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<article language="en">
	<journal>
		<journal_title>Astrophysics and Space Sciences Transactions</journal_title>
		<journal_url>www.astrophys-space-sci-trans.net</journal_url>
		<issn>1810-6528</issn>
		<eissn>1810-6536</eissn>
		<volume_number>2</volume_number>
		<issue_number>2</issue_number>
		<publication_year>2006</publication_year>
	</journal>
	<doi>10.5194/astra-2-63-2006</doi>
	<article_url>http://www.astrophys-space-sci-trans.net/2/63/2006/</article_url>
	<abstract_html>http://www.astrophys-space-sci-trans.net/2/63/2006/astra-2-63-2006.html</abstract_html>
	<fulltext_pdf>http://www.astrophys-space-sci-trans.net/2/63/2006/astra-2-63-2006.pdf</fulltext_pdf>
	<start_page>63</start_page>
	<end_page>72</end_page>
	<publication_date>2006-11-29</publication_date>
	<article_title content_type="html">Are heliospheric flows magnetic line- or flux-conserving?</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>D. H. Nickeler</name>
			<email>nickeler@asu.cas.cz</email>
		</author>
		<author numeration="2" affiliations="1">
			<name>M. Karlický</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Astronomical Institute Ond&amp;#x0159;ejov AV &amp;#x010C;R, Czech Republic</affiliation>
	</affiliations>
	<abstract content_type="html">This article discusses and tests
the validity of the frozen in magnetic field paradigm
(or &apos;ideal magnetohydrodynamics (MHD) constraint&apos;)
which is usually adopted by many authors dealing with
heliospheric physics.

&lt;br&gt;&lt;br&gt;
To show the problem of using ideal MHD in such a counterflow
configuration like the heliosphere, we first recapitulate the basic
concepts of freezing-in of magnetic fields, respectively
magnetic topology conservation and its violation
(= magnetic reconnection) in 3-D, already done by other authors with
different methods with respect to derivations and interpretations.
Then we analyse different heliospheric plasma environments.
As a model of the stagnation region/stagnation point
in front of the heliospheric nose, we present and discuss
the general solution of the ideal MHD Ohm&apos;s law in the vicinity
of a 2-D stagnation point, which was found by us.

&lt;br&gt;&lt;br&gt;
We show that ideal MHD either leads necessarily to a diverging
magnetic field strength in the vicinity of such a stagnation point,
or to a vanishing mass density on the heliopause boundaries.
In the case that components of the electric field
parallel to the magnetic field do not exist due to the chosen form
of the non-ideal Ohm&apos;s law, it is always possible to formulate
the transport equation of the magnetic field as a modified
ideal Ohm&apos;s law.

&lt;br&gt;&lt;br&gt;
We find that the form of the Ohm&apos;s law which is often used in
heliospheric physics (see e.g. Baranov and Fahr, 2003), is not able to
change magnetic topology and thus cannot lead to magnetic
reconnection, which necessarily has to occur at the stagnation point.
The diverging magnetic field, for instance, implies the breakdown
of the flux freezing paradigm for the heliosphere. Its application,
especially at the heliospheric nose, is therefore rather doubtful.
We conclude that it is necessary to search for an Ohm&apos;s law
which is able to violate magnetic topology conservation.</abstract>
	<references>
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</article>
