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Rossby waves

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(1)

1. Introduction

2. Physical concept

3. Dispersion relation (for shallow water system)

Rossby waves

Jin and Hoskins (1995)

(2)

Rossby waves

Stationary waves

Pacific North American (PNA) pattern from JISAO (U. Washington)


wave Source

Forced Rossby waves

Warm Arctic Cold Eurasian (WACE) Pattern

Kim et al. (2014)

(3)

Rossby waves

Stationary waves

(Charney and Eliasson, 1949 Tellus 


figure from Held,1983 )

(4)

Rossby waves

Transient waves

(5)

Rossby waves

(From S. Sörlin 2015, A Tribute to the Memory of Carl-Gustaf Rossby, 1898-1957

Royal Swedish Academy of Engineering Sciences)

(6)

Physical concept

Topographic Rossby wave

Holton (2004)

D

Dt ( ζ + f

h ) = 0

(7)

Physical concept

High PV

Low

(8)

Physical concept

(9)

Physical concept

High PV

Low

(10)

Physical concept

When 


dq/dy > 0

High PV

Low

Intrinsic phases speed is easterly when dq/dy > 0

(11)

Dispersion relation ω = ω(k, l, m)

For shallow water system, PV equation

Barotropic PV equation (in β-plane) D

Dt ( ζ + f

h ) = 0

D

Dt ( ζ + f ) = 0

(12)

(from Atmosphere, Weather and Climate)

High%PV%

Low%PV%

(,)%.ve%PV%anomaly%

% %=>%an.cyclonic%circ.%%

(+)%.ve%PV%anomaly%%

%=>%cyclonic%circ.%%

Wave%propaga.on%

Newly%displaced%parcels%

%by%induced%circula.on%

Dispersion relation ω = ω(k, l, m)

(13)

(from Atmosphere, Weather and Climate)

High%PV%

Low%PV%

(,)%.ve%PV%anomaly%

% %=>%an.cyclonic%circ.%%

(+)%.ve%PV%anomaly%%

%=>%cyclonic%circ.%%

Wave%propaga.on%

Newly%displaced%parcels%

%by%induced%circula.on%

Dispersion relation ω = ω(k, l, m)

(14)

Hoskins and James (2014) Chap. 9

Stationary case 
 Potential direction 


of propagation

c g = lim

Δk→0

Δω

Δk = ∂ω

k

Group velocity (m/s)

Dispersion relation ω = ω(k, l, m)

(15)

Dispersion relation ω = ω(k, l, m)

wave

Source

Referensi

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