{"id":104,"date":"2018-02-20T17:07:35","date_gmt":"2018-02-20T21:07:35","guid":{"rendered":"https:\/\/www2.whoi.edu\/staff\/mspall\/?page_id=104"},"modified":"2020-11-07T12:28:17","modified_gmt":"2020-11-07T16:28:17","slug":"project-5","status":"publish","type":"page","link":"https:\/\/www2.whoi.edu\/staff\/mspall\/projects\/project-5\/","title":{"rendered":"Mixing near Boundaries"},"content":{"rendered":"\n\t<h2>Mixing near Boundaries<\/h2>\n<p>The presence of lateral boundaries fundamentally changes the circulation driven by turbulent mixing processes. In the open ocean, weak diapycnal mixing can drive strong horizontal recirculation gyres, such as is found in the classical Stommel \/ Arons abyssal circulation model. However, as this mixing is confined more closely to a lateral boundary, the potential vorticity balance changes such that the strong horizontal recirculations, which cross planetary vorticity contours, are replaced by weak unidirectional flow along potential vorticity contours into and out of the mixing region. If the horizontal scale of the mixing region drops below the relevant viscous length scale, the horizontal recirculation is essentially eliminated.<\/p>\n<p>Lateral boundaries are similarly important for diapycnal mixing driven by atmospheric cooling. Essentially all of the downwelling limb of the thermohaline circulation takes place within narrow viscous boundary layers. For stratified flows, the downwelling occurs on horizontal scales of the internal deformation radius times the square root of the Prandl number. For weakly stratified flows, such as within the surface mixed layer, the downwelling is concentrated within very narrow boundary layers that scale as E^{1\/3}, where E is a horizonal Ekman number (a Stewartson layer). For typical oceanographic parameters, these boundary layers are O(100 m) wide. While the details of the boundary layers depend on the degree of stratification, the common result is that the net vertical motions for buoyancy-forced downwelling of the thermohaline circulation occurs in narrow visous boundary layers. The near boundary regions are preferred because the lateral viscous flux of vorticity into the wall can balance the vertical stretching of planetary vorticity.<\/p>\n<p>These results have strong implications for the impacts of near boundary processes (such as shelf-slope exchange, air-sea exchange, ice cover) on the large-scale thermohaline circulation. The dissipation experienced in such boundary layers can also alter the large-scale circulation around topographic features such as islands and ridges.<\/p>\n\t<h3>Funding Agencies<\/h3>\n<p>This work has been generously supported through grants from the National Science Foundation and the Office of Naval Research.<\/p>\n<p><img loading=\"lazy\" src=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/03\/nsf.png\" alt=\"\" width=\"100\" height=\"100\" \/> <img loading=\"lazy\" src=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/03\/ONR-e1513192905898.png\" alt=\"\" width=\"138\" height=\"63\" \/><\/p>\n\t<h3>Publications on these subjects:<\/h3>\n<p>Spall, M. A., 2008.\u00a0<a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/12\/2008_Spall_Buoyance_JPO.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Buoyancy-forced downwelling in boundary currents<\/a>.\u00a0 <i>Journal of Physical Oceanography,\u00a0 <\/i><strong>38<\/strong>(12), 2704\u20132721, doi: http:\/\/dx.doi.org\/10.1175\/2008JPO3993.1.<i><br \/><\/i><\/p>\n<p>Pickart, R. S. and M. A. Spall, 2007.\u00a0<a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/12\/2007_PIckart_Impact_JPO.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Impact of Labrador Sea convection on the North Atlantic meridional overturning circulation.<\/a>\u00a0<i>J. Phys. Oceanogr.\u00a0<\/i>37,2207-2227.<\/p>\n<p>Pedlosky, J. and M. A. Spall, 2005.\u00a0<a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/12\/2005_Pedlosky_Boundary_JPO.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Boundary intensification of vertical velocity in a beta-plane basin<\/a>.\u00a0<i>J. Phys. Oceanogr.\u00a0<\/i>35, 2487-2500.<\/p>\n<p>Katsman, C. A., M. A. Spall, R. S. Pickart, 2004.\u00a0<a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/12\/2004_Katsman_BoundaryCurrent_JPO.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Boundary current eddies and their role in the restratification of the Labrador Sea<\/a>. <i>Journal of Physical Oceanography<\/i>, 34, 1967-1983.<\/p>\n<p>Spall, M. A., 2003.\u00a0<a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/12\/2003_Spall_OnThermohaline_JMR.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">On the thermohaline circulation in flat bottom marginal seas<\/a>. <i>Journal of Marine Research<\/i>, 61, 1-25.<\/p>\n<p>Spall, M. A., 2003.\u00a0<a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2018\/02\/2003_Spall_Islands.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Islands in Zonal Flow.<\/a>\u00a0 <i>Journal of Physical Oceanography<\/i>. 33, 2689-2701.<br \/><\/p>\n<p>Spall, M. A., 2002.\u00a0<a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/12\/2002_Spall_WindAndBuoyance_JGR.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Wind- and buoyancy-forced upper ocean circulation in two-strait marginal seas with application to the Japan \/ East Sea<\/a>.\u00a0<i>Journal of Geophysical Research,<\/i>\u00a0107(C1), 6.1-6.12.<\/p>\n<p>Spall, M. A., and R. S. Pickart, 2001.\u00a0<a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/12\/2001_Spall_WhereDoes_JPO.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Where does dense water sink? A subpolar gyre example<\/a>.\u00a0 <i>Journal of Physical Oceanography,<\/i>\u00a031(3), 810-826.<\/p>\n<p>Spall, M. A., 2001.\u00a0<a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2018\/02\/2001_Spall_LargeScaleCirc.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Large-scale circulations forced by localized mixing over a sloping bottom<\/a>.\u00a0<i>Journal of Physical Oceanography<\/i>, 31(8), Part 2, 2369-2384.<\/p>\n<p>Spall, M. A., 2000.\u00a0<a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2018\/02\/2000_Spall_BuoyanceForcedCirc.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Buoyancy-forced circulation around islands and ridges<\/a>.\u00a0<i>Journal of Marine Research,<\/i>\u00a058(6), 957-982.<\/p>\n<p>Spall, M. A., 2010. <a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/12\/2010_Spall_Dynamics_JPO.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Dynamics of downwelling in an eddy-resolving convective basin<\/a>.\u00a0<i>Journal of Physical Oceanography,<\/i>\u00a040,2341-2347.<\/p>\n<p>Spall, M. A., 2008. <a href=\"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-content\/uploads\/sites\/162\/2017\/12\/2008_Spall_LowFrequency_GRL.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Low-frequency interaction between horizontal and overturning gyres in the ocean<\/a>. <i>Geophysical Research Letters, <\/i>35, L18614, doi:10.1029\/2008GL035206.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Mixing near Boundaries The presence of lateral boundaries fundamentally changes the circulation driven by turbulent mixing processes. In the open ocean, weak diapycnal mixing can drive strong horizontal recirculation gyres, such as is found in the classical Stommel \/ Arons abyssal circulation model. However, as this mixing is confined more closely to a lateral boundary,&hellip;<\/p>\n","protected":false},"author":67,"featured_media":0,"parent":13,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"_links":{"self":[{"href":"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-json\/wp\/v2\/pages\/104"}],"collection":[{"href":"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-json\/wp\/v2\/users\/67"}],"replies":[{"embeddable":true,"href":"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-json\/wp\/v2\/comments?post=104"}],"version-history":[{"count":3,"href":"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-json\/wp\/v2\/pages\/104\/revisions"}],"predecessor-version":[{"id":389,"href":"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-json\/wp\/v2\/pages\/104\/revisions\/389"}],"up":[{"embeddable":true,"href":"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-json\/wp\/v2\/pages\/13"}],"wp:attachment":[{"href":"https:\/\/www2.whoi.edu\/staff\/mspall\/wp-json\/wp\/v2\/media?parent=104"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}