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12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse Effect (continued) and Climate Sensitivity

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Page 1: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics

Topic 5 Greenhouse Effect (continued)

and Climate Sensitivity

Page 2: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Topic 5 Outline

1. Radiative transfer in the atmosphere2. A leaky greenhouse model that accounts for fact that atmosphere not opaque to longwave radiation3. Climate sensitivity to radiative forcing

Page 3: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Radiative transfer in the atmosphere

• Shortwave Absorption: clouds, H20, O3, O2

• Shortwave Reflection: clouds, surface

• Longwave Absorption: clouds, H20, CO2, CH4, N2O

Page 4: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Absorption and Emission in a Gas Vibrational and rotational transitions that dominate infrared absorption are associated with H2O and C02

(major greenhouse gases)

Page 5: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Principal Atmospheric Absorbers

Page 6: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

David Archer website

Model spectrum of upwelling longwave radiation at TOA(surface 270K, coldest point 215K)

Page 7: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

David Archer textbook

Page 8: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Leaky Greenhouse Model

Average solar radiation =Absorbed incoming radiation

Earth’s surface area=

S0⇤a2

4⇤a2 =S0

4(1)

A ⇥= 14(1��p)S0, ⌅T 4

a =14(1��p)S0 (2)

A ⇥= 14(1��p)S0 +(1� ⇥)S ⇥, ⌅T 4

a =14(1��p)S0 (3)

S ⇥= A ⇤+14(1��p)S0, ⌅T 4

s = ⌅T 4a +

14(1��p)S0 = 2⌅T 4

a (4)

S ⇥= A ⇤+14(1��p)S0 = A ⇤+

14(1��p)S0 =

24(1��p)S0 +(1� ⇥)S ⇥, (5)

Ta = Te = 255 K (6)

Ta =�

12� ⇥

⇥1/4

Te (7)

Ts = 21/4Ta = 288 K (8)

Ts =�

22� ⇥

⇥1/4

Te (9)

I = (1��p)S0/4 (10)

I = ⌅ T 41 =⌅ T1 = Te (11)

2 I = ⌅ T 42 =⌅ T2 = 21/4Te (12)

3 I = ⌅ T 42 =⌅ T2 = 31/4Te (13)

4 I = ⌅ T 4s =⌅ Ts = 41/4Te (14)

(15)

Etotal = Eatomic +Evibrational +Erotational +Etranslational (16)

1

Average solar radiation =Absorbed incoming radiation

Earth’s surface area=

S0⇤a2

4⇤a2 =S0

4(1)

A ⇥= 14(1��p)S0, ⌅T 4

a =14(1��p)S0 (2)

A ⇥= 14(1��p)S0 +(1� ⇥)S ⇥, ⌅T 4

a =14(1��p)S0 (3)

S ⇥= A ⇤+14(1��p)S0, ⌅T 4

s = ⌅T 4a +

14(1��p)S0 = 2⌅T 4

a (4)

S ⇥= A ⇤+14(1��p)S0 = A ⇤+

14(1��p)S0 =

24(1��p)S0 +(1� ⇥)S ⇥, (5)

Ta = Te = 255 K (6)

Ta =�

12� ⇥

⇥1/4

Te (7)

Ts = 21/4Ta = 288 K (8)

Ts =�

22� ⇥

⇥1/4

Te (9)

I = (1��p)S0/4 (10)

I = ⌅ T 41 =⌅ T1 = Te (11)

2 I = ⌅ T 42 =⌅ T2 = 21/4Te (12)

3 I = ⌅ T 42 =⌅ T2 = 31/4Te (13)

4 I = ⌅ T 4s =⌅ Ts = 41/4Te (14)

(15)

Etotal = Eatomic +Evibrational +Erotational +Etranslational (16)

1

Page 9: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Emission and Surface Temperatures

• Earth’s atmospheric emissivity in the infrared is 70-85% (very roughly!)

Ts = 21/4Ta = 288 K (12)

Ts =�

22� ⇤

⇥1/4

Te (13)

I = (1��p)S0/4 (14)

I = ⇧ T 41 =⇤ T1 = Te (15)

2 I = ⇧ T 42 =⇤ T2 = 21/4Te (16)

3 I = ⇧ T 42 =⇤ T2 = 31/4Te (17)

4 I = ⇧ T 4s =⇤ Ts = 41/4Te (18)

(19)

Etotal = Eatomic +Evibrational +Erotational +Etranslational (20)

⇥Ts = ⌅ ⇥Q =⇤ ⌅ =⌃Ts

⌃Q

⇤K

Wm�2

⌅(21)

⇥QBB = ⇥ (⇧T 4e ) = 4T 3

e ⇥Te = 4T 3e ⇥Ts =⇤ ⌅ =

14⇧T 3

e= 0.26

KWm�2 (22)

⇥QBB = ⇥ (⇧T 4e ) = 4T 3

e ⇥Te =4

21/4 T 3e ⇥Ts =⇤ ⌅ =

21/4

4⇧T 3e

= 0.31K

Wm�2 (23)

⌅ =⌃Ts

⌃QBB and H2O= 0.5

KWm�2 (24)

Te =�

12� ⇤

⇥1/4 ⇤(1��p)S0

4⇧

⌅1/4

⇥ (238�246)K (25)

Ts =�

22� ⇤

⇥1/4 ⇤(1��p)S0

4⇧

⌅1/4

⇥ (283�293)K (26)

2

Page 10: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Radiative Equilibrium Vertical Profile • Equilibrium state of atmosphere and surface with only radiative fluxes • Radiative heating drives actual state toward state of radiative equilibrium

Page 11: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Fig 6a, Manabe and Strickler, 1964

Radiative Equilibrium: Contributions

Page 12: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Problems with Radiative Equilibrium• Too hot at and near surface• Lapse rate of temperature too large below 10 km• Missing ingredient: circulations in atmosphere

Page 13: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Radiative Forcing and Climate Sensitivity Net radiation at top of atmosphere: R = S-OLRS = net absorbed shortwave OLR = outgoing longwave radiation

At equilibrium: R = 0

Introduce perturbation of �Rf E.g., �Rf = 3.7W/m2 for doubling of CO2(radiative forcing: hold temperature and other gases fixed)

Page 14: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Radiative forcing • Radiative forcing due to human activity is estimated at roughly 1.5 W/m2

Page 15: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

(Equilibrium) Climate Sensitivity

• Temperature change needed to re-attain equilibrium given the radiative forcing:

• Climate sensitivity � [K/(W/m2)] is ratio of change in global surface temperature �T to radiative forcing �Rf

Page 16: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Climate sensitivity for blackbody

• Climate sensitivity without atmosphere:

•Climate sensitivity with opaque isothermal atmosphere

Ts = 21/4Ta = 288 K (12)

Ts =�

22� ⇤

⇥1/4

Te (13)

I = (1��p)S0/4 (14)

I = ⇧ T 41 =⇥ T1 = Te (15)

2 I = ⇧ T 42 =⇥ T2 = 21/4Te (16)

3 I = ⇧ T 42 =⇥ T2 = 31/4Te (17)

4 I = ⇧ T 4s =⇥ Ts = 41/4Te (18)

(19)

Etotal = Eatomic +Evibrational +Erotational +Etranslational (20)

⇥Ts = ⌅ ⇥Q =⇥ ⌅ =⌃Ts

⌃Q

⇤K

Wm�2

⌅(21)

⇥QBB = ⇥ (⇧T 4e ) = 4T 3

e ⇥Te = 4T 3e ⇥Ts =⇥ ⌅ =

14⇧T 3

e= 0.26

KWm�2 (22)

⇥QBB = ⇥ (⇧T 4e ) = 4T 3

e ⇥Te =4

21/4 T 3e ⇥Ts =⇥ ⌅ =

21/4

4⇧T 3e

= 0.31K

Wm�2 (23)

⌅ =⌃Ts

⌃QBB and H2O= 0.5

KWm�2 (24)

2

Ts = 21/4Ta = 288 K (12)

Ts =�

22� ⇤

⇥1/4

Te (13)

I = (1��p)S0/4 (14)

I = ⇧ T 41 =⇥ T1 = Te (15)

2 I = ⇧ T 42 =⇥ T2 = 21/4Te (16)

3 I = ⇧ T 42 =⇥ T2 = 31/4Te (17)

4 I = ⇧ T 4s =⇥ Ts = 41/4Te (18)

(19)

Etotal = Eatomic +Evibrational +Erotational +Etranslational (20)

⇥Ts = ⌅ ⇥Q =⇥ ⌅ =⌃Ts

⌃Q

⇤K

Wm�2

⌅(21)

⇥QBB = ⇥ (⇧T 4e ) = 4T 3

e ⇥Te = 4T 3e ⇥Ts =⇥ ⌅ =

14⇧T 3

e= 0.26

KWm�2 (22)

⇥QBB = ⇥ (⇧T 4e ) = 4T 3

e ⇥Te =4

21/4 T 3e ⇥Ts =⇥ ⌅ =

21/4

4⇧T 3e

= 0.31K

Wm�2 (23)

⌅ =⌃Ts

⌃QBB and H2O= 0.5

KWm�2 (24)

2

Page 17: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Climate feedbacks are important

• Climate sensitivities in Atmosphere-Ocean General Circulation Models (GCMs) range from 0.5 to 1.2 K W-1 m2

• Include feedbacks (relative to blackbody) from:- water vapor (+ve: why?)- albedo (+ve: why?)- cloud (+ve: why?)- lapse rate (-ve: why?)

Page 18: 12.003 Introduction to Atmosphere, Ocean, and Climate ...pog.mit.edu/12.003/pdf_slides/Topic5.pdf · 12.003 Introduction to Atmosphere, Ocean, and Climate Dynamics Topic 5 Greenhouse

Observed temperature changes • Reconstruction of global surface temperature record suggests increase of about 1K