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In-situ aircraft observations of ice concentrations within clouds over the Antarctic Peninsula and Larsen Ice Shelf

机译:飞机实地观测南极半岛和拉森冰架上云中的冰浓度

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In-situ aircraft observations of ice crystal concentrations in Antarctic clouds are presented for the first time. Orographic, layer and wave clouds around the Antarctic Peninsula and Larsen Ice shelf regions were penetrated by the British Antarctic Survey's Twin Otter aircraft, which was equipped with modern cloud physics probes. The clouds studied were mostly in the free troposphere and hence ice crystals blown from the surface are unlikely to have been a major source for the ice phase. The temperature range covered by the experiments was 0 to ?21 °C. The clouds were found to contain supercooled liquid water in most regions and at heterogeneous ice formation temperatures ice crystal concentrations (60 s averages) were often less than 0.07 l−1, although values up to 0.22 l−1 were observed. Estimates of observed aerosol concentrations were used as input into the DeMott et al. (2010) ice nuclei (IN) parameterisation. The observed ice crystal number concentrations were generally in broad agreement with the IN predictions, although on the whole the predicted values were higher. Possible reasons for this are discussed and include the lack of IN observations in this region with which to characterise the parameterisation, and/or problems in relating ice concentration measurements to IN concentrations. Other IN parameterisations significantly overestimated the number of ice particles. Generally ice particle concentrations were much lower than found in clouds in middle latitudes for a given temperature. Higher ice crystal concentrations were sometimes observed at temperatures warmer than ?9 °C, with values of several per litre reached. These were attributable to secondary ice particle production by the Hallett Mossop process. Even in this temperature range it was observed that there were regions with little or no ice that were dominated by supercooled liquid water. It is likely that in some cases this was due to a lack of seeding ice crystals to act as rimers to initiate secondary ice particle production. This highlights the chaotic and spatially inhomogeneous nature of this process and indicates that the accurate representation of it in global models is likely to represent a challenge. However, the contrast between Hallett Mossop zone ice concentrations and the fairly low concentrations of heterogeneously nucleated ice suggests that the Hallet Mossop process has the potential to be very important in remote, pristine regions such as around the Antarctic coast.
机译:首次展示了飞机在南极云中冰晶浓度的现场观测。英国南极测量局的Twin Otter飞机穿透了南极半岛和拉森冰架地区周围的地形云,层云和波云,该飞机配备了现代云物理探测器。研究的云主要在自由对流层中,因此从表面吹出的冰晶不太可能是冰相的主要来源。实验覆盖的温度范围是0到?21°C。发现在大多数地区,云中都含有过冷的液态水,并且在非均质冰形成温度下,冰晶浓度(平均60 s)通常小于0.07 l -1 ,尽管其值高达0.22 l -1 。观测到的气溶胶浓度的估计值被用作DeMott等人的资料。 (2010)冰核(IN)参数化。尽管总体上预测值较高,但观测到的冰晶数浓度通常与IN预测大致吻合。讨论了可能的原因,包括在该区域缺乏IN观测值来表征参数设置,和/或在将冰浓度测量值与IN浓度相关时存在问题。其他IN参数设置大大高估了冰粒的数量。通常,在给定温度下,冰粒浓度远低于在中纬度地区的云层中。 有时在高于9°C的温度下观察到较高的冰晶浓度,达到每升几个值。这些归因于Hallett Mossop工艺产生的二次冰粒。即使在此温度范围内,也观察到有很少或根本没有冰的区域被过冷的液态水所控制。在某些情况下,这可能是由于缺乏晶种的冰晶来充当引发二次冰粒生产的限制因素。这突显了这一过程的混乱和空间上的不均匀性,并表明在全局模型中对其的准确表示很可能是一个挑战。但是,哈雷特莫索普带冰浓度与非均质成核冰浓度相当低之间的对比表明,哈雷莫索普过程在遥远的原始地区(如南极沿海地区)具有非常重要的潜力。

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