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Power Scaling and Seasonal Changes of Floe Areas in the Arctic East Siberian Sea

机译:东西伯利亚海北极浮冰区功率变化与季节变化

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摘要

The cumulative number versus floe area distribution of seasonal sea floes from six satellite images of the Arctic Ocean during the summer breakup and melting is fit by two scale-invariant power law scaling regimes for floe areas ranging from 30 to 28,400,000 m(2). Scaling exponents, beta, for larger floe areas range from -0.6 to -1.0 with an average of -0.8. Scaling exponents, beta, for smaller floe areas range from -0.3 to -0.6 with an average of -0.5. The inflection point between the two scaling regimes ranges from 283 x 10(2) to 4850 x 10(2) m(2) and generally moves from larger to smaller floe areas through the summer melting season. The stability of the power scaling results is demonstrated for two of the images by dividing each in half and analyzing each half separately, with the result that the scaling exponents and the size of the inflection points are nearly the same for each half as for the whole image. We propose that the two scaling regimes and the inflection between them are established during the initial breakup of sea ice solely by the process of fracture. The distributions of floe size regimes retain their scaling exponents as the floe pack evolves from larger to smaller floe areas from the initial breakup through the summer season, due to grinding, crushing, fracture, and melting. The scaling exponents for floe area distribution are in the same range as those reported in previous studies of Arctic floes and for the single scaling exponents found for crushed and ground geologic materials including streambed gravel, lunar debris, and artificially crushed quartz. The single scaling exponent found for fault gouge falls below the range for floes possibly because the fracturing and grinding process in fault gouge takes place under high confining pressure. A probabilistic model of fragmentation is proposed that generates a single power law scaling distribution of fragment size.
机译:从北冰洋的六张卫星图像中可以看出夏季破裂和融化期间季节性浮冰的累积数量与浮冰面积分布,由两个尺度不变的幂律尺度制度拟合,浮冰面积范围为30至28,400,000 m(2)。较大浮冰区域的标度指数 beta 范围为 -0.6 至 -1.0,平均值为 -0.8。较小浮冰区域的标度指数 beta 范围为 -0.3 至 -0.6,平均值为 -0.5。两种结垢机制之间的拐点范围为283 x 10(2)至4850 x 10(2) m(2),并且通常在整个夏季融化季节从较大到较小的浮冰区域移动。通过将两张图像分成两半并分别分析每一半,证明了功率缩放结果的稳定性,结果是每一半的缩放指数和拐点的大小与整个图像几乎相同。我们提出,两种缩放机制以及它们之间的拐点是在海冰最初破裂期间仅通过断裂过程建立的。由于研磨、压碎、断裂和熔化,浮冰包从最初的破裂到夏季从较大的浮冰区域演变为较小的浮冰区域,浮冰大小范围的分布保持其缩放指数。浮冰面积分布的标度指数与先前北极浮冰研究报告的标度指数以及碎屑和地面地质材料(包括河床砾石、月球碎片和人工压碎石英)的单一标度指数的标度指数相同。发现的断层凿削的单个标度指数低于浮冰的范围,这可能是因为断层凿削中的压裂和磨削过程是在高围压下进行的。提出了一种碎片化的概率模型,该模型生成了碎片大小的单一幂律标度分布。

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