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用于北极边缘冰区动力学的多尺度糊状层模型。

Multiscale mushy layer model for Arctic marginal ice zone dynamics.

作者信息

Strong Courtenay, Cherkaev Elena, Golden Kenneth M

机构信息

Department of Atmospheric Sciences, University of Utah, Salt Lake City, UT, USA.

Department of Mathematics, University of Utah, Salt Lake City, UT, USA.

出版信息

Sci Rep. 2024 Sep 3;14(1):20436. doi: 10.1038/s41598-024-70868-8.

DOI:10.1038/s41598-024-70868-8
PMID:39227413
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11372187/
Abstract

Perhaps the most dynamic component of the Arctic sea ice cover is the marginal ice zone (MIZ), the transitional region between dense pack ice to the north and open ocean to the south. It widens by a factor of four while seasonally migrating more than 1600 km poleward in the Bering-Chukchi Sea sector, impacting climate dynamics, ecological processes, and human accessibility to the Arctic. Here we showcase a transformative mathematical modeling approach to understanding changes in MIZ location and width, focusing on their seasonal cycles as observed by satellites. We view the MIZ as a liquid-solid phase transition region, or mushy zone, on the scale of the Arctic Ocean. Invoking the physics of phase changes, the MIZ is modeled as a dynamic, multiscale composite material layer; this model captures 96% of the annual cycle of MIZ location and 78% of the annual cycle of MIZ width. Temperature in the upper ocean is described by a nonlinear heat equation with effective parameters obtained using homogenization theory for a random medium of ice floes in a sea water host. Observations and simulations together indicate that MIZ location closely tracks the below-ice 273 K isotherm while the width of the MIZ follows vertical heat flux convergence, but with a three-week lag.

摘要

北极海冰覆盖层中最具动态变化的部分或许当属边缘冰区(MIZ),它是北部密集堆积冰与南部开阔海洋之间的过渡区域。在白令 - 楚科奇海区域,其宽度在季节性向极地方向迁移超过1600公里的过程中会扩大四倍,这对气候动态、生态过程以及人类进入北极的可达性均产生影响。在此,我们展示一种变革性的数学建模方法,用于理解边缘冰区位置和宽度的变化,重点关注卫星观测到的其季节性周期。我们将边缘冰区视为北冰洋尺度上的液 - 固相变区域,即糊状区。借助相变物理学原理,边缘冰区被建模为一个动态的多尺度复合材料层;该模型能够捕捉边缘冰区位置年周期的96%以及边缘冰区宽度年周期的78%。上层海洋的温度由一个非线性热方程描述,其有效参数通过对海水介质中随机分布的浮冰运用均匀化理论得到。观测和模拟共同表明,边缘冰区的位置紧密追踪冰下273K等温线,而边缘冰区的宽度则跟随垂直热通量汇聚,但存在三周的滞后。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95b/11372187/642070603be7/41598_2024_70868_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95b/11372187/632a43075704/41598_2024_70868_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95b/11372187/520cfc1d485a/41598_2024_70868_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95b/11372187/d5389d5f9233/41598_2024_70868_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95b/11372187/642070603be7/41598_2024_70868_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95b/11372187/632a43075704/41598_2024_70868_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95b/11372187/520cfc1d485a/41598_2024_70868_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95b/11372187/d5389d5f9233/41598_2024_70868_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95b/11372187/642070603be7/41598_2024_70868_Fig4_HTML.jpg

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本文引用的文献

1
Marginal ice zone fraction benchmarks sea ice and climate model skill.边缘冰区分数是衡量海冰和气候模型技能的基准。
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