Modeling Heat Transfer through Permafrost Soil Subjected to Seasonal Freeze-Thaw
The present paper proposes an iterative implicit numerical method for simulating the thaw depth of permafrost soil. For this purpose, the enthalpy-porosity model was used for the phase change process, and the finite difference scheme FTCS (Forward Time Centered Space) was used for discretization. An...
Published in: | Land |
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Main Authors: | , , |
Format: | Text |
Language: | English |
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Multidisciplinary Digital Publishing Institute
2022
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Subjects: | |
Online Access: | https://doi.org/10.3390/land11101770 |
_version_ | 1821681151565103104 |
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author | Alain Lubini Tshumuka Abdelkader Krimi Musandji Fuamba |
author_facet | Alain Lubini Tshumuka Abdelkader Krimi Musandji Fuamba |
author_sort | Alain Lubini Tshumuka |
collection | MDPI Open Access Publishing |
container_issue | 10 |
container_start_page | 1770 |
container_title | Land |
container_volume | 11 |
description | The present paper proposes an iterative implicit numerical method for simulating the thaw depth of permafrost soil. For this purpose, the enthalpy-porosity model was used for the phase change process, and the finite difference scheme FTCS (Forward Time Centered Space) was used for discretization. An artificial mushy zone was maintained with the same thickness by keeping the regularization parameter proportional to the temperature gradient. In doing so, we made the scheme more stable and convergence occurred faster. The model accuracy was validated by comparing the numerical results with the analytical Stefan solution and with the results of a derived numerical model, based on an explicit scheme. The model performance was also tested against observation data collected on four different landscapes with different soil profiles and located on a basin underlain by continuous permafrost. It was found that the proposed model matched noticeably well the analytical solution for a volumetric liquid fraction (phi) equal to 0.5 regardless of the grid resolution. Furthermore, compared with the observation data, the model reproduced the annual maximum thaw depth with an absolute error lying between 0.7 and 7.7%. In addition, the designed algorithm allowed the model to converge after a maximum of eight iterations, reducing the computational time by around 75% compared to the explicit model. The results were so encouraging that the model can be included in a hydrological modeling of permafrost watersheds or cold regions in general. |
format | Text |
genre | permafrost |
genre_facet | permafrost |
id | ftmdpi:oai:mdpi.com:/2073-445X/11/10/1770/ |
institution | Open Polar |
language | English |
op_collection_id | ftmdpi |
op_coverage | agris |
op_doi | https://doi.org/10.3390/land11101770 |
op_relation | https://dx.doi.org/10.3390/land11101770 |
op_rights | https://creativecommons.org/licenses/by/4.0/ |
op_source | Land; Volume 11; Issue 10; Pages: 1770 |
publishDate | 2022 |
publisher | Multidisciplinary Digital Publishing Institute |
record_format | openpolar |
spelling | ftmdpi:oai:mdpi.com:/2073-445X/11/10/1770/ 2025-01-17T00:14:30+00:00 Modeling Heat Transfer through Permafrost Soil Subjected to Seasonal Freeze-Thaw Alain Lubini Tshumuka Abdelkader Krimi Musandji Fuamba agris 2022-10-12 application/pdf https://doi.org/10.3390/land11101770 EN eng Multidisciplinary Digital Publishing Institute https://dx.doi.org/10.3390/land11101770 https://creativecommons.org/licenses/by/4.0/ Land; Volume 11; Issue 10; Pages: 1770 Stefan problem permafrost active layer finite difference iterative method thaw depth Text 2022 ftmdpi https://doi.org/10.3390/land11101770 2023-08-01T06:50:55Z The present paper proposes an iterative implicit numerical method for simulating the thaw depth of permafrost soil. For this purpose, the enthalpy-porosity model was used for the phase change process, and the finite difference scheme FTCS (Forward Time Centered Space) was used for discretization. An artificial mushy zone was maintained with the same thickness by keeping the regularization parameter proportional to the temperature gradient. In doing so, we made the scheme more stable and convergence occurred faster. The model accuracy was validated by comparing the numerical results with the analytical Stefan solution and with the results of a derived numerical model, based on an explicit scheme. The model performance was also tested against observation data collected on four different landscapes with different soil profiles and located on a basin underlain by continuous permafrost. It was found that the proposed model matched noticeably well the analytical solution for a volumetric liquid fraction (phi) equal to 0.5 regardless of the grid resolution. Furthermore, compared with the observation data, the model reproduced the annual maximum thaw depth with an absolute error lying between 0.7 and 7.7%. In addition, the designed algorithm allowed the model to converge after a maximum of eight iterations, reducing the computational time by around 75% compared to the explicit model. The results were so encouraging that the model can be included in a hydrological modeling of permafrost watersheds or cold regions in general. Text permafrost MDPI Open Access Publishing Land 11 10 1770 |
spellingShingle | Stefan problem permafrost active layer finite difference iterative method thaw depth Alain Lubini Tshumuka Abdelkader Krimi Musandji Fuamba Modeling Heat Transfer through Permafrost Soil Subjected to Seasonal Freeze-Thaw |
title | Modeling Heat Transfer through Permafrost Soil Subjected to Seasonal Freeze-Thaw |
title_full | Modeling Heat Transfer through Permafrost Soil Subjected to Seasonal Freeze-Thaw |
title_fullStr | Modeling Heat Transfer through Permafrost Soil Subjected to Seasonal Freeze-Thaw |
title_full_unstemmed | Modeling Heat Transfer through Permafrost Soil Subjected to Seasonal Freeze-Thaw |
title_short | Modeling Heat Transfer through Permafrost Soil Subjected to Seasonal Freeze-Thaw |
title_sort | modeling heat transfer through permafrost soil subjected to seasonal freeze-thaw |
topic | Stefan problem permafrost active layer finite difference iterative method thaw depth |
topic_facet | Stefan problem permafrost active layer finite difference iterative method thaw depth |
url | https://doi.org/10.3390/land11101770 |