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Angular Momentum Cycle 1. Balance Equations 2. Angular Momentum in the Climatic System 3. Observations 4. Closing the Cycle of Angular Momentum

Angular Momentum Cycle

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Angular Momentum Cycle. Balance Equations Angular Momentum in the Climatic System Observations Closing the Cycle of Angular Momentum. Angular momentum of a parcel with unit mass. Balance Equations The total angular momentum of the Earth remains constant. is the moment of force (torque). - PowerPoint PPT Presentation

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Page 1: Angular Momentum Cycle

Angular Momentum Cycle

1. Balance Equations

2. Angular Momentum in the Climatic System

3. Observations

4. Closing the Cycle of Angular Momentum

Page 2: Angular Momentum Cycle

Balance EquationsThe total angular momentum of the Earth remains constant

M Angular momentum of a parcel with unit mass

acrM Frdt

Md

If the total torque vanishes 0dt

Md

n

ncrrM .)(

coscos22 urrM icu .M Mr

rMMM

Fr is the moment of force (torque).

rR

smR /464Eq.:

Page 3: Angular Momentum Cycle

Angular Momentum in the Climatic System

1. Earth

s

mkgRmI ee

2332 .

1086.55

2

2a. Atmosphere (solid rotation)

s

mkgXIRmI eaa

22862 .

1001.1103

2

sphere

spherical shell

2b. Atmosphere (zonal wind, the relative angular momentum)

MM

dmuRdmM

r

r

01.0

cos Mr Mr (DJF-JJA)NH~5.31025kg m2 s-1 NH~9.41025kg m2 s-1

SH ~7.61025kg m2 s-1 SH ~-4.6 1025kg m2 s-1

me= ma~106

Page 4: Angular Momentum Cycle

3. Ocean (very coarse estimate, no reliable measurements exist)

a) Zonal circulation

450

00

100Sv

NP

-0.51025kg m2 s-1

Page 5: Angular Momentum Cycle

The observed changes of the angular momentum of atmosphere are 51025kg m2 s-1, Oceanic ones are< 11025kg m2 s-1

-600

600

12254

2

6

36

6

34

108.0

cos2cos2

skgmzR

ddzRM

b) Meridional shift of air and water masses

300

00

+ + +

z=2cm

Patm=2mb0.81025kg m2 s-1

Conclusion: Adjustment of the solid Earth‘s rotation to the rotation of fluid

Conclusion: Adjustment of the solid Earth‘s rotation to the rotation of fluid

Page 6: Angular Momentum Cycle

Because the angular momentum is conserved

atmV

e constdvurI cos

Because MrDJF > Mr

JJA , JJA > DJF

LOD[ms ]=0.168 Mr[1025kg m2 s-1]

If Mr=5x1025kg m2 s-1 LOD=0.8ms

The relative angular momentum can be computed actronomically, as well as from the observed velocities:

Mr =5x1025kg m2 s-1 correponds to u=2m s-1.

dmuRdmM r cos

Page 7: Angular Momentum Cycle
Page 8: Angular Momentum Cycle
Page 9: Angular Momentum Cycle
Page 10: Angular Momentum Cycle

Angular Momentum in the Atmosphere

Multiply the equation of momentum

...cos

Fp

dt

dca

with r

cos

1

1

Rx

RyHave in mind:

...cos

RF

p

t

M

Pressure, Friction Torques

Tropics-sourceMid-latitudes-sink of angular momentum} Meridional

Transportt

Page 11: Angular Momentum Cycle
Page 12: Angular Momentum Cycle

Observations

uvCD 0

Ship reports

Source

Sink

Page 13: Angular Momentum Cycle
Page 14: Angular Momentum Cycle
Page 15: Angular Momentum Cycle

Closing the Cycle of Angular Momentum

2

2

10 ~] [s

mvu

Wind~10ms-1

Currents~ 10-2ms-1 -10-1ms-1

2

2310~][s

mvu

410~][

][

ocean

atm

vu

vu 210~atm

ocean

m

m

Small contribution of the oceanic transport

Page 16: Angular Momentum Cycle
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Page 18: Angular Momentum Cycle