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<!DOCTYPE article SYSTEM "http://www.ocean-sci.net/inc/os/copernicus.dtd">
<article language="en">
	<journal>
		<journal_title>Ocean Science</journal_title>
		<journal_url>www.ocean-sci.net</journal_url>
		<issn>1812-0784</issn>
		<eissn>1812-0792</eissn>
		<volume_number>3</volume_number>
		<issue_number>2</issue_number>
		<publication_year>2007</publication_year>
	</journal>
	<doi>10.5194/os-3-337-2007</doi>
	<article_url>http://www.ocean-sci.net/3/337/2007/</article_url>
	<abstract_html>http://www.ocean-sci.net/3/337/2007/os-3-337-2007.html</abstract_html>
	<fulltext_pdf>http://www.ocean-sci.net/3/337/2007/os-3-337-2007.pdf</fulltext_pdf>
	<start_page>337</start_page>
	<end_page>344</end_page>
	<publication_date>2007-06-15</publication_date>
	<article_title content_type="html">Unpredictability of internal M&lt;sub&gt;2&lt;/sub&gt;</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>H. van Haren</name>
			<email>hansvh@nioz.nl</email>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Netherlands Institute for Sea Research (NIOZ), P.O. Box 59, 1790 AB Den Burg, The Netherlands</affiliation>
	</affiliations>
	<abstract content_type="html">Current observations from a shelf sea, continental slopes and the
abyssal North-East Atlantic Ocean are all dominated by the semidiurnal lunar
(M&lt;sub&gt;2&lt;/sub&gt;) tide. It is shown that motions at M&lt;sub&gt;2&lt;/sub&gt; vary
at usually large barotropic and coherent baroclinic scales, &amp;gt;50 km
horizontally and &amp;gt;0.5 H vertically. H represents the waterdepth. Such
M&lt;sub&gt;2&lt;/sub&gt;-scales are observed even close to topography, the potential
source of baroclinic, &quot;internal&quot; tidal waves. In contrast, incoherent
small-scale, ~10 km horizontally and ~0.1 H vertically,
baroclinic motions are dominated around f, the local inertial frequency,
and/or near 2&amp;Omega;&amp;#x2248;S&lt;sub&gt;2&lt;/sub&gt;, the semidiurnal solar
tidal frequency. &amp;Omega; represents the Earth&apos;s rotational vector. This
confirms earlier suggestions that small-scale baroclinic
M&lt;sub&gt;2&lt;/sub&gt;-motions generally do not exist in the ocean in any
predictable manner, except in beams very near, &amp;lt;10 km horizontally, to
their source. As a result, M&lt;sub&gt;2&lt;/sub&gt;-motions are not directly
important for generating shear and internal wave induced mixing. Indirectly 
however, they may contribute to ocean mixing if transfer
to small-scale motions at f and/or S&lt;sub&gt;2&lt;/sub&gt; and at high internal wave frequencies can be proven. Also far
from topography, small-scale motions are found at either one or both of the
latter frequencies. Different suggestions for the scales at these particular
frequencies are discussed, ranging from the variability of &quot;background&quot;
density gradients and associated divergence and focusing of internal wave
rays to the removal of the internal tidal energy by non-linear interactions.
Near f and S&lt;sub&gt;2&lt;/sub&gt; particular short-wave inertio-gravity
wave bounds are found in the limits of strong and very weak stratification, which are
often observed in small-scale layers.</abstract>
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</article>

