aoss 401, fall 2007 lecture 27 november 28 , 2007

61
AOSS 401, Fall 2007 Lecture 27 November 28, 2007 Richard B. Rood (Room 2525, SRB) [email protected] 734-647-3530 Derek Posselt (Room 2517D, SRB) [email protected] 734-936-0502

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AOSS 401, Fall 2007 Lecture 27 November 28 , 2007. Richard B. Rood (Room 2525, SRB) [email protected] 734-647-3530 Derek Posselt (Room 2517D, SRB) [email protected] 734-936-0502. Class News November 28 , 2007. Homework 7 (Posted tomorrow, Thursday) Due Next Friday Important Dates: - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

AOSS 401, Fall 2007Lecture 27

November 28, 2007

Richard B. Rood (Room 2525, SRB)[email protected]

734-647-3530Derek Posselt (Room 2517D, SRB)

[email protected]

Page 2: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Class News November 28, 2007

• Homework 7 (Posted tomorrow, Thursday)– Due Next Friday

• Important Dates: – December 10: Final Exam– December 7:

• Go over homework• Review session

– December 5: Hurricanes• Joint with AOSS 451

Page 4: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Material from Chapter 11

• Tropics– Tropics versus middle latitudes– Features of the tropical circulation

• Tropical scale analysis

• Tropical waves– Kelvin waves– Equatorial Rossby Waves– Mixed Rossby-gravity Waves

Page 5: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Picture of Earth: What can you say about this figure?

Page 6: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

What are the differences between the tropics and the middle latitudes on Earth?

• Tropics:– The area of the tropics – say + and – 30

degrees latitude is half the area of the Earth.– Might say the tropics is + and – 20 degrees of

latitude, and subtropics are between 20 and 30 degrees of latitude.

• The importance of rotation, the Coriolis parameter.

• What else is different?

Page 7: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

)sin(2constant

earth) theof radius=(a )-(=with

a

)cos(2=

:ionapproximat plane- eMidlatitud

)sin(2

00

0

0000

0

f

ay

yfyfyy

fff

f

Let’s think about the Coriolis parameter

Page 8: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

0constant

earth) theof radius=(a 0 )-(=with

a

)cos(2=

:ionapproximat plane- Tropical

)sin(2

0

00

0

0

f

ay

yyyy

ff

f

Coriolis parameter in the tropics

What latitude is coriolis parameter, say, 10% of mid-latitude value?

Page 9: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Recall our idealized Rossby wave equation and middle latitude scale analysis

Page 10: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Perturbation equation: Barotropic Rossby wave at middle latitudes

xxu

t

vvuuu

vfDt

D

g

ggggg

gg

2

02

)(

equation of formon perturbati

;

Page 11: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Wave like solutions

0))((

)Re(

)(

22

)(0

2

klkuk

e

xxu

t

g

tlykxi

g

Where does the coriolis parameter appear in this equation?

Page 12: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Coriolis force

• The coriolis parameter decreases to zero at the equator.– Approximated by X distance from the

equator.

• We see from our wave equation and the conservation of vorticity that is a parameter of central importance to the dynamics– Advection of planetary vorticity.

Page 13: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Recalling our simple wave solution and comparing

advection of planetary and relative vorticity.

))2

()2

((

coscos)()(

coscos)(

22

22

yx

gg

g

gg

g

LLU

v

lykxpAlkUk

lykxpkAv

V

V

Page 14: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Coriolis force

• Can we say that the advection of planetary vorticity is less important?– We will come back to this.

Page 15: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Differences between the tropics and middle latitudes

• What are other differences?

Page 16: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Differences between the tropics and middle latitudes

• The contrast between summer and winter is not as large as at middle and high latitudes.– There is lot of solar heating.

• There is a lot of water!– What is the “physical” difference between water and

land?– Sea surface temperature is important to dynamics.

• What happens to water when it is warm?

Page 17: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Let’s think about waves some more

• We assume that dependent variables like u and v can be represented by an average and deviation from the average.

vuvuvuvuuv

vvuuuv

vvvuuu

))((

and

Page 18: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Let’s think about waves some more

• Some fundamental ideas

)( average

linearized 0.01,order

ignore then ,1.0~say "small," are onsperturbati

))((

and

vuavevuave(uv)

vuvuvuuvvu

vuu

u

vuvuvuvuuv

vvuuuv

vvvuuu

Page 19: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Let’s think about waves some more

• Some fundamental ideas.– Waves have some sort of restoring force

• Buoyancy waves: gravity• Rossby waves: The gradient of planetary vorticity

– Think about the conservation of potential vorticity

– Waves tend to grow and decay at the expense of the “energy” in the mean state.

– Waves tend to respond to out of balance situations.– Waves tend to move things towards equilibrium– Waves propagate

• So they can communicate things happening in one part of the fluid to far away places.

Page 20: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

In middle latitudes:

• How do the Rossby waves that cause weather, the synoptic waves, get their energy?

Page 21: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Energetics of Midlatitude Cyclone Development

• The jet stream is commonly associated with strong temperature gradients in the middle/lower troposphere (thermal wind relationship)

• Midlatitude cyclones develop along waves in the jet stream

• Midlatitude cyclones are always associated with fronts (Norwegian cyclone model)

• There is a link between temperature gradients and cyclone development…

Page 22: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Idealized vertical cross section

Page 23: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Two important definitions

• barotropic – density depends only on pressure. – By the ideal gas equation, surfaces of constant

pressure are surfaces of constant density are surfaces of constant temperature (idealized assumption). = (p)

• baroclinic – density depends on pressure and temperature (as in

the real world). = (p,T)

Page 24: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Barotropic/baroclinic atmosphere

Barotropic: pp + pp + 2p

pp + pp + 2p

T+2TT+TT

T

T+2TT+T

Baroclinic:

ENERGY HERE THAT IS CONVERTED TO MOTION

Page 25: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Barotropic/baroclinic atmosphere

Barotropic: pp + pp + 2p

pp + pp + 2p

T+2TT+TT

T

T+2TT+T

Baroclinic:

DIABATIC HEATING KEEPS BUILDING THIS UP

Page 26: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Lifting and sinking

There are massive amounts of available energy in these sloping surfaces.And what do waves want to do?

Page 27: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Barotropic/baroclinic atmosphere

• Energetics:– Baroclinic = temperature contrast = density

contrast = available potential energy– Extratropical cyclones intensify through

conversion of available potential energy to kinetic energy

Page 28: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Energetics in the atmosphere

Ability to convert potential energy to kinetic energy directly related to tilt with height (offset) of low/high pressure

Page 29: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Tropics and middle latitudes

• In middle latitudes the waves grow from the energy available in the baroclinic atmosphere.– horizontal temperature gradients

• scale is large• latent heat release is on scales small compared to

baroclinic energy convergence.

• In the tropics the horizontal temperature gradients are small.

Page 30: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

An estimate of the January mean temperature

northwinter

southsummer

tropopause

stratopause

mesosphere

stratosphere

troposphere

note where the

horizontal temperature gradients are

large

Page 31: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Tropics and middle latitudes

• Baroclinicity is less important in the tropics– Latent heat release is generally most

important.

– What does this mean?

Page 32: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Equations of motion in pressure coordinates(using Holton’s notation)

written)explicitlynot (often

pressureconstant at sderivative horizontal and time

; )()

re temperatupotential ; velocity horizontal

ln ;

0)(

Dt

Dp

ptDt

D( )

vu

pTS

p

RT

p

c

JST

t

TS

y

Tv

x

Tu

t

T

ppy

v

x

u

fDt

D

pp

p

ppp

p

V

jiV

V

V

VkV

Page 33: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

What does importance of latent heat release mean.

• Diabatic processes are more important in the tropics.

• Hence, vertical velocity is more strongly related to diabatic heating than to temperature advection.– What about divergence?

• The scale of the forcing of motions is small– Related to the phase change of water.

Page 34: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Picture of Earth: What can you say about this figure?

Page 35: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Inter-tropical Convergence Zone(ITCZ)

Page 36: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

ITCZ Circulation

Page 37: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

A couple of things to note

• The winds at the surface in the tropics are, on average, easterly, from the east, towards the west.

• Go back to our mid-latitude wave:– What does this say about waves in the

tropics?– Well, it says, they are different!

• (Not that they don’t exist!)

Page 38: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

ITCZ: Seasonal differences

Page 39: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

ITCZ: Seasonal differences

What is happening here and here?

Page 40: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

South American Seasonal Cycle

CONVECTION GOES WILD

Page 41: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Cloud Liquid Water: Average

NOTE: Remarkable areas with no clouds! No rain!

Page 42: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Vertical circulation around the ITCZ

What is the direction of the zonal wind?

Page 43: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

ITCZ: Seasonal differences

What is happening here and here?

Page 44: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Monsoonal Flow

Page 45: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Lets return to our simple problem

Earth’s surface

warmcore

coldcore

PGF HL

LH PGF

DIVERGENCE

CONVERGENCE

CONVERGENCE

DIVERGENCE

LANDOCEANSUMMER TIME

Page 46: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Lets return to our simple problem

Earth’s surface

warming

cooling

PGF H

L

LH PGF

Earth’s surfaceLANDOCEAN

SUMMER TIME

Page 47: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Monsoonal Circulation

• Driven by land-sea temperature contrast.

• Reversal of flow from summer to winter.

• Tremendously important to precipitation.

• South and East Asian monsoon among most important of circulation features.

Page 48: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Circulation features of the tropics

• Inter-tropical convergence zone– Hadley circulation

• Monsoonal circulations

• Madden-Julian Oscillation

• African easterly waves

• Walker circulation

• El Nino and La Nina

Page 49: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Madden-Julian Oscillation

OLR = outgoing longwave radiation.Cold is the top of the clouds.Cold is the top of the hot towers.

Page 50: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

African easterly waves

Page 51: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

African easterly waves

What is happening here and here?

That’s north Africa. It’s summer.

Page 52: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

African easterly waves

• The Sahara gets SO HOT, that the meridional temperature gradient is important.– But it is reversed over our normal thinking!

Page 53: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

So let’s think about these scales of motion.

Page 54: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Equations of motion in pressure coordinates(using Holton’s notation)

written)explicitlynot (often

pressureconstant at sderivative horizontal and time

; )()

re temperatupotential ; velocity horizontal

ln ;

0)(

Dt

Dp

ptDt

D( )

vu

pTS

p

RT

p

c

JST

t

TS

y

Tv

x

Tu

t

T

ppy

v

x

u

fDt

D

pp

p

ppp

p

V

jiV

V

V

VkV

Page 55: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Scale factors for “large-scale” mid-latitude

s 10 /

m 10

m 10

! s cm 1

s m 10

5

4

6

1-

-1

UL

H

L

unitsW

U

1-1-11-

14-0

2

3-

sm10

10

10/

m kg 1

hPa 10

y

f

sf

P

Page 56: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Introduce another vertical coordinate.

Dt

Dzw

H

z

p

pHz

s

s

**

)*

exp(

)ln(*

0

Page 57: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Equations of motion in log pressure coordinates(using Holton’s notation)

*

*)()

velocity horizontal

* ;

*

**

0*

*1)(

**

2

2

0

0*

zw

tDt

D( )

vu

Hc

RT

z

T

H

RN

H

RT

z

Hc

RJwN

zyv

xu

t

z

w

y

v

x

u

fDt

D

zz

p

p

z

V

jiV

VkV

Page 58: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Scale factors for “large-scale” tropics

LHUW

UL

H

L

U

/

s 10 /

m 10

m 10

s m 10

5

4

6

-1

y

f

sf

15-0 10

Page 59: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Scaling: Momentum Equation

/)/(

1Ro/1/)/(

1)/()/(*

*

1)/(

/

2

2

U

UfLf

UHWLz

w

t

LU

VV

VVVk

VVV

VVV

VV

Page 60: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

Scaling: Momentum equation

• Geostrophic balance is not dominant.– How many km from the equator is geostrophic term no longer

small?– What about ?

• If the pressure gradient is balanced in the momentum equation, then ...

2U

Page 61: AOSS 401, Fall 2007 Lecture  27 November  28 , 2007

This means something!

• For a similar scale disturbances in the tropics and middle latitudes the geopotential perturbation is a smaller by an order of magnitude in the tropics.

• What does this mean– for the scales of motion?– for the important physical terms?