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首页> 外文期刊>Bulletin of the Seismological Society of America >An Analysis of P Travel Times for Nevada Test Site Explosions Recorded at Regional Distances
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An Analysis of P Travel Times for Nevada Test Site Explosions Recorded at Regional Distances

机译:区域距离内华达州测试地点爆炸的P行进时间分析

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摘要

The uncertainty in hypocenters and origin times depends on measurement error (the wrong onset is picked) and error in the travel-time tables (and thus earth model) used. The errors in the tables comprise a baseline shift (the average difference over all stations is not zero) and the residuals about the baseline. The residuals are usually referred to as model error. Baseline error only affects origin time and so is usually ignored. It is model error that can result in epicenter error. A priori variances of the model and measurement error are usually used to estimate the uncertainty on epicenters. Few estimates of these variances have been published. Here the two variances are estimated, relative to International Association for Seismology and the Physics of the Earth's Interior (IASPEI) 91, for the P times from explosions at the Nevada Test Site at stations at regional distances. The analysis shows that at a large signal-to-noise ratio (SNR) the variance of the measurement error is 0.01 sec2. The measurement error increases as SNR decreases. Further, the travel times appear to increase as SNR decreases. Model error has a formal variance of up to 1.9 sec2, but this variance is irrelevant to assessing the uncertainty in epicenter estimates. It is systematic bias (if any) caused by model error that contributes to epicenter uncertainty. Without knowing the bias it is only possible to estimate the precision of an epicenter and this depends on the measurement error. The analysis gives estimates of model error for each source-to-station path, and these path effects can be used to correct the travel times to give a revised model. With correction for path effects the estimated uncertainty in the epicenters becomes a measure of the accuracy of a location. The results presented here show that when estimating these effects, care must be taken to ensure that variations in SNR do not bias the estimates.
机译:震源和原点时间的不确定性取决于测量 误差(选择了错误的起点)和所使用的行进时间 表(以及地球模型)中的误差。表 中的误差包括基线偏移(所有测站上的平均差 不为零)和基线的残差。残差 通常称为模型误差。基线错误仅影响 原始时间,因此通常会被忽略。是 可能导致震中误差的模型错误。通常使用模型 的先验方差和测量误差来估计震中的不确定性 。关于这些方差的估计很少被发表。 这里是相对于国际 地震学和地球内部物理学协会 估计的两个方差。 (IASPEI)91,对于位于内华达州测试站点(sup> )的P次爆炸是在区域距离的站点进行的。分析表明,在较大的信噪比(SNR)下, 误差为0.01 sec 2 。测量误差随着SNR的降低而增加。 此外,传播时间似乎随着SNR的降低而增加。 模型误差的形式方差最大为1.9 sec 2 < / sup>,但是此 方差与评估震中 估计中的不确定性无关。由模型误差 引起的系统偏差(如果有)会导致震中不确定性。在不知道 偏差的情况下,只能估计震中 的精度,这取决于测量误差。分析给出了每个源到站点路径的模型误差的 估计,并且 这些路径效应可用于将传播时间校正为 给出修改后的模型。通过对路径影响进行校正,震中估计的不确定性 成为位置精度的度量。此处显示的 结果表明,在估计这些影响时,必须注意 ,以确保SNR的变化不会使估计值偏倚 。 >

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