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Thermal-rheological structure of lithosphere beneath the northern flank of Tarim Basin, western China: Implications for geodynamics

机译:塔里木盆地北翼下方岩石圈的热流变结构:对地球动力学的启示

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Based on the data of geo-temperature and thermophysical parameters of rocks in the Kuqa Depression and the Tabei Uplift, northern flank of the Tarim Basin, in terms of the analytical solution of 1-D heat transfer equation, the thermal structure of the lithosphere under this region is determined. Our results show that the average surface heat flow of the northern flank of the Tarim Basin is 45 mW/m~2, and the mantle heat flow is between 20 and 23 mW/m~2; the temperature at crust-mantle boundary (Moho) ranges from 514℃ to 603℃ and the thermal lithosphere where the heat conduction dominates is 138—182 km thick. Furthermore, in combination with the P wave velocity structure resulting from the deep seismic sounding profile across this region and rheological modeling, we have studied the local composition of the lithosphere and its rheological profile, as well as the strength distribution. We find that the rheological stratification of the lithosphere in this region is apparent. The lowermost of the lower crust is ductile; however, the uppermost of the mantle and the upper and middle parts of the crust are both brittle layers, which is typically the so-called sandwich-like structure. Lithospheric strength is also characterized by the lateral variation, and the uplift region is stronger than the depression region. The lithospheric strength of the northern flank of the Tarim Basin decreases gradually from south to north; the Kuqa Depression has the lowest strength and the south of the Tabei Uplift is strongest. The total lithospheric strength of this region is 4.77 x 10~(12)—5.03 x 10~(13) N/m under extension, and 6.5X10~(12)—9.4X10~(13) N/m under compression. The lithospheric brittle-ductile transition depth is between 20 km and 33 km. In conclusion, the lithosphere of the northern flank of the Tarim Basin is relatively cold with higher strength, so it behaves rigidly and deforms as a whole, which is also supported by the seismic activity in this region. This rigidity of the Tarim lithosphere makes it little deform interior, but only into flexure under the sedimentation and tectonic loading associated with the rapid uplift of the Tianshan at its northern margin during the Indian-Eurasian continental collision following the Late Eocene. Finally, the influences of factors, such as heat flow, temperature, crustal thickness, and especially basin sediment thickness, on the lithospheric strength are discussed here.
机译:基于塔里木盆地北侧库车De陷和塔北隆起的岩石的地温和热物理参数数据,以一维热传导方程的解析解,岩石圈的热结构确定该区域。我们的研究结果表明,塔里木盆地北翼的平均表面热流为45 mW / m〜2,地幔热流在20至23 mW / m〜2之间。地幔-边界温度(Moho)范围为514℃至603℃,导热占主导地位的热岩石圈厚度为138-182 km。此外,结合该区域深部地震测深剖面和流变学模型产生的P波速度结构,我们研究了岩石圈的局部组成及其流变学特征以及强度分布。我们发现该区域岩石圈的流变分层很明显。下地壳的最下部是延性的。然而,地幔的最上层和地壳的上部和中间部分都是脆性层,通常是所谓的三明治状结构。岩石圈强度的特征还在于侧向变化,隆起区比凹陷区强。塔里木盆地北翼的岩石圈强度从南到北逐渐减小;库车De陷强度最低,塔北隆起南部最强。该区域的岩石圈总强度在拉伸下为4.77 x 10〜(12)—5.03 x 10〜(13)N / m,压缩后为6.5X10〜(12)-9.4X10〜(13)N / m。岩石圈脆性-韧性过渡深度在20 km至33 km之间。总之,塔里木盆地北翼的岩石圈相对较冷,强度较高,因此其表现为刚性且整体变形,这也受到该地区地震活动的支持。塔里木岩石圈的这种刚性使其内部几乎不变形,而仅在沉积和构造载荷作用下才发生弯曲,这与晚始新世后印度-欧亚大陆碰撞期间天山北缘的快速隆升有关。最后,本文讨论了热流,温度,地壳厚度,尤其是盆地沉积物厚度等因素对岩石圈强度的影响。

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