Sea spray induced air-sea heat and salt fluxes based on the wave-steepness-dependent sea spray model
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Abstract: Sea spray, which comprises amounts of small ocean droplets, plays a significant role in the air-sea coupling, atmospheric and oceanic dynamics, and climate. However, it remains arduous to arrive at estimates for the efficiency and accuracy of the sea spray induced air-sea heat and salt fluxes. This is because the microphysical process of sea spray evolution in the air is of extreme complexity. In this study, we iteratively calculated the sea spray induced air-sea heat and salt fluxes at various weather condition. To do so, we implemented one novel wave-steepness-dependent sea spray model into a bulk air-sea fluxes algorithm and utilized other sea spray models as comparisons. Based on the improved wave-dependent bulk turbulent algorithm, we observed that despite the negative contribution of sea spray to the sensible heat fluxes, the sea spray positively contributes to the air-sea latent heat fluxes, leading to an overall increase in the total air-sea heat fluxes. The additional heat fluxes caused by sea spray may be the missing critical process that can clarify the discrepancies observed between measured and modelled Tropical Cyclone’s development and intensification. In addition to heat fluxes, we observed that sea spray has significant impacts on the air-sea salt fluxes. As the sea salt particles are one of the main sources of the atmosphere aerosol, our results imply that sea spray could impact global and regional climate. Thus, given the significance of sea spray on the air-sea boundary layer, sea spray effects need to be considered in studies of air-sea interaction, dynamics of atmosphere and ocean.
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Key words:
- sea spray /
- air-sea heat fluxes /
- air-sea salt fluxes /
- wave
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Figure 2. Sea spray volume fluxes against the 10-m reference height wind speed
$ {U}_{10} $ .The solid black lines are the sea spray volume fluxes based on Xu et al. (2021b) for different values of the mean wave steepness (i.e.,$ {H}_{\rm{s}}{k}_{{\rm{m}}}/2 $ varies from 0.1 to 0.4 with an increment of 0.1), the solid red line is based on Andreas (1992), and the solod green lines are based on (Zhao et al., 2006) for different values of the wave age ($ \ \beta $ ) (i.e.,$ \ \beta = 0.2 $ and 0.4, respectively).Figure 3. The air-sea sensible heat fluxes (SHF) against the 10-m reference height wind speed
$ {U}_{10} $ . The sea spray induced sensible heat fluxes,$ {H}_{{\rm{s,sp}}} $ , is based on Xu et al. (2021b) (the dashed black lines with same gray value as in Fig. 2), Andreas (1992) (the dashed red line), and Zhao et al. (2006) (the dashed green lines with same color value as in Fig. 2), respectively. The interfacial direct sensible heat fluxes without sea spray,$ {H}_{{\rm{s,int}}} $ , is the dash black line with circle marks, and the air-sea sensible heat fluxes with sea spray,$ {H}_{{\rm{s,tot}}} $ , are the solid black, red, and green lines for Xu et al. (2021b), Andreas (1992), and Zhao et al. (2006), respectively (please see the legend in Fig. 2).Figure 4. The air-sea latent heat fluxes (LHF) against the 10-m reference height wind speed
$ {U}_{10} $ . The sea spray induced latent heat fluxes,$ {H}_{{\rm{l,sp}}} $ , is based on Xu et al. (2021b) (the dashed black lines with same gray value as in Fig. 2), Andreas (1992) (the dashed red line), and (Zhao et al., 2006) (the dashed green lines with same color value as in Fig. 2), respectively. The interfacial direct latent heat fluxes without sea spray,$ {H}_{{\rm{l,int}}} $ , is the dash black line with circle marks, and the air-sea latent heat fluxes with sea spray,$ {H}_{{\rm{l,tot}}} $ , are the solid black, red, and green lines for Xu et al. (2021b), Andreas (1992), and Zhao et al. (2006), respectively (please see the legend in Fig. 2).Figure 5. The total air-sea heat fluxes (SHF+LHF) against the 10-m reference height wind speed
$ {U}_{10} $ . The sea spray induced heat fluxes,$ {H}_{{\rm{l,sp}}}+{H}_{{\rm{s,sp}}} $ , is based on Xu et al. (2021b) (the dashed black lines with same gray value as in Fig. 2) , Andreas (1992) (the dashed red line), and (Zhao et al., 2006) (the dashed green lines with same color value as in Fig. 2), respectively. The interfacial direct air-sea total heat fluxes without sea spray,$ {H}_{{\rm{l,int}}}+{H}_{{\rm{s,int}}} $ , are the dash black line with circle marks, and the air-sea total heat fluxes with sea spray,$ {H}_{{\rm{l,tot}}}+{H}_{{\rm{s,tot}}} $ , are the solid black, red, and green lines for Xu et al. (2021b), Andreas (1992), and Zhao et al. (2006), respectively (please see the legend in Fig. 2).Figure 6. The sea spray induced salt fluxes (M) against the 10-m reference height wind speed
$ {U}_{10} $ . The black lines are the sea spray induced salt fluxes,$ {M}_{{\rm{s,sp}}} $ , based on Xu et al. (2021b) for different$ {H}_{\rm{s}}{k}_{{\rm{m}}}/2 $ which varies from 0.1 to 0.4 with an increment of 0.1 (gray value as in Fig. 2), Andreas (1992) (the red line), and (Zhao et al., 2006) (the green lines with same color value as in Fig. 2), respectively (please see the legend in Fig. 2). -
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