Mechanisms of ocean- atmosphere interactions Arnaud Czaja SPAT PG lecture Nov. 2011
Atmosphere “feels” the ocean through: Momentum exchanges (friction) Surface heat exchanges Q atmosphere ocean ToTo
Atmosphere “feels” the ocean through: Momentum exchanges Surface heat exchange Q atmosphere ocean ToTo Radiative + “sensible” + “latent”
Ocean – atmosphere heat exchange Radiative = solar (up and down) and longwave (up and down). Weakly dependent upon To and hence upon ocean currents, thermocline depth, etc. Sensible & latent: bring the surface atmosphere into thermodynamic equilibrium with the ocean (Ta=To and RH = 100%). Very strongly dependent upon To.
Sensible heat flux climatology (Wm-2) Annual mean DJF JJA
Latent heat flux climatology (Wm-2) Annual mean DJF JJA
Net heat flux climatology (Wm-2) Annual mean DJF JJA
Over which atmospheric layer is Q=Qlat+Qsen felt? For given To, destabilize atm by advecting an unbalanced air mass ToTo advection Buoyancy of free atm (bf) Buoyancy of atm affected by Q(bs) Q T a, q a
Over which atmospheric layer is Qlat+Qsen felt? At same To, could observe very different atmospheric responses advection Situation when bs ≈bo << bf T a, q a ToTo Shallow perturbation
Over which atmospheric layer is Qlat+Qsen felt? At same To, could observe very different atmospheric responses advection Situation when bs ≈ bo ≈ bf T a, q a ToTo Deep perturbation
Atm. heating rate climatology (K/day) Annual mean DJFJJA
Global Infrared image
Response of the atmosphere to a prescribed heating / cooling Linear calculations on the board Follows the classic paper by Hoskins and Karoly (J. Atm. Sci., 1981)
“Gill’s response” to heating (1980)
Relevance of Hoskins/Karoly? Tropics: condensational heating occurs in cloud clusters and is balanced partly by upward motion in clouds and radiative cooling in the subsiding air in between clouds hard to know what to choose for Q!
Relevance of Hoskins/Karoly? Midlatitudes: does not take into account the weather (travelling baroclinic waves)...
Friday session...