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Reappraising elastic thickness variation at oceanic trenches

机译:重新评估海洋海沟的弹性厚度变化

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We reassess the variation of elastic thickness as a function of lithospheric plate age using a global database of bathymetric and free-air gravity profiles which are perpendicular to oceanic trenches. As in many previous studies, our starting point is the well-known floating elastic plate model. In order to remove the influence of short-wavelength features not associated with lithospheric bending, adjacent profiles from 10-Myr bins have been stacked together to construct average profiles with standard deviations. Each average profile was then inverted in a two-stage procedure. First, singular value decomposition was used to determine two unknown flexural parameters, together with a regional slope and offset, for any given elastic thickness. This procedure was repeated for a range of elastic thicknesses. Second, residual misfit was plotted as a function of elastic thickness, and the global minimum was identified. This two-stage procedure makes no prior assumptions about magnitude of the load, size of the bending moment, or whether the elastic plate is broken/continuous. We obtained excellent fits between theory and observation for both bathymetric and gravity profiles from lithosphere with an age range of 0–150 Ma. The shape of the residual misfit function indicates the degree of confidence we have in our elastic thickness estimates. The lower limit of elastic thickness is usually well determined but upper limits are often poorly constrained. Inverse modeling was carried out using a range of profile lengths (250–300, 500, and 700 km). In general, our estimates show no consistent increase of elastic thickness as a function of plate age. This surprising result is consistent with recent reassessments of elastic thickness beneath seamounts and implies either that elastic thickness is independent of plate age or that elastic thickness cannot be measured with sufficient accuracy to reveal such a relationship. Modeling of short free-air gravity profiles (250–300 km) does tentatively suggest that elastic thickness increases linearly from 5 to 10 km between 0 and 20 Ma and from 10 to 15 km between 20 and 150 Ma. This variation roughly matches the depth to the 200°C isotherm which corresponds to an homologous temperature of 0.4 for wet peridotite. Unfortunately, for longer profile lengths, there is no temporal dependence, and elastic thicknesses vary considerably for all plate ages. Bathymetric profile modeling yields similar results although uncertainties are larger.
机译:我们使用垂直于海洋海沟的测深和自由空气重力剖面的全球数据库,重新评估了弹性厚度随岩石圈板龄的变化。与以前的许多研究一样,我们的出发点是众所周知的浮动弹性板模型。为了消除与岩石圈弯曲无关的短波特征的影响,已将10-Myr箱中的相邻轮廓堆叠在一起以构造具有标准偏差的平均轮廓。然后将每个平均轮廓按两步过程进行反转。首先,对于任何给定的弹性厚度,使用奇异值分解来确定两个未知的挠曲参数,以及区域斜率和偏移量。对一定范围的弹性厚度重复该过程。其次,绘制残余失配作为弹性厚度的函数,并确定整体最小值。此两阶段过程没有事先假设载荷的大小,弯矩的大小或弹性板是否断裂/连续。我们获得了岩石年龄范围为0–150 Ma的岩石圈的测深和重力剖面的理论和观测值的极佳拟合。残留失配函数的形状表示我们在弹性厚度估计中的置信度。弹性厚度的下限通常可以很好地确定,但上限通常受限制。使用一系列轮廓长度(250-300、500和700 km)进行逆建模。通常,我们的估计表明,弹性厚度没有随板龄的增加而持续增加。这一令人惊讶的结果与最近对海山下的弹性厚度的重新评估相吻合,并暗示弹性厚度与板龄无关,或者弹性厚度无法以足够的准确度进行测量以揭示这种关系。短距离自由重力剖面(250-300 km)的模型确实表明,弹性厚度在0到20 Ma之间从5到10 km线性增加,在20到150 Ma之间从10到15 km线性增加。这种变化大致对应于200°C等温线的深度,相当于湿橄榄岩的0.4同源温度。不幸的是,对于更长的轮廓长度,没有时间依赖性,并且弹性厚度对于所有板龄都存在很大差异。尽管不确定性较大,但测深剖面模型也可得出相似的结果。

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