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Laboratory study of initial sea-ice growth: properties of grease ice and nilas

机译:海冰初始生长的实验室研究:油脂冰和尼拉斯的性质

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We investigate initial sea-ice growth in an ice-tank study by freezing an NaCl solution of about 29 g kgsupa??1/sup in three different setups grease ice grew in experiments with waves and in experiments with a current and wind, while nilas formed in a quiescent experimental setup. In this paper we focus on the differences in bulk salinity, solid fraction and thickness between these two ice types. brbr The bulk salinity of the grease-ice layer in our experiments remained almost constant until the ice began to consolidate. In contrast, the initial bulk-salinity evolution of the nilas is well described by a linear decrease of about 2.1 g kgsupa??1/sup hsupa??1/sup independent of air temperature. This rapid decrease can be qualitatively understood by considering a Rayleigh number that became maximum while the nilas was still less than 1 cm thick. brbr Comparing three different methods to measure solid fraction in grease ice based on (a) salt conservation, (b) mass conservation and (c) energy conservation, we find that the method based on salt conservation does not give reliable results if the salinity of the interstitial water is approximated as being equal to the salinity of the underlying water. Instead the increase in salinity of the interstitial water during grease-ice formation must be taken into account. In our experiments, the solid fraction of grease ice was relatively constant with values of 0.25, whereas it increased to values as high as 0.50 as soon as the grease ice consolidated at its surface. In contrast, the solid fraction of the nilas increased continuously in the first hours of ice formation and reached an average value of 0.55 after 4.5 h. brbr The spatially averaged ice thickness was twice as large in the first 24 h of ice formation in the setup with a current and wind compared to the other two setups, since the wind kept parts of the water surface ice free and therefore allowed for a higher heat loss from the water. The development of the ice thickness can be reproduced well with simple, one dimensional models that only require air temperature or ice surface temperature as input.
机译:在冰罐研究中,我们通过在三种不同的设置中冷冻约29 g kg a ?? 1 的NaCl溶液来研究海冰的初始生长,这三种不同的设置是在波浪实验和在波浪实验中生长的油脂冰气流和风,而尼拉斯则在静止的实验装置中形成。在本文中,我们着眼于这两种冰类型的总盐度,固体分数和厚度的差异。 在我们的实验中,油脂冰层的总体盐度几乎保持恒定,直到冰开始凝固。相比之下,尼罗河的初始盐度变化可以通过与空气无关的线性下降约2.1 g kg a ?? 1 h a ?? 1 很好地描述温度。通过考虑在尼拉斯的厚度仍小于1厘米时最大的瑞利数,可以定性地理解这种快速下降。 比较基于(a)节省盐,(b)质量节省和(c)能量节省的三种测量油脂冰中固体含量的方法,我们发现基于盐保存的方法不能提供可靠的结果如果间隙水的盐度近似等于下层水的盐度,则结果为。取而代之的是,必须考虑到油脂冰形成过程中间隙水盐度的增加。在我们的实验中,油脂冰的固含量相对恒定,值为0.25,而一旦油脂冰在其表面固结,其固含量便增加到高达0.50的值。相反,在冰层形成的最初几个小时中,尼拉斯的固体成分不断增加,并在4.5小时后达到平均值0.55。 与其他两个设置相比,在使用电流和风的设置中,在使用电流和风的设置中,在形成冰的最初24小时中,空间平均冰厚度是其他两个设置的两倍,因为风使水面的部分冰块保持自由状态,并且因此,允许从水中产生更高的热量损失。只需输入空气温度或冰面温度即可用简单的一维模型很好地再现冰厚度的变化。

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