Importance of soil thermal regime in terrestrial ecosystem carbon dynamics in the circumpolar north
Introduction
Permafrost is an important control on vegetation and soil carbon (C) dynamics by affecting hydrological and soil thermal conditions in northern high-latitude ecosystems (Wania et al., 2009a, Schaphoff et al., 2013), which account for a large portion of the global C stocks (Hugelius et al., 2014). Recent climate warming has caused significant thawing of the near-surface permafrost across the circumpolar region (Romanovsky et al., 2015), including Alaska (Jorgenson et al., 2006, Osterkamp, 2007), Canada (Camill, 2005), and Russia (Streletskiy et al., 2015). Projected warming over the 21st century is expected to greatly reduce the areal extent of permafrost and seasonally frozen ground (Lawrence et al., 2012). If permafrost thaws, a fraction of soil organic C (SOC) in previously frozen layers will decompose and be released as CO2 and CH4 (Olefeldt et al., 2012, Hayes et al., 2014, Johnston et al., 2014, Walter-Anthony et al., 2014). Furthermore, organic matter decomposition rates in unfrozen soils are sensitive to soil temperatures, which vary non-linearly across the soil column. Therefore, careful consideration of soil thermal regime changes (i.e. soil temperatures across the soil column from surface to deep soil layers) is important when simulating the potential future C loss from soils.
In addition to soil C, vegetation C pools are also sensitive to changes in soil thermal dynamics by permafrost thaw and rates of associated biogeochemical processes (Euskirchen et al., 2006). Field studies have indicated that permafrost thaw increases aboveground net primary production via increased nutrient availability (e.g., Schuur et al., 2007). While not explicitly testing the effects of thaw, other model studies have indicated a net C gain in circumpolar ecosystems because increased vegetation productivity more than compensated belowground C losses under a warming climate (Hartley et al., 2012, Koven, 2013). However, this net C gain may be optimistic as the effects of water stress and disturbances (e.g. insect infestations, wildfires) on permafrost-region biomass are not adequately incorporated in current models (Abbott et al., 2016). Thus, large uncertainties currently exist regarding the magnitude and timing of this permafrost-C feedback to the climate system (Schuur et al., 2013), due in part to the complexity of ecosystem C processes in areas of degrading permafrost (e.g., thermokarst, thermal erosion) and their heterogeneity across regions.
To date, a number of studies have used process-based land surface models to estimate permafrost-C feedbacks under projected thaw scenarios (Koven et al., 2011; Harden et al., 2012, MacDougall et al., 2012, Schneider von Deimling et al., 2012). Soil thermal dynamics within these models vary in their complexity, from calculations of the cumulative active layer thickness distribution (e.g., Harden et al., 2012) to more sophisticated parameterizations of soil physics (e.g., MacDougall et al., 2012). Thaw dynamics are typically considered in a top-down one-dimensional manner, and heat transfer via conduction is the primary mode considered. However, the importance of soil water in non-conductive heat transfer (e.g., latent heat exchange, convection) has long been recognized as an important control on soil thermal dynamics (e.g., Romanovsky and Osterkamp, 2000). In this regard, our recent modeling studies that incorporate interactions between heat and water transport (Jiang et al., 2012a) have shown improvements in simulating the soil thermal regime changes in both tundra and boreal forest ecosystems in the northern high latitudes (Jiang et al., 2015).
To provide a better quantification of the ecosystem C budget in northern high latitudes and how this budget may change in the future, we use the Lund-Potsdam-Jena Dynamic Global Vegetation Model (LPJ-DGVM, Sitch et al., 2003, Gerten et al., 2004) coupled with a sophisticated soil thermal model (STM) by Jiang et al. (2012a) to conduct a set of simulations for both historical and future periods. The standard version of LPJ-DGVM has been widely used to simulate the global C budget and its response to climate change (e.g., Sitch et al., 2008, Jiang et al., 2012b). However, the model has used simplified soil temperature parameterizations for high-latitude regions (Sitch et al., 2003). Although later studies by Wania et al., 2009a, Wania et al., 2009b have taken steps to improve soil thermal and hydrologic parameterizations for permafrost conditions in northern peatlands, soil temperature and water dynamics are still modeled separately. As a consequence, the modeled active layer thickness exhibits poor agreement with observations (Wania et al., 2009b). Moreover, the effects of the vertical soil C distribution on decomposition have not been considered. In an extended LPJ, which includes managed land (LPJmL), Schaphoff et al. (2013) have recently coupled the interactions of soil water and heat transport, and considered vertically differentiated soil C stocks based on an organized soil C dataset in Jobbagy and Jackson (2000). However, the discrete vertical differentiation of the soil temperature profile in LPJmL is relatively coarse and the vertical distribution of SOC down to 3 m is highly concentrated in the uppermost soil layers (e.g., 0–20 cm) and does not consider long-term SOC accumulation in deep soil layers (Hugelius et al., 2014).
In this study, we integrate STM into LPJ to improve simulations of soil temperature dynamics from the ground surface to a depth of three meters, and the consequent impact on soil organic C stabilization and release across the northern permafrost region. Because the newly coupled version of the model, LPJ-STM, considers a fine vertical differentiation of soil temperatures, interactions of soil water with heat transport, and a vertical distribution of SOC with more C in deeper soil layers, we expect LPJ-STM to provide a more accurate quantification of the C budget for historical periods and to improve projections of carbon dynamics under future scenarios. To examine if LPJ-STM improved estimates of soil temperatures and associated carbon dynamics over LPJ, we compare estimates of both models to site observations of soil temperatures and net ecosystem production (NEP). In addition, simulated atmospheric carbon dioxide concentrations determined by using the model NEP estimates combined with an atmospheric transport model are compared to atmospheric flask measurements. To examine how improvements in simulated soil thermal regime affect the estimates of the contemporary C budget of northern high latitude ecosystems and its projection into the 21st century, we compare estimates of net primary production (NPP), heterotrophic respiration (RH), and net ecosystem production (NEP) as well as vegetation and soil C stocks between LPJ and LPJ-STM.
Section snippets
Model description
The LPJ model simulates large-scale vegetation structure and land-atmosphere C and water fluxes in a modular framework (Sitch et al., 2003, Gerten et al., 2004). In the standard LPJ soil model, two soil layers have a fixed depth (i.e. 0.5 m and 1.0 m). The vertical distribution of soil C within these two soil layers is not explicitly considered. For permafrost thermal dynamics, LPJ calculates soil temperature at a depth of 25 cm in a very simplistic way based on the surface air temperature
Model performance
The LPJ-STM is able to well simulate the soil temperature profile for high latitude sites (Fig. 2). When compared with measured soil water content at 25 cm, LPJ-STM shows clearly better agreement than LPJ (Fig. 3). The LPJ-STM soil temperature estimates have lower root mean square error (RMSE) values than the LPJ estimates when compared against field measurements (Fig. 4). By replacing the LPJ soil temperature model with the STM, the seasonal temperature fluctuations are dampened with a much
Discussion
In this study, we examine how a more detailed representation of soil thermal dynamics, soil hydrology, and soil C dynamics influences estimates of C fluxes and pools of ecosystems in the circumpolar north. The detailed representation of these ecosystem processes in LPJ-STM estimates higher NPP, but lower RH for current circumpolar ecosystems than the more aggregated representation of these processes in LPJ. As a result, more C (0.8 to 1.0 Pg C yr− 1) is estimated to be sequestered in these
Conclusions
This study examines the importance of changes in the soil thermal regime on determining the C budget in the circumpolar north. With explicitly modeled temperatures at different depths, the LPJ-STM model estimates larger soil organic C stocks in the circumpolar north, which agrees well with empirical global data sources. Our model simulations indicate that, although most biogeochemical processes of C storage and decomposition take place in top soil layers (i.e. top 30 cm), deep layers also
Acknowledgment
We thank Jessica Drysdale for comments on earlier drafts of this manuscript. This research is supported by funded projects to Q. Z. National Science Foundation (NSF-1028291 and NSF- 0919331), the NSF Carbon and Water in the Earth Program (NSF-0630319), the NASA Land Use and Land Cover Change program (NASA- NNX09AI26G), and Department of Energy (DE-FG02-08ER64599). The computing is supported by Rosen Center of high performance computing at Purdue.
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