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<!DOCTYPE article SYSTEM "http://www.nonlin-processes-geophys.net/inc/npg/copernicus.dtd">
<article language="en">
	<journal>
		<journal_title>Nonlinear Processes  in Geophysics</journal_title>
		<journal_url>www.nonlin-processes-geophys.net</journal_url>
		<issn>1023-5809</issn>
		<eissn>1607-7946</eissn>
		<volume_number>12</volume_number>
		<issue_number>2</issue_number>
		<publication_year>2005</publication_year>
	</journal>
	<doi>10.5194/npg-12-299-2005</doi>
	<article_url>http://www.nonlin-processes-geophys.net/12/299/2005/</article_url>
	<abstract_html>http://www.nonlin-processes-geophys.net/12/299/2005/npg-12-299-2005.html</abstract_html>
	<fulltext_pdf>http://www.nonlin-processes-geophys.net/12/299/2005/npg-12-299-2005.pdf</fulltext_pdf>
	<start_page>299</start_page>
	<end_page>310</end_page>
	<publication_date>2005-02-17</publication_date>
	<article_title content_type="html">Parallel and perpendicular cascades in solar wind turbulence</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>S. Oughton</name>
		</author>
		<author numeration="2" affiliations="2">
			<name>W. H. Matthaeus</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Department of Mathematics, University of Waikato, Hamilton, New Zealand</affiliation>
		<affiliation numeration="2" content_type="html">Bartol Research Institute, University of Delaware, Newark, DE 19716, USA</affiliation>
	</affiliations>
	<abstract content_type="html">MHD-scale fluctuations in the velocity, magnetic, and density fields
of the solar wind are routinely observed.
The evolution of these fluctuations,
as they are transported radially outwards by the solar wind,
is believed to involve  both wave and turbulence processes.
The presence of an average magnetic field
has important
implications for the anisotropy of the fluctuations and the nature of
the turbulent wavenumber cascades in the directions parallel and
perpendicular to this field.
In particular, if the ratio of the rms magnetic fluctuation strength
to the mean field
is small, then the
        &lt;I&gt;parallel wavenumber cascade is expected to be weak&lt;/I&gt;
and there are difficulties in obtaining a cascade in frequency.   The latter
has been invoked in order to explain the heating of solar wind
fluctuations (above adiabatic levels) via energy transfer to scales
where ion-cyclotron damping can occur.Following a brief review of classical hydrodynamic and
magnetohydrodynamic (MHD) cascade theories, we discuss the distinct
nature of parallel and perpendicular cascades
and their roles in the evolution of solar wind fluctuations.</abstract>
	<references>
	</references>
</article>

