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Effect of Stratification

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Atmospheric dynamics 1

Effect of Stratification

(2)

Stratified fluid (atmosphere, ocean)

The Atmosphere and Ocean are good examples of 
 well stratified fluid

Image: wikiwand.com 
 ozonedepletiontheory.info

(3)

Stratified fluid (atmosphere, ocean)

The Atmosphere and Ocean are good examples of 
 well stratified fluid

Image: open.edu

(4)

Stratified fluid (atmosphere, ocean)

(Vallis, 2006; AOFD)

Fig. �.�

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Boussinesq Approximation

(Vallis section 2.4)

Notation (basic concept)

Can consider two types

1) (Boussinesq Approximation)

for a stratified ocean

2) (Anelestic Approximation)

for a stratified atmos

˜

ρ ( ¯ ρ)

ρ = ρ

0

+ ρ(z) + ̂ ρ′ (x, y, z, t) δρ

ρ = ρ

0

+ δρ(x, y, z, t)

ρ = ¯ ρ(z) + ρ′ (x, y, z, t)

(6)

Boussinesq Approximation

(Vallis section 2.4)

Basic Idea Assuming that

“Consider density perturbation only for the gravity term (ρg)

and Replace with for the other terms

ρ

0

≫ δρ ρ ρ

0

ρ Dw

Dt = − ∂ p

∂z − ρg + ρν ∇

2

w

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Boussinesq Approximation

(Vallis section 2.4)

Momentum equations

Dw

Dt = − 1

ρ

0

∂δp

∂z − δρ

ρ

0

g + ν ∇

2

w

Du

Dt − fv = − ϕ

x

Dv

Dt + fu = − ϕ

y

Dw

Dt = − ϕ

z

+ b

(8)

Boussinesq Approximation

(Vallis section 2.4)

Momentum equations

Dw

Dt = − 1

ρ

0

∂δp

∂z − δρ

ρ

0

g + ν ∇

2

w

Du

Dt − fv = − ϕ

x

Dv

Dt + fu = − ϕ

y

Dw

Dt = − ϕ

z

+ b

In fact, mostly

(1) (2) (3)

Du

Dt − fv = − ϕ′

x

Dv

Dt + fu = − ϕ′

y

Dw

Dt = − ϕ′

z

+ b′

ϕ ≡ δp

, (Buoyancy, m/s2)

ρ

0

b ≡ − δρ ρ

0

g

ϕ = ϕ(z) + ̂ ϕ′

,

b = b(z) + ̂ b′

(9)

Boussinesq Approximation

(Vallis section 2.4)

Need two more equations

(4)

(5) or

u

x

+ v

x

+ w

z

= 0 Db

Dt = . . . Db′

Dt = . . .

(10)

Boussinesq Approximation

(Vallis section 2.4)

Starting from the definition of b

where

N (Buoyancy frequency, 1/s)

Db

Dt = . . . b ≡ − δρ ρ

0

g

ρ = ρ(θ, q, p)

Dt = − ρ

0

g

c

s2

w ⇒ Db

Dt = g

2

c

s2

w Db′

Dt = − (

d b ̂

dz − g

2

c

s2

) w

≡ N

2

Adiabatic, no diffusion and displacement from 
 a well-balanced basic state (p is not disturbed)
 p = p0(z)

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Boussinesq Approximation

(Vallis section 2.4)

Summary

Du

Dt − fv = − ϕ

x

Dv

Dt + fu = − ϕ

y

Dw

Dt = − ϕ

z

+ b u

x

+ v

x

+ w

z

= 0

Db

Dt = · b

Adiabatic, no mixing case

Du

Dt − fv = − ϕ′

x

Dv

Dt + fu = − ϕ′

y

Dw

Dt = − ϕ′

z

+ b′

u

x

+ v

x

+ w

z

= 0 Db′

Dt = − N

2

w

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Buoyancy frequency (ocean)

The Atmosphere and Ocean are good examples of 
 well stratified fluid

(Vallis, 2006; AOFD)

Depth(km)

2 1 0

3

mixed layer pycnocline

abyss

~10 mins.

~20 mins.

~2–3 hours

Density Buoyancy frequency N(z)

Fig. �.��

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