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Influence of depth, focal mechanism, and tectonic setting on the shape and duration of earthquake source time functions

机译:深度,震源机制和构造背景对震源时间函数的形状和持续时间的影响

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Source time functions of 255 moderate to great earthquakes obtained from inversions of teleseismic body waves by Tanioka and Ruff [1997] and coworkers were compared in a systematic way. They were scaled to remove the effect of moment and to allow the direct comparison and averaging of time function shape as well as duration. Time function durations picked by Tanioka and Ryff[1997] are proportional to the cube root of seismic moment if moments from the Harvard centroid moment tenser catalog are used. The average duration of scaled time functions is shorter and the average shape has a more abrupt termination for deeper events than shallower ones, with a distinct change occurring at similar to 40 km depth. The complexity of the time functions, as quantified by the number of subevents, appears to decrease below similar to 40 km depth. Furthermore, among events shallower than 40 km, the average duration of scaled time functions is shorter, and their average shape has a more abrupt termination (1) for events with strike-slip focal mechanisms compared to thrust events and (2) for the few thrust events associated with an intraplate setting compared to the majority associated with an interplate (subduction) boundary. In each of these cases, events in more tectonically and seismically active settings have a longer duration and a more gradual termination. This can be interpreted in terms of lower stress drops and/or slower rupture velocities at active plate boundaries, suggesting that fault theology depends on slip rate and may evolve as total fault slip accumulates. Furthermore, differences in average time function shape and duration associated with different subduction zones suggest that differences exist in the theology on the plate boundaries at the various subduction zones. [References: 31]
机译:通过系统比较,比较了Tanioka和Ruff [1997]与同事通过远震体波反演获得的255次中至大地震的震源时间函数。他们被缩放以消除力矩的影响,并允许直接比较和平均时间函数形状以及持续时间。如果使用哈佛质心矩张量目录中的矩,那么Tanioka和Ryff [1997]选择的时间函数持续时间与地震矩的立方根成正比。标度时间函数的平均持续时间较短,并且对于较深的事件,平均形状具有比较浅的事件更突然的终止,并且在类似于40 km深度处发生明显变化。时间函数的复杂性(通过子事件的数量来量化)似乎在降低到类似于40 km深度以下。此外,在小于40 km的事件中,比例时间函数的平均持续时间较短,并且它们的平均形状具有更突然的终止(1)对于具有走滑震源机制的事件,与推力事件相比,(2)对于少数事件与板内(俯冲)边界相关的大多数相比,与板内设置相关的推力事件。在每种情况下,在构造和地震活动更活跃的环境中,事件持续时间更长,终止过程也更渐变。这可以用较低的应力降和/或活动板块边界处较慢的破裂速度来解释,这表明断层神学取决于滑动速率,并且可能随着总断层滑动的累积而发展。此外,与不同俯冲带相关的平均时间函数形状和持续时间的差异表明,在不同俯冲带的板块边界上,神学上存在差异。 [参考:31]

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