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A seismological determination of the temperature gradient in D″ beneath the western Pacific

机译:西太平洋下方D“温度梯度的地震测定

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The temperature gradient of the thermal boundary layer in the D″ region is one of the basic properties of the mantle that remains difficult to evaluate. We characterize this quantity for a region in the western Pacific using gradient-sensitive seismological probes. First, both the amplitudes and travel times of the diffracted P and S phases (P diff, S diff) were analyzed to constrain the regional-scale vertical gradients of V P and V S . Acceptable models were grid-searched using synthetic waveforms for trial models that employ only one velocity gradient zone in D″. The V S models were searched over the parameter space of the thickness (H) and the gradient. Solutions show negative deviation from Preliminary Reference Earth Model and a trade-off between gradient and H from ?0.00088 s?1, for190 km to ?0.00049 s?1, for 240 km with a typical error of ±0.00015 s?1. Rather than pinning down the best solution, we consider two sets of solutions for V S with H = 190 and 240 km. For these two H values, the gradients of V P were determined solely by amplitude to be -0.00032 s-1 for 190 km and 0.00015 s?1 for 240 km, shrouded in relatively large errors of 0.0002–0.0003 s?1. We derive the temperature gradient from the resolved velocity gradients using the seismological-thermodynamic equation of Doornbos et al. (1986) and arrive at 9.0 ± 5.8 K/km and 5.7 ± 4.1 K/km over 190 and 240 km, respectively. The difference in gradient between these two models is statistically significant at the 99% confidence level, and the odds that the apparent steeper gradient is caused by squeezing energy of diffracted waves into a thinner zone can also be rejected with high confidence. The combination of the two models is thus consistent with a nonlinear temperature profile that steepens toward the core-mantle boundary. Both models detect the superadiabatic gradient of temperature in the lowermost mantle.
机译:D“区域中的热边界层的温度梯度是仍然难以评估的地幔的基本性质之一。我们使用梯度敏感的地震探针对西太平洋地区的一个地区表示这一数量。首先,分析衍射P和S阶段(P Diff,S差异)的幅度和行进时间来限制V P和V S的区域级垂直梯度。可接受的模型是使用合成波形搜索的网格,用于试验模型,该模型仅在d“中仅使用一个速度梯度区域。在厚度(H)和梯度的参数空间上搜索V S模型。解决方案显示初步参考地球模型的负偏差和梯度和H之间的权衡,从?0.00088 s?1,持续190公里到0.00049 s?1,典型误差为±0.00015 s?1。而不是钉住最佳解决方案,我们考虑两组与H = 190和240公里的V S解决方案。对于这两个H值,V p的梯度仅通过幅度确定为-0.00032 s-1,对于190km和0.00015 s?1持续240 km,以0.0002-0.0003 s的相对大的误差覆盖。我们使用Doornbos等人的地震 - 热力学方程从分辨的速度梯度衍生温度梯度。 (1986)分别到达9.0±5.8 k / km,分别超过190和240公里的5.7±4.1 k / km。这两个模型之间的梯度之间的差异在99%的置信水平上具有统计学意义,并且表观陡峭梯度是通过挤出衍射波的能量引起的衍射波进入更薄的区域的差异也可以被高置信度。因此,两种模型的组合与非线性温度曲线朝向芯罩边界倾斜的非线性温度曲线一致。两种型号都检测到最下面的披风中温度的超级水准梯度。

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