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Heat and water budgets

  At thermal equilibrium, and characterized by a constant mean annual temperature of sea water, the heat budget of the Mediterranean Sea may be summarized by:
 equation114
where tex2html_wrap_inline615 is the solar heat input, A is the mean albedo, tex2html_wrap_inline619 is the heat gained by marine advection at the strait of Gibraltar, tex2html_wrap_inline621 is the flux of latent heat (evaporation), tex2html_wrap_inline623 the flux of sensible heat and tex2html_wrap_inline625 the net longwave radiation. Advection to the Mediterranean Sea may be written as:
equation117
where tex2html_wrap_inline627 represents the mean density of water, tex2html_wrap_inline629 is the specific heat, V equals flow, T represents temperature, with i and o subscripts for inflow and outflow, respectively, at the Strait of Gibraltar, and tex2html_wrap_inline639 the mean temperature of evaporated water (E), precipitation (P), and river runoff (R), respectively. A rough estimate of mean tex2html_wrap_inline639 can be obtained from mean surface temperature, tex2html_wrap_inline649 , which is not very different from either the outflow temperature, tex2html_wrap_inline651 , or from the mean inflow temperature tex2html_wrap_inline653 . Using values of tex2html_wrap_inline627 = 1027 kg tex2html_wrap_inline659 , tex2html_wrap_inline629 = 0.95 cal tex2html_wrap_inline665 tex2html_wrap_inline667 , tex2html_wrap_inline653 = 15.4tex2html_wrap_inline599 , tex2html_wrap_inline651 = 13.4tex2html_wrap_inline599 and tex2html_wrap_inline677 = 1.6 Sv (1 Sv = tex2html_wrap_inline683 tex2html_wrap_inline685 tex2html_wrap_inline687 ), tex2html_wrap_inline619 was calculated to be 5 tex2html_wrap_inline597 [Béthoux and Gentili, 1997]. It is noteworthy that this thermal input, tex2html_wrap_inline619 , is in addition to a solar radiation input of about 200 tex2html_wrap_inline597 , together with a third and less influential thermal input of earth heat flow across the sea-floor, at about 0.1 tex2html_wrap_inline597 , neglected in Eq. 1. An increase in water temperature over the 1959-1997 period denotes continuous changes in the different terms of heat budget. Changes in water temperatures permit estimates of changes in marine advection, dtex2html_wrap_inline619 , and in heat content of the water column, dtex2html_wrap_inline701 . If the solar radiation input, tex2html_wrap_inline615 (1-A), is assumed to be constant, marine data permits estimates to be made of changes in atmospheric transfer, as dtex2html_wrap_inline701 - dtex2html_wrap_inline619 = d(tex2html_wrap_inline621 + tex2html_wrap_inline623 + tex2html_wrap_inline625 ). Changes in thermal advection, dtex2html_wrap_inline619 , and in evaporation loss, dtex2html_wrap_inline621 , occur concomitantly with changes in water budget, which may therefore be written as: tex2html_wrap_inline719.

An increase in water salinity denotes a change in evaporation (with links to the tex2html_wrap_inline621 term in the heat budget and changes in water temperature) and/or freshwater input by precipitation and river runoff (with concomitant changes to the resultant tex2html_wrap_inline677 - tex2html_wrap_inline725 and heat advection tex2html_wrap_inline619 ).



Next: Marine data and surface changes Up: Warming and freshwater budget change in the Mediterranean since the Previous: Introduction