TY - GEN
T1 - Parameterization of air-ocean gas transfer
AU - Soloviev, A. V.
PY - 1991
Y1 - 1991
N2 - A renewal-type model, based on the physics of a molecular sublayer, allows the derivation of parameters to describe air-ocean gas transfer and the temperature difference across the cold film. The 'surface Richardson number' controls transition from convective instability to wind induced instability ('rollers' on breaking wavelets) and the Keulegan number controls transition from the regime of 'rollers' to long-wave breaking. Critical value of the 'surface Richardson number' and of a nondimensional constant can be evaluated by comparison of parameters describing the cold film with field data. Critical value of the Keulegan number can be determined from the wind speed at which long-wave breaking appears. The parameterization of air-ocean gas transfer predicts a constant value for the gas transfer coefficient at calm and low wind speed conditions (depending on the surface heat flux). The coefficient rises as a function of friction velocity at moderate wind speeds, and decreases inversely proportional to a half-power of the friction velocity at large wind speeds.
AB - A renewal-type model, based on the physics of a molecular sublayer, allows the derivation of parameters to describe air-ocean gas transfer and the temperature difference across the cold film. The 'surface Richardson number' controls transition from convective instability to wind induced instability ('rollers' on breaking wavelets) and the Keulegan number controls transition from the regime of 'rollers' to long-wave breaking. Critical value of the 'surface Richardson number' and of a nondimensional constant can be evaluated by comparison of parameters describing the cold film with field data. Critical value of the Keulegan number can be determined from the wind speed at which long-wave breaking appears. The parameterization of air-ocean gas transfer predicts a constant value for the gas transfer coefficient at calm and low wind speed conditions (depending on the surface heat flux). The coefficient rises as a function of friction velocity at moderate wind speeds, and decreases inversely proportional to a half-power of the friction velocity at large wind speeds.
UR - https://www.scopus.com/pages/publications/0025890524
UR - https://www.scopus.com/pages/publications/0025890524#tab=citedBy
M3 - Conference contribution
AN - SCOPUS:0025890524
SN - 0872628469
T3 - Air-Water Mass Transfer
SP - 637
EP - 646
BT - Air-Water Mass Transfer
PB - Publ by ASCE
T2 - 2nd International Symposium on Gas Transfer at Water Surfaces
Y2 - 11 September 1990 through 14 September 1990
ER -