The dominant periodicities are the same as those from astronomical calculations of changes in the...

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The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.
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Transcript of The dominant periodicities are the same as those from astronomical calculations of changes in the...

Page 1: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

Page 2: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

Our Planet’s Music has Many Beats:

(a) 1 DAY: Day- Night – Day Spins around its axis

(b) 1 Year: Winter – Summer – Winter Orbits the Sun

(c) 23,000 Years: Stronger Summer, Stronger Winter Precession

(d) 40,000 Years: Tilted axis rocks back and forth OBLIQUITY

(e) 100,000 Years: Eccentricity of the orbit varies

MILANKOVITCH CYCLES

SUN

Page 3: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

Seasonal Changes in Sunlight as a function of latitude:

ANNUAL Average

PRECESSION redistributes

sunlight in time so that the

the average over a year is

zero

OBLIQUITY redistributes

sunlight latitudinally so that

the average over the globe

is zero.

Page 4: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

WARM

COOLING TREND + AMPLIFYING 40K CYCLES

NONLINEAR

40 .. 80 .. 120K

THRESHOLD THRESHOLD ?

40K WORLD

Vt+1 - Vt = a + bt + c(Vt – V*) Obliquity(t)

0 1 2 3 4 5 6

x 106

1

1.2

1.4

1.6

1.8

2

2.2

2.4

2.6

2.8

3x 10

7

time

tem

perature

temperature versus time

Page 5: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

Ice Ages:

19th Century: Evidence for Ice Ages in the northern Hemisphere

Milankovitch: ICE ALBEDO

Sunlight at 65N in July is the controlling factor

Why is precession unimportant? Huybers

What causes the 110K cycle?

There is no 100K cycle! 40K…80K….120K..

Huybers and Wunsch

What caused the huge cycles of the past million years?

What feedbacks other than ice-albedo increased climate sensitivity?

Measurements in low latitudes provide an unexpected answer!!

Page 6: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

OBSERVATIONS: Obliquity variations affect mostly high latitudes….glaciers

Precession affects mostly low latitudes …. monsoons

Surprising Recent Observations:

The tropical Pacific responds mainly to Obliquity!

The records for SST are very similar to Ice Volume records

Page 7: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

~ 3 Ma Cold Surface Waters Start Appearing in Low Latitudes

Page 8: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

March 1998 - El Niño Apparently conditions similar to these persisted up to 3 million years ago

October 1988 - La Niña

Page 9: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

Tropical Sea Surface Temperature patterns strongly influence Rainfall patterns and hence the global climate.

Sea Surface Temperatures (Degrees Centigrade)

Page 10: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

W E W E

Dep

th

Latitude

Temperature along a section in the mid-Pacific (152W)

El Nino La NinaAdiabatic:

_ _ _ _ _ _ _ __________ El Padre La MadreDiabatic:

_ _ _ _ _ _ _ ______________

1000m

4000m

A shallow thermocline permits two different processes for varying

sea surface temperatures

Diabatic:

_ _ _ _ _ _ _ ______________

Diabatic:

_ _ _ _ _ _ _ ______________

Diabatic:

_ _ _ _ _ _ _ ______________

Diabatic:

_ _ _ _ _ _ _ ______________

Diabatic:

_ _ _ _ _ _ _ ______________

Diabatic:

_ _ _ _ _ _ _ ______________

Diabatic:

_ _ _ _ _ _ _ ______________

Diabatic:

_ _ _ _ _ _ _ ______________

Diabatic:

_ _ _ _ _ _ _ ______________

Diabatic:

_ _ _ _ _ _ _ ______________

Page 11: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

To remain cold, the ocean

must have a circulation

Page 12: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

An Easterly Wind blowing over a Rotating, Spherical Shell of Fluid maintains a Meridional Overturning Circulation

winds

Page 13: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

How the Flux of Heat across the Ocean Surface affects its Subsurface thermal structure.

Page 14: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

The Response, the Heat Gain, increases in amplitude as the Period of the forcing increases. Note that there is also a change in the phase of the response.

Response to Imposed Changes in Heat Loss in high latitudes. In the Four Different experiments the amplitude of the forcing remains constant but the period changes from 2 to 5 to 10 to 20 years.

2 years 5 Years

20 Years10 Years

Page 15: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

Heat Flux across the Ocean Surface

Page 16: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

IN A WARM WORLD: A small oceanic heat loss implies a small oceanic heat gain which requires a deep tropical thermocline.

IN A COLD WORLD ……. A large oceanic heat loss implies a large oceanic heat gain which requires a shallow tropical thermocline.

The Heat Budget determines the Depth of the Oceanic Thermocline

The ocean acts as a low pass filter:

The seasonal cycle in high latitudes can not induce

a seasonal cycle at the equator

Page 17: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

UP to 3 Million Years Ago: Drifting continents cause Global Cooling

Shoaling Thermocline

Around 3 Million Years Ago: Glaciers Appear in high northern latitudes

Ice albedo feedback

Cold Surface Water appear in low latitudes

air-sea interactions and stratus cloud feedback

3 Million Years ago onward: Trend in global ice volume

shoaling of the thermocline*

expansion of stratus clouds

oceanic salinity

Amplification of 40K Oscillations

Page 18: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

THE ROLE OF SALINITY TEMPERATURE SALINITY

• Salinity introduces an indirect mechanism for interfering with the oceanic heat budget

The MELTING of ICE, and variations in EVAPORATION and RAINFALL can profoundly affect the oceanic circulation, hence

Sea Surface Temperatures and the Global Climate.

1. Salinity and temperature have comparable effects on density.

2. The effects of temperature and salinity are in opposition because of heavy rainfall in cold high latitudes. (This introduces the possibility of singularities.)

3. Boundary conditions for temperature and salinity are different Heat Flux = a(T – T*) …. negative feedback! Salt Flux = b(Evaporation – Precipitation) No negative feedback.

Page 19: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

Surface Salinities

Page 20: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

The Slow, Deep Thermohaline Circulation

The Shallow, Swift Wind-driven Circulation

Antarctic Circumpolar Current

D = k1/3

D2 = D*2 + /T..

Page 21: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.
Page 22: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

.

Page 23: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

Temperature

Along the Equator Looking Down

Numerical Experiments in which the oceanic

surface waters are freshened in high latitudes.

Fedorov JPO

Hea

t T

rans

port

Freshening m/year

Page 24: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

1.022

1.024

1.026

1.028

Sur

face

Den

sity

gm

/cm

3

Page 25: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.
Page 26: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

41 K WORLD Nonlinear WorldWarm World

Threshold

Warm World (El Nino?)

Trend + Cycles

Page 27: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.

Since 3 Ma, feedbacks (glaciers, tropical stratus clouds) caused

Cooling Trends

that led to

Thresholds

followed by

Rapid Warming

followed by

Cooling Trend

Milankovitch forcing (Obliquity) is a pace maker

Page 28: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.
Page 29: The dominant periodicities are the same as those from astronomical calculations of changes in the Earth’s orbital parameters.