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Atmospheric Sciences 321 Science of Climate Lecture 20: More Ocean: Chapter 7

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Page 1: Science of Climate

Atmospheric Sciences 321 Science of Climate

Lecture 20: More Ocean: Chapter 7

Page 2: Science of Climate

Community Business �  Quiz discussion

�  Next Topic will be Chapter 8, Natural Climate variability in the instrumental record.

�  Homework #7 is due Wednesday

�  Nine lecture periods left after today that will be primarily on Chapters 11 and 12. Past and Future Climates. I don’t have 2nd Edition versions of these yet.

�  Questions?

Page 3: Science of Climate

Quiz #3 �  Remember in class several times, including on

Wednesday we talked about how 1m/yr of precipitation is equivalent to 80Wm-2

Page 4: Science of Climate

�  Mostly you nailed the angular momentum problem.

Quiz #3

Page 5: Science of Climate

Quiz #N �  1. The Mean Meridional circulation at 15 N

transports moisture,

�  a) toward the North Pole, b) toward the equator, or c) neither, its zero there.

�   

Page 6: Science of Climate

Quiz #N �  2. The largest transport of energy by the atmosphere at 50N

is,

�  a) potential energy transport by the mean meridional circulation, b) latent heat flux by eddies, c) internal energy transport by transient eddies, or d) potential energy transport by stationary waves.

Page 7: Science of Climate

Quiz #N �  3. The poleward flux of moisture by eddies is greatest near,

�  a) 15N/S, b) 30N/S, c) 40N/S, or d) 50N/S. ______

�   

Page 8: Science of Climate

Quiz #N �   4. The two largest terms in the energy balance of the global

atmosphere are,

�  a) Radiative heating and cooling by evaporation, b) Meridional transport and radiative heating, c) Latent heating and radiative cooling, or d) solar absorption and longwave emission.

LE=LP = 80, SH = 20, Ra = –100Wm-2

Page 9: Science of Climate

Quiz #N �   5. True or False: The global mean precipitation rate is

constrained by the rate at which radiation cools the atmosphere, minus the rate at which sensible heat flux heats the atmosphere.

LE=LP = 80, SH = 20, Ra = –100Wm-2

Ra + LE + SH = 0LE = −Ra − SHLE = RCRa − SHRCRa = −Ra

Page 10: Science of Climate

Quiz #N �  6. True or False: Angular momentum is moved poleward

across 30N by the Hadley Circulation.

�  ______

Eddies pump angular momentum to middle latitudes!!

Page 11: Science of Climate

Gulf Stream �  Gulf Stream

�  Boundary between Warm and Cold SST

�  Strong currents

�  Geostrophic currents shown

0

0.10.2

0.3 0.4 0.5Pr

essu

re (de

cibars

)

Latitude35 36 37 38 39 40 41

0

500

1000

1500

0 0.1 0.2 0.3 0.40.5

0.6

Pres

sure

(decib

ars)

Latitude35 36 37 38 39 40 41

0

500

1000

1500

46

812

16

20

January

4

6812

August

Fig. 7-11 Eastward geostrophic ocean current (black contours and shading) and potential temperature isolines (red contour lines) for January and August along a meridional cross section at 65W where the Gulf Stream travels approximately eastward. Current data are in meters per second and temperatures in ˚C. Temperature, pressure and salinity data from MIMOC were used to compute the density.

Page 12: Science of Climate

Structure of Gulf Stream �  Almost 2 m/s,

which is screaming for an ocean current. (how far would you drift in one day?

�  17.3 kilometers ~11 miles

�  How fast can you swim?

Page 13: Science of Climate

Gulf Stream

�  SST

Fig. 7-12 SST in the northwestern Atlantic showing meanders and rings in the Gulf Stream. (Courtesy of Dr. Otis Brown)

Page 14: Science of Climate

Gulf Stream Meanders and Rings �  SST Maps: Swordboats

Page 15: Science of Climate

Gulf Stream Meanders and Rings �  SST Maps: Rings are waves and vortices in

currents, too

Page 16: Science of Climate

Gulf Stream

�  Eddies

!Fig.!7'13!!Daily!sea!surface!temperature!in!the!western!Atlantic!for!three!days!in!February!2012,!plus!the!three'month!January'March!climatology!for!SST.!!Data!from!NOAA!OI!SST!high!resolution!data!set.!

19 Feb. 2012 22 Feb. 2012

25 Feb. 2012 January-March Climatology80W 70W 60W 50W 80W 70W 60W 50W

30N

40N

30N

40N

Page 17: Science of Climate

SST: Deviations from Zonal Average

�  Where is it warm and where is it cold, and why?

Page 18: Science of Climate

Cold Eastern Oceans & Stratus Clouds

Notice the correspondence between relatively cold SST and Low cloud fraction, especially in the subtropics. This is really important for climate and climate change sensitivity. Why, do you think?

Page 19: Science of Climate

Ekman Solution �  Ekman Spiral

Page 20: Science of Climate

Equatorial Pacific �  Sloping thermocline across Equatorial Pacific,

associated with Walker Circulation, Trade Winds, etc. This sets the stage for el Niño.

Page 21: Science of Climate

Ekman Layer Theory �  On a rotating planet, when the wind blows toward

the pole, the water flows to the east.

�  When the wind blows, the water flows to the right in the NH and to the left in the SH, due to the Coriolis acceleration.

U E = uE dz

−∞

0

∫ =τ y

ρo f; VE = υ E dz

−∞

0

∫ = −τ x

ρo f

Page 22: Science of Climate

Eastern Boundary Currents �  California Current, strong in summer.

�  If the winds are northerly along the west coast of the USA, what direction does the surface Ekman drift go?

�  West! if it can.

�  This Drives upwelling of cold water.

Page 23: Science of Climate

Eastern Boundary Currents �  Peru Current, strong in summer January in SH.

�  If the winds are northerly along the west coast of the Peru, what direction does the surface Ekman drift go?

�  West! if it can.

�  This Drives upwelling of cold water.

Page 24: Science of Climate

Equatorial Upwelling �  If the wind blows easterly along the equator, the

water north of the equator flows northward and the water south of the equator goes south, creating a divergence of the surface currents, which must be balanced by the upwelling of water from below.

Equator

N

WindsCurrents

E

Page 25: Science of Climate

SST and Wind Maps: Pacific �  SST and Winds

Billy Kessler

Page 26: Science of Climate

Equatorial Upwelling �  Tropical

Instability Waves

�  unstable waves develop on the sharp current and SST gradients along the “cold Tongue” in the equatorial East Pacific.

Page 27: Science of Climate

Chlorophyl: Upwelling Nutrients

�  Chlorophyl

Page 28: Science of Climate

Salinity: Upwelling less saline water �  Less salty at equator and in extratropics

Salty Atlantic

Fresher Water from CA Current

Fresher Water from Peru Current

Page 29: Science of Climate

Thanks!

Salty Atlantic

Fresher Water from CA Current

Fresher Water from Peru Current

Page 30: Science of Climate

Oxygen Saturation

�  Oxygen Saturation indicates time since air was at surface.

�  Less O2, longer time since air was at surface.

�  Pacific water at depth much ‘older’ than Atlantic water.

559045

40

95100

40

35

30

85

Depth

(mete

rs)

0

200

400

600

800

100065 70

856065

7570

75

Depth

(mete

rs)

−80 −60 −40 −20 0 20 40 60 80

2000

3000

4000

5000

80

90 95

15

100 100

85

100

75

Depth

(mete

rs)

0

200

400

600

800

1000

1015202530354045

50 505555

85

60

10

Depth

(mete

rs)

Latitude−80 −60 −40 −20 0 20 40 60 80

2000

3000

4000

5000

40

30

60

Atlantic

Pacific

Page 31: Science of Climate

Southern Ocean

�  Oxygen Saturation (color) and potential density (black contours).

�  Circulation can be diagnosed.

�  Water at depth does not cross isopycnals! Very slow diffusive mixing

Depth

(mete

rs)

80S 60S 40S 20S Eq 20N 40N 60N 80N

0

1000

2000

3000

4000

5000 0

20

40

60

80

100

Depth

(mete

rs)

80S 60S 40S 20S Eq 20N 40N 60N 80N

0

1000

2000

3000

4000

5000 0

20

40

60

80

100De

pth (m

eters)

Latitude

80S 60S 40S 20S Eq 20N 40N 60N 80N

0

1000

2000

3000

4000

5000 0

20

40

60

80

100

Global Ocean: Zonal Average

Atlantic Ocean: 30˚ West

Pacific Ocean: 165˚ West

27.8

27.8

27.8

27.6

27.6

27.6

Page 32: Science of Climate

Deep Circulation

Page 33: Science of Climate

Sargasso vs Norwegian Seas

−5 0 5 10 15 20 25

0

200

400

600

800

1000

1200

1400

1600

1800

2000

Potential Temperature

Pres

sure

Potential Temperature Profiles in January at lat=75, lon= 0

T 25N, 40WT 75N 0W

Sargasso Sea 25N, 40W

Norwegian Sea 75N, 0W

Mixed Layer

Where is the mixing deep?

Thermocline

Page 34: Science of Climate

Questions about Oceans �  How can fish survive in frozen lakes?

�  The density of seawater at high latitudes is mostly controlled by what?

�  Explain how evaporation mixes the surface layer of the ocean.

�  Explain why upwelling occurs in the eastern equatorial Pacific

�  Why does ocean water drift toward the equator at 30N?

�  What is the Atlantic Meridional Overturning Circulation?

�  Where and how is deep water formed?

Page 35: Science of Climate

�  Annual Mean SST distribution

SST Climatology

Warm Pool

Cold Tongue

Page 36: Science of Climate

Equatorial Pacific �  Sloping thermocline across Equatorial Pacific,

associated with Walker Circulation, Trade Winds, etc. This sets the stage for el Niño.

Potential Temperature at Latitude = 0 months=JAN−DEC

Depth

(mete

rs)

Longitude

50 100 150 200 250 300 350

0

50

100

150

200

250

300

350

400

5

10

15

20

25

Afric

a

Sout

h Am

erica

Indo

nesia

Page 37: Science of Climate

ENSO Warm Event

�  We are transitioning from La Niña to El Niño

Page 38: Science of Climate

Subsurface Heat Anomalies

Page 39: Science of Climate

Niño Indices

Page 40: Science of Climate

El Niño and La Niña

Page 41: Science of Climate

El Niño and La Niña

Page 42: Science of Climate

El Niño and La Niña

Page 43: Science of Climate

El Niño and La Niña

Page 44: Science of Climate

El Niño (warm event) is predicted

Page 45: Science of Climate

New Topic: Natural Climate Change

�  Solar Variability

�  Volcanic Eruptions, Asteroid impacts

�  Orbital Parameters

Page 46: Science of Climate

Total Solar Irradiance �  The solar constant 1361 Wm-2 at average distance

of Earth from Sun. This is down from estimate in 1994.

�  TSI varies with sunspots, more spots higher TSI, but only by 0.1%

�  Spots are darker and colder, but bright spots around dark spots slightly over match the dark spots, giving a net increase.

�  Shorter wavelengths vary more than total energy flux, thus lots of sunspots means more high energy photons and particles.

Page 47: Science of Climate

Total Solar Irradiance �  The solar constant 1361 Wm-2 at average distance

of Earth from Sun. This is down from estimate in 1994.

�  TSI varies with sunspots, more spots higher TSI, but only by 0.1%

Page 48: Science of Climate

Total Solar Irradiance �  The solar constant 1361 Wm-2 at average distance

of Earth from Sun. This is down from estimate in 1994.

�  TSI varies with sunspots, more spots higher TSI, but only by 0.1%

Page 49: Science of Climate

Electrical Substitution Radiometer (AKA Active Cavity Radiometer)

�  A reference cavity radiometer and a measurement one are maintained at the same temperature.

�  When one is exposed to the sun, you know how much energy you have to supply via electrical resistance heating to maintain the temperature, and hence the amount of energy being lost out the space view.

Page 50: Science of Climate

Electrical Substitution Radiometer (AKA Active Cavity Radiometer)

�  A reference cavity radiometer and a measurement one are maintained at the same temperature.

�  When one is exposed to the sun, you know how much energy you have to supply via electrical resistance heating to maintain the temperature, and hence the amount of energy being lost out the space view.

Page 51: Science of Climate

Sunspots & TSI �  Sunspots have been observed a long time.

�  You can use the relationship between sunspots and TSI in the previous figure to estimate TSI values prior to observations of it.

1 Wm-2

Page 52: Science of Climate

TSI forcing since Preindustrial Times

�  1 Wm-2 TSI change is about 0.175 Wm-2 Climate Forcing

�  Compared to 4 Wm-2 for doubling CO2 or about 2.7 Wm-2 human forcing since 1750.

�  It is small, unless high energy stuff does more than expected. Shortwave uv does affect ozone production in stratosphere.

ΔForcing = ΔS04

1−α p( ) = 1Wm−2

41− 0.3( ) = 0.175Wm−2

Page 53: Science of Climate

Volcanic Eruptions �  Volcanoes can spew large amount of SO2, sulfur

dioxide gas into the stratosphere

�  Where it is oxidized a couple times to form sulfuric acid H2SO4, which condenses into tiny droplets that reflect solar and absorb infrared.

�  The net effect of these small droplets is to reflect more solar radiation than they trap IR.

�  Even if they absorb solar radiation, they do so above the water vapor greenhouse and so cool the surface.

Page 54: Science of Climate

Volcanic Eruptions �  To be effective at cooling the climate, volcanic

eruptions must

�  1. Be explosive, so they throw a lot of stuff into the stratosphere.

�  2. Contain a lot of sulfur, so that they form lots of sulfuric acid aerosols in the stratosphere.

�  3. It’s best for cooling if they occur in the tropics where, �  a. there is lots of solar radiation to reflect �  b. The aerosols stay longer in the atmosphere, since

the stratosphere is flushed out in high latitudes in the Brewer-Dobson circulation

Page 55: Science of Climate

Volcanic Aerosols �  SO2 is the big item, most other stuff falls out

Page 56: Science of Climate

Volcanic Eruptions

�  History of eruptions

�  Quantitative observations only for past two major eruptions.

Page 57: Science of Climate

Radiative Effects �  Net Cooling

Page 58: Science of Climate

Quantitative Assessment �  We had a very good observing system for Pinatubo

in 1991, when we were measuring both the aerosols (SAGE) and the Earth’s Energy Balance (ERBE).

�  We can test our models to see if they produce the observed response.

�  We can test the effect of feedbacks like water vapor feedback, and the model simulation of them.

Page 59: Science of Climate

Quantitative Assessment

�  We had a very good observing system for Pinatubo in 1991, when we were measuring both the aerosols (SAGE) and the Earth’s Energy Balance (ERBE).

�  We can test our models to see if they produce the observed response.

�  We can test the effect of feedbacks like water vapor feedback, and the model simulation of them.

Soden, et al. 2011, Science

Page 60: Science of Climate

Model Tests �  Observed and predicted Temperature and Humidity

Response

�  Model gets Surface response and atmospheric vapor response as observed.

Page 61: Science of Climate

Model Tests �  Observed and predicted Temperature and Humidity

Response

�  Model gets Surface response and atmospheric vapor response as observed.

Page 62: Science of Climate

Model Validation �  Water vapor feedback is important to getting the

surface response correct

Page 63: Science of Climate

Model Validation �  Water vapor feedback is important to getting the

surface response correct

Page 64: Science of Climate

Thanks!