us- work of reference stakes. Across all glaciers, the RMSE was ing a Picarro model L2120-i water isotope analyzer (Picarro between 0.12 and 0.33 m w.e. and averaged 0.23 m w.e., with Inc., Sunnyvale, USA) (Lis et al., 2008). Results are reported a mean bias of zero. in the standard delta notation δ 18 O relative to the Vienna In this paper, we used the model to (1) simulate the snow- Standard Mean Ocean Water. The analytical precision was pack evolution at some of the glacier sites sampled during ±0.1 ‰. the spring 2016 survey and (2) quantify the variability of snowfall and snow cover over the Brøgger Peninsula for the Atmos. Chem. Phys., 21, 3035–3057, 2021 https://doi.org/10.5194/acp-21-3035-2021
C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow 3043 period 2008–2018, during which surface snow was sampled pack (Fig. S4). This was not the case for Csnow WIOC , which for EC and WIOC. For the spring 2016 survey snowpits, sim- showed no systematic enrichment in surface layers relative ulations were limited to sites located close to or above the to the bulk of the snowpack. In the spring 2016 snowpack, local equilibrium line altitude (identified in Table S1). As in EC > 10 ng g−1 were only found on glaciers of southern Csnow van Pelt et al. (2019), the model was forced with downscaled, Spitsbergen (Hornsund, HB and Werenskioldbreen, WSB; 3-hourly meteorological fields generated with the High Res- max. 22.8 ng g−1 ). The snowpack on these two glaciers also olution Limited Area Model (HIRLAM, version 6.4.2; Reis- had the most snow layers with Csnow WIOC > 100 ng g−1 . Com- tad et al., 2009). Since our objective (1) was to estimate the paring the snow surface layers sampled on glaciers in north- relative timing of snow accumulation and not absolute snow western Spitsbergen in the springs of 2016 (April) and 2017 depth, precipitation at all the modeled glacier sites was lo- (April and May) suggests higher springtime EC and WIOC cally calibrated (scaled with a factor) to ensure matching be- deposition in 2017. On the glacier Kongsvegen (KVG), tween modeled and observed snow depths at the time of ob- EC and C̃ WIOC were which was sampled in both years, the C̃snow snow servation (April 2016). For objective (2), however, no such 4 and 12 times higher in 2017, respectively. adjustments were made. No statistically meaningful differences in C̃snow EC were found in the spring 2016 snowpack between the northwest- ern, central and southern sectors of Spitsbergen (Fig. 3, 3 Results range: 1.1–2.4 ng g−1 ; Kruskal–Wallis test, p > 0.1). How- ever, the snowpack on Austfonna (AF) on the island of EC and C WIOC for all samples an- Descriptive statistics of Csnow Nordaustlandet, northeastern Svalbard, had a significantly snow EC lower C̃snow (1.1 ng g−1 ) than on glaciers of northwest- alyzed in this study are summarized in Table 3. The probabil- EC and C WIOC are positively skewed ity distributions of Csnow ern and southern Spitsbergen. This held true even if val- snow EC , C̃ WIOC ) EC < 1 ng g−1 were excluded. The C WIOC in the ues of Csnow (right-tailed); therefore, we use medians (C̃snow snow snow as measures of their central tendency but also report arith- spring 2016 snowpack were generally lowest on Lomonosov- metic and geometric means for comparisons with other pub- fonna (LF; central Spitsbergen) and on Austfonna (AF) and EC and C WIOC are left-censored by lished data. As both Csnow highest on southern Spitsbergen glaciers (HB and WSB). snow the LOD, the median and mean were estimated by replac- Binning the 2016 snowpit data by elevation (Fig. 4; 200 m EC ing values < 1 ng g−1 with 0.5 × LOD (0.5 ng g−1 ), follow- bins) showed no meaningful differences in C̃snow (2.2– WIOC (50.3–103.0 ng g−1 ) over the ∼ 1100 m 2.8 ng g−1 ) or C̃snow ing Hornung and Reed (1990), while the geometric mean was estimated by the beta factor method of Ganser and altitude range of the 22 glacier sampling sites (Kruskal– EC and C WIOC < LOD are, how- Hewett (2010). Values of Csnow snow Wallis test, p > 0.1). The calculated LEC snow in the spring 2016 ever, included in plots (see below) to provide as complete snowpack were between 0.1 and 2.6 mg m−2 with a median EC ranged as possible a description of our data. Overall, Csnow of 0.7 mg m−2 (mean 0.9 mg m−2 ), while LWIOC snow were be- −1 WIOC from < 1.0 to 266.6 ng g , while Csnow ranged from < 1 to tween 1.7 and 173.2 mg m−2 , with a median of 20.5 mg m−2 9426 ng g−1 . The highest CsnowEC (> 50 ng g−1 ) were mea- (mean 41.2 mg m−2 ). There were no discernible patterns of sured in spring surface snow near Ny-Ålesund (Sverdrup and variation of LEC WIOC snow or Lsnow with respect to geographic lo- EC at these two sites over the pe- Gruvebadet sites). The C̃snow cation, but on most glaciers LEC WIOC snow and/or Lsnow increased −1 riod 2007–2018 (9.8 ng g ) was ∼ 1.4 to 4.0 times higher with elevation along with hSWE (see Sect. 4.2.2). than in surface snow layers at glacier sites (2.4–6.8 ng g−1 ). At most sampling sites, EC accounted for < 30 % (most 3.2 Surface snow monitoring (2007–2018), Brøgger typically, < 5 %) of the total mass of particulate carbon Peninsula (EC + WIOC) in snow, except near Ny-Ålesund, where it ac- EC and C WIOC measured in the surface Variations of Csnow counted for up to 61 %. snow snow of central Brøgger Peninsula between 2007 and 2018 EC was between are shown in Fig. 5. In most months, Csnow 3.1 Snow on glaciers, spring 2016 and 2017 surveys WIOC 1 and 100 ng g and Csnow between 10 and 1000 ng g−1 . −1 EC and C WIOC across the glacier The spatial variations of Csnow For years in which snow samples from both the glacier snow sites surveyed in spring 2016 are summarized in Figs. 3 Austre Brøggerbreen (ABG) and Ny-Ålesund were ob- and 4. Data from samples collected on glaciers of north- tained, the range of variations at ABG (Csnow EC : < 1 − western Spitsbergen in spring 2017 are shown in these plots −1 WIOC −1 45.1 ng g ; Csnow : < 1–1076.1 ng g ) overlapped with for comparison but are limited to surface snow layers. In that near Ny-Ålesund (CsnowEC : < 1–266.5 ng g−1 ; C WIOC : snow EC ranged from the spring 2016 snowpack (n = 22 sites), Csnow −1 < 1–7250.3 ng g ; two outliers excluded; Fig. 5a and b). −1 EC −1 WIOC < 1.0 to 22.7 ng g , with C̃snow = 2.9 ng g , while Csnow EC near Ny-Ålesund was 2– However, in most years, C̃snow −1 WIOC ranged from 12 to 550 ng g , with C̃snow = 49 ng g . At−1 5 times greater than at ABG. Likewise, C̃snowWIOC was fre- EC in surface layers (top 5–10 cm) nearly all the sites, the Csnow quently 2–3 times larger. There were significant interannual was larger than the weighted mean for the whole snow- EC (range: 0.4–8.2 ng g−1 ) and variations in springtime C̃snow https://doi.org/10.5194/acp-21-3035-2021 Atmos. Chem. Phys., 21, 3035–3057, 2021
3044 C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow Figure 3. Measurements of (a) Csnow EC and (b) C WIOC on Svalbard glaciers, grouped by geographic sectors (defined in Fig. 2). The box– snow whisker plots only include measurements from snowpit samples taken on the glaciers surveyed in April 2016. Box heights give the interquar- tile range, and plus signs (“+”) are outliers. Notches bracket the 95 % confidence limits on the median. The ±1σ error bar in the legend box EC or C WIOC values. The dotted horizontal traits shown in some of the box corresponds to a coefficient of variation of 40 % on individual Csnow snow EC −1 plots are the estimated medians if Csnow values < 1 ng g are excluded. Green circles are CsnowEC in surface snow layers sampled on glaciers of northwestern Spitsbergen in 2017 (Table S2), and blue circles are the median values of CsnowEC and C WIOC in snowpit samples collected snow EC and C WIOC measured in on glaciers in 2007–2009 (Forsström et al., 2013). The grey dashed lines bracket the interquartile range of Csnow snow surface snow layers on the glacier Austre Brøggerbreen, northwestern Spitsbergen, between 2007 and 2018 (this study). WIOC (range: 1.8–691.4 ng g−1 ) between 2007 and 2018. C̃snow 4 Discussion EC and C̃ WIOC occurred in the spring of 2017 The highest C̃snow snow and the lowest in the spring of 2014. Depending on the 4.1 Snow on glaciers, spring 2016 and 2017 surveys EC in 2017 was 23–27 times higher than in 2014, site, C̃snow WIOC and C̃snow was 146–217 times higher, the largest differ- EC or C WIOC 4.1.1 Spatial patterns in Csnow snow ences being observed in the snow near Ny-Ålesund. Fur- thermore, in years in which samples were obtained from The spring 2016 survey showed no discernible zonal or lat- both ABG and Ny-Ålesund, the variations were clearly syn- EC or C WIOC across Svalbard. As itudinal gradient of Csnow snow chronous and coherent at these two sites, which are sepa- noted earlier, only on Austfonna (AF) was C̃snow EC signif- rated by ∼ 5.5 km and ∼ 400 m in elevation (Fig. 5c). The icantly lower than in some sectors of Spitsbergen. This EC between Ny-Ålesund and ABG tended to in- ratio of C̃snow EC at both sites, as did the ratio of C̃ WIOC contrasts with findings from surveys made in the springs crease with C̃snow snow EC on AF snow was either com- of 2007–2009, in which C̃snow WIOC (Fig. 5d). The EC/WIOC between these sites with C̃snow parable to, or larger than, that in central or northwestern in snow varied between 0.01 and 0.42, and, in years when Spitsbergen (Forsström et al., 2009, 2013). Based on data the comparison was possible, the variations in springtime from sites where direct comparisons with the 2007–2009 sur- EC/WIOC on ABG (2007–2018 median: 0.08) tracked those EC in the seasonal snowpack varies, veys are possible, C̃snow at Ny-Ålesund (2010–2018 median: 0.10) (Fig. 5e). from year to year, by at least one order of magnitude, and EC , sometimes more (Fig. 3). This was also evident for C̃snow WIOC but also for C̃snow , in the surface snow layers sampled on KVG, northwestern Spitsbergen, in springs 2016 and 2017. Our ability to detect possible spatial patterns in either EC or C̃ WIOC across Svalbard is presently limited by C̃snow snow (1) the large variability in the observed data in both space and time (spread of individual observations), (2) differ- Atmos. Chem. Phys., 21, 3035–3057, 2021 https://doi.org/10.5194/acp-21-3035-2021
C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow 3045 EC , C WIOC and % EC in samples analyzed in this study. n∗ is the number of values > 1 ng g−1 . Two Table 3. Descriptive statistics for Csnow snow EC −1 outliers with Csnow > 1700 ng g were excluded from calculations. Spring 2016 Spring Austre Sverdrup and glacier survey 2017 Brøggerbreen Gruvebadet (22 sites) glacier 2007–2018 2010–2018 All surface Survey (1 site) (2 sites) layers (17 sites) surface Surface Surface EC (ng g−1 ) Csnow n 87 22 26 115 84 n∗ 68 21 25 87 73 Minimum < 1.0 < 1.0 1.6 < 1.0 < 1.0 Maximum 22.7 22.7 25.4 45.2 266.6 Median 1.9 2.4 6.8 3.4 9.8 Mean 2.9 4.7 8.1 6.4 35.1 Geo. mean 1.9 3.2 5.9 2.9 8.8 WIOC (ng g−1 ) Csnow n 87 22 26 109 79 n∗ 87 22 26 108 78 Minimum 12 21 18
3046 C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow Figure 4. Measurements of (a) Csnow EC and (b) C WIOC on Svalbard glaciers, grouped into discrete elevation bins. Data symbols and box snow EC and C WIOC (C̃ EC , C̃ WIOC ) are shown separately on linear plots are defined as in Fig. 3. Altitudinal profiles of the median values of Csnow snow snow snow EC WIOC are computed from sample data collected at sites scales. Note that the elevations on the latter plots are ordinal only, as C̃snow and C̃snow spanning a different range of altitudes within each bin. (Forsström et al., 2013). For their part, Ruppel et al. (2017) models were also tested to account for the error in hSWE val- estimated an annual mean LEC snow of 10 mg m −2 using snow ues arising from the snowpack model uncertainties, and the samples and a firn core from Holtedahlfonna (HDF) span- results were closely comparable. Our calculated LEC snow for ning ∼ 8 years (2006–2014). The corresponding mean LEC snow sites with low hSWE , such as those on the lower reaches of in the late winter (end April) snowpack could be less than glaciers exposed to wintertime katabatic winds, likely un- half of this value (∼ 5 mg m−2 ), but the high interannual vari- derestimate both dry- and wet-deposited EC owing to wind ability in net snow accumulation at this site (Pramanik et al., scouring of the snowpack. Nevertheless, the intercept of our 2019; Van Pelt and Kohler, 2015) and the uncertainty in the linear model for LEC snow suggests that the contribution of dry chronology of the firn core make such an estimate tentative deposition to the winter 2015–2016 EC mass accumulation at best. Differences between our estimates of LEC snow and those on Svalbard glaciers was likely negligible. In this respect, from the 2007–2009 surveys probably reflect, to a large ex- our findings are consistent with those of Sinha et al. (2018) tent, the variability of atmospheric EC transport and deposi- based on direct observations of BC deposition at Ny-Ålesund tion between years and seasons, but also in space (local scale; in winter 2012–2013, but they contrast with those of Jacobi Svensson et al., 2013). et al. (2019), who postulated a ∼ 50 % contribution of BC dry deposition on the glacier Kongsvegen (our site KVG3, 4.1.3 Variations of LEC WIOC snow and Lsnow on glaciers with elev. 672 m a.s.l.) in spring 2012, using calculations of depo- elevation and snow accumulation sition fluxes constrained by measurements in melted snow- pack. The estimated LEC WIOC snow and Lsnow in the spring 2016 snow- We applied the linear models for LEC WIOC snow and Lsnow from pack were generally largest at higher elevations on glaciers, Fig. 6 to a map of late winter (30 April) hSWE gener- where snow accumulation is greater. For the winter 2015– ated with the snowpack model in order to project the ge- 2016 snowpack, we modeled the relationship between LEC snow ographic pattern of EC and WIOC accumulation across and hSWE across all snowpits by robust least-squares linear the whole of Svalbard for the winters 2015–2016 (Fig. 7). regression (Fig. 6a; R 2 = 0.91; RMSE = 0.3). A linear model The hSWE data used for this purpose were extracted from applied to LWIOC snow against hSWE gave a poorer fit (Fig. 6b; the output presented in Van Pelt et al. (2019). Summing R 2 = 0.51; RMSE = 8), owing to the much greater scatter the predicted values for LEC WIOC snow and Lsnow across the land in the LWIOC snow data. Total least-squares (“type-2”) regression Atmos. Chem. Phys., 21, 3035–3057, 2021 https://doi.org/10.5194/acp-21-3035-2021
C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow 3047 EC and (b) C WIOC in surface layers on central Brøgger Peninsula, Svalbard, 2008–2018. The double-headed arrow in (a) Figure 5. (a) Csnow snow EC measured near Ny-Ålesund in March 2008 by Aamaas et al. (2011). (c) Median values of the data is the interquartile range of Csnow EC WIOC (C̃snow , C̃snow ) near Ny-Ålesund and on Austre Brøggerbreen, with error bars representing 95 % confidence bounds (see text for details). EC (upright triangles) and of C̃ WIOC (inverted triangles) near Ny-Ålesund and on Austre Brøggerbreen. (e) Ratio between (d) Ratio of C̃snow snow EC WIOC C̃snow and C̃snow at these sites. (f) Weekly averages of the BC aerosol absorption coefficient σAP measured by two methods at Zeppelin Observatory (normalized units; Eleftheriadis et al., 2009). The latter data are only shown here to highlight the timing of winter/spring maxima in BC aerosol mixing ratios in the study area. https://doi.org/10.5194/acp-21-3035-2021 Atmos. Chem. Phys., 21, 3035–3057, 2021
3048 C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow Figure 7. Map of the estimated LEC WIOC snow and Lsnow in the late win- ter 2015–2016 snowpack over Svalbard, based on the empirical re- lationships shown in Fig. 6, applied to the map of hSWE between 1 September 2015 and 30 April 2016 generated using the snow- pack model (Van Pelt et al., 2019). Note that these maps do not in- clude EC or WIOC deposition in snow from local point sources of pollution around settlements such as Longyearbyen or Ny-Ålesund. 4.1.4 Relative timing of EC and WIOC accumulation on glaciers, winter 2015–2016 Using the snowpack model, we also estimated the rela- tive contributions to LEC WIOC snow and Lsnow made by each of the snowpack layers sampled in the accumulation zone of the seven glaciers surveyed in spring 2016. The num- ber of layers sampled varied from four on Austre Lovén- breen (ALB3) and Lomonosovfonna (LF3) to seven on Werenskioldbreen (WSB3). On-site surface height soundings by AWSs at several glaciers (Fig. S7) indicate that snow ac- Figure 6. Scatterplot of (a) LEC WIOC cumulation in the 2015–2016 winter was more or less equally snow and (b) Lsnow against hSWE based on measurements from Svalbard glacier snowpits from the divided between the autumn period, leading to the late De- April 2016 survey. The vertical error bars are ±1σ and take into cember 2015 snowstorm, and the months that followed up EC , and C WIOC . The horizontal account uncertainties in hSWE , Csnow to mid/late April 2016, when the snowpits were sampled. snow error bars (±1σ ) are based on the RMSE of the values of hSWE The snowpack model simulations, forced with downscaled predicted by the snow model, relative to field observations (Table 2 HIRLAM precipitation data, gave similar results (Fig. 8). in van Pelt et al., 2019). Weighted linear regression models fitted to The AWSs also show that the December 2015 storm saw the data are shown with 95 % confidence bounds. winter temperatures on nearly all glaciers rise above 0 ◦ C for several days, the warming being largest in southern Spitsber- grid provides estimates of the total particulate carbon mass gen. Clear evidence for this was found in a > 0.2 m thick that accumulated in the snowpack. The area-averaged loads icy snow layer at mid depth in the snowpack on Hansbreen were 1.1 ± 0.1 mg EC m−2 and 38.3 ± 0.2 mg WIOC m−2 . (site HB3). The depth of the layer is in good agreement with These figures translate to monthly mean accumulation rates that predicted by the snowpack model at this site, showing of ∼ 0.1 mg EC m−2 per month and ∼ 4.8 mg WIOC m−2 that the simulation provides a reasonable estimate of local per month, respectively, over the period of snow accumula- surface conditions. Icy layers also occurred in the lower half tion from 1 September 2015 and 30 April 2016. of the seasonal snowpack on other glaciers, but none of these could be unambiguously ascribed to the late December 2015 storm period. Atmos. Chem. Phys., 21, 3035–3057, 2021 https://doi.org/10.5194/acp-21-3035-2021
C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow 3049 Figure 8. Simulated evolution of the snowpack from September 2015 to April 2016 at three glacier sites on Spitsbergen, compared with measured profiles of density, cumulative hSWE , δ 18 O, as well as cumulative LEC WIOC snow and Lsnow in the snowpack. The hSWE over the EC and WIOC sampling intervals was computed using the discrete snow layer density data. Where density measurements were missing, values from comparable layers in other snowpits were used. Snow layers with Csnow EC < 1 ng g−1 were assigned a value of 0.5 ng g−1 for LEC snow calculations. Icy snow and discrete ice layers are shown as pale and darker blue lines, respectively. https://doi.org/10.5194/acp-21-3035-2021 Atmos. Chem. Phys., 21, 3035–3057, 2021
3050 C. Zdanowicz et al.: Elemental and water-insoluble organic carbon in Svalbard snow The relative timing of EC and WIOC accumulation, in- permanent atmospheric observatory (Braathen et al., 1990). ferred from the snowpack model chronology, varied con- The diesel-fueled power plant in Ny-Ålesund is a candidate siderably between glaciers (Fig. 9). On Austfonna (AF), source of EC and semi-volatile organic compounds (precur- ∼ 80 % of the EC and WIOC was found in snow layers es- sors for WIOC), as is wintertime vehicular traffic of cars, timated to have been deposited in or after December 2015. snowmobiles, and aircrafts (Shears et al., 1998; Robinson On glaciers of northwestern and central Spitsbergen (ALB, et al., 2007; Dekhtyareva et al., 2016). In a previous sur- KVG, HDF and LF), the accumulation sequence was more vey in April 2008, Aamaas et al. (2011) could find no de- variable and differed between EC and WIOC. On the glaciers tectable local EC pollution in coastal snow within 20 km of Hansbreen (HB) and Werenskioldbreen (WSB) in southern Ny-Ålesund, although none was sampled downwind of the Spitsbergen, most of the EC and WIOC was contained in settlement. Our data, however, suggest that that winter/spring the deep layers of the seasonal snowpack, estimated to have surface snow near Ny-Ålesund is commonly enriched in EC been deposited prior to January 2016. Surface meteorologi- when compared to snow deposited higher up on ABG. If lo- cal records from the Polish Polar Station Hornsund and from cally emitted dust (e.g., mobilized by road traffic in or near an AWS on WSB show that several large snowfall events oc- the town) caused under-estimation of EC in local snow due curred in this area during the autumn of 2015, as well as some to dust-BC aggregates being formed, then the difference be- thaw events (Fig. S7). The stratigraphy of snowpits excavated tween the median EC in snow near Ny-Ålesund and that in on HB and WSB in April 2016 also showed clear evidence of snow at Austre Brøggerbreen may in fact be larger than we melt-freeze events in the early part of the 2015–2016 winter surmised. Ice-free open water areas or frost flowers on sea (e.g., site HB3; Fig. 8). Also visible in these snowpits were ice are also potential sources of particulate WIOC (e.g., mi- multiple positive excursions in δ 18 O (i.e., shifts to less nega- crobes, diatoms, plankton, exopolymers from biofilms) dur- tive values) indicative of snowfall events presumably associ- ing autumn and winter, some of which are likely deposited ated with relatively moist and warm southerly air intrusions in snow by settling or through ice nucleation (Bowman and over Spitsbergen. Conceivably, the relatively elevated Csnow EC Deming, 2010; Campbell et al., 2018; Karl et al., 2019). Sta- WIOC and Csnow in the deeper snowpack layers on HB and WSB ble inversion layers established by strong surface radiative might have resulted from a few large autumn or early winter cooling could trap aerosols emitted from Ny-Ålesund itself snowfall events, as previously observed for wet deposition of or from nearby open waters or sea ice, leading to enhanced SO2− − 4 , NO3 and WIOC on glaciers near Hornsund (Kühnel concentrations of these aerosols in coastal surface snow dur- et al., 2013; Kozioł et al., 2019). Alternatively, or concur- ing these periods. The frequent occurrence of near-surface rently, meltwater percolation during surface thaws (or rain temperature inversions below ∼ 500 m in winter and spring on snow) may have redistributed or concentrated some of the months was previously shown to enhance the concentration more hydrophilic EC and WIOC into snow layers near the of airborne sulfate aerosols (from fuel combustion and/or base of the snowpack (Aamaas et al., 2011; Xu et al., 2012). marine sources) in Ny-Ålesund relative to the Zeppelin Ob- servatory (Dekhtyareva et al., 2018). It thus seems plausible 4.2 Surface snow monitoring (2007–2018), Brøgger that a similar effect may apply to EC and WIOC aerosols. If Peninsula a gradient in EC and WIOC deposition to snow does exist between Ny-Ålesund and ABC, it would not necessarily per- EC and C WIOC Two features of the ∼ 11-year record of Csnow sist in all winter or spring months. For example, Aamaas et snow from Ny-Ålesund and from Austre Brøggerbreen (ABG) EC of 6.6 ng g−1 near Ny-Ålesund al. (2011) measured a C̃snow (Fig. 5) are noteworthy, in that they reveal some spatio- in March 2008, which was very close to the mean of 6.3 ng temporal patterns in the data. One such feature is the mean −1 on ABG snow during the same month. EC and C̃ WIOC between the two sites (as difference in C̃snow EC and C̃ WIOC be- Coherent interannual variations in C̃snow snow snow noted in Sect. 3.2); the other is the synchronous interan- tween Ny-Ålesund and the accumulation area of ABG EC and C WIOC at both sites. The gen- nual variations in Csnow (Fig. 5c) were described in Sect. 3.2. The amplitude of these snow EC WIOC near Ny-Ålesund compared erally higher C̃snow and C̃snow variations was frequently larger than the uncertainty of medi- to ABG suggests that a gradient in atmospheric EC and ans for individual seasons (estimated using the same Monte WIOC deposition exists between these sites in late winter Carlo approach described in Sect. 4.1.1). It thus seems un- and spring, which may be a function of relative distance likely that such a coherent pattern arose by chance alone, e.g., from the coast and/or elevation, Ny-Ålesund and ABG be- owing to random methodological errors. Several possible ex- ing separated by ∼ 5.5 horizontal kilometers and an alti- planations could account for it. One is that year-to-year varia- tude difference of ∼ 400 m. One plausible explanation for tions in springtime long-range transport and deposition of EC such a gradient is that, owing to its greater remoteness, and WIOC aerosols in this part of the Brøgger Peninsula im- the accumulation area of ABG is less influenced by local pact the surface snow chemistry in Ny-Ålesund and at ABG aerosol emissions from Ny-Ålesund (EC and WIOC) or from in a similar way. Another is that in some years, local meteo- coastal waters (WIOC). This was in fact the rationale for the rological conditions promote more efficient dispersion and/or choice of Zeppelin Mountain (474 m a.s.l.) as the site for a scavenging of aerosols emitted from Ny-Ålesund (EC and Atmos. Chem. Phys., 21, 3035–3057, 2021 https://doi.org/10.5194/acp-21-3035-2021
You can also read