Physics-based SNOWPACK model improves representation of near-surface Antarctic snow and firn density
- 1Department of Atmospheric and Oceanic Sciences, University of Colorado, Boulder, CO, USA
- 2Department of Atmospheric and Oceanic Sciences, University of Maryland, College Park, MD, USA
- 3Cryospheric Sciences Laboratory, NASA Goddard Space Flight Center, Greenbelt, MD, USA
- 4Institute for Marine and Atmospheric Research, Utrecht University, Utrecht, the Netherlands
Correspondence: Eric Keenan (email@example.com)
Estimates of snow and firn density are required for satellite-altimetry-based retrievals of ice sheet mass balance that rely on volume-to-mass conversions. Therefore, biases and errors in presently used density models confound assessments of ice sheet mass balance and by extension ice sheet contribution to sea level rise. Despite this importance, most contemporary firn densification models rely on simplified semi-empirical methods, which are partially reflected by significant modeled density errors when compared to observations. In this study, we present a new drifting-snow compaction scheme that we have implemented into SNOWPACK, a physics-based land surface snow model. We show that our new scheme improves existing versions of SNOWPACK by increasing simulated near-surface (defined as the top 10 m) density to be more in line with observations (near-surface bias reduction from −44.9 to −5.4 kg m−3). Furthermore, we demonstrate high-quality simulation of near-surface Antarctic snow and firn density at 122 observed density profiles across the Antarctic ice sheet, as indicated by reduced model biases throughout most of the near-surface firn column when compared to two semi-empirical firn densification models (SNOWPACK kg m−3, IMAU-FDM kg m−3, GSFC-FDM mean bias=15.5 kg m−3). Notably, our analysis is restricted to the near surface where firn density is most variable due to accumulation and compaction variability driven by synoptic weather and seasonal climate variability. Additionally, the GSFC-FDM exhibits lower mean density bias from 7–10 m (SNOWPACK kg m−3, GSFC-FDM bias=10.6 kg m−3) and throughout the entire near surface at high-accumulation sites (SNOWPACK kg m−3, GSFC-FDM kg m−3). However, we found that the performance of SNOWPACK did not degrade when applied to sites that were not included in the calibration of semi-empirical models. This suggests that SNOWPACK may possibly better represent firn properties in locations without extensive observations and under future climate scenarios, when firn properties are expected to diverge from their present state.
The Antarctic ice sheet (AIS) is the largest freshwater reservoir on Earth and if melted entirely would raise globally averaged sea level by 58 m (The IMBIE team, 2018). The AIS is contributing to sea level rise via net mass loss, at an increasing rate from 40±9 Gt yr−1 in 1979–1990 to 252±26 Gt yr−1 in 2009–2017 (Rignot et al., 2019). In order to quantify ice sheet contribution to sea level rise, glaciologists compute the mass balance (MB), defined as the difference between the grounded ice sheet surface mass balance (SMB) and solid ice discharge across the grounding line (Lenaerts et al., 2019). MB is typically calculated using one of three methods, namely the input–output method (Rignot et al., 2019), gravimetry (Velicogna et al., 2020), or satellite altimetry (e.g., Shepherd et al., 2012; Smith et al., 2020), the latter of which combines measurements of ice sheet volume change with modeled snow and firn density estimates. Similar to MB, spatial variations in SMB can be determined from combined density and radar-derived annual snow accumulation estimates (e.g., Medley et al., 2013; Dattler et al., 2019; Kausch et al., 2020). However, in all cases, density estimates represent one of the largest sources of uncertainty (Shepherd et al., 2012; Montgomery et al., 2020) due to an uncertain and simplified representation of snow and firn densification (Alexander et al., 2019; Montgomery et al., 2020), particularly over the low-accumulation interior of ice sheets (Weinhart et al., 2020).
Antarctic new snow density and subsequent densification are known to vary in both space and time and are influenced by, among other factors, local meteorology and drifting snow (Herron and Langway, 1980; Sommer et al., 2018). In particular, surface snow and firn density are known to be strongly impacted by wind-driven compaction, a process hereafter referred to as drifting-snow compaction, whereby mobilized snow particles in the saltation layer, defined as the lowermost 10 cm of the atmosphere (Pomeroy, 1989), break apart upon collision with the snow surface. This process results in fragmented and rounded grains which pack together more efficiently, resulting in increased density (Vionnet et al., 2012). Drifting snow occurs up to 75 % of the time in the AIS escarpment zone (Lenaerts et al., 2012; Palm et al., 2017; van Wessem et al., 2018; Amory and Kittel, 2019), and because of drifting-snow redistribution, precipitating snow particles are not always permanently incorporated into the snowpack at the time or location of precipitation. In fact, observations show that in the high-elevation, dry, and windy areas of the AIS, pockets of fresh snow can be found alongside snow that is more than 1 year old (Picard et al., 2019). Including processes such as drifting-snow compaction, snow metamorphism, and compaction due to overburden stress has been shown to improve model representation of polar snow and firn (van Kampenhout et al., 2017). However, despite this finding, as well as the demonstrated complexity of snow and firn densification, many AIS MB studies (e.g., Zwally et al., 2015; Smith et al., 2020) rely on relatively simplified semi-empirical models (e.g., Ligtenberg et al., 2011; Li and Zwally, 2011; Medley et al., 2020). Semi-empirical densification models successfully capture broad regional variability in firn characteristics (van den Broeke, 2008; Ligtenberg et al., 2011). However, due to their limited complexity, as measured by the inclusion of ephemeral processes such as drifting-snow compaction, they cannot capture high-frequency variability in near-surface snow density originating from varying atmospheric conditions such as temperature and wind speed. Such variability, which can act on hourly timescales, is known to exist from field observations (e.g., Sommer et al., 2018) and may therefore drive erroneous density estimates that are ultimately used in satellite altimetry volume-to-mass conversions.
Additionally, semi-empirical models are tuned to observations representative of the past or present climate (Herron and Langway, 1980; Ligtenberg et al., 2011; Li and Zwally, 2011), which may not be representative under future climate change scenarios (Ligtenberg et al., 2014). Furthermore, because semi-empirical models rely on extensive tuning to observations, they may not perform well in climates poorly sampled by observations (e.g., the East Antarctic plateau). Alternatively, physics based models, for example CROCUS (Vionnet et al., 2012) and SNOWPACK (Bartelt and Lehning, 2002; Lehning et al., 2002a, b), do not explicitly tune simulated density to observations. Instead, physics-based models represent densification using a constitutive relationship between stress and strain for snow. However, physics-based approaches are hindered by a variety of factors including computational expense, the requirement to estimate unknown parameters such as surface roughness length (controlling turbulent fluxes and friction velocity) and snow activation energy (controlling snow viscosity), and the need to calculate intermediate prognostic variables including thermal conductivity, viscosity, and snow grain shape and size. Despite these drawbacks, the complex material properties of snow, combined with an acute scarcity of snow and firn density measurements, lead us to hypothesize that a physics-based modeling approach is preferred.
In order to improve model representation of Antarctic snow and firn properties compared to semi-empirical models, we compare results from the physics-based snow model, SNOWPACK, forced by hourly weather data from MERRA-2 atmospheric reanalysis (Sect. 2.2) to nine automatic weather stations (AWSs), 55 borehole 10 m depth temperatures, and 122 observed near-surface density profiles for a total of 186 locations across the AIS. First, we describe model setup and a new drifting-snow routine designed to improve representation of near-surface (depth ≤10 m) snow and firn density (Sect. 2.1). Next, we evaluate SNOWPACK's ability to simulate the surface energy balance by comparing with available surface temperature proxies (Sect. 3.1). We then explore the sensitivity of SNOWPACK-simulated density profiles to uncertainties in atmospheric forcing and prescribed snow physics (Sects. 3.3–3.4). Next, we compare SNOWPACK to observed density profiles and compare the relative performance of SNOWPACK to two other firn densification models (Sects. 3.5–3.8). Finally, we conclude with a discussion of SNOWPACK-predicted surface density variability and its implications for satellite-altimetry-based measurements of ice sheet MB (Sect. 3.9).
2.1 Physics-based snow model SNOWPACK
Models commonly assume a high (>250 kg m−3) new snow density over Antarctica (Ligtenberg et al., 2011; Groot Zwaaftink et al., 2013) despite observational evidence of occasional relatively low (<100 kg m−3) new snow density (Groot Zwaaftink et al., 2013; Sommer et al., 2018). This difference can be explained by accumulation of snowfall without sufficient wind speed required for drifting-snow compaction to occur. In order to account for this, we have implemented a new drifting-snow compaction routine into the vertical, one-dimensional physics-based land-surface snow model, SNOWPACK (Bartelt and Lehning, 2002; Lehning et al., 2002a, b), which contrasts most existing firn models (Sects. 2.5–2.6) in that it calculates densification using an overburden stress formulation as opposed to an empirical relationship and explicitly determines snow viscosity by calculating the snow microstructure (e.g., grain size and shape) and temperature. Originally designed as an alpine snow cover model capable of describing snow cover properties, including accumulation, densification, temperature, energy balance, and snow microstructure, SNOWPACK has been applied to both the Greenland and Antarctic ice sheets (Groot Zwaaftink et al., 2013; Van Tricht et al., 2016; Steger et al., 2017; Izeboud et al., 2020; Dunmire et al., 2020). These studies have shown that SNOWPACK is capable of capturing important processes in the ice sheet firn layer, namely accumulation in windy environments, surface meltwater production, and subsequent liquid water retention in the firn. However, these studies have not implemented a polar snow accumulation scheme that allows for initial accumulation of low-density (<250 kg m−3) snow and subsequent drifting-snow compaction. Additionally, no previous study has evaluated SNOWPACK-simulated near-surface firn density across the entire AIS.
Our new drifting-snow compaction routine combines an existing alpine new snow density parameterization with a polar snow compaction routine. In particular, we impose the key physical restraint that drifting snow is required for near-surface compaction in addition to overburden stress compaction. This mechanism has previously been proposed in the literature (Brun et al., 1997) and recently confirmed in both laboratory experiments (Sommer et al., 2017) and field observations on the AIS (Sommer et al., 2018). In our scheme, new snowfall is assigned a typically low (30–150 kg m−3) density ρnew, Eq. (1), according to the default SNOWPACK alpine new snow density parameterization, which is a multiple linear regression derived from observations in the Swiss Alps (Lehning et al., 2002a) and varies as a function of 2 m air temperature T2 m (∘C), snow surface temperature Ts (∘C), relative humidity RH (0–1), and 10 m wind speed U10 m (m s−1).
Densification then occurs via two distinct processes, (a) densification due to overburden stress and (b) densification due to drifting-snow compaction. Densification due to overburden stress is calculated nearly identically as described in Steger et al. (2017), who adapted SNOWPACK for use in the percolation zone of the Greenland Ice Sheet by tuning the viscosity parameters including the snow activation energy Qs and critical exponent β. Here, we find that the parameter tuning proposed by Steger et al. (2017) leads to significantly overestimated densities (bias >50 kg m−3) in the dry snow zone of Antarctica. Therefore we revert to original SNOWPACK viscosity parameters by setting Qs and β to 67 000 J mol−1 and 0.7, respectively. The second mechanism driving densification, i.e., drifting-snow compaction, occurs when the friction velocity u* (m s−1) exceeds the snow threshold friction velocity u*th (m s−1), the minimum friction velocity at which surface snow grains are mobilized by the wind (Fig. 1). In our implementation of SNOWPACK, u* is estimated by scaling hourly averaged 10 m wind speeds from the MERRA-2 atmospheric reanalysis (Sect. 2.2) using a logarithmic wind profile and stability corrections (Michlmayr et al., 2008) with a roughness length, z0, of 2 mm. Note that although 2 mm is approximately an order of magnitude larger than typically observed values over the AIS (e.g., Vignon et al., 2017), even larger values have been observed in sastrugi-dominated environments (Amory et al., 2017) where drifting-snow erosion and deposition are common. Meanwhile, u*th, Eq. (2), is calculated as a function of snow microstructural properties internally determined by SNOWPACK, including snow grain sphericity SP (0–1), radius rg (m), bond radius rb (m), and coordination number N3 (Lehning and Fierz, 2008).
In Eq. (2), ρi is the density of ice (917 kg m−3), ρa is the density of air (1.1 kg m−3), g is the gravitational acceleration (9.8 m s−2), σ is a reference shear strength set to 300 Pa, and constants A and B are set to 0.02 and 0.0015, respectively. When u* exceeds u*th, a saltation mass transport rate Q () is calculated following Lehning and Fierz (2008) and then scaled to a saltation mass flux Φ (), Eq. (3), by dividing Q by a characteristic horizontal length scale L.
L can be interpreted as a fetch length and characteristic horizontal length scale over which the originally upwind and now mobilized snow particles, which make up the saltation mass flux Φ, have been eroded from the snow surface. We choose a magnitude for L of 10 m, as this is a typical horizontal length scale of wind erosion features including sastrugi and barchan dunes (Filhol and Sturm, 2015). Given a lack of direct observations, L can effectively be considered a tuning parameter, whose magnitude is inversely proportional to Φ. Note that as suspension of drifting snow is not considered in the saltation model (Lehning and Fierz, 2008), the saltation mass transport rate Q may underestimate the total mass flux in the saltation and suspension layers. However, the scaling of the mass transport rate by the poorly constrained fetch length L to obtain the saltation mass flux Φ could be considered a way to include both suspension and saltation in the simulations.
Following erosion, the drifting-snow mass flux is redeposited at the snow surface with an updated density ρredeposit (kg m−3), Eq. (4), parameterized according to field measurements of surface snow deposited during drifting-snow events (Groot Zwaaftink et al., 2013, Eq. 1). Note that, in contrast to Groot Zwaaftink et al. (2013), who use 100 h average wind speeds, we calculate ρredeposit using hourly mean MERRA-2 10 m wind speeds. We implement this distinction in order to better resolve the temporal evolution of redeposited snow density during ephemeral (i.e., shorter than 100 h) drifting-snow events.
2.2 SNOWPACK atmospheric forcing
At the snow surface, we force SNOWPACK with 1980–2017 MERRA-2 global atmospheric reanalysis (Gelaro et al., 2017) hourly mean 2 m air temperature, relative humidity, 10 m wind speed, incoming shortwave and longwave radiation (ISWR and ILWR), and precipitation rate. At the bottom of the simulated snowpack, we apply the MERRA-2 1980–2017 mean annual surface temperature as a thermodynamic boundary condition. We choose MERRA-2 because it provides a low release latency (approximately 1 month) and publicly available description of the state of the atmosphere, whereas regional climate models are not always regularly updated. This advantage, although not strictly necessary for this study as we focus on a past period (1980–2017), would be advantageous for future applications where timely estimates of snow properties are required, for example rapid interpretation of satellite imagery and altimetry, or determining the status of field assets (e.g., weather stations). Additionally, Medley and Thomas (2019) reported MERRA-2 to have the lowest accumulation bias compared to observations among comparable reanalysis products. Furthermore, Gossart et al. (2019) report generally good agreement between MERRA-2 and observed near-surface climatology, including 2 m air temperature and wind speeds; however MERRA-2 appears to overestimate SMB, with an ice-sheet-wide mean absolute error of 58.5 . According to Gossart et al. (2019), MERRA-2 captures coastal and ice shelf SMB well but generally overestimates SMB in the escarpment zone and at elevations from 500–3000 m.
We evaluate MERRA-2 atmospheric reanalysis as forcing for SNOWPACK by comparing with monthly averaged observations at nine automatic weather stations (AWSs), whose locations are shown in Fig. 2. Note that in contrast to Gossart et al. (2019), our meteorological forcing evaluation relies on AWSs located primarily in Dronning Maud Land and therefore may not be representative of the diverse range of Antarctic surface climates. By evaluating meteorological forcing at monthly timescales, we determine whether there are any consistent biases that can impact simulated firn density and temperature profiles. However, it also smooths out high-frequency discrepancies that may be important when evaluating instantaneous simulated density profiles. The AWSs measure temperature, relative humidity, wind speed and direction, air pressure, and the full radiation balance, i.e., incoming and reflected shortwave radiation, and incoming and outgoing longwave radiation. Data from these stations are presented in Reijmer (2002) and Jakobs et al. (2020) and have been previously used to evaluate remote sensing retrievals (Trusel et al., 2013), ice core paleoclimate records (Medley et al., 2018), and climate models (van Wessem et al., 2018). According to our analysis and consistent with the findings of Lenaerts et al. (2017) and Gossart et al. (2019), MERRA-2 captures observed 2 m air temperature, relative humidity, and wind speed well but significantly underestimates both ISWR and ILWR. We calculated an average MERRA-2 bias across all nine AWSs of −15.1 W m−2 (corresponding to 19.4 %) and −16.9 W m−2 for ISWR and ILWR, respectively (Fig. A1). In order to reduce this bias in incoming radiation and thus better capture AWSs observations, we increase MERRA-2 ISWR by 19.4 % and ILWR by 16.9 W m−2. Note that we choose a multiplicative correction for ISWR because a constant increase would be inappropriate when ISWR is low or zero, for example during twilight or polar night. Following bias correction, MERRA-2 ISWR and ILWR biases are reduced to 8.7 and −0.6 W m−2, respectively. Additionally, ISWR root-mean-squared error (RMSE) is reduced from 22.7 to 20.3 W m−2 while ILWR RMSE is reduced from 21.5 to 14.1 W m−2. Note that this bias correction only impacts ISWR and ILWR forcing, not 2 m air temperature, relative humidity, 10 m wind speed, and precipitation rate. Additionally, for the rest of this study, all simulations are driven by bias-corrected ISWR and ILWR, unless explicitly stated otherwise.
2.3 SNOWPACK model initialization
In our scheme, new snow layers are added on top of the snow column when precipitation is prescribed by the atmospheric forcing, in steps of 2 cm. Layers are initialized with a density given by Eq. (1) when they originate from precipitation. When snow layers are eroded and redeposited, the layers originating from drifting snow are initialized with a density given by Eq. (4). Initial grain size for all newly added layers is 0.2 mm (Groot Zwaaftink et al., 2013). There are two sets of microstructural properties for grain shape (dendricity and sphericity), for high and low wind speed (Groot Zwaaftink et al., 2013). Note that precipitation is treated before assessing snow erosion, such that low-density snow from precipitation can erode immediately when conditions allow. To reduce computational costs, a sophisticated snow layer merging scheme merges layers with very low ice content due to sublimation or melt and layers with similar properties (density, water content, grain size, and grain shape parameters). The criteria for layer merging are relaxed with depth, to allow for more aggressive layer merging. At 10 m depth, typical layer spacing is around 10–20 cm. Near the surface, layers can be split to maintain a vertical resolution of a few centimeters in order to numerically represent steep temperature gradients.
In order to ensure a realistic representation of snow and firn properties throughout the entire near surface, we complete a SNOWPACK model spinup such that simulated snow depth is 10 m at all sites before comparison with observations or other SNOWPACK simulations. We choose 10 m in order to resolve seasonal variability in snow and firn characteristics as well as energy exchange with the atmosphere. For spinup, we mimic the method presented in Ligtenberg et al. (2011) by repeating the 1980–2017 model period until initial simulated snow depth on 1 January 1980 is at least 10 m. Once spinup is complete, we perform one final 1980–2017 model simulation, which we use for the analysis.
2.4 Borehole 10 m temperature as mean annual surface temperature proxy
To test MERRA-2 and SNOWPACK's ability to capture the surface energy balance (SEB) across a range of AIS surface climates, we compare 1980–2017 mean MERRA-2 surface temperature and SNOWPACK snow surface temperature with 10 m depth temperatures from 55 boreholes whose locations are shown in Fig. 2. In the absence of significant surface meltwater percolation, 10 m depth temperature equilibrates with mean annual surface temperature and can therefore be used as a proxy for surface temperature and by extension SEB in the absence of direct observations (van den Broeke, 2008; Lenaerts et al., 2012; van Wessem et al., 2014).
2.5 IMAU-FDM model
To aid in the evaluation of SNOWPACK-modeled near-surface density, we also compare with the widely used Institute for Marine and Atmospheric research Utrecht firn densification model (IMAU-FDM v1.1) (Ligtenberg et al., 2011, 2018; Kuipers Munneke et al., 2015). The IMAU-FDM is a semi-empirical firn densification model designed to represent snow and firn cover processes including densification, meltwater refreezing and percolation, and surface height change. Gridded IMAU-FDM density profiles are available at 27 km horizontal, 4 cm vertical, and 30 d temporal resolution with atmospheric forcing provided by the regional climate model RACMO 2.3p2 (van Wessem et al., 2018). In contrast to SNOWPACK, which relies on an overburden stress compaction scheme, IMAU-FDM uses a calibrated semi-empirical dry snow densification scheme based on Arthern et al. (2010), which describes densification as a function of density as well as annual average accumulation and temperature. In further contrast to SNOWPACK, the IMAU-FDM parameterizes new snow density as a function of annual average, rather than hourly, meteorology and currently includes no post-deposition mechanism to increase surface snow density due to drifting-snow processes.
2.6 GSFC-FDM model
In addition to IMAU-FDM we also compare SNOWPACK to the NASA Goddard Space Flight Center firn densification model (GSFC-FDMv1) which provides simulated firn properties over the past 40 years (1980–2019) for both the Greenland and Antarctic ice sheets (Medley et al., 2020). GSFC-FDM uses the Community Firn Model, a modular, open-source framework for Lagrangian modeling of several firn and firn-air-related processes within a single column (Stevens et al., 2020). The GSFC-FDM simulations are forced by an enhanced-resolution hybridized MERRA-2 that was developed by exploiting a 15-year, 12.5 km resolution offline MERRA-2 reanalysis. The hybridized MERRA-2 forcing retains the spatial gradients in the high-resolution reanalysis while maintaining the temporal variations from the original MERRA-2 variables (see Medley et al., 2020, for complete details). The dry snow and firn compaction model, based on Arthern et al. (2010), was calibrated to observed depth–density profiles from both Greenland and Antarctica. A simple initial density scheme was implemented based on mean annual MERRA-2 climate, which provides a spatially variable initial density that does not, in contrast to SNOWPACK, vary in time or vary due to drifting-snow processes.
2.7 SNOWPACK, IMAU-FDM, and GSFC-FDM comparison with density observations
We evaluate skill for all three firn models in representing surface and near-surface snow and firn density, defined here as the average density between depths of 0–1 and 0–10 m, respectively, by comparing with community-sourced and publicly available density profiles from the Surface Mass Balance and Snow on Sea Ice Working Group (SUMup) dataset (Albert, 2007; Medley et al., 2013; Montgomery et al., 2018). We first identified all available Antarctic SUMup density observations in the near surface and then retrieved spatially and temporally consistent SNOWPACK, IMAU-FDM, and GSFC-FDM model output. For all models, we retrieve the simulated density profile whose time step is closest to that of the observed profile. SNOWPACK, IMAU-FDM, and GSFC-FDM report simulated density profiles every 1, 30, and 5 d respectively. This classification yielded 122 unique observed profiles (Fig. 2) that are located primarily on the grounded ice sheet, where surface melt is limited (<50 ), absent, or very rare (Trusel et al., 2013). Observations and models report different vertical resolution density; therefore we compute the mean and standard deviation of all 122 density profiles at ten 1 m thick vertical levels, beginning at 0–1 m and ending with 9–10 m depths.
3.1 Surface energy balance
The large variability in observed 10 m depth borehole temperatures, ranging from −57.0 to −14.4 ∘C, is well captured by MERRA-2, non-bias-corrected SNOWPACK, and bias-corrected SNOWPACK, indicating proper representation of the average SEB (Fig. 3). In particular, the R-squared values and slope of linear regressions are 0.96 and 1.00 for MERRA-2, 0.97 and 0.98 for non-bias-corrected SNOWPACK, and 0.97 and 0.95 for bias-corrected SNOWPACK. MERRA-2 overestimates Ts, with an average bias of 0.52 ∘C, while non-bias-corrected SNOWPACK underestimates Ts with an average bias of −0.99 ∘C. Meanwhile, bias-corrected SNOWPACK yields excellent agreement, with an average bias of 0.06 ∘C. MERRA-2 shows the largest RMSE, 2.38 ∘C, while the non-bias-corrected and bias-corrected versions of SNOWPACK display an RMSE of 2.16 and 1.94 ∘C, respectively.
Since the MERRA-2 bias in ISWR and ILWR is determined using only nine AWSs located primarily in Dronning Maud Land (Sect. 2.2), we were initially concerned with the bias' spatial representativeness. However, following bias correction, the statistically significant reduction in both RMSE and bias (p<0.01) magnitude when compared to 10 m depth temperatures indicates a clear improvement in SNOWPACK's representation of Antarctic SEB, including locations outside of Dronning Maud Land.
3.2 Evaluation of MERRA-2 95th percentile hourly wind speeds
Accurate model representation of drifting-snow frequency and intensity, as well as the density of drifting-snow accumulation, relies on a realistic representation of the strongest wind events. Although Gossart et al. (2019) report good agreement between annual mean observed and MERRA-2-simulated wind speeds, this finding does not necessarily apply to the strongest wind events, when drifting snow is most significant. Therefore, to better understand the quality of MERRA-2 atmospheric forcing during strong drifting-snow events, we compare observed and MERRA-2-simulated 95th percentile hourly 10 m wind speeds at 80 AWSs across the AIS (Sanz Rodrigo et al., 2013). MERRA-2 demonstrates relatively good model performance (R2=0.64, bias = 0.05 m s−1, RMSE = 2.02 m s−1, Fig. 4), and despite occasional (5 out of 80 AWSs) considerable differences (magnitude >4 m s−1), we see no systematic errors. Furthermore, MERRA-2 shows no appreciable spatial pattern in bias, for example in the ice sheet interior or coast. Thus, we conclude that MERRA-2 demonstrates considerable skill in representing the 5 % strongest hourly wind speeds and can therefore be used to reliably estimate the friction velocity u* and saltation mass flux Φ, Eq. (3).
3.3 SNOWPACK density profiles' sensitivity to atmospheric forcing uncertainty
Although we have performed an evaluation of MERRA-2 SEB, and introduced a bias correction for ISWR and ILWR, uncertainties in bias-corrected MERRA-2 atmospheric forcing likely still exist and can impact simulated density profiles. To understand the effect of these uncertainties on SNOWPACK-simulated density, we perform an ensemble of SNOWPACK simulations at the South Pole and the West Antarctic Ice Sheet (WAIS) divide, where we perturb MERRA-2 prescribed 10 m wind speed, 2 m air temperature, and precipitation. We choose the South Pole (90∘ S, 0∘ E) and WAIS divide (79.5∘ S, 112∘ W) because these are well-known points of interest and represent distinct climatic and accumulation regimes with mean annual surface temperatures of −52.4 and −29.4 ∘C and annual snow accumulation of 56 and 207 , respectively. Because MERRA-2 exhibits mean absolute errors of 2.4 m s−1 and 3.1 ∘C for annual average 10 m wind speeds and near-surface temperature (Gossart et al., 2019) and typical relative accumulation errors of 20 % (Medley and Thomas, 2019), we independently increase and decrease MERRA-2 10 m wind speed, 2 m air temperature, and precipitation at the South Pole and WAIS by 2.4 m s−1, 3.1 ∘C, and 20 %, respectively.
SNOWPACK-simulated density sensitivities to uncertainties in 10 m wind speed are considerably larger than those of 2 m air temperature and precipitation and range from −46.6 kg m−3 at 0–1 m in the South Pole −2.4 m s−1 simulation to 58.5 kg m−3 at 2–3 m in the WAIS +2.4 m s−1 simulation (Fig. 5). Meanwhile, across our 2 m air temperature and precipitation ensemble, differences in simulated density are generally less than 5 % of non-perturbed density in 75 out of 80 cases and never exceed 10 %. Because these simulated density differences are typically small compared to absolute density, we conclude that uncertainties arising due to 2 m air temperature and precipitation alone are smaller in magnitude than uncertainties arising from firn densification model choice (Sects. 3.5–3.7). On the other hand, density differences in the 10 m wind speed experiments are larger, particularly from 0–3 m depth, and exceed 5 % of non-perturbed density in 24 out of 40 cases. Thus, a realistic representation of wind speed is crucial for simulating realistic density profiles. However, in the context of our study, simulated density uncertainties arising from uncertainties in MERRA-2 wind speed cannot be easily reduced because, consistent with Gossart et al. (2019), we find no substantial bias in MERRA-2 wind speed compared to observations (Sect. 3.2). We must therefore acknowledge that density variations due to uncertainty in wind speed represent the largest source of uncertainty with regard to SNOWPACK-simulated near-surface density and in fact exceed uncertainties arising from firn densification model choice.
3.4 Effect of new SNOWPACK drifting-snow compaction routine on simulated density profiles
In earlier studies, SNOWPACK described enhanced surface compaction under the influence of wind by increasing the strain rate of snow in the top 7 cm (Groot Zwaaftink et al., 2013). For simulations in Antarctica, a higher strain rate was proposed when compared to simulations of seasonal snow cover in alpine terrain. Alternatively, the new drifting-snow compaction scheme we have introduced in this study does not modify the strain rate. Instead, surface compaction by wind is only introduced when the friction velocity is sufficient to first erode and then subsequently redeposit snow with a higher density. To demonstrate the influence of our new drifting-snow compaction scheme on simulated near-surface density profiles, we have plotted 30 December 1997 observed and SNOWPACK-simulated density profiles at Kohnen Station in Dronning Maud Land, East Antarctica (75∘ S, 0∘ E, 2891 m, Fig. 6). For SNOWPACK, we have included three sets of model physics: (1) this study, denoted “Redeposit”; (2) the wind-enhanced surface compaction scheme using the strain rate proposed by Groot Zwaaftink et al. (2013), denoted “Enhanced Compaction”; and (3) the default alpine SNOWPACK snow physics, which includes only a modest wind-enhanced surface compaction using the strain rate (Bartelt and Lehning, 2002; Lehning et al., 2002a, b), denoted “Default”.
From our analysis, it is immediately clear that the default SNOWPACK snow physics significantly underestimate observed surface density (>150 kg m−3), suggesting that the wind effect described in the new snow density parameterization (Eq. 1) and the increased strain rate in this variant are insufficient for drifting-snow-dominated polar environments. However, in the case of Default snow physics, this underestimation of density decreases with depth, which can be explained by the reduced viscosity of relatively lower-density snow and therefore more rapid densification due to overburden stress. For the Enhanced Compaction simulation, we see similar behavior; however modeled surface density errors are reduced compared to the Default simulation. Compared to Redeposit, the Enhanced Compaction simulation significantly underestimates near-surface density. This demonstrates that the enhanced wind compaction mechanism via the strain rate is not sufficient to capture observations. Instead, describing compaction of surface snow due to wind using wind-driven erosion and subsequent redeposition at a higher density (Redeposit), which resembles the experimentally determined mechanism (Sommer et al., 2017), adequately captures observed near-surface density.
3.5 Surface snow density
A comparison between SNOWPACK-, IMAU-FDM-, and GSFC-FDM-simulated surface snow density, defined as the top meter, with 79 unique observations is shown in Fig. 7. Observed densities range from 272–507 kg m−3, with a mean of 362 kg m−3 and standard deviation of 39 kg m−3. Since it is known that meteorological conditions including annual accumulation and temperature influence Antarctic snow and firn density (Herron and Langway, 1980), we tested this hypothesis. We find a modest relationship between MERRA-2 1980–2017 mean annual SMB and observed surface snow density (p<0.01, R2=0.23) as well as a significant but weak correlation between elevation and observed surface snow density (p<0.01, R2=0.16), likely due to the relationship between elevation and surface climate. Note that we find no significant correlation between MERRA-2 1980–2017 mean wind speed and observed surface density (p=0.14, R2=0.03) but do in fact find a significant albeit weak relationship between 1980–2017 maximum wind speed and surface density (p<0.01, R2=0.09). Because drifting-snow compaction is known to partially control snow density on daily to hourly timescales (Sommer et al., 2018), the lack of a significant relationship between mean annual wind speed and surface snow density combined with the significant relationship between maximum wind speed and surface density indicates the importance of resolving drifting-snow compaction with high-temporal-resolution (daily to hourly) meteorological forcing as opposed to annual means or climatology.
SNOWPACK (linear fit slope = 0.51, R2=0.20), IMAU-FDM (linear fit slope = 0.20, R2=0.19), and GSFC-FDM (linear fit slope = 0.22, R2=0.36) all modestly capture observed surface snow density variability. Both SNOWPACK and IMAU-FDM underestimate surface snow density with an average bias of −8.2 and −20.4 kg m−3 and RMSE of 45.3 and 40.7 kg m−3, respectively. Meanwhile GSFC-FDM, on average overestimates surface snow density, with a bias of 20.4 kg m−3 and RMSE of 38.5 kg m−3. For all models, we identify no clear relationship between geographic location and model bias. However, we find a significant but weak negative relationship between observed density and modeled surface density bias for SNOWPACK (p<0.01, R2=0.19) as well as a moderately strong negative relationship for IMAU-FDM (p<0.01, R2=0.80) and strong negative relationship for GSFC-FDM (p<0.01, R2=0.87).
According to our analysis, SNOWPACK better captures the range in observed surface density when compared to IMAU-FDM, as evidenced by a lower-magnitude bias, higher R2, and linear fit slope closer to unity, but the typical error is larger, as expressed by a slightly larger RMSE (Table 1). Likewise, when compared to GSFC-FDM, SNOWPACK exhibits a lower surface density bias magnitude and has a linear slope closer to unity, while it shows a larger RMSE and lower R2. Additionally, we calculate a p value of 0.06 for a two-sided t test in which the null hypothesis states that SNOWPACK and IMAU-FDM have identical average biases. This information combined with SNOWPACK's larger RMSE compared to IMAU-FDM and GSFC-FDM and smaller R2 compared to GSFC-FDM leads us to conclude that neither model is superior, and instead that all three models perform comparably with regard to surface density. Note that all three models perform particularly poorly when observed surface density exceeds 400 kg m−3 (SNOWPACK: kg m−3, RMSE = 65.8 kg m−3; IMAU-FDM: kg m−3, RMSE = 74.7 kg m−3; GSFC-FDM: kg m−3, RMSE = 35.6 kg m−3). The origin of this poor performance at high observed surface densities is still unknown, but we can come up with at least three potential explanations. First, we speculate that high surface densities are found in areas with locally steep topography. However, we find no significant relationship between surface slope derived from a 1 km horizontal resolution digital elevation model (Helm et al., 2014) and modeled surface density bias (not shown), so this mechanism is an unlikely candidate to explain the bias. Second, this model degradation at high observed surface densities could potentially be explained by an underestimation of new snow density and/or the frequency and intensity of simulated drifting-snow compaction due to the presence of local meteorological phenomena not captured by MERRA-2 or RACMO2. Lastly, we cannot rule out the possibility of larger errors in the observational data for densities above 400 kg m−3. For example, some surface density observations, particularly those from deep firn and ice cores, may not be representative of an undisturbed snow surface and could therefore report an artificially high surface density. Moreover, surface snow samples taken from cores are often compressed by the drill and can sometimes break into multiple pieces, therefore confounding density measurements.
3.6 Near-surface snow and firn densification
In a comparison with 122 observed density profiles, SNOWPACK exhibits a lower bias compared to IMAU-FDM for the entire near surface and a lower bias compared to GSFC FDM from 0–7 m depth (Fig. 8). Observed mean densities range from 362 kg m−3 at depth 0–1 m to 510 kg m−3 at 9–10 m. Meanwhile, SNOWPACK mean densities range from 354 kg m−3 at depth 0–1 m to 489 kg m−3 at 9–10 m. SNOWPACK underestimates observed density with biases varying from a minimum of −0.6 kg m−3 at depth 2–3 m to a maximum of −25.3 kg m−3 at 8–9 m. Note that the SNOWPACK mean density bias from 0–7 m is typically small (<10 kg m−3) and has approximately the same magnitude as density uncertainties that arise from uncertainties in atmospheric forcing (Sect. 3.3). The IMAU-FDM likewise underestimates near-surface density with biases ranging from −20.4 kg m−3 at depth 0–1 m to −40.1 kg m−3 at 8–9 m. Meanwhile, GSFC-FDM overestimates near-surface density with biases ranging from 8.5 kg m−3 at depth 8–9 m to 23.7 kg m−3 at 2–3 m. Furthermore, SNOWPACK correctly predicts observed variability in mean density, as shown by similar standard deviations between SNOWPACK and observations (Fig. 8a). Alternatively, IMAU-FDM and GSFC-FDM both underestimate observed mean density variability at the surface but converge towards the observed variability with increasing depth. Note that 95 % confidence intervals on the SNOWPACK mean bias contain zero in the top 7 m (Fig. 8); thus we conclude that SNOWPACK is consistent with observations at these depths. However, the IMAU-FDM and GSFC-FDM mean bias 95 % confidence intervals never contain zero and are therefore not consistent with observations. Despite these contrasting conclusions, SNOWPACK's mean bias confidence intervals occasionally overlap with those of IMAU-FDM and GSFC-FDM (e.g., 0–1 and 8–10 m in the case of IMAU-FDM) and therefore should not be considered uniformly statistically indistinguishable.
To test for the potential effect of compensating biases on our analysis of near-surface densification, we partition the 122 observed density profiles into 35 high- and 87 low-SMB categories by applying a mean annual SMB threshold of 200 according to MERRA-2 (Fig. 9). We choose 200 because it roughly approximates the area-weighted mean annual SMB over the grounded AIS (172.8 according to Agosta et al., 2019). Again, for both high- and low-SMB sites, we find that SNOWPACK, when compared to IMAU-FDM, shows lower absolute density biases throughout the entire near-surface firn column, from the surface down to 10 m depth. Compared to GSFC-FDM, SNOWPACK exhibits a smaller absolute near-surface density bias only from 0–8 and 9–10 m at low-accumulation sites. For high-SMB sites, SNOWPACK mean biases range from −55.9 kg m−3 at 8–9 m to −3.9 kg m−3 at 0–1 m, while for low-SMB sites, mean biases are generally reduced in magnitude and range from −14.3 kg m−3 at 9–10 m to 8.3 kg m−3 at 5–6 m. Given SNOWPACK's mean bias reduction, when compared to IMAU-FDM, and comparable performance relative to GSFC-FDM, we have demonstrated our physics-based modeling approach is capable of reliably capturing Antarctic near-surface snow and firn density. Consistent with our analysis of all profiles in Fig. 8, SNOWPACK, as measured by the mean bias 95 % confidence intervals, is generally consistent with observations and statistically distinguishable from IMAU-FDM and GSFC-FDM at low-accumulation sites. However, at high-accumulation sites, SNOWPACK exhibits significantly worse performance as indicated by a strongly negative bias and confidence intervals that do not contain zero, particularly below 6 m depth.
3.7 Simulated near-surface firn densification at sites not included in the calibration of IMAU-FDM and GSFC-FDM.
Semi-empirical firn densification models, including IMAU-FDM and GSFC-FDM, are calibrated against observed density profiles in order to improve model agreement with observations. However, because near-surface density observations are sparse, not evenly distributed in space, and typically collected in summer, semi-empirical models may be biased towards climate regimes which are well sampled by observations. Alternatively, SNOWPACK, and other physics-based models, simulates density profiles which are not calibrated against observations and could therefore potentially outperform semi-empirical models in climate regimes not well sampled in semi-empirical model calibrations. To test this hypothesis, we examine the 69 of 122 observed density profiles which were not included in the IMAU-FDM and GSFC-FDM calibrations, hereafter referred to as the 69 independent sites. We then compare the mean near-surface density biases of SNOWPACK, IMAU-FDM, and GSFC-FDM at these 69 independent sites against the same statistics calculated for all 122 sites (Sect. 3.6).
Figure 10 shows simulated density profiles along with observations and biases at the 69 sites not used for calibration. The SNOWPACK mean density bias for the 69 independent sites is 1.1 kg m−3, down from −9.7 kg m−3 for all 122 sites (Table 2). IMAU-FDM also exhibits a smaller absolute bias, decreasing in magnitude from −32.5 to −20.4 kg m−3 for the 122 and 69 sites, respectively. However, the SNOWPACK model demonstrates a smaller absolute bias than IMAU-FDM, irrespective of including the calibration sites. For the GSFC-FDM model, the mean density bias increases throughout the near surface from 15.5 to 22.3 kg m−3 for the 122 and 69 sites, respectively, indicating a degraded performance when calibration sites are excluded. These results show that physics-based firn models do not need specific calibration for the application and could yield an advantage over calibrated firn models, where the application for non-calibrated sites is not guaranteed to yield good performance.
3.8 SNOWPACK and semi-empirical models' hierarchical complexity
Although all three models are presented on similar footing, it is important to contextualize their performance by noting the different original purposes for developing SNOWPACK, IMAU-FDM, and GSFC-FDM as well as their different levels of complexity in representing physical processes. The IMAU-FDM and GSFC-FDM are relatively simplified semi-empirical firn models designed to represent spatial and temporal evolution of firn density and surface height. On the other hand, SNOWPACK is a higher-order-complexity physics-based land-surface snow model originally intended for simulating snow microstructural properties relevant for avalanche formation in seasonally snow-covered terrain. IMAU-FDM and GSFC-FDM are usually used to study the entire ice sheet firn column, which can be greater than 100 m thick, while SNOWPACK is typically used to simulate seasonal snowpacks a few meters thick. Despite the much thicker simulated firn column in IMAU-FDM and GSFC-FDM (40–120 m) when compared to our imposed restriction for SNOWPACK to the near surface (i.e., depths 0–10 m), SNOWPACK is considerably more computationally expensive to run. It is therefore important to acknowledge the inherent tradeoff between process representation and cost, particularly for simulations which require long spinup or involve long time frames, e.g., paleoclimate applications or future climate scenarios.
Because SNOWPACK exhibits a lower mean snow and firn density bias throughout most of the near surface compared to IMAU-FDM and GSFC-FDM, it is necessary to describe particular model distinctions which could explain their different behavior. First, SNOWPACK and IMAU-FDM rely on different meteorological forcing (MERRA-2 and RACMO2 2.3p2, respectively), which somewhat confounds their direct comparison. Next, in our implementation of SNOWPACK, new snowfall density is determined by hourly mean MERRA-2 weather conditions while in IMAU-FDM and GSFC-FDM, new snow density is determined by annual average meteorologic variables including accumulation rate, 10 m wind speed, and surface temperature. SNOWPACK therefore calculates a variable new snow density driven by both seasonal and synoptic-scale variability in surface meteorology, while IMAU-FDM and GSFC-FDM do not resolve this process. Additionally, SNOWPACK allows for drifting-snow compaction of previously fallen snow (Fig. 1), while IMAU-FDM and GSFC-FDM only account for the impact of wind on density by including this processes in the new snow density parameterization. This difference in process representation of new snow density and drifting-snow compaction is reflected by SNOWPACK's larger variability in predicted surface density (281–479 kg m−3) compared to IMAU-FDM (328–429 kg m−3) and GSFC-FDM (364–436 kg m−3). By allowing for initial low-density new snow accumulation and subsequent drifting-snow compaction, SNOWPACK, more in line with observations (272–507 kg m−3), predicts a wider range of surface snow densities than IMAU-FDM and GSFC-FDM (Fig. 7a, c, and e). Finally, SNOWPACK's higher-temporal-resolution density output (daily) compared to IMAU-FDM (30 d) and GSFC-FDM (5 d) can resolve processes relevant for surface snow density which act on timescales of less than 30 and 5 d, respectively (e.g., snowfall and drifting-snow compaction).
3.9 SNOWPACK-simulated surface density variability
SNOWPACK predicts a wide range of simulated surface densities (mean of top meter), ranging from 230–684 kg m−3 with a mean of 370 kg m−3 and standard deviation of 64 kg m−3 across 186 simulations (Fig. 11a). Furthermore, SNOWPACK exhibits large seasonal surface density variability (mean magnitude = 53 kg m−3), when measured as the maximum difference between summer and winter surface density found in the period 1980–2017 (Fig. 11b). Seasonal surface density variability is primarily driven by seasonal cycles in temperature, accumulation rate, and compaction rate. However, superimposed onto these processes at even shorter timescales (e.g., hourly to weekly) are individual accumulation events and snow microstructural evolution (Fig. 11c). Because satellite altimetry relies on instantaneous measurements of surface height, rather than temporal means, firn models used to reliably convert changes in volume into mass must capture high-frequency variability in firn density and surface height.
Accurate snow and firn density models are required to reliably determine ice sheet mass balance using satellite altimetry. However, firn densification models currently used in altimetry studies do not resolve observed temporal increases in surface snow density under the influence of wind. In this study, we demonstrate improved simulation of Antarctic near-surface (depths ≤10 m) snow and firn density upon implementation of a new drifting-snow compaction routine into SNOWPACK, a detailed, physics-based land-surface snow model. In particular, we show that when compared to two other semi-empirical firn densification models (IMAU-FDM and GSFC-FDM), SNOWPACK exhibits a lower mean snow and firn density bias throughout most of the near surface at 122 observed density profiles across the Antarctic ice sheet. Despite this improvement, SNOWPACK generally underestimates density, with a mean surface density bias of −8.2 kg m−3 and mean near-surface biases ranging from −0.6 kg m−3 at 2–3 m depth to −25.3 kg m−3 at 8–9 m depth. Meanwhile, IMAU-FDM exhibits a mean surface density bias of −20.4 kg m−3 and mean near-surface biases between −20.4 kg m−3 at depths 0–1 m and −40.1 kg m−3 at depths of 8–9 m while GSFC-FDM shows a mean surface density bias of 20.4 kg m−3 and mean near-surface biases from 8.5 kg m−3 at depths 8–9 m to 23.7 kg m−3 at 2–3 m. SNOWPACK exhibits a lower density bias than IMAU-FDM throughout the entire near surface; however the GSFC-FDM shows a lower-magnitude bias than SNOWPACK below 7 m depth and throughout the entire near surface at high-accumulation sites. Note that our analysis is limited to the top 10 m in order to focus on the most dynamic and variable part of the Antarctic firn layer. Because SNOWPACK is a physics-based model, extensive model tuning in order to fit observations is not required. By analyzing the simulations, excluding the sites used for calibration of the semi-empirical models, we found SNOWPACK to also have the lowest absolute bias. IMAU-FDM showed a lower bias when excluding the calibration sites, whereas GSFC-FDM showed larger bias. Because SNOWPACK outperforms the IMAU-FDM and GSFC-FDM at sites not included in calibration, SNOWPACK, compared to semi-empirical models, could possibly simulate firn density more accurately in regions without extensive observations or under future climate scenarios, where firn properties are expected to diverge from their current state.
All software and code required to replicate this study are available open-access at https://doi.org/10.5281/zenodo.4560829 (Keenan, 2021a). SNOWPACK model source code can be accessed at https://github.com/snowpack-model/snowpack (last access: 26 February 2021), while the precise version used in this study can be accessed at https://doi.org/10.5281/zenodo.3891846 (SNOWPACK team, 2020). MERRA-2 atmospheric reanalysis is available at https://gmao.gsfc.nasa.gov/reanalysis/MERRA-2/ (last access: 24 February 2021) and can be retrieved and processed using our workflow available at https://doi.org/10.5281/zenodo.4560825 (Keenan, 2021b). SUMup density data are available at https://doi.org/10.18739/A26D5PB2S (Koenig and Montgomery, 2019). Borehole 10 m depth temperature data are available from Michiel van den Broeke (m.r.vandenBroeke@uu.nl). AWS data are available from Carleen Reijmer (firstname.lastname@example.org). IMAU-FDM data are available from Peter Kuipers Munneke (email@example.com). GSFC-FDM data are available from Brooke Medley (firstname.lastname@example.org).
All authors contributed to preparing this paper. EK carried out SNOWPACK simulations, performed the analysis, and produced the figures. NW implemented the new drifting-snow compaction routine into SNOWPACK and contributed to the experimental design and analysis. MD and JTML contributed to the experimental design and analysis. BM contributed to the experimental design and analysis and provided GSFC-FDM output. PKM provided IMAU-FDM output. CR provided AWS data.
The authors declare that they have no conflict of interest.
Eric Keenan, Nander Wever, Jan T. M. Lenaerts, and Brooke Medley acknowledge support from the National Aeronautics and Space Administration (NASA), grant 80NSSC18K0201 (ROSES-2016: studies with ICESat-2 and CryoSat-2). Eric Keenan, Nander Wever, and Jan T. M. Lenaerts are also supported by BELSPO Research Contract, grant BR/165/A2:Mass2Ant. Peter Kuipers Munneke is funded by the Netherlands Earth System Science Centre (NESSC). Carleen Reijmer acknowledges the support of the Dutch Polar program of the Dutch Research Council NPP-NWO. This work utilized the RMACC Summit supercomputer, which is supported by the National Science Foundation (awards ACI-1532235 and ACI-1532236), the University of Colorado Boulder, and Colorado State University. The Summit supercomputer is a joint effort of the University of Colorado Boulder and Colorado State University. Data storage is supported by the University of Colorado Boulder “PetaLibrary”. Thank you to Xavier Fettweis, Charles Amory, and the anonymous reviewer for providing helpful and insightful comments which helped to improve the paper considerably. The authors thank Lynn Montgomery for their useful insight into the SUMup dataset and constructive comments on this paper.
This research has been supported by the National Aeronautics and Space Administration (grant no. 80NSSC18K0201) and the Belgian Federal Science Policy Office (grant no. BR/165/A2:Mass2Ant).
This paper was edited by Xavier Fettweis and reviewed by Charles Amory and one anonymous referee.
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