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Introductory Climate Modeling. Presented by Dr. Robert MacKay Clark College physics and meteorology [email protected]. Earth in space. See the first 4 videos at: http://earthobservatory.nasa.gov/Experiments/PlanetEarthScience/GlobalWarming/GW.php - PowerPoint PPT Presentation
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Introductory Climate Modeling
Presented by Dr. Robert MacKayClark College physics and meteorology
Earth in space
See the first 4 videos at:http://earthobservatory.nasa.gov/Experiments/PlanetEarthScience/GlobalWarming/GW.php
These are a very nice introduction to radiation from Earth and Sun.
Earth in space
The rate of Solar energy absorption by Earth is
R2*(1-)So where
R is Earth’s radius is the mean planetary albedoSo is the solar constant ~1365 W/m2
The mean emission rate for terrestrial (longwave) radiation is
R2*T4 where
=5.67x10-8 W/m2/K4
T is Earth’s mean annual temperature
Earth in space
Setting absorption equal to emission gives
R2*(1-)So =R2*T4
or
K 255
4σ
α1ST
41
0
This is about 33 K lower than Earth’s mean surface temperature of 288 K
Adding an atmosphere
A “flat” earth with an atmosphere that absorbs no solar radiation but absorbs all long-wave radiation coming from Earth’s surface. Both the earth’s surface and the atmosphere are assumed to be black bodies for longwave radiation. The atmosphere emits radiant energy equally towards and awy from Earth’s surface.
4A2
4E1
σTF
σTF
A “flat” earth with an atmosphere that absorbs no solar radiation but absorbs all long-wave radiation coming from Earth’s surface. Both the earth’s surface and the atmosphere are assumed to be black bodies for longwave radiation. The atmosphere emits radiant energy equally towards and awy from Earth’s surface.
4A2
4E1
σTF
σTF
KmKWx
mW303
)/(1067.5
/239*2Tor
2SF gives Ffor Solving
unknowns as F and Fwith
equationst independen just tworeally are equations above the
)atmosphere of at top balance(energy SF 3)
)atmospherefor balance(energy F2F 2)
surface)at balance(energy FSF 1)
41
248
2
E
11
21
2
12
21
This is about 15 K higher than Earth’s mean surface temperature of 288 K
S
From K. Trenberth, J. Fasullo, and J. Kiehl, EARTH’S GLOBAL ENERGY BUDGET BAMS 2009
Atmosphere absorbs a fraction, ,of the total solar radiation absorbed by the planet
Atmosphere absorbs a fraction, of all long-wave radiation coming from Earth’s surface. Through Kirchoff’s radiation law the emissivity of the atmosphere for long-wave radiation equals its absorptivity.
Earth’s surface is assumed to be a black bodies for long-wave radiation.
The atmosphere emits radiant energy equally towards and away from Earth’s surface.
4A2
4E1
σTF
σTF
S
A “flat” earth with an atmosphere that absorbs no solar radiation but absorbs all long-wave radiation coming from Earth’s surface. Both the earth’s surface and the atmosphere are assumed to be black bodies for longwave radiation. The atmosphere emits radiant energy equally towards and awy from Earth’s surface.
4A2
4E1
σTF
σTF
unknowns as F and Fwith
equationst independen just tworeally are equations above the
)atmosphere of at top balance(energy S)F-(1F 3)
)atmospherefor balance(energy SF2F 2)
surface)at balance(energy FS)1(F 1)
21
12
12
21
Estimating =0.29 and =0.9 from Khiel and Trenberth Energy Balance diagram
A “flat” earth with an atmosphere that absorbs no solar radiation but absorbs all long-wave radiation coming from Earth’s surface. Both the earth’s surface and the atmosphere are assumed to be black bodies for longwave radiation. The atmosphere emits radiant energy equally towards and awy from Earth’s surface.
4A2
4E1
σTF
σTF
K5.284S
2ε
1
2γ
1Tor S
2ε
1
2γ
1F
2) and 1) equations (combining S2
F2
S)1(F
41
E1
11
Estimating =0.29 and =0.9 from Khiel and Trenberth Energy Balance diagram
This is about 3.5 K lower than Earth’s mean surface temperature of 288 K
Thermal Inertia Of Oceans
d C
I
t
T
T dA C tA I
I Net radiation intensity (W/m2)A Area of surfaced depth of ocean mixed layerC specific heat capacity of oceans the density of water
day
Co
14
I
t
T
If d=100 m
http://www.atmosedu.com/Geol390/physlets/GEBM/EBMGame.htm
http://www.youtube.com/watch?v=y2m7OTv-cAc
http://www.atmosedu.com/Geol390/physlets/GEBM/ebm.htm
Stella version: http://www.atmosedu.com/WSU/esrp310-550/Activities/Gebm.STM
Feedbacks
Feedbacks
http://www.thesystemsthinker.com/tstcld.html
http://www.atmosedu.com/ENVS109/PP/CausalLoopDiagramsA.ppt
Diagram from VUE.Visual Understanding environment
Conclusions
• Simple conceptual climate models can help students learn about climate modeling and the climate system.
• Climate models of all sort provide Interactive engagement opportunities for students.
• Causal loop diagrams offer an excellent visual communication tool for both student and instructor.