翻訳と辞書
Words near each other
・ Iceland at the 1912 Summer Olympics
・ Iceland at the 1936 Summer Olympics
・ Iceland at the 1948 Summer Olympics
・ Iceland at the 1948 Winter Olympics
・ Iceland at the 1952 Summer Olympics
・ Iceland at the 1952 Winter Olympics
・ Iceland at the 1956 Summer Olympics
・ Iceland at the 1956 Winter Olympics
・ Iceland at the 1960 Summer Olympics
・ Iceland at the 1960 Winter Olympics
・ Iceland at the 1964 Summer Olympics
・ Iceland at the 1964 Winter Olympics
・ Iceland at the 1968 Summer Olympics
・ Ice-nine (disambiguation)
・ Ice-Pick Lodge
Ice-sheet dynamics
・ Ice-sheet model
・ Ice-T
・ Ice-T discography
・ Ice-T's Rap School
・ Ice-type model
・ Ice-water separation
・ Ice2sea
・ Iceage
・ Iceal Hambleton
・ Iceane
・ ICEARRAY
・ Icebar Orlando
・ Iceberg
・ Iceberg (Banks novel)


Dictionary Lists
翻訳と辞書 辞書検索 [ 開発暫定版 ]
スポンサード リンク

Ice-sheet dynamics : ウィキペディア英語版
Ice-sheet dynamics

Ice sheet dynamics describe the motion within large bodies of ice, such those currently on Greenland and Antarctica. Ice motion is dominated by the movement of glaciers, whose gravity-driven activity is controlled by two main variable factors: the temperature and strength of their bases. A number of processes alter these two factors, resulting in cyclic surges of activity interspersed with longer periods of inactivity, on both hourly and centennial time scales. Ice-sheet dynamics are of interest in modelling future sea level rise.

==Flow dynamics==

The main cause of flow within glaciers can be attributed to an increase in the surface slope, brought upon by an imbalance between the amounts of accumulation vs. ablation. This imbalance increases the shear stress on a glacier until it begins to flow. The flow velocity and deformation will increase as the equilibrium line between these two processes is approached, but are also affected by the slope of the ice, the ice thickness and temperature.〔Easterbrook, Don J., Surface Processes and Landforms, 2nd Edition, Prentice-Hall Inc., 1999〕
When the amount of strain (deformation) is proportional to the stress being applied, ice will act as an elastic solid. Ice will not flow until it has reached a thickness of 30 meters (98 ft), but after 50 meters (164 ft), small amounts of stress can result in a large amount of strain, causing the deformation to become a plastic flow rather than elastic. At this point the glacier will begin to deform under its own weight and flow across the landscape. According to the Glen–Nye Flow law, the relationship between stress and strain, and thus the rate of internal flow, can be modeled as follows:〔〔
:
\Sigma = k \tau^n,\,

where:
:\Sigma\, = shear strain (flow) rate
:\tau\, = stress
:n\, = a constant between 2–4 (typically 3 for most glaciers) that increases with lower temperature
:k\, = a temperature-dependent constant
The lowest velocities are near the base of the glacier and along valley sides where friction acts against flow, causing the most deformation. Velocity increases inward toward the center line and upward, as the amount of deformation decreases. The highest flow velocities are found at the surface, representing the sum of the velocities of all the layers below.〔〔
Glaciers may also move by basal sliding, where the base of the glacier is lubricated by meltwater, allowing the glacier to slide over the terrain on which it sits. Meltwater may be produced by pressure-induced melting, friction or geothermal heat. The more variable the amount of melting at surface of the glacier, the faster the ice will flow.
The top 50 meters of the glacier form the fracture zone, where ice moves as a single unit. Cracks form as the glacier moves over irregular terrain, which may penetrate the full depth of the fracture zone.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Ice-sheet dynamics」の詳細全文を読む



スポンサード リンク
翻訳と辞書 : 翻訳のためのインターネットリソース

Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.