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Partitioning the CO2 Flux Mediated by Droplets Released from Breaking Waves

机译:用液滴介导的二氧化碳助焊剂释放出来的波浪

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摘要

The CO2 flux from spume droplets occurs in two steps. First, the initial droplet-air gas concentration gradient del C is immediately removed with no change in the droplet solubility. Then, the solubility changes with droplet temperature T and radius r evolution, but the flux maintains the condition del C = 0. The gas content of a droplet can be determined by del C = 0 since the parameters T and r are known. Therefore, the net gas influx of a droplet depends on the values of T and r in its return to the sea. In the second step, the droplet temperature T evolves to an equilibrium temperature T-eq, and the radius r is then reduced by evaporation at constant T-eq. For the droplet spectrum, a cut-off radius r(cut) is used to separate short-lived (r > r(cut), returning to the sea before T = T-eq) and long-lived r <= r(cut) conditions. The net influx is split into three contributions: the first (S-2S) is mediated by short-lived mechanisms, and the second and the third by long-lived (S-2L) mechanisms that are further separated into temperature-varying (S-2L(T)) and radius-varying (S-2L(R)) stages. The results show that, in the cases with large air-sea temperature differences, the first stage S-2S dominates the net gas input, but its importance decreases as the value of r(cut) increases. The temperature-varying stage S-2L(T) is dominant in cases with both large values of r(cut) and large temperature differences, while the radius-varying stage S-2L(R) increases as either the temperature difference decreases or as the value of r(cut) increases.
机译:来自烟尘液滴的二氧化碳通量发生在两个步骤中。首先,立即除去初始液滴 - 气体浓度梯度Del C,液滴溶解度没有变化。然后,溶解度随液滴温度T和半径r进化而变化,但磁通量保持状态del c = 0.由于参数t和r是已知的,可以通过del c = 0确定液滴的气体含量。因此,液滴的净气体流入取决于T和R的返回海的值。在第二步中,液滴温度T演化到平衡温度T-EQ,然后通过在恒定的T-eq下蒸发降低半径R.对于液滴频谱,截止半径R(切割)用于分离短寿命(R> R(切割),在T = T-EQ之前返回到大海)和长寿命的R <= R(切割) 状况。净流入分为三个贡献:第一(S-2S)由短寿命机构介导,第二和第三个由长寿命(S-2L)机制进一步分成温度变化(s -2L(t))和半径变化(S-2L(R))阶段。结果表明,在大型空中海水温度差异的情况下,第一阶段S-2S主导净气体输入,但由于R(切割)的值增加,其重要性降低。温度变化阶段S-2L(T)在r(切割)的大值和大的温度差异的情况下是显性的,而半径变化阶段S-2L(R)随着温度差减小或如此R(切割)的值增加。

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