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作 者:王绳祖[1]
机构地区:[1]中国地震局地质研究所
出 处:《地震》2002年第3期21-26,共6页Earthquake
基 金:国家自然科学基金资助项目 (4 983 40 0 2 );地震科学联合基金资助课题 (1 990 61 ) ;中国地震局地质研究所论著 2 0 0 1 C0 0 1 0
摘 要:青藏高原构造应力场可按岩石圈下层、多震层和浅层地壳区分为三层。除了震源机制解方法和井孔原地测量方法可分别用于推测多震层和浅层的应力状况外 ,还可根据下层塑性流动网络 ,采用平分网络共轭角的方法估计下层的应力方向。对比岩石圈下层与上层 (多震层 )的构造应力场 ,其结果表明 :由于板块边缘驱动力主要通过下层的网络状流动实现其远程传递 ,故在总体作用趋势上 ,上层的应力方向受控于下层 ;又由于高原靠近喜马拉雅驱动边界 ,部分驱动力直接沿上层传递 ,致使局部地区上。The tectonic stress field in the lithosphere is divided into three layers in the Qinghai Tibet plateau, i.e. the lower lithosphere, the seismogenic layer and the shallow curst. In addition to that stress directions in the upper two layers can be estimated respectively using the focal mechanism solution method or in situ measurement methods, the method bisecting conjugate angles of plastic flow belts is suggested to estimate those in the lower lithosphere in which two families of plastic flow belts intersect each other forming plastic flow network. The comparison between the tectonic stress fields in the lower lithosphere and the seismogenic layer indicates that the stress directions in the upper layer are identical with and controlled by those in the lower layer in general tendency because the long range transmission of plate boundary driving force carried out mainly by the netlike flow in the lower lithosphere, while the considerable differences between the upper and lower layers exist in some local areas near the Himalayan driving boundary, where a part of the driving force is transmitted directly along the upper layer.
关 键 词:青藏高原 岩石圈 塑性流动网络 多震层 构造应力场 震源机制解
分 类 号:P315.2[天文地球—地震学] P313[天文地球—固体地球物理学]
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