<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE ArticleSet PUBLIC "-//NLM//DTD PubMed 2.7//EN" "https://dtd.nlm.nih.gov/ncbi/pubmed/in/PubMed.dtd">
<ArticleSet>
<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Investigation of Vortex-Induced Vibrations of an elastically-mounted 
Circular Cylinder Beneath a Free Surface: Modes &amp; Frequencies</ArticleTitle>
<VernacularTitle>Numerical Investigation of Vortex-Induced Vibrations of an elastically-mounted 
Circular Cylinder Beneath a Free Surface: Modes &amp; Frequencies</VernacularTitle>
			<FirstPage>1169</FirstPage>
			<LastPage>1186</LastPage>
			<ELocationID EIdType="pii">2765</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2017.13236.5578</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Seyed Mostafa</FirstName>
					<LastName>Hosseinalipoor</LastName>
<Affiliation>Iran University of Science and Technology</Affiliation>

</Author>
<Author>
					<FirstName>Navid</FirstName>
					<LastName>Haji Ghafoori Boukani</LastName>
<Affiliation>Iran University of Science and Technology</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>08</Month>
					<Day>05</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, a two-dimensional numerical simulation is applied to study the Vortex[1]Induced Vibrations (VIV) of an elastically mounted rigid circular cylinder beneath a free surface of fluid. The effect of free surface in laminar flow (60 &lt; Re &lt; 130) with Fr=0.2 is investigated with considering two Gap-Ratios of 2.5, 1.5. The natural structural frequency of oscillator is assumed to match the vortex shedding frequency for a stationary cylinder at Re=100. Simulations of VIV and Free Surface of fluid flow have separately shown good agreement with previous results. User Defined Function (UDF) hooked in the Software is given to couple the motion of cylinder to flow motion. For simulation of free surface, Volume of fluid (VOF) method is used. This paper is the second part of an investigation about effects of Free Surface of fluid on VIV phenomena. The effects of Free Surface is investigated with using a comparison of vortex shedding modes and non-dimensional frequency diagrams for the two Gap-Ratios. With approaching cylinder to free surface, results shows changing type of vortex shedding modes, abatement in lock-in region, increasing Strouhal number and non[1]dimensional frequency ratio.</Abstract>
			<OtherAbstract Language="FA">In this paper, a two-dimensional numerical simulation is applied to study the Vortex[1]Induced Vibrations (VIV) of an elastically mounted rigid circular cylinder beneath a free surface of fluid. The effect of free surface in laminar flow (60 &lt; Re &lt; 130) with Fr=0.2 is investigated with considering two Gap-Ratios of 2.5, 1.5. The natural structural frequency of oscillator is assumed to match the vortex shedding frequency for a stationary cylinder at Re=100. Simulations of VIV and Free Surface of fluid flow have separately shown good agreement with previous results. User Defined Function (UDF) hooked in the Software is given to couple the motion of cylinder to flow motion. For simulation of free surface, Volume of fluid (VOF) method is used. This paper is the second part of an investigation about effects of Free Surface of fluid on VIV phenomena. The effects of Free Surface is investigated with using a comparison of vortex shedding modes and non-dimensional frequency diagrams for the two Gap-Ratios. With approaching cylinder to free surface, results shows changing type of vortex shedding modes, abatement in lock-in region, increasing Strouhal number and non[1]dimensional frequency ratio.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Vortex Induced Vibration</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">free surface</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Lock-in region</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Vortex shedding modes</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2765_370bfb31abd222b582245b977ea5f25a.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigating the Influence of Geometry on Performance Characteristics of Mounted 
Cushions in Hydraulic Cylinders</ArticleTitle>
<VernacularTitle>Investigating the Influence of Geometry on Performance Characteristics of Mounted 
Cushions in Hydraulic Cylinders</VernacularTitle>
			<FirstPage>1187</FirstPage>
			<LastPage>1200</LastPage>
			<ELocationID EIdType="pii">2872</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.13391.5617</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Moein</FirstName>
					<LastName>Majnouni Mehrdar</LastName>
<Affiliation>Sari agricultural sciences and natural resources</Affiliation>

</Author>
<Author>
					<FirstName>Davoud</FirstName>
					<LastName>Kalantari</LastName>
<Affiliation>biosystem mechanics, agricultural engineering, Sari university of agricultural sciences and natural resources,</Affiliation>

</Author>
<Author>
					<FirstName>Seyed Reza</FirstName>
					<LastName>Mousavi Seyedy</LastName>
<Affiliation>Sari agricultural sciences and natural resources</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>09</Month>
					<Day>07</Day>
				</PubDate>
			</History>
		<Abstract>In this research, design, fabrication and evaluation of 5 different hydraulic cushions have been considered in order to optimize the stopping mechanism of pistons at the end of the course. The comparison of 5 cushion spears including Cylindrical, Conical, Sagittal, Double conical and Parabolic cushion have been studied with reviewing the motion behavior of piston and measuring displacement, speed, acceleration, flow rate and hydraulic pressure in an one way hydraulic cylinder. Results showed that the sagittal cushion with maximum pressure increasing of 1.98% for 200 kg load and 0.35% for 350 kg load had the lowest percentage of hydraulic pressure rise and cylindrical cushion with maximum pressure increasing of 11.98% for 200 kg load and 3.92% for 350 kg load had highest percentage of hydraulic pressure rise. Also operational time of sagittal cushion in experiments with 350 kg load was respectively 33.8 and 63.9 percent lower than that of conical and cylindrical cushion. Also double conical cushion has the nearest performance to the sagittal cushion. As a concluding result with tacking into account the low response time, steady speed reduction and steady rate of hydraulic oil discharge, sagittal cushion is recommended to be used in industries.</Abstract>
			<OtherAbstract Language="FA">In this research, design, fabrication and evaluation of 5 different hydraulic cushions have been considered in order to optimize the stopping mechanism of pistons at the end of the course. The comparison of 5 cushion spears including Cylindrical, Conical, Sagittal, Double conical and Parabolic cushion have been studied with reviewing the motion behavior of piston and measuring displacement, speed, acceleration, flow rate and hydraulic pressure in an one way hydraulic cylinder. Results showed that the sagittal cushion with maximum pressure increasing of 1.98% for 200 kg load and 0.35% for 350 kg load had the lowest percentage of hydraulic pressure rise and cylindrical cushion with maximum pressure increasing of 11.98% for 200 kg load and 3.92% for 350 kg load had highest percentage of hydraulic pressure rise. Also operational time of sagittal cushion in experiments with 350 kg load was respectively 33.8 and 63.9 percent lower than that of conical and cylindrical cushion. Also double conical cushion has the nearest performance to the sagittal cushion. As a concluding result with tacking into account the low response time, steady speed reduction and steady rate of hydraulic oil discharge, sagittal cushion is recommended to be used in industries.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Cushion</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Sagittal cushion</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Conical cushion</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Circular cushion</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Hydraulic cylinder</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2872_7e0a0209b929d097bd3e8ef30567a5c1.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Experimental Comparison of Breakup and Flow Characteristics of Rectangular and 
Elliptical Water Jets</ArticleTitle>
<VernacularTitle>Experimental Comparison of Breakup and Flow Characteristics of Rectangular and 
Elliptical Water Jets</VernacularTitle>
			<FirstPage>1201</FirstPage>
			<LastPage>1216</LastPage>
			<ELocationID EIdType="pii">2892</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.13828.5725</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Amin</FirstName>
					<LastName>Jaberi</LastName>
<Affiliation>Department of Aerospace Engineering, Amirkabir University of Technology</Affiliation>
<Identifier Source="ORCID">0000-0001-7629-2626</Identifier>

</Author>
<Author>
					<FirstName>Mehran</FirstName>
					<LastName>Tadjfar</LastName>
<Affiliation>Department of Aerospace Engineering, Amirkabir University of Technology</Affiliation>
<Identifier Source="ORCID">0000-0002-7381-1491</Identifier>

</Author>
<Author>
					<FirstName>Armin</FirstName>
					<LastName>Sheidani</LastName>
<Affiliation>Department of Aerospace Engineering, Amirkabir University of Technology</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>12</Month>
					<Day>13</Day>
				</PubDate>
			</History>
		<Abstract>The flow characteristics of water jets issuing from rectangular and elliptical injectors into quiescent air were experimentally investigated. Injectors were of the same cross-sectional area and a circular injector was also employed as the reference case. Digital images taken by a diffused backlight technique were processed to extract the main characteristics of the jet column at different jet velocities. The measurements were carried out for mass flow rates varying from 2 L/h to 120 L/h with small enough steps at low speeds to capture Rayleigh regime. Aside from the qualitative description of the jet flows, stability curve was plotted to make a comparison between different jets. The comparison revealed that the ellipse jet is the first one to reach the critical Weber number, while the circular jet remains laminar at higher velocities than the other two jets. Moreover, axis-switching phenomenon was carefully studied as the common characteristic of rectangular and elliptical jets. The wavelength and maximum amplitude of axis-switching were measured at different flow conditions and the results were compared. Though the axis-switching wavelength of both jets demonstrated a linear increment with Weber number, the rectangular jet was found to increase with a higher slope.</Abstract>
			<OtherAbstract Language="FA">The flow characteristics of water jets issuing from rectangular and elliptical injectors into quiescent air were experimentally investigated. Injectors were of the same cross-sectional area and a circular injector was also employed as the reference case. Digital images taken by a diffused backlight technique were processed to extract the main characteristics of the jet column at different jet velocities. The measurements were carried out for mass flow rates varying from 2 L/h to 120 L/h with small enough steps at low speeds to capture Rayleigh regime. Aside from the qualitative description of the jet flows, stability curve was plotted to make a comparison between different jets. The comparison revealed that the ellipse jet is the first one to reach the critical Weber number, while the circular jet remains laminar at higher velocities than the other two jets. Moreover, axis-switching phenomenon was carefully studied as the common characteristic of rectangular and elliptical jets. The wavelength and maximum amplitude of axis-switching were measured at different flow conditions and the results were compared. Though the axis-switching wavelength of both jets demonstrated a linear increment with Weber number, the rectangular jet was found to increase with a higher slope.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Liquid jet؛ Elliptical jet</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Rectangular jet</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Axis switching</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2892_6fe131632103526e3a6e8114c78eb1e1.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Experimental Analysis of Operating Modes Effect of Open-end and Dead-end on 
Water Management in H2/O2 Proton-Exchange Membrane Fuel Cells Stack</ArticleTitle>
<VernacularTitle>Experimental Analysis of Operating Modes Effect of Open-end and Dead-end on 
Water Management in H2/O2 Proton-Exchange Membrane Fuel Cells Stack</VernacularTitle>
			<FirstPage>1217</FirstPage>
			<LastPage>1234</LastPage>
			<ELocationID EIdType="pii">3007</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.13945.5759</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mazaher</FirstName>
					<LastName>Rahimi Esboee</LastName>
<Affiliation>Fuel Cell Technology Research Laboratory, Malek Ashtar University of Technology, Fereydounkenar, Iran.</Affiliation>

</Author>
<Author>
					<FirstName>Ebrahim</FirstName>
					<LastName>Alizadeh</LastName>
<Affiliation>Fuel Cell Technology Research Laboratory, Malek Ashtar University of Technology, Freydounkenar, Iran.</Affiliation>

</Author>
<Author>
					<FirstName>Ali Akbar</FirstName>
					<LastName>Ranjbar</LastName>
<Affiliation>Department of Mechanical Engineering, Babol &amp;ldquo;Noshiravani&amp;rdquo; University of Technology, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Seyed Majid</FirstName>
					<LastName>Rahgoshay</LastName>
<Affiliation>Fuel Cell Technology Research Laboratory, Malek Ashtar University of Technology, Fereydounkenar, Iran.</Affiliation>

</Author>
<Author>
					<FirstName>Sayed Hossein</FirstName>
					<LastName>Masrouri Saadat</LastName>
<Affiliation>Fuel Cell Technology Research Laboratory, Malek Ashtar University of Technology</Affiliation>
<Identifier Source="ORCID">0000-0002-2869-4935</Identifier>

</Author>
<Author>
					<FirstName>Majid</FirstName>
					<LastName>Khorshidian</LastName>
<Affiliation>Fuel Cell Technology Research Laboratory, Malek Ashtar University of Technology, Fereydounkenar, Iran.</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2018</Year>
					<Month>01</Month>
					<Day>10</Day>
				</PubDate>
			</History>
		<Abstract>The management of consumption the reactive gas in proton-exchange membrane fuel cells is classified into three types: open-end, recirculation and dead-end. In dead-end mode, reactant gasses due to accumulating of water and inert gas should be purged alternatively. In this paper a protonexchange membrane fuel cells stack with transparent end plates and a unique design for investigation of water management is designed, manufactured and fabricated. In this paper, for the first time, the discussion of water management in a dead-end anode and cathode proton-exchange membrane fuel cells stack with details of form and remove of water has been investigated. The results have shown that at the current density of lower than 200 mA/cm2, the produced water is in the form of separate droplets and there is no film flow and slug flow of water in the channel. Also, as expected, the accumulation of droplets and film flow in the lower half was more than the upper half and therefore the reduction of the number of channels to increase gas speed and effective water removal in this part was essential. The results have shown that for steady-state operation, the maximum time possible for closing the output valves is 5 seconds and the minimum time required to open it is 5 seconds.</Abstract>
			<OtherAbstract Language="FA">The management of consumption the reactive gas in proton-exchange membrane fuel cells is classified into three types: open-end, recirculation and dead-end. In dead-end mode, reactant gasses due to accumulating of water and inert gas should be purged alternatively. In this paper a protonexchange membrane fuel cells stack with transparent end plates and a unique design for investigation of water management is designed, manufactured and fabricated. In this paper, for the first time, the discussion of water management in a dead-end anode and cathode proton-exchange membrane fuel cells stack with details of form and remove of water has been investigated. The results have shown that at the current density of lower than 200 mA/cm2, the produced water is in the form of separate droplets and there is no film flow and slug flow of water in the channel. Also, as expected, the accumulation of droplets and film flow in the lower half was more than the upper half and therefore the reduction of the number of channels to increase gas speed and effective water removal in this part was essential. The results have shown that for steady-state operation, the maximum time possible for closing the output valves is 5 seconds and the minimum time required to open it is 5 seconds.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Transparent proton-exchange membrane fuel cells</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Water film flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Purge time</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Dead-end mode</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Voltage variation</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_3007_a724b9124acc7b5058ed75a31a9c2919.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Study of Lock Exchange Turbidity Current Depositional Behavior in Stratified Environment</ArticleTitle>
<VernacularTitle>Numerical Study of Lock Exchange Turbidity Current Depositional Behavior in Stratified Environment</VernacularTitle>
			<FirstPage>1235</FirstPage>
			<LastPage>1252</LastPage>
			<ELocationID EIdType="pii">2925</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.14062.5789</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Saba</FirstName>
					<LastName>Teymouri</LastName>
<Affiliation>Department of Mechanical Engineering, University Of Zanjan, Zanjan, Iran.</Affiliation>

</Author>
<Author>
					<FirstName>Ehsan</FirstName>
					<LastName>Khavasi</LastName>
<Affiliation>Mechanical engineering department, University of Zanjan</Affiliation>

</Author>
<Author>
					<FirstName>Hamid</FirstName>
					<LastName>Yousefi</LastName>
<Affiliation>Department of Mechanical Engineering, University Of Zanjan, Zanjan, Iran.</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2018</Year>
					<Month>02</Month>
					<Day>08</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, three-dimensional numerical simulation was conducted to study the lock exchange turbidity current depositional behavior in a stratified environment. Simulations are carried out using Large Eddy Simulation method. The obtained results in stratified case are in good agreement with experimental data. Also, the presence of stratified environment reduces the current velocity, so that the front location is reduced by 57%, but does not have any significant effect on the sedimentation pattern. In addition, the results showed that increasing the slope to 12 degrees increases the sedimentation rate by 15 and 40 percent compared to the slopes 9 and 6 degrees. It was also observed that increasing the particle diameter reduced the momentum and the current sedimentation increases 0.75 and 3.7 times higher. For more accurate representation of the particle interaction, the particle settling velocity also varies with concentration. The results of this analysis indicate that assuming the variable settling velocity in the early stages of the current progression leads to insignificant change in the front velocity, but when the current propagates more, the faster front velocity will be predicted. In variable velocity case, the current separation location increases by 22%..</Abstract>
			<OtherAbstract Language="FA">In this paper, three-dimensional numerical simulation was conducted to study the lock exchange turbidity current depositional behavior in a stratified environment. Simulations are carried out using Large Eddy Simulation method. The obtained results in stratified case are in good agreement with experimental data. Also, the presence of stratified environment reduces the current velocity, so that the front location is reduced by 57%, but does not have any significant effect on the sedimentation pattern. In addition, the results showed that increasing the slope to 12 degrees increases the sedimentation rate by 15 and 40 percent compared to the slopes 9 and 6 degrees. It was also observed that increasing the particle diameter reduced the momentum and the current sedimentation increases 0.75 and 3.7 times higher. For more accurate representation of the particle interaction, the particle settling velocity also varies with concentration. The results of this analysis indicate that assuming the variable settling velocity in the early stages of the current progression leads to insignificant change in the front velocity, but when the current propagates more, the faster front velocity will be predicted. In variable velocity case, the current separation location increases by 22%..</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Density current</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Lock-exchange</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Stratified environment</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Large Eddy Simulation: Sloping bed</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2925_ac34ae1fda29b8fe781ac8d6d32a6bc7.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Semi-empirical Investigation of Trailing Edge Noise by Measuring Unsteady Surface 
Pressures</ArticleTitle>
<VernacularTitle>Semi-empirical Investigation of Trailing Edge Noise by Measuring Unsteady Surface 
Pressures</VernacularTitle>
			<FirstPage>1253</FirstPage>
			<LastPage>1270</LastPage>
			<ELocationID EIdType="pii">1005</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2017.12480.5352</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Abbas</FirstName>
					<LastName>Afshari</LastName>
<Affiliation>phd student / yazd university</Affiliation>

</Author>
<Author>
					<FirstName>Ali Akbar</FirstName>
					<LastName>Dehghan</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Mohammad</FirstName>
					<LastName>Farmani</LastName>
<Affiliation>phd student/ yazd university</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>02</Month>
					<Day>04</Day>
				</PubDate>
			</History>
		<Abstract>Turbulent boundary layer trailing edge noise is one of the main sources of aerodynamic noise and extensive studies have been devoted to trailing edge noise identification during the past decades. In the present study, for measuring the main parameters affecting the trailing edge noise including the surface pressure spectra, the spanwise length scale of the surface pressure fluctuations and eddy convection velocity in the trailing edge region, a flat-plate model equipped with several streamwise and spanwise surface pressure transducers is designed and built. The spanwise length scale and eddy convection velocity are calculated by simultaneously measuring of unsteady surface pressure in both streamwise and spanwise directions. The results show that the best collapses in the surface pressure spectra at low frequency and mid to high frequencies can be obtained by using outer and inner layer scales respectively. Furthermore, the longitudinal and lateral coherences can provide adequate information about the lifespan of the turbulent eddies and their physical size. Finally, the far-field trailing edge noise induced by the turbulent flow over the flat plate has been predicted by using the Amit-Roger model and results show the effectiveness of this model for prediction of far-field turbulent boundary layer trailing edge noise.</Abstract>
			<OtherAbstract Language="FA">Turbulent boundary layer trailing edge noise is one of the main sources of aerodynamic noise and extensive studies have been devoted to trailing edge noise identification during the past decades. In the present study, for measuring the main parameters affecting the trailing edge noise including the surface pressure spectra, the spanwise length scale of the surface pressure fluctuations and eddy convection velocity in the trailing edge region, a flat-plate model equipped with several streamwise and spanwise surface pressure transducers is designed and built. The spanwise length scale and eddy convection velocity are calculated by simultaneously measuring of unsteady surface pressure in both streamwise and spanwise directions. The results show that the best collapses in the surface pressure spectra at low frequency and mid to high frequencies can be obtained by using outer and inner layer scales respectively. Furthermore, the longitudinal and lateral coherences can provide adequate information about the lifespan of the turbulent eddies and their physical size. Finally, the far-field trailing edge noise induced by the turbulent flow over the flat plate has been predicted by using the Amit-Roger model and results show the effectiveness of this model for prediction of far-field turbulent boundary layer trailing edge noise.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Trailing edge noise</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Turbulent boundary layer</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Surface pressure spectra</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Eddy convection velocity</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Spanwise length scale</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_1005_2387337ba1e0b0249ba90f55b2ba2521.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Computational Investigation of the Effect of Adhesion between Cancer Cells and 
Vessel Walls on the Movement of the Cells in Blood Vessels</ArticleTitle>
<VernacularTitle>Computational Investigation of the Effect of Adhesion between Cancer Cells and 
Vessel Walls on the Movement of the Cells in Blood Vessels</VernacularTitle>
			<FirstPage>1271</FirstPage>
			<LastPage>1288</LastPage>
			<ELocationID EIdType="pii">2882</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.11903.5569</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Asghar</FirstName>
					<LastName>Khorram</LastName>
<Affiliation>MSc/University of Tehran</Affiliation>

</Author>
<Author>
					<FirstName>Bahman</FirstName>
					<LastName>Vahidi</LastName>
<Affiliation>Assistant professor/University of Tehran</Affiliation>
<Identifier Source="ORCID">0000-0001-5597-3748</Identifier>

</Author>
<Author>
					<FirstName>Zahra</FirstName>
					<LastName>Mollahoseini</LastName>
<Affiliation>MSc student/University of Tehran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>07</Month>
					<Day>29</Day>
				</PubDate>
			</History>
		<Abstract>Cancer is a disease that causes mortality in the world. Despite of improvements in medicine, there is not still sufficient knowledge of cancer. Therefore, there is a strong need for engineering modeling to understand it. The motion and adhesion of cancer cells in a blood vessel during metastasis is a complex mechanism that occurs in body. A two[1]dimensional model of the movement of cancer cells has been developed that is solved in two different modes in a straight line in a blood vessel. These modes are related to presence and absence of adhesion between cancer cell and blood vessel wall in presence of adhesion between cancer cell and white blood cell. The analysis is performed using FEM and FSI equations. It is assumed that the properties of blood and cells are homogeneous and fluid is incompressible and Newtonian. Cancer cell is modeled as a rigid body and white blood cell is assumed as linear elastic. The analysis shows that the influence of adhesion between the cell and the vessel wall is more important from cell-cell adhesion. Through consideration in the adhesion charts along with medical issues such as drug delivery to patients can affect the treatment or prevention of metastasis.</Abstract>
			<OtherAbstract Language="FA">Cancer is a disease that causes mortality in the world. Despite of improvements in medicine, there is not still sufficient knowledge of cancer. Therefore, there is a strong need for engineering modeling to understand it. The motion and adhesion of cancer cells in a blood vessel during metastasis is a complex mechanism that occurs in body. A two[1]dimensional model of the movement of cancer cells has been developed that is solved in two different modes in a straight line in a blood vessel. These modes are related to presence and absence of adhesion between cancer cell and blood vessel wall in presence of adhesion between cancer cell and white blood cell. The analysis is performed using FEM and FSI equations. It is assumed that the properties of blood and cells are homogeneous and fluid is incompressible and Newtonian. Cancer cell is modeled as a rigid body and white blood cell is assumed as linear elastic. The analysis shows that the influence of adhesion between the cell and the vessel wall is more important from cell-cell adhesion. Through consideration in the adhesion charts along with medical issues such as drug delivery to patients can affect the treatment or prevention of metastasis.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Cancer cells</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Cell mechanics</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Metastasis</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Computational modeling</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Adhesion</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2882_2ef35a8b78b572a47f56846acbeef5d3.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Simultaneous Simulation of Gas Diffusion Layer and Air Channel in a Polymer  Electrolyte Membrane Fuel Cell: Pore-Scale Modeling of Water Flooding</ArticleTitle>
<VernacularTitle>Simultaneous Simulation of Gas Diffusion Layer and Air Channel in a Polymer  Electrolyte Membrane Fuel Cell: Pore-Scale Modeling of Water Flooding</VernacularTitle>
			<FirstPage>1289</FirstPage>
			<LastPage>1304</LastPage>
			<ELocationID EIdType="pii">875</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2016.875</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mohsen</FirstName>
					<LastName>Nazari</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2016</Year>
					<Month>08</Month>
					<Day>12</Day>
				</PubDate>
			</History>
		<Abstract>In this study, Lattice Boltzmann method is used to investigate liquid water transport in a carbon paper gas diffusion layer and gas channel of polymer electrolyte membrane fuel cells. The effects of gas diffusion layer wettability on the removal process and liquid water distribution are investigated. In addition, liquid water dynamic behaviors and liquid water saturation within the gas diffusion layer in two case of steady and transient are explored. This study focuses on the effects of surface wettability on the number of effective clusters, merging of clusters, and the required time for reaching the steady-state water distribution. The results show that the wettability of surface affects on the saturation of liquid water in the gas diffusion layer and in  100lu&lt;Y&lt;160lu, this effect is noticeable. The steady-  water distribution is observed at time step of 1590000 and 1500000 (lattice unit) for the contact angles of 115° and 145°, respectively. Thus the simulation results show that by increasing the contact angle of fibers in gas diffusion layer, the required time to obtain a steady state water distribution is reduced. Therefore, if the solid surface becomes more hydrophobic, water management will be improved in the gas diffusion layer.</Abstract>
			<OtherAbstract Language="FA">In this study, Lattice Boltzmann method is used to investigate liquid water transport in a carbon paper gas diffusion layer and gas channel of polymer electrolyte membrane fuel cells. The effects of gas diffusion layer wettability on the removal process and liquid water distribution are investigated. In addition, liquid water dynamic behaviors and liquid water saturation within the gas diffusion layer in two case of steady and transient are explored. This study focuses on the effects of surface wettability on the number of effective clusters, merging of clusters, and the required time for reaching the steady-state water distribution. The results show that the wettability of surface affects on the saturation of liquid water in the gas diffusion layer and in  100lu&lt;Y&lt;160lu, this effect is noticeable. The steady-  water distribution is observed at time step of 1590000 and 1500000 (lattice unit) for the contact angles of 115° and 145°, respectively. Thus the simulation results show that by increasing the contact angle of fibers in gas diffusion layer, the required time to obtain a steady state water distribution is reduced. Therefore, if the solid surface becomes more hydrophobic, water management will be improved in the gas diffusion layer.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">LIQUID WATER</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Gas diffusion layer</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">WETTABILITY</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">LIQUID WATER SATURATION</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_875_4b0a59ddf11c58e7446c9df0da541a84.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Droplet Deformation Between Two Moving Parallel Plates</ArticleTitle>
<VernacularTitle>Droplet Deformation Between Two Moving Parallel Plates</VernacularTitle>
			<FirstPage>1305</FirstPage>
			<LastPage>1324</LastPage>
			<ELocationID EIdType="pii">2885</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.13067.5525</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mahdi</FirstName>
					<LastName>Salami Hosseini</LastName>
<Affiliation>Polymer Engineering Department, Sahand University of Technology</Affiliation>

</Author>
<Author>
					<FirstName>Mohammad Ali</FirstName>
					<LastName>Moeeni</LastName>
<Affiliation>sahand university student</Affiliation>

</Author>
<Author>
					<FirstName>Mirkarim</FirstName>
					<LastName>Razavi Aghjeh</LastName>
<Affiliation>faculty member</Affiliation>

</Author>
<Author>
					<FirstName>Mahdi</FirstName>
					<LastName>Mostafaian</LastName>
<Affiliation>Leibniz Institute for Polymer Research, Dresden University of Technology</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>06</Month>
					<Day>29</Day>
				</PubDate>
			</History>
		<Abstract>One of the most important and challenging subjects for scientists is the numerical simulation of the transport phenomena in heterogeneous media. The discontinuity in the properties causes computational errors leading to incorrect estimation of the exact values. The extended finite element method is one of the powerful tools to predict the behavior of heterogenic materials and phenomena. In the present study, we attempted to adapt the extended finite element method to study the flow of a two phase system and investigate the effect of different material and operational parameters such as Capillary number on the drop deformation process in Newtonian/Newtonian and non-Newtonian/ Newtonian systems. The results showed a good agreement with the experimental ones and complete compliance with other methods in benchmark studies. The results indicated that increasing the initial radius of the droplet would increase the steady-state deformation parameter. Moreover, it was shown that increasing viscosity ratio suppressed the droplet deformation. The effect of non-Newtonian fluid behavior was also investigated for a Carreau fluid. Furthermore, the distribution of shear rate around the droplet was discussed.</Abstract>
			<OtherAbstract Language="FA">One of the most important and challenging subjects for scientists is the numerical simulation of the transport phenomena in heterogeneous media. The discontinuity in the properties causes computational errors leading to incorrect estimation of the exact values. The extended finite element method is one of the powerful tools to predict the behavior of heterogenic materials and phenomena. In the present study, we attempted to adapt the extended finite element method to study the flow of a two phase system and investigate the effect of different material and operational parameters such as Capillary number on the drop deformation process in Newtonian/Newtonian and non-Newtonian/ Newtonian systems. The results showed a good agreement with the experimental ones and complete compliance with other methods in benchmark studies. The results indicated that increasing the initial radius of the droplet would increase the steady-state deformation parameter. Moreover, it was shown that increasing viscosity ratio suppressed the droplet deformation. The effect of non-Newtonian fluid behavior was also investigated for a Carreau fluid. Furthermore, the distribution of shear rate around the droplet was discussed.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">extended finite element method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">droplet deformation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Two-phase systems</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">viscosity</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Interfacial tension</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2885_e98741479a7b998f88b8f8c9f0b6b6f1.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Study of the Hemodynamic Parameters of Y-Bypass Graft at Rest and
Exercise State</ArticleTitle>
<VernacularTitle>Numerical Study of the Hemodynamic Parameters of Y-Bypass Graft at Rest and
Exercise State</VernacularTitle>
			<FirstPage>1325</FirstPage>
			<LastPage>1338</LastPage>
			<ELocationID EIdType="pii">2764</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2017.12944.5479</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Ghassem</FirstName>
					<LastName>Heidarinejad</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Hamidreza</FirstName>
					<LastName>Babakhani</LastName>
<Affiliation>tmu</Affiliation>

</Author>
<Author>
					<FirstName>Alireza</FirstName>
					<LastName>Rostami</LastName>
<Affiliation>Arak</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>05</Month>
					<Day>30</Day>
				</PubDate>
			</History>
		<Abstract>The simulation of blood flow in bypass grafts can help medical evaluation. Numerical simulation of blood flow in Configurations recommended by the surgeon Such as the configurations of Y is the aim of this study in order to predict hemodynamic parameters of this configuration in a patient with double stenosis 65 and 50 percent is examined at rest and during exercise. The computational domain was created from CT images from the human cardiac. In this study, blood is assumed homogeneous, non-Newtonian and pulsatile. For real modeling of flow and blood pressure, lumped model is used in outlet at rest and exercise states.The results indicate using this configuration is compensated the pressure drop and flow and time average wall shear stress has reduced in stenosis region and oscillatory shear index and relative residence time range has reduced in area pre and post-stenosis.Y bypass grafting investigation indicates time average wall shear is low at the bifurcation graft and There is possibility of creating restenosis in these areas, but These parameters are in the ideal range at the exercise state.</Abstract>
			<OtherAbstract Language="FA">The simulation of blood flow in bypass grafts can help medical evaluation. Numerical simulation of blood flow in Configurations recommended by the surgeon Such as the configurations of Y is the aim of this study in order to predict hemodynamic parameters of this configuration in a patient with double stenosis 65 and 50 percent is examined at rest and during exercise. The computational domain was created from CT images from the human cardiac. In this study, blood is assumed homogeneous, non-Newtonian and pulsatile. For real modeling of flow and blood pressure, lumped model is used in outlet at rest and exercise states.The results indicate using this configuration is compensated the pressure drop and flow and time average wall shear stress has reduced in stenosis region and oscillatory shear index and relative residence time range has reduced in area pre and post-stenosis.Y bypass grafting investigation indicates time average wall shear is low at the bifurcation graft and There is possibility of creating restenosis in these areas, but These parameters are in the ideal range at the exercise state.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Blood</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Non-Newtonian</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Coronary Artery</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Configuration</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Hemodynamic parameter</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2764_98d8a23fd60826a2a474c5b4f5811707.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical and Experimental Analysis for Fluid Flow Inside Corrugated Tube quipped with Twisted Tapes</ArticleTitle>
<VernacularTitle>Numerical and Experimental Analysis for Fluid Flow Inside Corrugated Tube quipped with Twisted Tapes</VernacularTitle>
			<FirstPage>1339</FirstPage>
			<LastPage>1362</LastPage>
			<ELocationID EIdType="pii">3058</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.14398.5847</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Hossein</FirstName>
					<LastName>Ghalyanchi Langeroudi</LastName>
<Affiliation>PhD student of Department of Mechanical Engineering, ,University Campus 2, University of Guilan, Rasht, Iran,</Affiliation>

</Author>
<Author>
					<FirstName>Kourosh</FirstName>
					<LastName>Javaherdeh</LastName>
<Affiliation>Instructor of Department of Mechanical Engineering, Faculty of Engineering, University of Guilan</Affiliation>
<Identifier Source="ORCID">0000-0002-1570-011X</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2018</Year>
					<Month>05</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>The aim of present paper is to study numerical simulation by using finite volume method for Newtonian and non-Newtonian fluid flow inside corrugated tube equipped with typical twisted tape and V-cut twisted tape at constant heat flux. For validation of this simulation, this results compared with empirical correlations of researchers. In this analysis water was as Newtonian fluid and 0.2 wt % carboxymethyle cellulse in water was as a non-Newtonian fluid, the range of Reynolds number for Newtonian and non-Newtonian fluid varied 5300 to 25700 and 2400 to 6800 respectively. In this analysis, the effects of using different turbulence models, variable heat flux and creating V-cut on Nusselt number and friction factor is investigated. The obtained results showed that standard κ -ω model of turbulence for Newtonian fluid is a proper model rather than the other models and it had good agreements between experimental data, and the average differences for Nusselt number in typical and V-cut twisted tapes were less than 15.2% and 14.4% respectively. On other hand, in identical condition for non-Newtonian fluid, using of standard κ - ε model of turbulence is a proper model rather than the other models and the average differences on Nusselt number for typical twisted tape were less than 18%..</Abstract>
			<OtherAbstract Language="FA">The aim of present paper is to study numerical simulation by using finite volume method for Newtonian and non-Newtonian fluid flow inside corrugated tube equipped with typical twisted tape and V-cut twisted tape at constant heat flux. For validation of this simulation, this results compared with empirical correlations of researchers. In this analysis water was as Newtonian fluid and 0.2 wt % carboxymethyle cellulse in water was as a non-Newtonian fluid, the range of Reynolds number for Newtonian and non-Newtonian fluid varied 5300 to 25700 and 2400 to 6800 respectively. In this analysis, the effects of using different turbulence models, variable heat flux and creating V-cut on Nusselt number and friction factor is investigated. The obtained results showed that standard κ -ω model of turbulence for Newtonian fluid is a proper model rather than the other models and it had good agreements between experimental data, and the average differences for Nusselt number in typical and V-cut twisted tapes were less than 15.2% and 14.4% respectively. On other hand, in identical condition for non-Newtonian fluid, using of standard κ - ε model of turbulence is a proper model rather than the other models and the average differences on Nusselt number for typical twisted tape were less than 18%..</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">computational fluid dynamics</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Twisted tape</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Corrugated tube</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Nusselt number</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Friction factor</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_3058_3f5ee243547dee91fbd053c1c4a845aa.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical and Experimental Investigation of Non-Newtonian High Viscosity Flow
Field in Multi Materials Extrusion Process</ArticleTitle>
<VernacularTitle>Numerical and Experimental Investigation of Non-Newtonian High Viscosity Flow
Field in Multi Materials Extrusion Process</VernacularTitle>
			<FirstPage>1363</FirstPage>
			<LastPage>1380</LastPage>
			<ELocationID EIdType="pii">3009</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.13960.5763</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Seyed Mohammad</FirstName>
					<LastName>Javadi</LastName>
<Affiliation>Quchan university of technology</Affiliation>

</Author>
<Author>
					<FirstName>Ali Mohammad</FirstName>
					<LastName>Naserian-Nik</LastName>
<Affiliation>Department of mechanical engineering, Faculty of engineering, Quchan university of technology</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2018</Year>
					<Month>01</Month>
					<Day>14</Day>
				</PubDate>
			</History>
		<Abstract>Predicting and reducing of the rubber cross-section dimensions after exiting die channel are of great importance in the design process of extrusion die. In this research, the effect of velocity distribution at the die exit on the rubber dimensions is experimentally and numerically studied with the aid of finite volume method. Three-dimensional simulation of non-Newtonian high-viscosity flow was performed to predict the distribution of velocity and pressure in the die channels. Recognizing the soft and hard materials boundaries in the multi-material cross-sections, the two-phase volume of fluid method is employed. The viscosity of melted rubber flow in the die is calculated by interpolating the experimental data obtained from Rubber Process Analyzer apparatus based on least squares method. A comparison between primary (with nonuniform profile) and modified dies shows more precise dimensions of the modified die. In the narrow portions of the profile in the vicinity of wide regions, because of the impossibility of achieving a uniform velocity distribution, the produced cross-section is smaller than the design value. In addition, optimizing channel geometries by the employed numerical method reduces the pressure loss in the modified die by 40% in comparison with that of the primary designed die.</Abstract>
			<OtherAbstract Language="FA">Predicting and reducing of the rubber cross-section dimensions after exiting die channel are of great importance in the design process of extrusion die. In this research, the effect of velocity distribution at the die exit on the rubber dimensions is experimentally and numerically studied with the aid of finite volume method. Three-dimensional simulation of non-Newtonian high-viscosity flow was performed to predict the distribution of velocity and pressure in the die channels. Recognizing the soft and hard materials boundaries in the multi-material cross-sections, the two-phase volume of fluid method is employed. The viscosity of melted rubber flow in the die is calculated by interpolating the experimental data obtained from Rubber Process Analyzer apparatus based on least squares method. A comparison between primary (with nonuniform profile) and modified dies shows more precise dimensions of the modified die. In the narrow portions of the profile in the vicinity of wide regions, because of the impossibility of achieving a uniform velocity distribution, the produced cross-section is smaller than the design value. In addition, optimizing channel geometries by the employed numerical method reduces the pressure loss in the modified die by 40% in comparison with that of the primary designed die.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">numerical simulation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Non-Newtonian</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">high viscosity</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Multi-phase</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">polymer</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_3009_ee16fa83c0f151ef85e617f5aa3867a6.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>A New Approach for Uncertainty Analysis of the Numerical Data Using Genetic Algorithm Based on Grid Refinement</ArticleTitle>
<VernacularTitle>A New Approach for Uncertainty Analysis of the Numerical Data Using Genetic Algorithm Based on Grid Refinement</VernacularTitle>
			<FirstPage>1381</FirstPage>
			<LastPage>1394</LastPage>
			<ELocationID EIdType="pii">2829</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.13246.5581</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mahnaz</FirstName>
					<LastName>Dehghan</LastName>
<Affiliation>Science andResearch Branch, Azad University</Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Dehghan, M.</LastName>
<Affiliation>MAlek Ashtar University</Affiliation>

</Author>
<Author>
					<FirstName>Ali R.</FirstName>
					<LastName>Davari</LastName>
<Affiliation>Department of MEchanical and Aerospace Eng., Schience and Research Branch, Azad University</Affiliation>
<Identifier Source="ORCID">0000-0003-0101-7069</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>08</Month>
					<Day>08</Day>
				</PubDate>
			</History>
		<Abstract>A new approach using the genetic algorithms has been presented to estimate the uncertainties in numerical pressure calculation on a 3D wing. The amount of error in this method has been estimated in the form of power series as a function of the element size. The error tensor is expressed as the sum of squares and has been used as the fitness function in the genetic algorithm. The conventional method for error minimization has been differentiation which is replaced by the genetic algorithm in this paper. The error analysis along with a safety factor has been introduced as the uncertainties in numerical calculations. According to the results, refining the grids down to 25% of the initial size, reduced the error by an amount of 50%. The total uncertainty calculated in this paper was 0.03. This value determines a confidence level of 97.6%. The reliability of the results on three baselines higher than 97% approves the high accuracy of the present calculations. The highest and the lowest reliability in the present calculations was 99.16% and 97.6%, respectively</Abstract>
			<OtherAbstract Language="FA">A new approach using the genetic algorithms has been presented to estimate the uncertainties in numerical pressure calculation on a 3D wing. The amount of error in this method has been estimated in the form of power series as a function of the element size. The error tensor is expressed as the sum of squares and has been used as the fitness function in the genetic algorithm. The conventional method for error minimization has been differentiation which is replaced by the genetic algorithm in this paper. The error analysis along with a safety factor has been introduced as the uncertainties in numerical calculations. According to the results, refining the grids down to 25% of the initial size, reduced the error by an amount of 50%. The total uncertainty calculated in this paper was 0.03. This value determines a confidence level of 97.6%. The reliability of the results on three baselines higher than 97% approves the high accuracy of the present calculations. The highest and the lowest reliability in the present calculations was 99.16% and 97.6%, respectively</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Uncertainty</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">genetic algorithm</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">power series</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Computational fluid dynamics          3D wing</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2829_46b2644cbdf489fac0e2d192212d206d.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Design of a Pelton Turbine Installed on Centrifugal Pump in Reverse Osmosis System
for Energy Recovery</ArticleTitle>
<VernacularTitle>Design of a Pelton Turbine Installed on Centrifugal Pump in Reverse Osmosis System
for Energy Recovery</VernacularTitle>
			<FirstPage>1395</FirstPage>
			<LastPage>1410</LastPage>
			<ELocationID EIdType="pii">2962</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.13874.5735</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Abdollah</FirstName>
					<LastName>Eskandari</LastName>
<Affiliation>Payame Noor University - Faculty of Engineering</Affiliation>
<Identifier Source="ORCID">0000-0003-4441-6473</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>12</Month>
					<Day>27</Day>
				</PubDate>
			</History>
		<Abstract>In this work, injector regulating valve and Pelton turbine impeller has been numerically and analytically designed and simulated. The impeller of the Pelton turbine added on the shaft of a high pressure multistage pump which is used in sea water reverse osmosis package to recover a part of input power from rejected flow return back after filter unit. Using ANSYS CFX, flow through the regulating valve for many outlet injector diameters has been numerically simulated to obtain head loss. For the point of operation, dimension of turbine impeller calculated using turbomachinery relations and some experimental data in order to synchronize as much as possible with the pump. The exact point of operation for the pump, turbine and injector obtained by intersecting performance curves of pump and turbine. In order to investigate the results, the full-scale Pelton turbine and regulating valve manufactured with the material of duplex and installed on the pump. Performance test on the site shown about 26% decrease in input power. Because of the affinity relation for turbomachinery, the results can be validated for other point of operation due to change in pump speed.</Abstract>
			<OtherAbstract Language="FA">In this work, injector regulating valve and Pelton turbine impeller has been numerically and analytically designed and simulated. The impeller of the Pelton turbine added on the shaft of a high pressure multistage pump which is used in sea water reverse osmosis package to recover a part of input power from rejected flow return back after filter unit. Using ANSYS CFX, flow through the regulating valve for many outlet injector diameters has been numerically simulated to obtain head loss. For the point of operation, dimension of turbine impeller calculated using turbomachinery relations and some experimental data in order to synchronize as much as possible with the pump. The exact point of operation for the pump, turbine and injector obtained by intersecting performance curves of pump and turbine. In order to investigate the results, the full-scale Pelton turbine and regulating valve manufactured with the material of duplex and installed on the pump. Performance test on the site shown about 26% decrease in input power. Because of the affinity relation for turbomachinery, the results can be validated for other point of operation due to change in pump speed.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Pelton turbine</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">injector</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">numerical simulation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Performance Curve</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Reverse osmosis package</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2962_3b2d8f129ae2f408f2153cd9ce663043.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Investigation of Flow Behavior Around Chordwise Morphing NACA 0012</ArticleTitle>
<VernacularTitle>Numerical Investigation of Flow Behavior Around Chordwise Morphing NACA 0012</VernacularTitle>
			<FirstPage>1411</FirstPage>
			<LastPage>1426</LastPage>
			<ELocationID EIdType="pii">2815</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.13708.5699</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Seyed Esmail</FirstName>
					<LastName>Razavi</LastName>
<Affiliation>Professor at University of Tabriz</Affiliation>

</Author>
<Author>
					<FirstName>Mir Hossein</FirstName>
					<LastName>Negahban</LastName>
<Affiliation>M.Sc. Graduate Student of University of Tabriz</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>11</Month>
					<Day>17</Day>
				</PubDate>
			</History>
		<Abstract>In the present study, numerical simulation of transonic flow around chordwise morphing airfoil has been accessed. Fluid-Structure interaction for analyzing flow field behavior in conjunction with morphing airfoil is used. In this regard, a two-dimensional finite element model is established and the arbitrary Lagrangian-Eulerian formulation (ALE), in the flow field and structure configuration is applied to accommodate the deforming boundaries and due to the good conformation of flow filed and deforming boundaries in this formulation, the distortion of computational grid is diminished after the deformation. The procedure incorporates the one-equation Spalart-Allmaras turbulence model which is a suitable model for aerodynamics. In this study, the preferable Mach number for the transonic regime is 0.7. Chordwise elastic deformability by uniformly varying extended parabolic load on both leading and trailing edges is considered for morphing purposes. The model is validated against conventional rigid airfoil for various angles of attack, and the comparisons show considerable improvement in the aerodynamic performance and prove the efficiency of elastic morphing airfoil. Moreover, the ultimate results indicate that chordwise morphing contributes to the best flight conditions for cruise flight which contains a wide flight endurance. All the simulations are steady-state and are carried out by COMSOL Multiphysics software.</Abstract>
			<OtherAbstract Language="FA">In the present study, numerical simulation of transonic flow around chordwise morphing airfoil has been accessed. Fluid-Structure interaction for analyzing flow field behavior in conjunction with morphing airfoil is used. In this regard, a two-dimensional finite element model is established and the arbitrary Lagrangian-Eulerian formulation (ALE), in the flow field and structure configuration is applied to accommodate the deforming boundaries and due to the good conformation of flow filed and deforming boundaries in this formulation, the distortion of computational grid is diminished after the deformation. The procedure incorporates the one-equation Spalart-Allmaras turbulence model which is a suitable model for aerodynamics. In this study, the preferable Mach number for the transonic regime is 0.7. Chordwise elastic deformability by uniformly varying extended parabolic load on both leading and trailing edges is considered for morphing purposes. The model is validated against conventional rigid airfoil for various angles of attack, and the comparisons show considerable improvement in the aerodynamic performance and prove the efficiency of elastic morphing airfoil. Moreover, the ultimate results indicate that chordwise morphing contributes to the best flight conditions for cruise flight which contains a wide flight endurance. All the simulations are steady-state and are carried out by COMSOL Multiphysics software.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Morphing airfoil</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Transonic flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Elastic deformation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">compressible flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Shock Wave</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2815_f5b1b89d98b7286673128a5fb112cb9a.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Study of Water Droplet Impact on a Surface Using a Sharp Approach for
Interface Modeling</ArticleTitle>
<VernacularTitle>Numerical Study of Water Droplet Impact on a Surface Using a Sharp Approach for
Interface Modeling</VernacularTitle>
			<FirstPage>1427</FirstPage>
			<LastPage>1442</LastPage>
			<ELocationID EIdType="pii">1024</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2017.12679.5395</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mohammad</FirstName>
					<LastName>Emdadi</LastName>
<Affiliation>Yasouj University, Yasouj, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>03</Month>
					<Day>19</Day>
				</PubDate>
			</History>
		<Abstract>In this research, water droplet impact process on a solid surface is simulated using a sharp approach for interface modeling. This approach is based on the solving momentum and continuity equations and imposing appropriate jump conditions at the interface. The level set method is used for interface tracking and the ghost fluid method is used to impose jump conditions at the interface accurately. In this way, smearing of quantities across interface is prevented and discontinuities are preserved at interface. The accuracy of numerical procedure is approved via comparison of simulation results with experimental and numerical data. Simulation results show that the used numerical method in comparison with the volume of fluid method represents more accurate prediction of droplet behavior during impact process. The effect of contact angle between water droplet and surface on the impact process is investigated. For contact angles less than 90°, water droplet spreads on the surface after impact. But, for contact angles greater than 90°, droplet starts to recoil after spreading. In this case, it is possible that droplet rebound from surface after recoiling. Maximum spreading radius of droplet decreases by an increase in contact angle.</Abstract>
			<OtherAbstract Language="FA">In this research, water droplet impact process on a solid surface is simulated using a sharp approach for interface modeling. This approach is based on the solving momentum and continuity equations and imposing appropriate jump conditions at the interface. The level set method is used for interface tracking and the ghost fluid method is used to impose jump conditions at the interface accurately. In this way, smearing of quantities across interface is prevented and discontinuities are preserved at interface. The accuracy of numerical procedure is approved via comparison of simulation results with experimental and numerical data. Simulation results show that the used numerical method in comparison with the volume of fluid method represents more accurate prediction of droplet behavior during impact process. The effect of contact angle between water droplet and surface on the impact process is investigated. For contact angles less than 90°, water droplet spreads on the surface after impact. But, for contact angles greater than 90°, droplet starts to recoil after spreading. In this case, it is possible that droplet rebound from surface after recoiling. Maximum spreading radius of droplet decreases by an increase in contact angle.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Droplet Impact</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Level set Method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Ghost Fluid Method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">contact angle</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_1024_021bbc7ee20b71134d53e20206bd6feb.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Performance Investigation of Hybrid Darrieus-Savonius Wind Turbine Compared to
Straight-Bladed Darrieus Turbine by Three-Dimensional Numerical Simulation</ArticleTitle>
<VernacularTitle>Performance Investigation of Hybrid Darrieus-Savonius Wind Turbine Compared to
Straight-Bladed Darrieus Turbine by Three-Dimensional Numerical Simulation</VernacularTitle>
			<FirstPage>1443</FirstPage>
			<LastPage>1454</LastPage>
			<ELocationID EIdType="pii">2820</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.13505.5651</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Nozar</FirstName>
					<LastName>Akbari</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Abolfazl</FirstName>
					<LastName>Abdolahifar</LastName>
<Affiliation>Aerodynamics,Aerospace Faculty,AmirKabir University of Technology(Tehran Polytechnic),Tehran,Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>10</Month>
					<Day>08</Day>
				</PubDate>
			</History>
		<Abstract>The purpose of this research is to investigate the performance of hybrid Darrieus- Savonius wind turbines to achieve a model with high starting moment and suitable performance conditions. Straight-bladed Darrieus wind turbines have high-amplitude fluctuations in moment and, at some angles, this moment is not enough to start the turbine motion. The hybrid turbine is compared with two equivalent models of straight-bladed Darrieus wind turbines. The first model has equal available power and the second model has equal height with the hybrid turbine. Three-dimensional simulation is performed using computational fluid dynamics and solving unsteady Reynolds averaged Navier-Stokes equations with finite volume method, using turbulence model and rotating mesh for rotation of the turbine. According to the results, at the self-starting, the hybrid turbine possesses 22.24% and 17.5% less standard deviation and 69.8% and 56.9% more average moment, respectively, compared to the first and second equivalent turbines. In operational mode, the hybrid turbine at the rotational speed of 30 RPM possesses 16.1% and 27.3% less standard deviation and 19.1% and 1.03% more average moment, respectively. Therefore, the hybrid turbine at the self-starting, as well as at low rotational speeds, possesses more average moment and less fluctuations compared to equivalent Darrieus turbines.</Abstract>
			<OtherAbstract Language="FA">The purpose of this research is to investigate the performance of hybrid Darrieus- Savonius wind turbines to achieve a model with high starting moment and suitable performance conditions. Straight-bladed Darrieus wind turbines have high-amplitude fluctuations in moment and, at some angles, this moment is not enough to start the turbine motion. The hybrid turbine is compared with two equivalent models of straight-bladed Darrieus wind turbines. The first model has equal available power and the second model has equal height with the hybrid turbine. Three-dimensional simulation is performed using computational fluid dynamics and solving unsteady Reynolds averaged Navier-Stokes equations with finite volume method, using turbulence model and rotating mesh for rotation of the turbine. According to the results, at the self-starting, the hybrid turbine possesses 22.24% and 17.5% less standard deviation and 69.8% and 56.9% more average moment, respectively, compared to the first and second equivalent turbines. In operational mode, the hybrid turbine at the rotational speed of 30 RPM possesses 16.1% and 27.3% less standard deviation and 19.1% and 1.03% more average moment, respectively. Therefore, the hybrid turbine at the self-starting, as well as at low rotational speeds, possesses more average moment and less fluctuations compared to equivalent Darrieus turbines.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Savonius</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Darrieus</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Self-starting</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Hybrid turbine</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">computational fluid dynamics</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2820_aee92f16efd522b9326c25cc3237ac15.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Investigation of a Pulse-Jet Filter Cleaning System Performance</ArticleTitle>
<VernacularTitle>Numerical Investigation of a Pulse-Jet Filter Cleaning System Performance</VernacularTitle>
			<FirstPage>1455</FirstPage>
			<LastPage>1468</LastPage>
			<ELocationID EIdType="pii">2891</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.12920.5469</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Amir</FirstName>
					<LastName>Arefian</LastName>
<Affiliation>Department of Mechanical Engineering, Amirkabir University of Technology, Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Navid</FirstName>
					<LastName>Zehtabiyan-Rezaie</LastName>
<Affiliation>Department of Mechanical Engineering, Amirkabir University of Technology, Tehran, Iran</Affiliation>
<Identifier Source="ORCID">0000-0003-1189-0507</Identifier>

</Author>
<Author>
					<FirstName>Reza</FirstName>
					<LastName>Hosseini Abardeh</LastName>
<Affiliation>Department of Mechanical Engineering, Amirkabir University of Technology, Tehran, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>05</Month>
					<Day>21</Day>
				</PubDate>
			</History>
		<Abstract>In this study, numerical simulation of a pulse-jet filter cleaning system is conducted and its performance is investigated under pre-defined conditions. In the first step, 3D simulation of the system from a high pressure tank to the filter inlet is performed and the output is used as the input of second step. In the second step, simulation is performed for filters with inlet mass flow rates calculated from the previous step. To validate the model, the results are compared to experimental data showing acceptable agreement. The results show that regardless of the valve type, the cleaning pulse generates after 0.5 s and suddenly decreases afterward. No shock or choking is observed in the system. Another interesting result is the induced flow, generated after the nozzles, which increases the filter inlet mass flow rate. In addition, the axial distribution of the filter outlet flow is not uniform, degrading from inlet to outlet. Finally, a complete parametric study is performed to investigate the effect of the tank pressure on the pressure difference in the filter which is an important index in the cleaning performance analysis.</Abstract>
			<OtherAbstract Language="FA">In this study, numerical simulation of a pulse-jet filter cleaning system is conducted and its performance is investigated under pre-defined conditions. In the first step, 3D simulation of the system from a high pressure tank to the filter inlet is performed and the output is used as the input of second step. In the second step, simulation is performed for filters with inlet mass flow rates calculated from the previous step. To validate the model, the results are compared to experimental data showing acceptable agreement. The results show that regardless of the valve type, the cleaning pulse generates after 0.5 s and suddenly decreases afterward. No shock or choking is observed in the system. Another interesting result is the induced flow, generated after the nozzles, which increases the filter inlet mass flow rate. In addition, the axial distribution of the filter outlet flow is not uniform, degrading from inlet to outlet. Finally, a complete parametric study is performed to investigate the effect of the tank pressure on the pressure difference in the filter which is an important index in the cleaning performance analysis.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Pulse-jet</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">filter cleaning system</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">gas filter</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">compressible flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Transient Flow</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2891_7a006957be65e608e863301eb98e1808.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Steady Simulation of the Flow inside the Internal Combustion Engine Turbocharger’s
Turbine</ArticleTitle>
<VernacularTitle>Steady Simulation of the Flow inside the Internal Combustion Engine Turbocharger’s
Turbine</VernacularTitle>
			<FirstPage>1469</FirstPage>
			<LastPage>1486</LastPage>
			<ELocationID EIdType="pii">2998</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.14098.5810</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mojtaba</FirstName>
					<LastName>Farajpoor Khanaposhtani</LastName>
<Affiliation>Mechanical Engineering Department, AmirKabir University of Technology.</Affiliation>

</Author>
<Author>
					<FirstName>S.Mostafa</FirstName>
					<LastName>Agha Mirsalim</LastName>
<Affiliation>Mechanical Engineering Department of Amirkabir University, Iran, Tehran</Affiliation>

</Author>
<Author>
					<FirstName>Seyyed Shahaboldin</FirstName>
					<LastName>Alavioun</LastName>
<Affiliation>Expert of Designing Department of Iran Khodro&amp;#039;s Research Institute (IPCO Company)</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>03</Day>
				</PubDate>
			</History>
		<Abstract>Turbocharger systems, can increase volumetric efficiency and decrease fuel consumption and emissions of an engine due to compressing the entering air to the engine. Flow characteristic inside turbine is sophisticated and several phenomena like flow separation and high turbulent flow can occur inside turbine. Determining exact performance behavior of turbine can alter the matching process of the turbocharger with the engine. The main goal of this research is 3D and steady simulation of the flow inside turbocharger’s turbine and analysis of the performance behavior of turbine under different working conditions. To this end, 3D flow inside turbine including volute, rotor, diffuser and wastegate passage is investigated steadily. Validating simulation results by experimental results shows that there exist 3 to 9 percent of error between these. In order to control the rotational speed of turbine, turbocharger is equipped with wastegate. By measuring the exact amount of wastegate opening in different working conditions of turbine on a test cell, flow simulation inside turbine is accomplished in different wastegate openings and the effect of wastegate opening on the turbine performance and isentropic efficiency is investigated. The results shows that opening of wastegate can reduce isentropic efficiency and power produced by the turbine significantly.</Abstract>
			<OtherAbstract Language="FA">Turbocharger systems, can increase volumetric efficiency and decrease fuel consumption and emissions of an engine due to compressing the entering air to the engine. Flow characteristic inside turbine is sophisticated and several phenomena like flow separation and high turbulent flow can occur inside turbine. Determining exact performance behavior of turbine can alter the matching process of the turbocharger with the engine. The main goal of this research is 3D and steady simulation of the flow inside turbocharger’s turbine and analysis of the performance behavior of turbine under different working conditions. To this end, 3D flow inside turbine including volute, rotor, diffuser and wastegate passage is investigated steadily. Validating simulation results by experimental results shows that there exist 3 to 9 percent of error between these. In order to control the rotational speed of turbine, turbocharger is equipped with wastegate. By measuring the exact amount of wastegate opening in different working conditions of turbine on a test cell, flow simulation inside turbine is accomplished in different wastegate openings and the effect of wastegate opening on the turbine performance and isentropic efficiency is investigated. The results shows that opening of wastegate can reduce isentropic efficiency and power produced by the turbine significantly.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Turbocharger</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Turbine</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">3D simulation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Wastegate</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">isentropic efficiency</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2998_71887f62f073a78511cbac56f8cab53f.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>51</Volume>
				<Issue>6</Issue>
				<PubDate PubStatus="epublish">
					<Year>2020</Year>
					<Month>02</Month>
					<Day>20</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Experimental Study of Hydrodynamic Behavior and Breakup of Liquid Jet with/
without the Electric Field</ArticleTitle>
<VernacularTitle>Experimental Study of Hydrodynamic Behavior and Breakup of Liquid Jet with/
without the Electric Field</VernacularTitle>
			<FirstPage>1487</FirstPage>
			<LastPage>1498</LastPage>
			<ELocationID EIdType="pii">2795</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2018.13591.5679</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Reza</FirstName>
					<LastName>Gharraei Khosroshahi</LastName>
<Affiliation>Mechanical Engineering Department, Azarbaijan Shahid Madani University</Affiliation>

</Author>
<Author>
					<FirstName>Mahdi</FirstName>
					<LastName>Tavana</LastName>
<Affiliation>Mechanical Engineering Department, Azarbaijan Shahid Madani University, Tabriz, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Sima</FirstName>
					<LastName>Baheri Islami</LastName>
<Affiliation>Associate Professor/ University of Tabriz</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>10</Month>
					<Day>25</Day>
				</PubDate>
			</History>
		<Abstract>In this study, the hydrodynamic behavior of fluid jet with/without application of electric field is studied and intensity and direction of the electrical field are investigated experimentally on instability and jet breakup. The study of the shape and size of produced droplets after the fluid jet breakup are another cases in this study. Results show that fluid jet characteristics depend on Reynolds number in jets which are only based on gravity. Jet mean diameter and its breakup length in this type of jets are directly related to Reynolds number. Studies show that jet mean diameter is increased and breakup length is decreased by applying electrical field. According to investigations, increasing of electrical field intensity leads to decreasing in jet breakup length and direct field has a significant effect in comparison with reverse one on it. Studies show that jet mean diameter and breakup length are decreased by applying electrical field. Increasing of electrical field intensity leads to decreasing in jet breakup length and direct field has a significant effect in comparison with reverse one on it. By applying a 6 kV electric field, the upper jet breakup length can be reduced by 27% in comparison with non-field state. The standard deviation of produced droplets in non-filed state and reverse electrical field with 2kV intensity is equal to 1.3 and 1.1, respectively which indicates a more uniform droplet in presence of reverse electric field. The investigation of produced droplets in term of roundness showed that electrical field leads to producing circular droplets and reducing the frequency of irregular droplets.</Abstract>
			<OtherAbstract Language="FA">In this study, the hydrodynamic behavior of fluid jet with/without application of electric field is studied and intensity and direction of the electrical field are investigated experimentally on instability and jet breakup. The study of the shape and size of produced droplets after the fluid jet breakup are another cases in this study. Results show that fluid jet characteristics depend on Reynolds number in jets which are only based on gravity. Jet mean diameter and its breakup length in this type of jets are directly related to Reynolds number. Studies show that jet mean diameter is increased and breakup length is decreased by applying electrical field. According to investigations, increasing of electrical field intensity leads to decreasing in jet breakup length and direct field has a significant effect in comparison with reverse one on it. Studies show that jet mean diameter and breakup length are decreased by applying electrical field. Increasing of electrical field intensity leads to decreasing in jet breakup length and direct field has a significant effect in comparison with reverse one on it. By applying a 6 kV electric field, the upper jet breakup length can be reduced by 27% in comparison with non-field state. The standard deviation of produced droplets in non-filed state and reverse electrical field with 2kV intensity is equal to 1.3 and 1.1, respectively which indicates a more uniform droplet in presence of reverse electric field. The investigation of produced droplets in term of roundness showed that electrical field leads to producing circular droplets and reducing the frequency of irregular droplets.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Fluid Jet</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Breakup Length</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Electrohydrodynamic</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Dielectric</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_2795_a7f592cef8b130a6967a90617db5681b.pdf</ArchiveCopySource>
</Article>
</ArticleSet>
