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<article language="en">
	<journal>
		<journal_title>Advances in Radio Science</journal_title>
		<journal_url>www.adv-radio-sci.net</journal_url>
		<issn>1684-9965</issn>
		<eissn>1684-9973</eissn>
		<volume_number>1</volume_number>
		<volume_title>Kleinheubacher Berichte 2002</volume_title>
		<publication_year>2003</publication_year>
	</journal>
	<doi>10.5194/ars-1-87-2003</doi>
	<article_url>http://www.adv-radio-sci.net/1/87/2003/</article_url>
	<abstract_html>http://www.adv-radio-sci.net/1/87/2003/ars-1-87-2003.html</abstract_html>
	<fulltext_pdf>http://www.adv-radio-sci.net/1/87/2003/ars-1-87-2003.pdf</fulltext_pdf>
	<start_page>87</start_page>
	<end_page>92</end_page>
	<publication_date>2003-05-05</publication_date>
	<article_title content_type="html">Comparison of errors and stability in FDTD and FVTD</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>P. Leuchtmann</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>C. Fumeaux</name>
		</author>
		<author numeration="3" affiliations="1">
			<name>D. Baumann</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Institut für Feldtheorie und Höchstfrequenztechnik, ETH Zürich, CH-8092 Zürich, Switzerland</affiliation>
	</affiliations>
	<abstract content_type="html">The methods of finite-difference time-domain
(FDTD) and finite-volume time-domain (FVTD) are well
known techniques for solving electromagnetic problems.
While for FDTD a number of commercial codes is available
there are only few based on FVTD. However, FVTD has
advantages since it allows completely unstructured meshes.
This paper 1. deals with the principle errors made in both approaches
and 2. gives a theoretical comparison of the (local)
stability of an FVTD scheme as opposed to the conventional
Yee-scheme commonly used in FDTD. Finally the principles
of a new FVTD program is presented. Its capabilities are
demonstrated by the field of an antenna array.</abstract>
	<references>
	</references>
</article>

