Equatorial kelvin wave: Difference between revisions

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<div class="definition"><div class="short_definition">An eastward propagating [[wave]] centered about the [[equator]] with [[zonal]] but  no [[meridional]] velocity.</div><br/> <div class="paragraph">The zonal velocity has a Gaussian meridional structure centered about the equator with [[standard  deviation]] equal to the equatorial [[Rossby radius of deformation]]. In the [[shallow water approximation]]  the waves are nondispersive with [[frequency]] <div class="display-formula"><blockquote>[[File:ams2001glos-Ee47.gif|link=|center|ams2001glos-Ee47]]</blockquote></div> in which ''k'' is the along-boundary [[wavenumber]], and the [[phase speed]] <div class="display-formula"><blockquote>[[File:ams2001glos-Ee48.gif|link=|center|ams2001glos-Ee48]]</blockquote></div> with ''g'' the [[acceleration of gravity]] and ''H'' the mean fluid depth. The equatorial Rossby radius of  deformation in this case is  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee49.gif|link=|center|ams2001glos-Ee49]]</blockquote></div> in which &#x003b2; is the meridional gradient of the [[Coriolis parameter]] at the equator. A [[Kelvin wave]]  propagating equatorward along the western boundary of an ocean basin can generate an equatorial  Kelvin wave when reaching the equator. Upon reaching the eastern boundary of an ocean basin,  an equatorial Kelvin wave can generate a coastal Kelvin wave propagating poleward along the  eastern boundary of the ocean basin.</div><br/> </div>
<div class="definition"><div class="short_definition">An eastward propagating [[wave]] centered about the [[equator]] with [[zonal]] but  no [[meridional]] velocity.</div><br/> <div class="paragraph">The zonal velocity has a Gaussian meridional structure centered about the equator with [[standard deviation|standard  deviation]] equal to the equatorial [[Rossby radius of deformation]]. In the [[shallow water approximation]]  the waves are nondispersive with [[frequency]] <div class="display-formula"><blockquote>[[File:ams2001glos-Ee47.gif|link=|center|ams2001glos-Ee47]]</blockquote></div> in which ''k'' is the along-boundary [[wavenumber]], and the [[phase speed]] <div class="display-formula"><blockquote>[[File:ams2001glos-Ee48.gif|link=|center|ams2001glos-Ee48]]</blockquote></div> with ''g'' the [[acceleration of gravity]] and ''H'' the mean fluid depth. The equatorial Rossby radius of  deformation in this case is  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee49.gif|link=|center|ams2001glos-Ee49]]</blockquote></div> in which &#x003b2; is the meridional gradient of the [[Coriolis parameter]] at the equator. A [[Kelvin wave]]  propagating equatorward along the western boundary of an ocean basin can generate an equatorial  Kelvin wave when reaching the equator. Upon reaching the eastern boundary of an ocean basin,  an equatorial Kelvin wave can generate a coastal Kelvin wave propagating poleward along the  eastern boundary of the ocean basin.</div><br/> </div>
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Latest revision as of 15:55, 25 April 2012



equatorial Kelvin wave

An eastward propagating wave centered about the equator with zonal but no meridional velocity.

The zonal velocity has a Gaussian meridional structure centered about the equator with standard deviation equal to the equatorial Rossby radius of deformation. In the shallow water approximation the waves are nondispersive with frequency
ams2001glos-Ee47
in which k is the along-boundary wavenumber, and the phase speed
ams2001glos-Ee48
with g the acceleration of gravity and H the mean fluid depth. The equatorial Rossby radius of deformation in this case is
ams2001glos-Ee49
in which β is the meridional gradient of the Coriolis parameter at the equator. A Kelvin wave propagating equatorward along the western boundary of an ocean basin can generate an equatorial Kelvin wave when reaching the equator. Upon reaching the eastern boundary of an ocean basin, an equatorial Kelvin wave can generate a coastal Kelvin wave propagating poleward along the eastern boundary of the ocean basin.


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