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<ArticleSet>
<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>AUT Journal of Mechanical Engineering</JournalTitle>
				<Issn>2588-2937</Issn>
				<Volume>6</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>06</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Study of Kelvin-Helmholtz Instability of Newtonian and Non-Newtonian Fluids</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>249</FirstPage>
			<LastPage>260</LastPage>
			<ELocationID EIdType="pii">4649</ELocationID>
			
<ELocationID EIdType="doi">10.22060/ajme.2021.20382.5996</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>Reyhaneh</FirstName>
					<LastName>Farajzadeh</LastName>
<Affiliation>Department of Mechanical Engineering, Shahrekord University, Shahrekord, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Morteza</FirstName>
					<LastName>Bayareh</LastName>
<Affiliation>Department of Mechanical Engineering, Shahrekord University, Shahrekord, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>08</Month>
					<Day>07</Day>
				</PubDate>
			</History>
		<Abstract>Kelvin-Helmholtz instability is a hydrodynamic instability generated by the relative motion of immiscible, irrotational, incompressible, and inviscid fluids. In the present study, the Kelvin-Helmholtz instability is assessed for Newtonian and non-Newtonian fluids by solving two-dimensional Navier-Stokes equations using the finite volume method. ANSYS FLUENT software is used to simulate the two-phase flow field. The numerical method is the finite volume method. Using the semi-implicit method for pressure-linked equations algorithm, the velocity and pressure fields are coupled and the Navier-Stokes equations are solved. The second-order upwind method is used to discretize the convection terms in Navier-Stokes equations and the central difference method is employed to approximate the time derivative. In the case of Newtonian fluids, it was found that for  the growth rate of Kelvin-Helmholtz instability depends on the surface tension when the surface tension is in the range of 0.000192-0.000993 N/m. The results demonstrate that the critical wavenumber is enhanced by increasing the power-law index (&lt;em&gt;n&lt;/em&gt;) for shear-thinning and shear-thickening non-Newtonian fluids; however, at a specific time, the amount of critical wavenumber for shear-thickening fluids is smaller than that for shear-thinning ones. It is also concluded that as the power-law index increases, the wave stability can be reached more rapidly.</Abstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Kelvin-Helmholtz instability</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">two-phase flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Non-Newtonian fluids</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Surface tension</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ajme.aut.ac.ir/article_4649_205c3608ecb984c1f5f5d2f52c934428.pdf</ArchiveCopySource>
</Article>
</ArticleSet>
