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Salinity and solid fraction of frazil and grease ice

机译:弗拉齐尔和油脂冰的盐度和固体分数

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Under turbulent conditions ice growth in sea water often occurs as tiny suspended frazil ice crystals. When the turbulence is insufficient to keep the crystals in suspension, they may accumulate in a surface grease layer of pure ice and sea water. Here we give an account of this grease of low solid fraction and high salinity prior to its freeze-up into a solid ice cover. We provide equations for determining the bulk salinity, Sg, and solid ice volume fraction, φs, of the grease layer by indirect and direct methods, review previous observations, and present new data. For the evolution of the solid fraction of accumulating grease ice we find (I) an early mode 0.08 <φs < 0.12 and (II) a long-term packing limit of 0.28 < φs < 0.31, which for sea water of salinity 34 corresponds to 29.5 < Sg <31.5 and 24 < Sg < 26, respectively. We associate (I) with a mechanical limit related to initial random packing of frazil crystals and (II) with a thermodynamic limit, beyond which the grease will freeze-up into a solid ice cover. By comparing the results with a simple model of random close packing of anisotropic particles, we find that the results are consistent with frazil flocs having an aspect ratio of ~10, much smaller than values assumed in most model applications that include sea-water frazil ice processes.
机译:在动荡的条件下,海水中的冰通常会以微小的悬浮巴西冰晶出现。当湍流不足以使晶体保持悬浮状态时,它们可能会积聚在纯冰和海水的表面油脂层中。在此,我们将介绍这种低固含量和高盐度的润滑脂,然后将其冻结成固态冰盖。我们提供了通过间接和直接方法确定油脂层的总盐度Sg和固体冰体积分数φs的方程式,回顾了先前的观察并提出了新的数据。对于累积的油脂冰的固体成分的演化,我们发现(I)早期模式0.08 <φs<0.12和(II)长期填充极限0.28 <φs<0.31,这对于盐度为34的海水而言29.5

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