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Addendum to “Sea spray aerosol flux estimation based on long-term variation of wave statistics”: estimation based on long-term variation of wind statistics ☆

机译:“基于波浪统计的长期变化的海喷雾气溶胶磁通估计”:基于风统计长期变化的估计

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Summary This note provides estimates of the mean whitecap coverage and the mean sea spray aerosol flux based on long-term wind statistics from the Northern North Sea. Here the improved sea spray aerosol production flux model by Callaghan (2013) is used. The results are compared with those in Myrhaug et al. (2015) based on long-term wave statistics from the Northern North Sea and the North Atlantic. Keywords Sea spray aerosol flux ; Whitecap coverage ; Mean wind speed ; Wind statistics prs.rt("abs_end"); 1. Introduction Myrhaug et al. (2015) (hereafter referred to as MWH15) provided estimates of the mean sea spray aerosol flux based on long-term variation of wave statistics using the whitecap method applying the limiting steepness and threshold vertical acceleration criteria. Here the long-term wave statistics represented open ocean deep water waves in the Northern North Sea and the North Atlantic. This note is supplementary to MWH15 with the purpose of demonstrating how similar results for the mean sea spray aerosol flux can be obtained by using estimates of the whitecap coverage based on long-term variation of wind statistics. Moreover, the whitecap method used in MWH15 has been replaced by the Callaghan (2013) improved sea spray aerosol production flux model. The whitecap coverage, which is defined as the area of whitecaps per unit sea surface, has often been used to quantify the occurrence of breaking wind waves at sea. There are many parameterizations of whitecap coverage available in the literature; comprehensive reviews are given in Anguelova and Webster (2006) , Massel (2007) and de Leeuw et al. (2011) . Parameterizations are based on U 10 and u *. Here U 10 [m?s?1] is the mean wind speed at the 10?m elevation, and u * [m?s?1] is the friction velocity equal to the square root of the vertical flux of horizontal momentum at the sea surface. However, when plotting the whitecap coverage versus U 10 and versus u * it is often found that the data scatter is larger when plotted versus u * than when plotted versus U 10 (see e.g. Sugihara et al., 2007 ). This is attributed to the larger uncertainties in estimating u * than measuring U 10. Therefore the parameterizations in the present study are based on U 10. Other important factors affecting the whitecap coverage are the stratification of the near-surface air boundary layer and the state of development of surface waves, see e.g. Sugihara et al. (2007) and Myrhaug and Holmedal (2008) . Reviews of whitecap coverage at sea and how it is linked to marine aerosol production are given by Massel (2007) , de Leeuw et al. (2011) and Callaghan (2013) . 2. Whitecap coverage and sea spray aerosol flux estimation based on long-term variation of wind statistics 2.1. Whitecap coverage estimation The following whitecap coverage ( W c ) parameterizations will be considered here to demonstrate the use of wave statistics. The Monahan and O’Muircheartaigh (1980) (hereafter referred to as MO80) parameterization is widely used and recognized ( de Leeuw et al., 2011 ), given as fraction, equation ( 1 ) W c = 3.84 × 10 ? 6 U 10 3.41 . The Callaghan et al. (2008) (hereafter referred to as C08) parameterization is based on data collected in the North East Atlantic inside a geographical area defined by 9.5°W, 13°W, 55.5°N and 57.5°N, given in percent, equation ( 2 ) W c = 0.00318 ( U 10 ? 3.70 ) 3 ; 3.70 m?s ? 1 It should be noted that the wave statistics in BGGS07 ( Bitner-Gregersen and Guedes Soares, 2007 ) Data Sets 1 to 5 used in MWH15 is from the same ocean area, i.e. from the North Atlantic.
机译:发明内容本说明提供了基于北海北海长期风统计的平均白斑覆盖和平均海喷雾气溶胶源的估计。在这里,使用了Callaghan(2013)的改进的海浪喷雾气溶胶生产助推器模型。结果与Myrhaug等人的结果进行了比较。 (2015)基于北海北海和北大西洋的长期波统计。关键词海浪喷雾气溶胶助焊剂;怀孕覆盖;平均风速;风统计PRS.rt(“ABS_END”); 1.介绍Myrhaug等人。 (以下)(以下称为MWH15)提供了基于使用限制陡度和阈值垂直加速标准的WHITECAP方法的波统计的长期变化的平均海喷雾气溶胶通量的估计。在这里,长期波浪统计在北部北海和北大西洋的开阔海洋深水波。本说明对MWH15进行了补充,目的是通过使用基于风统计的长期变化,通过使用WhiteCap覆盖的估计来获得平均海喷雾气溶胶通量的类似结果。此外,MWH15中使用的WHITECAP方法已被CALLAGHAN(2013)改进的海浪气溶胶生产助焊剂模型所取代。被定义为每单位海面的白斑面积的WhiteCap覆盖率通常用于量化在海上打破风波的发生。文献中有许多Whitecap覆盖范围的参数化;综合评论是在安伊尔瓦娃和韦伯斯特(2006),马塞尔(2007)和De Leeuw等人的中。 (2011)。参数化基于U 10 和u * 。这里U 10 [m?s ?1 ]是10?m升高的平均风速,而U * [m?s α1]是摩擦速度等于海表面水平动量垂直通量的平方根。然而,当绘制WhiteCAP覆盖率与U 10 和U * 时,通常发现当绘制的数据散射与u * 时,数据散射更大比绘制与U 10 (参见Sugihara等,2007)。这归因于估计U * 10 。因此,本研究中的参数化基于U 10 。影响WhiteCAP覆盖的其他重要因素是近表面空气边界层的分层和表面波的发展状态,参见。 Sugihara等。 (2007)和Myrhaug和Holmedal(2008)。海上覆盖的评论以及如何与海洋气溶胶生产联系到Massel(2007),De Leeuw等人。 (2011)和Callaghan(2013年)。 2.基于风统计的长期变化2.1,WhiteCap覆盖和海浪曝气磁通估计2.1。 WhiteCAP覆盖估计下列WhiteCAP覆盖范围(W C )参数化将在此处考虑参数以演示波浪统计的使用。 Monahan和O'Muircheartaigh(1980)(以下称为MO80)参数化广泛使用和识别(De Leeuw等,2011),作为分数,等式(1)W C = 3.84×10? 6 U 10 3.41。 Callaghan等人。 (以后)(以下简称C08)参数化基于位于9.5°W,13°W,55.5°N和57.5°N的地理区域内收集的地理区域内收集的数据,以百分比,等式(2 )W C = 0.00318(U 10?3.70)3; 3.70 m?s? 1应该注意的是,BGGS07(Bitner-Gregersen和Guedes Soares,2007)的波统计数据集1到5在MWH15中使用的1至5来自同一个海洋区域,即来自北大西洋。

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