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<ArticleSet>
<Article>
<Journal>
				<PublisherName>University of Isfahan</PublisherName>
				<JournalTitle>Mathematics and Society</JournalTitle>
				<Issn>2345-6493</Issn>
				<Volume>4</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>05</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Level set method for motion by mean curvature</ArticleTitle>
<VernacularTitle>Level set method for motion by mean curvature</VernacularTitle>
			<FirstPage>7</FirstPage>
			<LastPage>17</LastPage>
			<ELocationID EIdType="pii">23953</ELocationID>
			
<ELocationID EIdType="doi">10.22108/msci.2019.113074.1296</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mehran</FirstName>
					<LastName>Aminian</LastName>
<Affiliation>Vali-e-Asr University of Rafsanjan,  Rafsanjan</Affiliation>

</Author>
<Author>
					<FirstName>Mehran</FirstName>
					<LastName>Namjoo</LastName>
<Affiliation>Vali-e-Asr University of Rafsanjan,  Rafsanjan</Affiliation>
<Identifier Source="ORCID">0000-0001-5949-6766</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2018</Year>
					<Month>09</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>This paper is a translation of the the following paper into Persian:&lt;br /&gt;[T. H. Colding and W. P. Minicozzi II, Level Set Method For Motion by Mean Curvature, &lt;em&gt;Notices of the AMS&lt;/em&gt;, &lt;strong&gt;63 &lt;/strong&gt;no. 10 (2016) 1148–1153.]&lt;br /&gt; &lt;br /&gt; &lt;span class=&quot;fontstyle0&quot;&gt;Modeling of a wide class of physical phenomena, such as crystal growth and flame propagation, leads to tracking fronts moving with curvature-dependent speed. When the speed is the curvature this leads to one of the classical degenerate nonlinear second-order differential equations on Euclidean space. One naturally wonders, “What is the regularity of solutions?” A priori solutions are only defined in a weak sense, but it turns out that they are always twice differentiable classical solutions. This result is optimal; their second derivative is continuous only in very rigid situations that have a simple geometric interpretation. The proof weaves together analysis and geometry. Without deeply understanding the underlying geometry, it is impossible to prove fine analytical properties.&lt;/span&gt;</Abstract>
			<OtherAbstract Language="FA">This paper is a translation of the the following paper into Persian:&lt;br /&gt;[T. H. Colding and W. P. Minicozzi II, Level Set Method For Motion by Mean Curvature, &lt;em&gt;Notices of the AMS&lt;/em&gt;, &lt;strong&gt;63 &lt;/strong&gt;no. 10 (2016) 1148–1153.]&lt;br /&gt; &lt;br /&gt; &lt;span class=&quot;fontstyle0&quot;&gt;Modeling of a wide class of physical phenomena, such as crystal growth and flame propagation, leads to tracking fronts moving with curvature-dependent speed. When the speed is the curvature this leads to one of the classical degenerate nonlinear second-order differential equations on Euclidean space. One naturally wonders, “What is the regularity of solutions?” A priori solutions are only defined in a weak sense, but it turns out that they are always twice differentiable classical solutions. This result is optimal; their second derivative is continuous only in very rigid situations that have a simple geometric interpretation. The proof weaves together analysis and geometry. Without deeply understanding the underlying geometry, it is impossible to prove fine analytical properties.&lt;/span&gt;</OtherAbstract>
<ArchiveCopySource DocType="pdf">https://math-sci.ui.ac.ir/article_23953_e3e6bdaa31e2225b3f23cd23f4a810d4.pdf</ArchiveCopySource>
</Article>
</ArticleSet>
