Abstract. The high-latitude freezing and melting cycle can variously result in haline convection, freshwater capping, or freshwater injection into the interior ocean. An example of the latter process is a secondary salinity minimum near 800 m depth within the Arctic Ocean that results from the transformation on the Barents Sea shelf of Atlantic water from the Norwegian Sea and its subsequent intrusion into the Arctic Ocean. About onethird of the freshening on the shelf of that initially saline water appears to result from ice melt, although the actual sea ice flux is small, only about 0.005 Sv. A curious feature of this process is that water distilled at the surface of the Arctic Ocean by freezing ends up at mid-depth in the same ocean. This is a consequence of the ice being exported southward onto the shelf, melted, and then entrained into the northerly Barents Sea throughflow that subsequently sinks into the Arctic Ocean. Prolonged reduction in sea ice in the region and in the concomitant freshwater injection would likely result in a warmer and more saline interior Arctic Ocean below 800 m.
Some Thoughts on the Freezing and Melting of Sea Ice and TheirEffects on the Ocean
K. Aagaard and R. A. WoodgateIntroduction Evaporation and precipitation rates over the Arctic Ocean are quite low, respectively about 5-10 cm yr -1 and 20-30 cm yr -1 in liquid water equivalent (Barry and Serreze, 2000). The primary cycling of freshwater in the Arctic Ocean is therefore instead accomplished by the freezing and melting of sea ice, for which characteristic rates are about 100 cm yr -1 and 50 cm yr -1 , respectively (Steele and Flato, 2000). If the ice drifts during the long intervals between the phase changes, the result is a net local distillation, since the freezing process expels the majority of the salt in the freezing water into the underlying ocean. This freezing and melting of sea ice, with their accompanying salinity changes, provide buoyancy forcing that is particularly effective in influencing the circulation because of the primary control of density by salinity at the prevailing low temperatures. For example, Holland, Mysak and Oberhuber (1996) concluded that buoyancy forcing is critical to maintaining the mixed layer circulation in the Arctic Ocean. The present note points to the range of buoyancy forcing that is possible in the high-latitude ocean. We begin with an example from the northern North Atlantic extension, viz., the cooling and freshening of the Atlantic water on the Barents shelf. We then place this process in the broader context of interactions between sea ice and the ocean. The intent is to thereby call attention to some appropriate, and even necessary, considerations in modelling the high-latitude ocean, especially in regard to the possible restructuring of ocean properties under altered climatic conditions.