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<Article>
<Journal>
				<PublisherName>University of Kashan</PublisherName>
				<JournalTitle>Mathematics Interdisciplinary Research</JournalTitle>
				<Issn>2538-3639</Issn>
				<Volume>1</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2016</Year>
					<Month>07</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Motion of Particles under Pseudo-Deformation</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>273</FirstPage>
			<LastPage>277</LastPage>
			<ELocationID EIdType="pii">34108</ELocationID>
			
<ELocationID EIdType="doi">10.22052/mir.2016.34108</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>Akhilesh Chandra</FirstName>
					<LastName>Yadav</LastName>
<Affiliation>Department of Mathematics,
Mahatma Gandhi Kashi Vidyapith Varanasi,
Uttar Pradesh, India</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2016</Year>
					<Month>04</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>In this short article, we observe that the path of particle of mass m moving along r = r(t) under pseudo-force A(t), t denotes the time, is given by r&lt;sub&gt;d&lt;/sub&gt; =∫(dr/dt A(t))dt + c. We also observe that the effective force F&lt;sub&gt;e&lt;/sub&gt; on that particle due to pseudo-force A(t), is given by F&lt;sub&gt;e&lt;/sub&gt; = FA(t) + LdA(t)/dt, where F = m d&lt;sup&gt;2&lt;/sup&gt;r/dt&lt;sup&gt;2&lt;/sup&gt; and L = m dr/dt. We have discussed stream lines under pseudo-force.</Abstract>
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			<Param Name="value">right transversals</Param>
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			<Param Name="value">gyrotransversals</Param>
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<ArchiveCopySource DocType="pdf">https://mir.kashanu.ac.ir/article_34108_1020df1e5666b6a0fea4c5f804264b84.pdf</ArchiveCopySource>
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