上、下地幔流动的地球动力学结构及其热传递

A. Kirdyashkin, Yu. Nepogodina
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引用次数: 0

摘要

研究对象是地幔的两层地球动力学模型,包括上地幔和下地幔。研究的主题是下地幔顶部和底部的流动方向。它是在已知的上地幔地球动力学结构、已知的上地幔顶部流动方向和洋中脊地区存在抬升流的情况下确定的。研究的目的是揭示上、下地幔大型自由流动单元之间相互作用的特征。在上-下地幔边界,上-下地幔流动的相互作用可能有两种类型:单向流动(共流)或反向流动(逆流)。在自由对流条件下,670 km边界的水平大尺度流是水平温度梯度的结果。流动界面的换热发生在自由对流条件下,该边界处的换热强度由垂直温度梯度决定。本文分析了670 km边界上地幔和下地幔共流和逆流的换热问题。估计下地幔热边界层在670 km边界附近的平均流动温度下降,并在该边界处存在逆流。给出了大陆和海洋下地幔的密度和温度差异,提供了大陆表面水平高于洋底水平等于7公里的过剩。将估计的特征温差与海洋和大陆下地幔热流数据进行比较,可以得出在670 km边界处存在上地幔和下地幔流共流的结论。分析了670 km边界共流对大尺度地幔流结构的影响。针对海洋下地幔与大陆下地幔相互作用的两种不同情况,提出了上、下地幔的大尺度流动
本文章由计算机程序翻译,如有差异,请以英文原文为准。
GEODYNAMIC STRUCTURE OF UPPER AMD LOWER MANTLE FLOWS AND HEAT TRANSFER BETWEEN THEM
The object of the study is a two-layer geodynamic model of the Earth's mantle, including the upper and lower mantle. The subject of the study is the direction of flow at the top and bottom of the lower mantle. It is determined under the known geodynamic structure in the upper mantle, the known direction of the flow at its roof and in the presence of a lifting flow in the mid-ocean ridge area. The aim of the study is to reveal the character of interaction between the upper and lower mantle large-scale free flowing cells. At the upper-lower mantle boundary, two types of interaction of upper- and lower-mantle flows are possible: either unidirectional flows - cocurrent flow, or oppositely directed - counterflow. Horizontal large-scale currents at the 670 km boundary are a consequence of the horizontal temperature gradient under conditions of free convection. Heat transfer from the flow interface occurs under conditions of free convection, and the intensity of heat transfer at this boundary is determined by the vertical temperature gradient. The analysis of heat transfer in upper-mantle and lower-mantle flows at the 670 km boundary with cocurrent flow and counterflow is presented. The decrease in the average flow temperature for the lower mantle thermal boundary layer near the 670 km boundary with a counterflow at this boundary is estimated. The density and temperature differences in the mantle under the continent and the ocean, providing an excess of the surface level of the continent above the level of the ocean floor, equal to 7 km, are presented. Comparison of the estimated characteristic temperature difference with data on heat flows in the mantle under the ocean and the continent leads to the conclusion that there is a cocurrent flow of upper mantle and lower mantle flows at the 670 km boundary. The influence of the cocurrent flow at the 670 km boundary on the structure of large-scale mantle flows is analyzed. For two different situations of interaction of upper mantle flows under the ocean with the mantle under the continent, large-scale flows in the upper and lower mantle are presented
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