2021
DOI: 10.1080/11956860.2021.1949819
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Numerical modelling of permafrost dynamics under climate change and evolving ground surface conditions: application to an instrumented permafrost mound at Umiujaq, Nunavik (Québec), Canada

Abstract: Numerical simulations were carried out based on a conceptual cryohydrogeological model of a permafrost mound near Umiujaq, Nunavik (Québec), Canada, to assess the impacts of climate warming and changes in surface conditions on permafrost degradation. The 2D model includes groundwater flow, advective-conductive heat transport, phase change and latent heat. Changes in surface conditions which are characteristic of the site were represented empirically in the model by applying spatially-and temporally-variable gr… Show more

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Cited by 6 publications
(12 citation statements)
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References 58 publications
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“…(2020), and Perreault et al. (2021). In the Kuuguluk River model, simulated summer recharge rates across the thawed active layer generally varied between 50 and 200 mm/year, depending on the topography‐constrained heads, the local hydraulic conductivities (Table 2), and depth to the permafrost table.…”
Section: Numerical Modelingmentioning
confidence: 95%
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“…(2020), and Perreault et al. (2021). In the Kuuguluk River model, simulated summer recharge rates across the thawed active layer generally varied between 50 and 200 mm/year, depending on the topography‐constrained heads, the local hydraulic conductivities (Table 2), and depth to the permafrost table.…”
Section: Numerical Modelingmentioning
confidence: 95%
“…The top surface of the model was divided into three boundary classes, based on their thermal and topographic conditions, being (1) riverbed, (2) floodplain, and (3) plateau (Figures 4 and 6b). These three surfaces were each assigned with specified temperature boundary conditions determined as follows: T s k = m k thawing T air for T air 0 ° normalC ${T}_{\mathrm{s}}^{k}={{m}^{k}}_{\text{thawing}}\cdot {T}_{\text{air}}\quad \text{for}\quad {T}_{\text{air}}\ge 0{}^{\circ}\mathrm{C}$ T s k = m k freezing T air for T air < 0 ° C ${T}_{\mathrm{s}}^{k}={{m}^{k}}_{\text{freezing}}\cdot {T}_{\text{air}}\quad \text{for}\quad {T}_{\text{air}}< 0{}^{\circ}\text{C}$ where T s k ${T}_{s}^{k}$ is the assigned surface temperature (°C) for a specific boundary class k , T air is the air temperature (°C), and m k t h a w i n g ${{m}^{k}}_{thawing}$ and m k f r e e z i n g ${{m}^{k}}_{freezing}$ are the so‐called thawing and freezing slopes for each class k , respectively (Perreault et al., 2021). These slopes were determined from simple linear regressions forced to pass through the origin of the graph of mean daily ground surface temperatures as a function of mean daily air temperatures, for air temperatures above and below 0 °C for each specific boundary class (Figure 7 and Table 3).…”
Section: Numerical Modelingmentioning
confidence: 99%
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