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Assume geostrophic balance on -plane approximation, i.e.,

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Presentation on theme: "Assume geostrophic balance on -plane approximation, i.e.,"— Presentation transcript:

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2 Assume geostrophic balance on -plane approximation, i.e.,
( is a constant) Vertically integrating the vorticity equation barotropic we have The entrainment from bottom boundary layer The entrainment from surface boundary layer We have where

3 Quasi-Geostrophic Approximation
Quasi-geostrophic approximation has three components (1) The β-plane apporximation (2) Small surface deviation (3) Geostrophic approximation in terms of fo Basic condition

4 Quasi-Geostrophic Approximation
Potential Vorticity Quasi-Geostrophic Potential Vorticity Quasi-Geostrophic Potential Vorticity Equation Defines the evolution of geostrophic stream function ψ

5 Quasi-Geostrophic Approximation
If we ignore the surface change (or have a rigid lid), we have the absolute vorticity conservation, i.e.,

6 What does QG momentum equation look like?
Continuity equation is ageostrophic flow is responsible for the divergence in the QG system has a rotational component is totally determined by geostrophic flow at any given instance

7 Quasi-Geostrophic Approximation
Replace the relative vorticity by its geostrophic value Approximate the horizontal velocity by geostrophic current in the advection terms Under -plane approximation, f=fo+y, we have

8 Quasi-geostrophic vorticity equation
and , we have For and where (Ekman transport is negligible) Moreover, We have where

9 Boundary Value Problem
Boundary conditions on a solid boundary L (1) No penetration through the wall (2) No slip at the wall

10 Quasi-geostrophic vorticity equation
where Boundary conditions on a solid boundary L (1) No penetration through the wall (used for the case of no horizontal diffusion) along the boundary L (2) No slip at the wall along the boundary L n is the unit vector perpendicular to the boundary L

11 Different terms are important at different places of the basin
f-plane -plane

12 Non-dimensionalize Quasi-Geostrophic Vorticity Equation
Define non-dimensional variables based on independent scales L and o The variables with primes, as well as their derivatives, have no unit and generally have magnitude in the order of 1. e.g.,

13 Note that U has not been decided yet.

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16 Non-dmensional vorticity equation
If we choose we have Sverdrup relation Define the following non-dimensional parameters , nonlinearity. , , bottom friction. , , lateral friction. ,

17 Interior (Sverdrup) solution
If <<1, S<<1, and M<<1, we have the interior (Sverdrup) equation: (satistfying eastern boundary condition) (satistfying western boundary condition) Example: Let , . Over a rectangular basin (x=0,1; y=0,1)

18 Westward Intensification
It is apparent that the Sverdrup balance can not satisfy the mass conservation and vorticity balance for a closed basin. Therefore, it is expected that there exists a “boundary layer” where other terms in the quasi-geostrophic vorticity is important. This layer is located near the western boundary of the basin. Within the western boundary layer (WBL), , for mass balance The non-dimensionalized distance is , the length of the layer  <<L In dimensional terms, The Sverdrup relation is broken down.

19 The Stommel model Bottom Ekman friction becomes important in WBL.
at x=0, 1; y=0, 1. No-normal flow boundary condition (Since the horizontal friction is neglected, the no-slip condition can not be enforced. No-normal flow condition is used). Interior solution

20 , we have Let Re-scaling in the boundary layer: Take into
As =0, =0. As ,I

21 can be the interior solution under different winds)
The solution for is , .  A=-B , ( can be the interior solution under different winds) For , , . For , , .

22 The dynamical balance in the Stommel model
In the interior, Vorticity input by wind stress curl is balanced by a change in the planetary vorticity f of a fluid column.(In the northern hemisphere, clockwise wind stress curl induces equatorward flow). In WBL, Since v>0 and is maximum at the western boundary, , the bottom friction damps out the clockwise vorticity. Question: Does this mechanism work in an eastern boundary layer?


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