The University of Southampton
University of Southampton Institutional Repository

Isopycnal averaging at constant height. Part II: relating to the residual streamfunction in Eulerian space

Isopycnal averaging at constant height. Part II: relating to the residual streamfunction in Eulerian space
Isopycnal averaging at constant height. Part II: relating to the residual streamfunction in Eulerian space
In Part I , the “vertical” transport streamfunction was defined as resulting from isopycnic averaging at constant height in the same way that the meridional streamfunction results from averaging at constant latitude. Part II here discusses the relationship between these two isopycnic streamfunctions and the Eulerian residual streamfunction that arises from the transformed Eulerian mean (TEM). It is known that the meridional isopycnic streamfunction can be approximated by a Taylor expansion to give an Eulerian residual streamfunction involving the horizontal eddy flux. This Taylor expansion approximation works well in the interior, removing the spurious mixing associated with the simple Eulerian-averaged streamfunction. However, it fails near the surface where isopycnals outcrop to the surface. It can be shown in a similar way that the vertical isopycnic streamfunction can formally be approximated by a residual streamfunction involving the vertical eddy flux. However, if horizontal isopycnal displacements are large, this approximation fails even in the ocean interior. Inspired by the two different residual streamfunctions, a more general form of TEM formulation is explored. It is shown that the different TEM residual streamfunctions arise from decomposing the eddy flux into a component along isopycnals, which leads to advective flow, and a remaining diffusive component, which is oriented either vertically or horizontally. In theory the diffusive flux can be oriented in any direction, although in practice the orientation should be such that neither the advective flow nor the diffusive flux cross any boundary (surface, sidewalls, and bottom). However, it is not clear how to merge the continuously changing orientation in a physically meaningful way. A variety of approaches are discussed.
0022-3670
2740-2755
Nurser, A.J.G.
2493ef9a-21e9-4d8b-9c32-08677e7e145a
Lee, M-M.
1b073ef1-2eb9-45a6-862b-8dd8cb3df52d
Nurser, A.J.G.
2493ef9a-21e9-4d8b-9c32-08677e7e145a
Lee, M-M.
1b073ef1-2eb9-45a6-862b-8dd8cb3df52d

Nurser, A.J.G. and Lee, M-M. (2004) Isopycnal averaging at constant height. Part II: relating to the residual streamfunction in Eulerian space. Journal of Physical Oceanography, 34 (12), 2740-2755. (doi:10.1175/JPO2650.1).

Record type: Article

Abstract

In Part I , the “vertical” transport streamfunction was defined as resulting from isopycnic averaging at constant height in the same way that the meridional streamfunction results from averaging at constant latitude. Part II here discusses the relationship between these two isopycnic streamfunctions and the Eulerian residual streamfunction that arises from the transformed Eulerian mean (TEM). It is known that the meridional isopycnic streamfunction can be approximated by a Taylor expansion to give an Eulerian residual streamfunction involving the horizontal eddy flux. This Taylor expansion approximation works well in the interior, removing the spurious mixing associated with the simple Eulerian-averaged streamfunction. However, it fails near the surface where isopycnals outcrop to the surface. It can be shown in a similar way that the vertical isopycnic streamfunction can formally be approximated by a residual streamfunction involving the vertical eddy flux. However, if horizontal isopycnal displacements are large, this approximation fails even in the ocean interior. Inspired by the two different residual streamfunctions, a more general form of TEM formulation is explored. It is shown that the different TEM residual streamfunctions arise from decomposing the eddy flux into a component along isopycnals, which leads to advective flow, and a remaining diffusive component, which is oriented either vertically or horizontally. In theory the diffusive flux can be oriented in any direction, although in practice the orientation should be such that neither the advective flow nor the diffusive flux cross any boundary (surface, sidewalls, and bottom). However, it is not clear how to merge the continuously changing orientation in a physically meaningful way. A variety of approaches are discussed.

This record has no associated files available for download.

More information

Published date: 2004

Identifiers

Local EPrints ID: 14861
URI: http://eprints.soton.ac.uk/id/eprint/14861
ISSN: 0022-3670
PURE UUID: 188c4174-4059-47f2-a356-ea1fb669233a

Catalogue record

Date deposited: 07 Mar 2005
Last modified: 15 Mar 2024 05:32

Export record

Altmetrics

Contributors

Author: A.J.G. Nurser
Author: M-M. Lee

Download statistics

Downloads from ePrints over the past year. Other digital versions may also be available to download e.g. from the publisher's website.

View more statistics

Atom RSS 1.0 RSS 2.0

Contact ePrints Soton: eprints@soton.ac.uk

ePrints Soton supports OAI 2.0 with a base URL of http://eprints.soton.ac.uk/cgi/oai2

This repository has been built using EPrints software, developed at the University of Southampton, but available to everyone to use.

We use cookies to ensure that we give you the best experience on our website. If you continue without changing your settings, we will assume that you are happy to receive cookies on the University of Southampton website.

×