Waves have been called the gearbox of the climate system (Semedo et al., 2011). The analogy highlights the mediating role of the wave field between the atmosphere and the ocean interior. It may seem surprising that the sea surface demands its own class of numerical model. The other components (atmosphere, ocean, sea ice, land surface) have real substance, i.e. they each represent a three-dimensional chunk of the Earth system. In contrast, the wave model is a representation of a surface between two media, namely the air and the sea (Figure 10.4). There are, however, good practical reasons for this split. If we had access to unlimited computing power, we could model the ocean and the atmosphere with a grid resolution approaching Kolmogorov’s microscale. That would mean that the Navier Stokes equations could be solved in the approximative limit known as DNS (Moin and Mahesh, 1998). In this case, the (liquid) ocean would presumably interact with the (gaseous) atmosphere and on their interface would form a wavy surface that, given a sufficiently strong momentum flux (mostly from the atmosphere to the ocean), would form droplets and bubbles as the waves start to break. The computational reality is far from this. At present, we can model the ocean and the atmosphere with models that have grid cells of tens of metres in the horizontal if we limit ourselves to small domains, whereas the waves that form under the influence of the wind have wavelengths of the order of some metres to hundreds of metres and so cannot be explicitly resolved together with the bulk ocean properties.
The behaviour of these waves determines the mass and momentum fluxes between the ocean and the atmosphere. As waves grow under the influence of the wind, they become steeper. In this phase they are also choppier than they will be later on. All this means that the momentum flux between the atmosphere and the ocean is affected by the presence of waves (Janssen et al., 2004; Breivik et al., 2015). There is also very important feedback between the waves and the atmosphere. As waves grow, the sea surface becomes rougher, slowing the near-surface winds and increasing the momentum flux from the atmosphere to the wave field. This has the effect of stemming the deepening of low-pressure systems. This is important in the formation and growth of extratropical lows (Janssen, 1991 and 2004), but also in the evolution of tropical cyclones (discussed further below).
A secondary effect of waves on the air-sea interaction is through their ability to impart momentum and turbulent kinetic energy to the ocean interior(Figure 10.4). As waves grow, they absorb momentum that would otherwise go directly to the formation of ocean currents. As waves break, they part with this momentum, and also inject turbulent kinetic energy into the ocean (Janssen et al., 2004; Rascle et al., 2006; Ardhuin et al., 2008 and 2009). This leads to a redistribution of momentum and kinetic energy in time and space (Ardhuin and Jenkins, 2006; Breivik et al., 2015; Staneva et al., 2017; Wu et al., 2019), and has a profound effect on near-shore processes (Uchiyama et al., 2010; Kumar et al., 2012) where waves interact strongly with the currents. It is also clear that in open ocean conditions the mixed-layer depth is a function of the wave activity, in part sustained by the Langmuir turbulence (McWilliams et al., 1997; Fan and Griffies, 2014; Li et al., 2016 and 2017; Li and Fox-Kemper, 2017; Ali et al., 2019). The enhanced mixing due to waves is thus important for the sea surface temperature, which helps to determine the air-sea heat flux and thus constitutes an important feedback mechanism between the atmosphere and the ocean.
Land-sea interactions take place on a wide range of spatial and temporal scales. The presence of land modifies the weather in the coastal zone, e.g. the daily variations in wind speed and direction due to the sea breeze, and hence the atmosphere provides an indirect link between the land and the ocean. Another example of this indirect coupling is the way large-scale weather systems can influence the transport pathways of river water (Osadchiev et al., 2020).
The physical couplings between land, ocean, and atmosphere are not necessarily equal in strength and importance, and we often observed a lagged response. The runoff from rivers is dependent on the precipitation over a potentially very large catchment area, with significant lag between specific precipitation events and the freshwater discharge to the coastal ocean. This lag is particularly pronounced in temperate and polar regions where the precipitation accumulates as snow during parts of the year. This is reflected by the state-of-the-art of coupled modelling, as very few systems couple the ocean to the land, but rather use the atmosphere as a mediator.
At high latitudes, air-sea exchange is modified by the presence of sea ice. Varying in thickness up to a couple of metres, sea ice is sensitive to forcing from both air and sea and the air, sea, and sea ice are strongly coupled. Geophysical scale sea ice is essentially a mixture of ice floes of varying size and thickness, with the added complexity of being rafted and ridged. Describing accurately the sea ice mechanical behaviour is extremely challenging, although modelling sea ice as plastic materials at the large scale has long been a successful approach (Coon et al., 1974; Hibler, 1979; Hunke and Dukwicz, 1997; Girard et al., 2011). In medium to high model resolutions (≤ 10km), such models can generate small-scale features such as the ice leads (Hutchings et al., 2005; Wang and Wang, 2009; Girard et al., 2011; Spreen et al., 2017). This thin ice cover has a very small heat content and easily melts away during summer, resulting in large seasonal variations of sea ice extent.
In much of the pack ice region, the thermodynamic and dynamic interactions between air and sea are greatly suppressed. During wintertime, the air-sea heat flux through leads is two orders of magnitude larger than that through thick ice (Maykut, 1978). Dynamically, pack ice behaves as a low-pass filter, the air and sea surface stresses act on the ice cover thus driving the advection and deformation of sea ice, while ocean waves are generally suppressed. The MIZ is a highly complex region consisting of ice floes of varying dimensions and shapes. Wave energy propagating into the MIZ can lead to rapid breakup. The damping of waves in sea ice is directly related to the amount of energy imparted on the sea ice. This is a field of active research, and it is presently not fully clear how the MIZ attenuates wave energy (Doble and Bidlot, 2013; Williams et al., 2013; Kohout et al., 2014; Sutherland and Rabault, 2016; Ardhuin et al., 2016; Rabault et al., 2020).
Landfast ice is a special region where the air-sea interaction nearly ceases. It generally appears in winter seasons and often occurs in shallow waters where ridged ice grounds on the seabed (Mahoney et al., 2014), or occurs where islands are close to each other (Divine et al., 2003). Modelling studies have shown that adding base stress due to grounding ridges and increasing ice tensile strength improve the simulation of landfast ice evolution (Lemieux et al., 2016), although in some Arctic shelf seas the time duration needs to be further improved.
In coupled modelling, a key consideration is whether to couple the sea ice directly to the atmosphere or only through the ocean model. In some recent coupled models, particularly for high-resolution short-term atmosphere, ocean, and sea ice forecasts, the timestep for coupling has decreased to one hour or less, e.g. the coupled ocean-ice model METROMS at the Norwegian Meteorological Institute (Naughten et al., 2018), or the atmosphere-ice coupled model at UKMO (Ridley et al., 2018). In these cases, the difference between using the atmosphere timestep or ocean timestep is generally negligible.
Air-sea exchange really comes to the fore in the development of tropical cyclones. The sea surface temperature must as a general rule exceed 26.5ºC to sustain the growth of the cyclone (Emanuel, 1986). However, the depth to which the ocean’s temperature must be above this critical threshold is also important. As the cyclone moves across the sea surface, the Ekman transport will lead to divergence, and vertical Ekman pumping will eventually lead cooler water to the surface. If the cyclone is moving sufficiently slowly, this will eventually kill the cyclone (Mogensen et al, 2017). Thus, it is essential to include an ocean model component that responds to the atmospheric forcing.
Polar lows are of a decidedly less extreme nature than tropical cyclones, but they share the same dependence on sea surface temperature (Rasmussen and Turner, 2003). As winds blow off the sea ice, the air is rapidly warmed by the (relatively) warm ocean surface. Under the appropriate atmospheric conditions (Kolstad, 2015), this can lead to the formation of polar lows. These are small-scale, intense cyclones, typically with gale-force winds. If the cyclone is rather stationary, a shallow layer of warmer water can mix with cooler waters through Ekman pumping. As the ocean temperature is key to sustaining a cyclone, the water mixing can sometimes be enough to inhibit further growth of the polar low.
Examples of instantaneous coupling between land, ocean, and atmosphere also include coastal inundation during landfall of tropical cyclones (Lee et al., 2019). In these cases, heavy precipitation leads to a swelling of local rivers, which is often coincidental with a large storm surge. The result is a rapid sea-level rise that may cause extensive damage to coastal infrastructure, especially when combined with large surface waves and strong winds.
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