Download presentation
Presentation is loading. Please wait.
2
Annual-mean TOA radiation (ERBE, W/m 2 ) Absorbed SW Outgoing LW
3
Surface temp (NCEP, o C) January July
4
Surface wind (NCEP, m/s) January July
7
Temperature ( o C) and zonal wind (m/s) (NCEP) January July
8
km 10 4 –2 –8 –14 14 8 2 –4 –10 1620 24 28 32 36 24 28 32 36 40 1620 1 2 3 4 5 T decreases by 6 o C/kmincreases by 4 o C/km Temperature and potential temperature surfaces
9
Potential temperature (K) and zonal wind (m/s) (NCEP) January July
10
The “bare rock” temperature In steady state, E in = E out E in = π R 2 S (1– ) E out = 4π R 2 T 4 R =radius =albedo Putting it all together:
11
Radiative-convective equilibrium (Manabe & Strickler, 1964)
12
Cloud–SW interaction
13
Cloud–LW interaction
14
Net cloud forcing from simple model (Hartmann, p. 74)
15
Annual-mean cloud water path (g m –2 )
16
Annual-mean total cloud amount (%)
17
Annual mean low cloud amount
18
Annual mean middle cloud amount
19
Annual mean high cloud amount
20
Annual mean SW cloud forcing (ERBE, W m –2 )
21
Annual mean LW cloud forcing (ERBE, W m –2 )
22
Annual mean net cloud forcing (ERBE, W m –2 )
23
Climate feedback: the general idea What happens if we perturb the climate away from its equilibrium, for instance by increasing CO 2 concentration? +++ CO 2 positive feedback TX + CO 2 negative feedback TY – +++
24
In the real world, both positive and negative feedbacks act simultaneously Overall, the negative feedbacks win: otherwise temperature would run away to very high values (runaway greenhouse) However, the presence of positive feedbacks means that the temperature increase we get for a given increase in CO2 is greater than we would get in their absence: more bang for the buck Dominant feedbacks: –Negative: Planck (radiative) feedback Lapse rate feedback –Positive : Surface albedo feedback Water vapour feedback Cloud feedback?
25
Ice albedo feedback As surface temperature increases, some of the ice in the polar ice caps melts, exposing ocean or boreal forest Ice is much more reflective to sunlight than ocean or forest So the feedback goes like this: Increased CO 2 —› raises T —› melts some ice —› decreases reflectivity —› more insolation is absorbed —› raises T even further
26
Water vapour feedback Relative humidity stays roughly constant as climate warms Since RH = w/w s (T) and w s (T) increases exponentially with T, then humidity increases rapidly with T So the feedback goes like this: Increased CO 2 —› raises emission level —› raises T —› raises humidity —› raises emission level even further —› raises T even further
27
Feedback strengths in climate models (Soden&Held, 2006)
33
Insolation at TOA Absorbed insolation
34
Insolation at TOA Absorbed insolation
37
SHF into ground!
38
The moist equations of motion latent heat evap condensation evaporation water vapour mixing temperature mixing momentum mixing (friction)
39
Energetics Total energy per unit mass: Rate of change of: kinetic energy: potential energy: thermal internal energy: latent internal energy:
40
Energetics Rate of change of total energy per unit volume: but: Finally: Note that: moist static energysmall
44
AB A B Seasonal cycle of surface temperature Temp ( o C) Amplitude of seasonal cycle ( o C)
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.