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<ArticleSet>
<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Experimental investigation on natural frequencies of thin rectangular plates using contact and non-contact methods</ArticleTitle>
<VernacularTitle>Experimental investigation on natural frequencies of thin rectangular plates using contact and non-contact methods</VernacularTitle>
			<FirstPage>1</FirstPage>
			<LastPage>11</LastPage>
			<ELocationID EIdType="pii">1225</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.6725.2563</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>P.</FirstName>
					<LastName>Oliazadeh</LastName>
<Affiliation>Mechanic,Engineering,Fedowsi University of Mashhad, Mashhad, Iran</Affiliation>
<Identifier Source="ORCID">0000-0002-2820-8079</Identifier>

</Author>
<Author>
					<FirstName>A.</FirstName>
					<LastName>Farshidianfar</LastName>
<Affiliation>Mechanic,Engineering,Ferdowsi University of Mashhad, Mashhad, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2018</Year>
					<Month>02</Month>
					<Day>02</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, two excitation methods, namely contact and non-contact methods were used to excite a thin rectangular plate with clampled boundary conditions at all four edges. A modal hammer was used to apply an impact on the surface of the plate in the contact method while for the non-contact method, three loudspeakers were utilized to excite the plate by emitting a white noise signal. The loudspeakers covered low, medium and high ranges of frequency. Different positions for excitation point were suggested in order to find the best position in which the accelerometer is more capable of measuring the vibration of plate surface at natural frequencies. By comparing two types of excitation, the non-contact method was discovered to have advantages over contact method in medium and high frequency ranges and the contact method had better performance in low frequency range. An approximate analytical method based on Rayleigh-Ritz method was also studied in order to compare and validate the experimental results in predicting natural frequencies of a thin rectangular plate.</Abstract>
			<OtherAbstract Language="FA">In this paper, two excitation methods, namely contact and non-contact methods were used to excite a thin rectangular plate with clampled boundary conditions at all four edges. A modal hammer was used to apply an impact on the surface of the plate in the contact method while for the non-contact method, three loudspeakers were utilized to excite the plate by emitting a white noise signal. The loudspeakers covered low, medium and high ranges of frequency. Different positions for excitation point were suggested in order to find the best position in which the accelerometer is more capable of measuring the vibration of plate surface at natural frequencies. By comparing two types of excitation, the non-contact method was discovered to have advantages over contact method in medium and high frequency ranges and the contact method had better performance in low frequency range. An approximate analytical method based on Rayleigh-Ritz method was also studied in order to compare and validate the experimental results in predicting natural frequencies of a thin rectangular plate.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Contact method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Non-contact method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Thin rectangular plate</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Natural frequency</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1225_d164bf0055e30a33ddba9e7129d16311.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Stress and Strain Analysis of Femur in Taylor Spatial Frame</ArticleTitle>
<VernacularTitle>Stress and Strain Analysis of Femur in Taylor Spatial Frame</VernacularTitle>
			<FirstPage>13</FirstPage>
			<LastPage>21</LastPage>
			<ELocationID EIdType="pii">1235</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.5543.2362</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>P.</FirstName>
					<LastName>Chavoshnejad</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Ayati</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Baniassadi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>A.</FirstName>
					<LastName>Abbaspour</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Mazraeh Ei Farahani</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>A.</FirstName>
					<LastName>Heidary Rouchi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>04</Month>
					<Day>09</Day>
				</PubDate>
			</History>
		<Abstract>Correction of femur deformity can be accomplished using both external and internal fixtures. The advantages of using circular external fixture include less soft tissue injury, better bone alignment and enhanced strain on cutting section, which causes less healing time. This paper focuses on experimental and Finite Element Analysis (FEA) study of circular external fixture, including two rings and six adjustable struts, with six degrees of freedom (Taylor Spatial Frame (TSF)). Femur 3d model was created using Mimics® software while FEA was accomplished using ABAQUS® software. The FEA was based on the assumptions, that the bone is loaded equal to a standing person load. The femur model was assumed to be isotropic and homogeneous in both cortical and spongy phases. FEA results were verified by corresponding strain measured in experimental tests. Based on these results, the maximum value of stress occurs in the location of pins and half-pins. Moreover, the maximum stress in the connection location of pins is higher than those of half-pins. Results show that substitution of half-pins with pins, in the points with maximum stress, causes reduction of stress and thus the pain is reduced.</Abstract>
			<OtherAbstract Language="FA">Correction of femur deformity can be accomplished using both external and internal fixtures. The advantages of using circular external fixture include less soft tissue injury, better bone alignment and enhanced strain on cutting section, which causes less healing time. This paper focuses on experimental and Finite Element Analysis (FEA) study of circular external fixture, including two rings and six adjustable struts, with six degrees of freedom (Taylor Spatial Frame (TSF)). Femur 3d model was created using Mimics® software while FEA was accomplished using ABAQUS® software. The FEA was based on the assumptions, that the bone is loaded equal to a standing person load. The femur model was assumed to be isotropic and homogeneous in both cortical and spongy phases. FEA results were verified by corresponding strain measured in experimental tests. Based on these results, the maximum value of stress occurs in the location of pins and half-pins. Moreover, the maximum stress in the connection location of pins is higher than those of half-pins. Results show that substitution of half-pins with pins, in the points with maximum stress, causes reduction of stress and thus the pain is reduced.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Femur</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Taylor Spatial Frame (TSF)</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Stress analysis</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Bone Biomechanics</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Femur deformity</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1235_1e59b76c5d78438aad3e7e4372a85fdc.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>optimization of  locomotive structure by using of natural frequency and maximum stress constraints</ArticleTitle>
<VernacularTitle>optimization of  locomotive structure by using of natural frequency and maximum stress constraints</VernacularTitle>
			<FirstPage>23</FirstPage>
			<LastPage>33</LastPage>
			<ELocationID EIdType="pii">1200</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2017.925.0</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Ghamami</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Shariat Panahi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Mondali</LastName>
<Affiliation>mapna locomotive</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2013</Year>
					<Month>06</Month>
					<Day>18</Day>
				</PubDate>
			</History>
		<Abstract>In today&#039;s design, the system complexity and increasing demand for safer, more efficient and less costly has created new challenges in science and engineering. Locomotives is product that is designed according to customer order and technical needs of most customers, targets of companies based designer and manufacturer of locomotives always be on the path of progress, and seeks to offer products with higher technology than other competitors.&lt;br /&gt; In each engineering and design problem, optimization can be applied. The objective of the op-timization is to choose the best plan among acceptable plans. Body structures quality based primarily on indicators such as natural frequency, displacement, fatigue life and the maximum stress occurring in the body takes place. Natural frequency of the various components of the system and adapt them to each other in order to avoid the phenomenon of resonance is impor-tant.In this study, body structures locomotive ER 24 has been studied. A combination of particle swarm algorithm (PSO) and artificial neural networks is proposed to find the optimal weight of structures subject to multiple natural frequency constraints. Optimization of locomotive&#039;s structure has been done with an emphasis on maintaining locomotive abilities in Static and dynamic field. The results indicate that the use of optimization techniques in the design process is powerful and effective tool for identifying and improving the main dynamic characteristics of structures and also op-timizing performance in stress, noise &amp; vibration field.</Abstract>
			<OtherAbstract Language="FA">In today&#039;s design, the system complexity and increasing demand for safer, more efficient and less costly has created new challenges in science and engineering. Locomotives is product that is designed according to customer order and technical needs of most customers, targets of companies based designer and manufacturer of locomotives always be on the path of progress, and seeks to offer products with higher technology than other competitors.&lt;br /&gt; In each engineering and design problem, optimization can be applied. The objective of the op-timization is to choose the best plan among acceptable plans. Body structures quality based primarily on indicators such as natural frequency, displacement, fatigue life and the maximum stress occurring in the body takes place. Natural frequency of the various components of the system and adapt them to each other in order to avoid the phenomenon of resonance is impor-tant.In this study, body structures locomotive ER 24 has been studied. A combination of particle swarm algorithm (PSO) and artificial neural networks is proposed to find the optimal weight of structures subject to multiple natural frequency constraints. Optimization of locomotive&#039;s structure has been done with an emphasis on maintaining locomotive abilities in Static and dynamic field. The results indicate that the use of optimization techniques in the design process is powerful and effective tool for identifying and improving the main dynamic characteristics of structures and also op-timizing performance in stress, noise &amp; vibration field.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Locomotive</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Modal Analysis</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Artificial nural network</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Particle swarm algorithm</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Stress analysis</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1200_a267c9621f8930c975bc3176c87847c6.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>The effects of arbitrary boundary conditions on a laminated composite plate response subjected to large mass &amp; low velocity impact</ArticleTitle>
<VernacularTitle>The effects of arbitrary boundary conditions on a laminated composite plate response subjected to large mass &amp; low velocity impact</VernacularTitle>
			<FirstPage>35</FirstPage>
			<LastPage>49</LastPage>
			<ELocationID EIdType="pii">1228</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.6333.2495</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>R.</FirstName>
					<LastName>Paknejad</LastName>
<Affiliation>Fac. of Mech. Eng., Shahid Rajaee Teacher Training University (SRTTU), Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>F.</FirstName>
					<LastName>Ashenai Ghasemi</LastName>
<Affiliation>Faculty of Mechanical Engineering, Shahid Rajaee Teacher Training University, Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>K.</FirstName>
					<LastName>Malekzadeh Fard</LastName>
<Affiliation>Department of Aerospace Structures, Aerospace University Complex, Malek Ashtar University of Technology, Tehran, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>10</Month>
					<Day>21</Day>
				</PubDate>
			</History>
		<Abstract>In this research, the effects of arbitrary boundary conditions on a laminated composite plate response subjected to large mass and low-velocity impact has been studied. When the impactor is defined large-mass, its mass ratio to the target mass is greater than 2. For this purpose, the first-order shear deformation theory was considered as the displacement field of the composite laminated plate. Then, using the analytic method based on suitable algebraic polynomials and the Galerkin function, the motion equations for several types of different boundary conditions was solved. Also in this work, the interaction between the impactor and the composite laminated plate were modeled using a two degrees-of-freedom system, consisting of springs-masses. The results indicate that the arbitrary boundary conditions are effective on the natural frequency of the composite plate. These effects are remarkable on contact forces and displacements of the composite plate for clamped to simply support and free boundary conditions. Some of parameters like arbitrary boundary conditions, mass and velocity of the impactor in a constant impact energy level and radius of impactor are important factors affecting the impact process and the design of structures.</Abstract>
			<OtherAbstract Language="FA">In this research, the effects of arbitrary boundary conditions on a laminated composite plate response subjected to large mass and low-velocity impact has been studied. When the impactor is defined large-mass, its mass ratio to the target mass is greater than 2. For this purpose, the first-order shear deformation theory was considered as the displacement field of the composite laminated plate. Then, using the analytic method based on suitable algebraic polynomials and the Galerkin function, the motion equations for several types of different boundary conditions was solved. Also in this work, the interaction between the impactor and the composite laminated plate were modeled using a two degrees-of-freedom system, consisting of springs-masses. The results indicate that the arbitrary boundary conditions are effective on the natural frequency of the composite plate. These effects are remarkable on contact forces and displacements of the composite plate for clamped to simply support and free boundary conditions. Some of parameters like arbitrary boundary conditions, mass and velocity of the impactor in a constant impact energy level and radius of impactor are important factors affecting the impact process and the design of structures.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Impact</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Composite Plate</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Arbitrary Boundary Conditions</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Galerkin's Method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Springs-Masses Model</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1228_ad8fc89ce922bee0ba5953faef358d29.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Experimental Analysis of Effective Parameters on Human Balance During Standing and Gaiting</ArticleTitle>
<VernacularTitle>Experimental Analysis of Effective Parameters on Human Balance During Standing and Gaiting</VernacularTitle>
			<FirstPage>51</FirstPage>
			<LastPage>57</LastPage>
			<ELocationID EIdType="pii">1226</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.6614.2546</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>S. A.</FirstName>
					<LastName>Hoseini Sabzevari</LastName>
<Affiliation>University of Gonabad</Affiliation>

</Author>
<Author>
					<FirstName>E.</FirstName>
					<LastName>Amiri</LastName>
<Affiliation>University of Gonabad</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2018</Year>
					<Month>01</Month>
					<Day>08</Day>
				</PubDate>
			</History>
		<Abstract>Sudden falls are known as the second cause of accidental injury deaths by the world health organization. In this paper effective parameters caused in human balance are analyzed in order to prevent fall. As experimental examples, effect of the parameters on human balance during standing and gaiting were investigated. For this purpose, a database is gathered. These information were recorded while 30 student balances were affected by the parameters changing in both standing and gaiting situation. In the specified pattern, the effect of vision, vestibular system and muscle strength were studied in both standing and gaiting, individually. Furthermore, in order to study the human balance while using a cell phone in gaiting, several experiments were extended. The results show the influence of the parameters on human balance. Although, men had better balance rather than women while standing but women were shown beter balanve while using a cell phone in gaiting.</Abstract>
			<OtherAbstract Language="FA">Sudden falls are known as the second cause of accidental injury deaths by the world health organization. In this paper effective parameters caused in human balance are analyzed in order to prevent fall. As experimental examples, effect of the parameters on human balance during standing and gaiting were investigated. For this purpose, a database is gathered. These information were recorded while 30 student balances were affected by the parameters changing in both standing and gaiting situation. In the specified pattern, the effect of vision, vestibular system and muscle strength were studied in both standing and gaiting, individually. Furthermore, in order to study the human balance while using a cell phone in gaiting, several experiments were extended. The results show the influence of the parameters on human balance. Although, men had better balance rather than women while standing but women were shown beter balanve while using a cell phone in gaiting.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Sudden Fall</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Human Balance</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Gaiting</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Cell Phone</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1226_f211406c0668e0ec922464e60ca59a65.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>An Experimental Study and Statistical Modelling on Compressive Properties of Epoxy/ Graphene/ Hydroxyapatite Nanocomposites</ArticleTitle>
<VernacularTitle>An Experimental Study and Statistical Modelling on Compressive Properties of Epoxy/ Graphene/ Hydroxyapatite Nanocomposites</VernacularTitle>
			<FirstPage>59</FirstPage>
			<LastPage>70</LastPage>
			<ELocationID EIdType="pii">1196</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.5873.2414</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>S.</FirstName>
					<LastName>Fooladpanjeh</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>A.</FirstName>
					<LastName>Dadrasi</LastName>
<Affiliation>Member of Board in Islamic Azad University- Shahrood Branch</Affiliation>

</Author>
<Author>
					<FirstName>A.</FirstName>
					<LastName>Alavi Gharebagh</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>06</Month>
					<Day>11</Day>
				</PubDate>
			</History>
		<Abstract>In this article, an experimental and numerical study on compression strength, energy and elongation at break of epoxy based nanocomposites reinforced by graphene oxide and hydroxyapatite has been done. Graphene oxide and hydroxyapatite were used up to 0.5 &amp; 7 wt.%, respectively. Filler&#039;s weight fractions that used as design parameters have been achieved by design of experiment through central composite design method. Weight fractions of fillers have been considered as input parameters for modeling by RSM, ANN &amp; regression tree method. Experimental results show the addition of nanoparticles increase compression strength. Also, modeling results show that average error of ANN has the lowest average error. Optimization has been done by genetic algorithm method and the results show that the optimum value of compression strength was 23.95 Mpa in 7 wt.% of HA and 0.289 wt.% of GO. The optimum value of energy has been reported 33.3 J in 0.239 wt.% GO and in absence of HA nanoparticles. Also, the optimum value of elongation at break is in 0.224 wt.% GO and absence of HA that is equal to 23.98 percent.</Abstract>
			<OtherAbstract Language="FA">In this article, an experimental and numerical study on compression strength, energy and elongation at break of epoxy based nanocomposites reinforced by graphene oxide and hydroxyapatite has been done. Graphene oxide and hydroxyapatite were used up to 0.5 &amp; 7 wt.%, respectively. Filler&#039;s weight fractions that used as design parameters have been achieved by design of experiment through central composite design method. Weight fractions of fillers have been considered as input parameters for modeling by RSM, ANN &amp; regression tree method. Experimental results show the addition of nanoparticles increase compression strength. Also, modeling results show that average error of ANN has the lowest average error. Optimization has been done by genetic algorithm method and the results show that the optimum value of compression strength was 23.95 Mpa in 7 wt.% of HA and 0.289 wt.% of GO. The optimum value of energy has been reported 33.3 J in 0.239 wt.% GO and in absence of HA nanoparticles. Also, the optimum value of elongation at break is in 0.224 wt.% GO and absence of HA that is equal to 23.98 percent.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Compression strength</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Artificial Neural Network</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Hydroxyapatite</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Graphene oxide</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Genetic Algorithm</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1196_c76b1ab5df275dc1d4b8ff2d7bd03c56.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Optimization of Radiation Shields Parameters in Multi-Layer Thermal Insulations</ArticleTitle>
<VernacularTitle>Optimization of Radiation Shields Parameters in Multi-Layer Thermal Insulations</VernacularTitle>
			<FirstPage>71</FirstPage>
			<LastPage>81</LastPage>
			<ELocationID EIdType="pii">1216</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.4076.2082</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Sedighi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>B.</FirstName>
					<LastName>Ghanbari Oranj</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>A. H.</FirstName>
					<LastName>Jabbari Mostahsan</LastName>
<Affiliation>Iran University of Science and Technology</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>01</Month>
					<Day>02</Day>
				</PubDate>
			</History>
		<Abstract>Multi-layer thermal insulations are fabricated by locating consequtive porous insulation and radition shields, which could be used at high temperature and cryogenic applications. In this type of insulations, different heat transfer methods such as conduction, convection and radiation would be occurred, although by using high density insulation (more than 20 kg/m^3 ), convection could be neglected. In this paper, radiation shiels parameters such as thickness, emissivity, distance and number of screens are studied and optimized. For investigating the effect of these parameters on effective thermal conductivity of multi-layer thermal insulation, a mathematical code has been improved in EES software. Then, the obtained results have been validated by another study. Moreover, Powell method has been applied in order to optimize the parameters. The results show that the amount of shield emssivity and shields arrangement have the most impact on the effective thermal conductivity of multi-layer thermal insulations. Also, the optimized distances between radiation shields indicate that this distance increased in the direction of heat transfer.</Abstract>
			<OtherAbstract Language="FA">Multi-layer thermal insulations are fabricated by locating consequtive porous insulation and radition shields, which could be used at high temperature and cryogenic applications. In this type of insulations, different heat transfer methods such as conduction, convection and radiation would be occurred, although by using high density insulation (more than 20 kg/m^3 ), convection could be neglected. In this paper, radiation shiels parameters such as thickness, emissivity, distance and number of screens are studied and optimized. For investigating the effect of these parameters on effective thermal conductivity of multi-layer thermal insulation, a mathematical code has been improved in EES software. Then, the obtained results have been validated by another study. Moreover, Powell method has been applied in order to optimize the parameters. The results show that the amount of shield emssivity and shields arrangement have the most impact on the effective thermal conductivity of multi-layer thermal insulations. Also, the optimized distances between radiation shields indicate that this distance increased in the direction of heat transfer.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Multi-Layer Thermal Insulation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Radiation Shield</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Porous Insulation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Optimization</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1216_744600627c3a52941dc39d4b5546e029.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Analysis Of Turbulent Combined Heat Transfer (Mixed Convection-Thermal Radiation) Heat Transfer in a Vertical Three Dimensional Duct With Variable Thermo-physical Properties</ArticleTitle>
<VernacularTitle>Analysis Of Turbulent Combined Heat Transfer (Mixed Convection-Thermal Radiation) Heat Transfer in a Vertical Three Dimensional Duct With Variable Thermo-physical Properties</VernacularTitle>
			<FirstPage>83</FirstPage>
			<LastPage>97</LastPage>
			<ELocationID EIdType="pii">1231</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.5939.2424</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>F.</FirstName>
					<LastName>Bazdidi-Tehrani</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>V.</FirstName>
					<LastName>Emdadi Hor</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>S.</FirstName>
					<LastName>Moghaddam</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>06</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>The aim of the present paper is to analyse the effect of thermal radiation on turbulent mixed convection in a vertical duct with variable thermos-physical properties. The Reynolds number based on duct width is 6200 and the Grashof number based on duct width and hot to cold wall temperature difference is 107. The right wall is the hot wall and buoyancy effect in its vicinity is aiding where the left wall is cold and buoyancy effect in its vicinity is opposing. Changes of dynamic viscosity and thermal conductivity of the medium follow the power law. Density is based on the perfect gas equation of state. Results show that with the presence of thermal radiation, due to the reduction in bouyancy effects, temperature profiles become more flattened. Also, radiation causes an increase in heat transfer on both the aiding and opposing sides whereby the velocity gradient reduces on the aiding side and increases on opposing side. Also, the assumption of variable properties results in a reduction of the velocity and temperature gradients on the aiding side and an augmentation on the opposing side.</Abstract>
			<OtherAbstract Language="FA">The aim of the present paper is to analyse the effect of thermal radiation on turbulent mixed convection in a vertical duct with variable thermos-physical properties. The Reynolds number based on duct width is 6200 and the Grashof number based on duct width and hot to cold wall temperature difference is 107. The right wall is the hot wall and buoyancy effect in its vicinity is aiding where the left wall is cold and buoyancy effect in its vicinity is opposing. Changes of dynamic viscosity and thermal conductivity of the medium follow the power law. Density is based on the perfect gas equation of state. Results show that with the presence of thermal radiation, due to the reduction in bouyancy effects, temperature profiles become more flattened. Also, radiation causes an increase in heat transfer on both the aiding and opposing sides whereby the velocity gradient reduces on the aiding side and increases on opposing side. Also, the assumption of variable properties results in a reduction of the velocity and temperature gradients on the aiding side and an augmentation on the opposing side.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Combined Heat Transfer</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Turbulent Flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Vertical Duct</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Variable Thermophysical properties</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Discrete Ordinates Method</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1231_3be4a46f477e8a47005d7fe78a150ec0.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Simulation of 3-D Pollution Propagated from a Gaseous Source Through ‎Indoor Space by Applying Pressure Zonal Model</ArticleTitle>
<VernacularTitle>Numerical Simulation of 3-D Pollution Propagated from a Gaseous Source Through ‎Indoor Space by Applying Pressure Zonal Model</VernacularTitle>
			<FirstPage>99</FirstPage>
			<LastPage>109</LastPage>
			<ELocationID EIdType="pii">1199</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2017.3590.1986</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>A.</FirstName>
					<LastName>Azimi</LastName>
<Affiliation>Scientific Member of Shahid Chamran University of Ahvaz</Affiliation>

</Author>
<Author>
					<FirstName>E.</FirstName>
					<LastName>Daneshgar</LastName>
<Affiliation>Shahid Chamran University</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2015</Year>
					<Month>11</Month>
					<Day>12</Day>
				</PubDate>
			</History>
		<Abstract>Simulating the distribution of emissions in indoor spaces is usually done using very time-consuming and costly ‎computational fluid dynamics methods. In this paper, in order to achieve a suitable accuracy and high-speed method for ‎simulating three-dimensional emission propagation in a room due to a gaseous pollution source, a pressure version of the ‎zonal method has been developed. To demonstrate the capabilities of this developing method, two problems of the air ‎emission within a room have been investigated. At the first problem, for validating the results of this research, the emission ‎simulation through contaminated air into a room with dimension of 3×4×2.5 m via an air-conditioning gate mounted on the ‎wall near the ceiling is done and the results have been compared with the experimental data and the results of the numerical ‎solution of Navier-Stocks Equations. According to this comparison, the percentage of average error between the present ‎results and the experimental data is 26.8 and also the percentage of average error between the present results and the results ‎of numerical solution is 10. After that, considering both constant and instantaneous gaseous pollution sources in a room with ‎dimensions of 3×4×3 m, pollution distributions in the room have been evaluated. According to the results of this research, ‎this zonal method can obtain acceptable results in far less time than those of the experimental and computational fluid ‎dynamics methods. Therefore, this method can be efficient for considering time-consuming environmental problems.‎</Abstract>
			<OtherAbstract Language="FA">Simulating the distribution of emissions in indoor spaces is usually done using very time-consuming and costly ‎computational fluid dynamics methods. In this paper, in order to achieve a suitable accuracy and high-speed method for ‎simulating three-dimensional emission propagation in a room due to a gaseous pollution source, a pressure version of the ‎zonal method has been developed. To demonstrate the capabilities of this developing method, two problems of the air ‎emission within a room have been investigated. At the first problem, for validating the results of this research, the emission ‎simulation through contaminated air into a room with dimension of 3×4×2.5 m via an air-conditioning gate mounted on the ‎wall near the ceiling is done and the results have been compared with the experimental data and the results of the numerical ‎solution of Navier-Stocks Equations. According to this comparison, the percentage of average error between the present ‎results and the experimental data is 26.8 and also the percentage of average error between the present results and the results ‎of numerical solution is 10. After that, considering both constant and instantaneous gaseous pollution sources in a room with ‎dimensions of 3×4×3 m, pollution distributions in the room have been evaluated. According to the results of this research, ‎this zonal method can obtain acceptable results in far less time than those of the experimental and computational fluid ‎dynamics methods. Therefore, this method can be efficient for considering time-consuming environmental problems.‎</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Air Zonal Method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Pressure Version</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Contaminant Distribution</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Gaseous Contaminant Source</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1199_a405e3060ae8b537f3e68bd9134802a1.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigation of Magnetic Field Effect on Nanofluid Mixed Convection inside Lid-Driven K-shaped Enclosure Using Lattice Boltzmann Method</ArticleTitle>
<VernacularTitle>Investigation of Magnetic Field Effect on Nanofluid Mixed Convection inside Lid-Driven K-shaped Enclosure Using Lattice Boltzmann Method</VernacularTitle>
			<FirstPage>111</FirstPage>
			<LastPage>126</LastPage>
			<ELocationID EIdType="pii">1229</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.6263.2494</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>A. R.</FirstName>
					<LastName>Rahmati</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Nemati</LastName>
<Affiliation>Department of Mec. Eng., Univ. of Kashan</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>10</Month>
					<Day>19</Day>
				</PubDate>
			</History>
		<Abstract>In the present work, for the first time, mixed convection heat transfer of nanofluid in a uniform magnetic field inside a lid-driven K-shaped cavity is simulated via lattice Boltzmann method. Both left and right walls are maintained at constant cold temperature. The bottom -horizontal wall is maintained at constant hot temperature. Temperature on the top-horizontal wall is varied linearly. The flow and temperature field is calculated by solving flow and temperature distribution functions. The effects of different parameters such as Reynolds number (50-200), Hartman number (0-60), aspect ratio of the K-shaped cavity (0.4-1), nanoparticle volume fraction (0-0.05) on mixed convective heat transfer are investigated. The obtained result show that for a fixed Hartman number, increase in aspect ratio and Reynolds number causes increase in heat transfer. Also in a fixed Reynolds number and aspect ratio, increasing of Hartman number decreases velocity of flow and heat transfer. In addition, changing solid volume fraction can affect heat transfer directly.</Abstract>
			<OtherAbstract Language="FA">In the present work, for the first time, mixed convection heat transfer of nanofluid in a uniform magnetic field inside a lid-driven K-shaped cavity is simulated via lattice Boltzmann method. Both left and right walls are maintained at constant cold temperature. The bottom -horizontal wall is maintained at constant hot temperature. Temperature on the top-horizontal wall is varied linearly. The flow and temperature field is calculated by solving flow and temperature distribution functions. The effects of different parameters such as Reynolds number (50-200), Hartman number (0-60), aspect ratio of the K-shaped cavity (0.4-1), nanoparticle volume fraction (0-0.05) on mixed convective heat transfer are investigated. The obtained result show that for a fixed Hartman number, increase in aspect ratio and Reynolds number causes increase in heat transfer. Also in a fixed Reynolds number and aspect ratio, increasing of Hartman number decreases velocity of flow and heat transfer. In addition, changing solid volume fraction can affect heat transfer directly.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Keywords: Lattice Boltzmann Method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Mixed Convection</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Nanofluid</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Magnetic Field</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">K-shaped Enclosure</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1229_b582383e2a1710862177ee545a454964.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Flow field modeling and performance improving of an axial turbine's using Adjoint method</ArticleTitle>
<VernacularTitle>Flow field modeling and performance improving of an axial turbine&#039;s using Adjoint method</VernacularTitle>
			<FirstPage>127</FirstPage>
			<LastPage>133</LastPage>
			<ELocationID EIdType="pii">1217</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2017.4712.2201</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>H.</FirstName>
					<LastName>Jafari</LastName>
<Affiliation>Aerodynamics &amp;amp; Propulsion, Aerospace Engineering, Malek Ashtar University O Tech., Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>H.</FirstName>
					<LastName>Parhizkar</LastName>
<Affiliation>Aerodynamics &amp;amp; Propulsion, Aerospace Engineering, Malek Ashtar University Of Tech. ,  Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>R.</FirstName>
					<LastName>Aghaei Tog</LastName>
<Affiliation>Mechanical &amp;amp; Aerospace Engineering, Engineering Faculty, ., Science &amp;amp; Research branch of Islamic Azad Univ., Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>R.</FirstName>
					<LastName>Mardani</LastName>
<Affiliation>Aerodynamics &amp;amp; propulsion, Aero. Eng., Sharif Univ. of Tech., Tehran, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2016</Year>
					<Month>08</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>In recent years, optimization of Turbomachinery performance parameters is one of the most important topics for researchers and industrial scholars. The aerodynamic optimization of blades has been done by variety of algorithms and methods until now; however new tools have better suggestions in this field.&lt;br /&gt; This paper reports a 3D numerical analysis and geometrical optimization of fully turbulent flow around a turbine&#039;s rotor blades. Numerical analysis is done using the AUSM+ scheme and SST k –ω turbulence model. An Ad-joint Algorithm gradient method is used in geometrical aerodynamic optimization of blades. This algorithm has been used previously for 2D models as build-in codes and for 3D models is done for the first time in this research.&lt;br /&gt; The total to total isentropic efficiency as objective function and other performance parameters have a good agreement with the experimental measurements in validation process. Through the optimization process, the objective function is improved by 0.18, which in comparison with others&#039; reported works is a good progress in performance improvement.</Abstract>
			<OtherAbstract Language="FA">In recent years, optimization of Turbomachinery performance parameters is one of the most important topics for researchers and industrial scholars. The aerodynamic optimization of blades has been done by variety of algorithms and methods until now; however new tools have better suggestions in this field.&lt;br /&gt; This paper reports a 3D numerical analysis and geometrical optimization of fully turbulent flow around a turbine&#039;s rotor blades. Numerical analysis is done using the AUSM+ scheme and SST k –ω turbulence model. An Ad-joint Algorithm gradient method is used in geometrical aerodynamic optimization of blades. This algorithm has been used previously for 2D models as build-in codes and for 3D models is done for the first time in this research.&lt;br /&gt; The total to total isentropic efficiency as objective function and other performance parameters have a good agreement with the experimental measurements in validation process. Through the optimization process, the objective function is improved by 0.18, which in comparison with others&#039; reported works is a good progress in performance improvement.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Turbine blade</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Adjoint optimization method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Isentropic efficiency</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1217_269ddad9727d02819f14490224606ea5.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Reducing the undesirable effects of thermal asymmetry for a bus passengers by using airflow asymmetry under summer conditions</ArticleTitle>
<VernacularTitle>Reducing the undesirable effects of thermal asymmetry for a bus passengers by using airflow asymmetry under summer conditions</VernacularTitle>
			<FirstPage>135</FirstPage>
			<LastPage>146</LastPage>
			<ELocationID EIdType="pii">1197</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.5277.2300</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>A.R.</FirstName>
					<LastName>Zolfaghari</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>H.</FirstName>
					<LastName>Hassanzadeh</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Raeesi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Taheri</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>01</Month>
					<Day>11</Day>
				</PubDate>
			</History>
		<Abstract>Improving thermal comfort in vehicles, especially in public transport due to design constraints in locating inlet diffusers, overpopulation and difference condition for passengers, is always faced with many challenges. In this paper, the effect of thermal asymmetry on the sensation of passenger inside a bus with overhead mixing ventilation system in three different air distribution patterns is studied by using the 65-nodes thermal comfort model. Moreover, the inlet air temperature has been set at the value which can maintain the passengers’ predicted mean votes within the allowable range. Also, the Airpak solver has been utilized for solving the flow and energy equations; and a numerical code has been developed for solving the local thermal comfort equations. The results show that under thermal asymmetry conditions, it is necessary to use an asymmetric air distribution in order to provide more uniform thermal sensation for the passengers. In this case, air temperature of the head segment is about 22℃ which is less about 2℃ in symmetric flow pattern. The results of 65-nodes model show that using an asymmetrical distribution pattern in the mixing ventilation system improving its performance and under the mentioned conditions, the skin temperature is closer to neutral skin temperature.</Abstract>
			<OtherAbstract Language="FA">Improving thermal comfort in vehicles, especially in public transport due to design constraints in locating inlet diffusers, overpopulation and difference condition for passengers, is always faced with many challenges. In this paper, the effect of thermal asymmetry on the sensation of passenger inside a bus with overhead mixing ventilation system in three different air distribution patterns is studied by using the 65-nodes thermal comfort model. Moreover, the inlet air temperature has been set at the value which can maintain the passengers’ predicted mean votes within the allowable range. Also, the Airpak solver has been utilized for solving the flow and energy equations; and a numerical code has been developed for solving the local thermal comfort equations. The results show that under thermal asymmetry conditions, it is necessary to use an asymmetric air distribution in order to provide more uniform thermal sensation for the passengers. In this case, air temperature of the head segment is about 22℃ which is less about 2℃ in symmetric flow pattern. The results of 65-nodes model show that using an asymmetrical distribution pattern in the mixing ventilation system improving its performance and under the mentioned conditions, the skin temperature is closer to neutral skin temperature.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Bus</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Thermal asymmetry</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Mixing ventilation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Local thermal comfort</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">65-nodes comfort model</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1197_ca3a46bbe46cb6959c208a092d24a70b.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigating the limit behavior of cavitation phenomana around circular cylinder with various diameters at high speed cavitation tunnel</ArticleTitle>
<VernacularTitle>Investigating the limit behavior of cavitation phenomana around circular cylinder with various diameters at high speed cavitation tunnel</VernacularTitle>
			<FirstPage>147</FirstPage>
			<LastPage>156</LastPage>
			<ELocationID EIdType="pii">1218</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2017.5645.2388</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Iraj</FirstName>
					<LastName>Jafari Gavzan</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>A. M.</FirstName>
					<LastName>Jadidi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>04</Month>
					<Day>30</Day>
				</PubDate>
			</History>
		<Abstract>To investigate the limit behaviors of cavitation flow around a circular cylinder at a high speed cavitation tunnel, stainless steel models with different diameters, including 10 mm, 15 mm and 20 mm were made and tested in a supercavitation tunnel.Two holes designed in a way that the radial hole is connected to the axial one to measure the back pressure at various cavitation numbers. Before appearing clear silver regime at the model back pressure fluctuating is violent and after becoming visible stable clear silver regime the fluctuating pressure will be reduced and the length of attached bubble will be increased strongly. In this case, the longitudinal oscillation occurs randomly. The minimum back pressure for all models is the same and is equal to 13500 Pa. When the cavitation length is small, shedding vortices occur regularly, based on von-karmen pattern. In supercavitation regime, the collapse noise of bubble for 20 mm model is very stronger than 10 mm model. The ultimate cavitation number (chocking regime), will be reduced by decreasing the model diameter. The minimum cavitation number for 10 and 20 mm models are 0.125 and 0.49 respectively. The results show that the difference in ultimate cavitation number between experimental and theory methods are approximately 14%.</Abstract>
			<OtherAbstract Language="FA">To investigate the limit behaviors of cavitation flow around a circular cylinder at a high speed cavitation tunnel, stainless steel models with different diameters, including 10 mm, 15 mm and 20 mm were made and tested in a supercavitation tunnel.Two holes designed in a way that the radial hole is connected to the axial one to measure the back pressure at various cavitation numbers. Before appearing clear silver regime at the model back pressure fluctuating is violent and after becoming visible stable clear silver regime the fluctuating pressure will be reduced and the length of attached bubble will be increased strongly. In this case, the longitudinal oscillation occurs randomly. The minimum back pressure for all models is the same and is equal to 13500 Pa. When the cavitation length is small, shedding vortices occur regularly, based on von-karmen pattern. In supercavitation regime, the collapse noise of bubble for 20 mm model is very stronger than 10 mm model. The ultimate cavitation number (chocking regime), will be reduced by decreasing the model diameter. The minimum cavitation number for 10 and 20 mm models are 0.125 and 0.49 respectively. The results show that the difference in ultimate cavitation number between experimental and theory methods are approximately 14%.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">high speed cavitation tunnel</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">cloud cavitation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Cylinder</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">limit behavior</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">experimental measurement</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1218_893ffa6056fbfdf36a2924da2e3e4712.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Stability Analysis of Natural Convection with Variable Physical Coefficients Using Linear Stability Theory</ArticleTitle>
<VernacularTitle>Stability Analysis of Natural Convection with Variable Physical Coefficients Using Linear Stability Theory</VernacularTitle>
			<FirstPage>157</FirstPage>
			<LastPage>169</LastPage>
			<ELocationID EIdType="pii">1230</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.6153.2462</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Varmazyar</LastName>
<Affiliation>Shahid Rajaee Teacher Training University</Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Miralam</LastName>
<Affiliation>Shahid Rajaee Teacher Training University</Affiliation>

</Author>
<Author>
					<FirstName>M.R.</FirstName>
					<LastName>Habibi</LastName>
<Affiliation>Research Institute of Petroleum Industry</Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Dehghani Mobarake</LastName>
<Affiliation>Research Inst. of Petroleum Industry</Affiliation>

</Author>
<Author>
					<FirstName>A.</FirstName>
					<LastName>Mohammadi</LastName>
<Affiliation>Shaihd Rajaee Teacher Training Uni</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>08</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>In this research, the effects of variation of physical transport coefficient of fluid, such as kinematic viscosity and thermal diffusivity coefficient, on the primary instability of natural convection has been investigated. Accordingly, the governing equations are calculated for the onset of free convective flow by using the perturbation theory on the variation of temperature and velocity. Using the theory of linear stability and the wave function, it can be defined the minimum Rayleigh number as critical Rayleigh number in assumed eigenvalue problem. It is assumed that the flow variables, such as the thermal diffusivity coefficient and kinematic viscosity, change exponentially relative to the location. The simulation results show that the critical-wave number function is a even function. Also, the dependence of the amplitude and frequency of oscillation of temperature and velocity disturbances on effective parameters on properties changes was evaluated and the results were analyzed. It can be said that critical Rayleigh number behavior is completely inverse in relation to the thermal emission and kinematic viscosity coefficients, and therefore their simultaneous effect in solving the equations will lead to a decrease in the critical interval of the oscillation.</Abstract>
			<OtherAbstract Language="FA">In this research, the effects of variation of physical transport coefficient of fluid, such as kinematic viscosity and thermal diffusivity coefficient, on the primary instability of natural convection has been investigated. Accordingly, the governing equations are calculated for the onset of free convective flow by using the perturbation theory on the variation of temperature and velocity. Using the theory of linear stability and the wave function, it can be defined the minimum Rayleigh number as critical Rayleigh number in assumed eigenvalue problem. It is assumed that the flow variables, such as the thermal diffusivity coefficient and kinematic viscosity, change exponentially relative to the location. The simulation results show that the critical-wave number function is a even function. Also, the dependence of the amplitude and frequency of oscillation of temperature and velocity disturbances on effective parameters on properties changes was evaluated and the results were analyzed. It can be said that critical Rayleigh number behavior is completely inverse in relation to the thermal emission and kinematic viscosity coefficients, and therefore their simultaneous effect in solving the equations will lead to a decrease in the critical interval of the oscillation.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Linear Stability Theory</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Variation of Physical Coefficient</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Free Convection</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Critical Rayleigh Number</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1230_f74b4985bcb52c54053f6353ba4b6283.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>A new model for two-phase flow in a solar still improved by a porous layer</ArticleTitle>
<VernacularTitle>A new model for two-phase flow in a solar still improved by a porous layer</VernacularTitle>
			<FirstPage>171</FirstPage>
			<LastPage>182</LastPage>
			<ELocationID EIdType="pii">1227</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.6463.2516</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>A.R.</FirstName>
					<LastName>Pourmoayed</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>R.</FirstName>
					<LastName>Rahmati</LastName>
<Affiliation>Department of Mechanical Engineering, Khatmol Anbia Air Defense, Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Golami</LastName>
<Affiliation>Department of Mechanical Engineering, K. N. Tossi University of Technology, Tehran, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>11</Month>
					<Day>24</Day>
				</PubDate>
			</History>
		<Abstract>In this research, the volume of fluid (VOF) model is used to simulate the vapor-liquid two-phase flow in a single slope solar still. This model has an ability to track the interface between liquid and vapor phases during the phase change. To benchmark the accuracy of VOF model, the numerical results are compared with the experimental data and the results of previous model for simulating solar still (moist air model). It was found that the volume of ﬂuid model predicts the experimental data with more accuracy in comparison with the moist air model. After simulation, the effect of using a sponge layer as the cheap porous material on productivity of the solar still is investigated. Sponge layer provides more effective area for evaporation and solar radiation absorption inside the solar still. Moreover, this material has wick property and transfers the water to evaporation surface. The results showed that the productivity of the solar still enhances about 10% by using a sponge layer with porosity of 0.6. Moreover, it is observed that the productivity increases with decreasing the porosity of sponge layer for porosities higher than 0.6, while the productivity decreases with decreasing the porosity of sponge layer for porosities less than 0.6.</Abstract>
			<OtherAbstract Language="FA">In this research, the volume of fluid (VOF) model is used to simulate the vapor-liquid two-phase flow in a single slope solar still. This model has an ability to track the interface between liquid and vapor phases during the phase change. To benchmark the accuracy of VOF model, the numerical results are compared with the experimental data and the results of previous model for simulating solar still (moist air model). It was found that the volume of ﬂuid model predicts the experimental data with more accuracy in comparison with the moist air model. After simulation, the effect of using a sponge layer as the cheap porous material on productivity of the solar still is investigated. Sponge layer provides more effective area for evaporation and solar radiation absorption inside the solar still. Moreover, this material has wick property and transfers the water to evaporation surface. The results showed that the productivity of the solar still enhances about 10% by using a sponge layer with porosity of 0.6. Moreover, it is observed that the productivity increases with decreasing the porosity of sponge layer for porosities higher than 0.6, while the productivity decreases with decreasing the porosity of sponge layer for porosities less than 0.6.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Single slope solar still</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Volume of fluid model</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Sponge</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Productivity</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1227_271517b3929138153e6b3e7495a72c72.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigation on the tank vehicle dynamic performance influenced by fluid sloshing using multidisciplinary simulation technique</ArticleTitle>
<VernacularTitle>Investigation on the tank vehicle dynamic performance influenced by fluid sloshing using multidisciplinary simulation technique</VernacularTitle>
			<FirstPage>183</FirstPage>
			<LastPage>202</LastPage>
			<ELocationID EIdType="pii">1236</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.3687.2004</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>B.</FirstName>
					<LastName>Ghasemi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M. H.</FirstName>
					<LastName>Marashi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Abdol M.</FirstName>
					<LastName>Khoshnood</LastName>
<Affiliation>K.N. Toosi university of technology</Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Fathali</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2015</Year>
					<Month>12</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>In the current study impacts of fluid sloshing on the dynamic performance of a partially filled tank vehicle have been investigated. A nonlinear and three-dimensional solver of fluid flow equations were coupled with dynamic equations of a three degrees of freedom moving tank vehicle through an intermediate software to simulate the fluid sloshing behavior inside the tank and the vehicle dynamic performance influenced by liquid sloshing. The fluid sloshing solver is based on corrected Navier-Stokes equations which are included some additional terms owed to taking tank vehicles motions into account. In the present work we used “body weighted method” to consider the effects of accelerating motions of the tank on fluid’s elements. The mentioned method was used to simulate the partially filled container during accelerating horizontal motion which crashed an obstacle after a while from the start point. Computed results were compared to experimental results from literatures to valid the proposed method. The water level evolution on the left wall of the container compared to the experimental one showed a good agreement. Moreover, the two-dimensional rectangular container subjected to periodic external excitation was considered. The pressure history on the tank wall was compared to the measured impact pressure to figure out the ability of the scheme to capture the flow properties to anticipate the exerted forces on the walls. One is observed that there is a good agreement between the computed and measured results. Furthermore, the coupled tank vehicle-fluid simulation has been done during vertical excitations through passing symmetric bumps.</Abstract>
			<OtherAbstract Language="FA">In the current study impacts of fluid sloshing on the dynamic performance of a partially filled tank vehicle have been investigated. A nonlinear and three-dimensional solver of fluid flow equations were coupled with dynamic equations of a three degrees of freedom moving tank vehicle through an intermediate software to simulate the fluid sloshing behavior inside the tank and the vehicle dynamic performance influenced by liquid sloshing. The fluid sloshing solver is based on corrected Navier-Stokes equations which are included some additional terms owed to taking tank vehicles motions into account. In the present work we used “body weighted method” to consider the effects of accelerating motions of the tank on fluid’s elements. The mentioned method was used to simulate the partially filled container during accelerating horizontal motion which crashed an obstacle after a while from the start point. Computed results were compared to experimental results from literatures to valid the proposed method. The water level evolution on the left wall of the container compared to the experimental one showed a good agreement. Moreover, the two-dimensional rectangular container subjected to periodic external excitation was considered. The pressure history on the tank wall was compared to the measured impact pressure to figure out the ability of the scheme to capture the flow properties to anticipate the exerted forces on the walls. One is observed that there is a good agreement between the computed and measured results. Furthermore, the coupled tank vehicle-fluid simulation has been done during vertical excitations through passing symmetric bumps.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Multidisciplinary simulation (MDS)</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Coupled simulation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Fluid sloshing</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Volume of fluid method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Multi-body dynamics</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1236_05b2cc696e2eb87d6a19ae62992fac58.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>The Effect of the Kind of Attachment of Primary Cilium to Cell in Its Response to the Fluid Flow: A 3D Computational Simulation</ArticleTitle>
<VernacularTitle>The Effect of the Kind of Attachment of Primary Cilium to Cell in Its Response to the Fluid Flow: A 3D Computational Simulation</VernacularTitle>
			<FirstPage>203</FirstPage>
			<LastPage>213</LastPage>
			<ELocationID EIdType="pii">1232</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.5839.2410</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>A.H.</FirstName>
					<LastName>Abbasszadeh Rad</LastName>
<Affiliation>MSc/University of Tehran</Affiliation>

</Author>
<Author>
					<FirstName>B.</FirstName>
					<LastName>Vahidi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>06</Month>
					<Day>05</Day>
				</PubDate>
			</History>
		<Abstract>The primary cilium is an organelle which occurs singly on nearly every cell in the vertebrate body. This organelle which extends out of the cell surface like an antenna is known as cell sensor which is able to sense mechanical and chemical stimuli applied to the cell. Upon flow of fluid over the cell surface, primary cilium bends and the surrounding membrane experiences strain resulting in activation of ion channels and transfer of calcium ions. Thus, primary cilium is able to transduce mechanical stimuli to ion signals and to make the cell somehow sense the surrounding fluid flow. In this study a novel model which accommodates for both pivoting and bending of cilium in response to the fluid flow was presented. In this 3D model primary cilium is attached to the cell using a thin elastic layer which is a kind of boundary condition. The domain of the cilium is modeled with linear elastic material and finite element method was used along with fluid-structure interaction teqniques to solve the fully coupled governing equations. The maximum stress obtained at the base of the cilium is between 10 to 50 kPa depending on the stiffness of the elastic layer. Results show that application of this boundary condition causes the maximum stress and strain to move from the inner parts of the ciliary base to the lateral parts of it. That is why this model is able to better explain the sensitivity of response of the primary cilium to mechanical stimuli.</Abstract>
			<OtherAbstract Language="FA">The primary cilium is an organelle which occurs singly on nearly every cell in the vertebrate body. This organelle which extends out of the cell surface like an antenna is known as cell sensor which is able to sense mechanical and chemical stimuli applied to the cell. Upon flow of fluid over the cell surface, primary cilium bends and the surrounding membrane experiences strain resulting in activation of ion channels and transfer of calcium ions. Thus, primary cilium is able to transduce mechanical stimuli to ion signals and to make the cell somehow sense the surrounding fluid flow. In this study a novel model which accommodates for both pivoting and bending of cilium in response to the fluid flow was presented. In this 3D model primary cilium is attached to the cell using a thin elastic layer which is a kind of boundary condition. The domain of the cilium is modeled with linear elastic material and finite element method was used along with fluid-structure interaction teqniques to solve the fully coupled governing equations. The maximum stress obtained at the base of the cilium is between 10 to 50 kPa depending on the stiffness of the elastic layer. Results show that application of this boundary condition causes the maximum stress and strain to move from the inner parts of the ciliary base to the lateral parts of it. That is why this model is able to better explain the sensitivity of response of the primary cilium to mechanical stimuli.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Primary Cilium</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Thin Elastic Layer</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Mechanosensation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Fluid-Structure Interaction</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1232_ac6c5b437a66a2643b3cfdd4af048c2b.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Extraction of hydrodynamic coefficients applying planning mechanism motion maneuver using computational fluid dynamics</ArticleTitle>
<VernacularTitle>Extraction of hydrodynamic coefficients applying planning mechanism motion maneuver using computational fluid dynamics</VernacularTitle>
			<FirstPage>215</FirstPage>
			<LastPage>228</LastPage>
			<ELocationID EIdType="pii">1198</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.4527.2168</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>J.</FirstName>
					<LastName>Amini Foroushani</LastName>
<Affiliation>Researcher, Dept. Marine Sci. and Eng., Malek-e AshtarUnivercity of Technology., Isfahan, Iran</Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Gandomkar</LastName>
<Affiliation>faculty of Dept. Marine Sci. and Eng., Malek-e Ashtar Uni. Tech., Isfahan, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2016</Year>
					<Month>07</Month>
					<Day>02</Day>
				</PubDate>
			</History>
		<Abstract>This article describes how to extract some hydrodynamic coefficients of an underwater vehicle using computational fluid dynamics, and has been implemented on DARPA Suboff geometric model. In this article, a procedure has been provided to efficiently extract hydrodynamic coefficients, without using mesh regeneration for each maneuver. In this method by using simulation of some standard dynamic maneuvers, such as pure yaw and pure sway, a number of hydrodynamic coefficients have been obtained such as Y_v , Y_v ̇ , N_v , N_v ̇ and Y_r , Y_r ̇ , N_r, N_r ̇ . The parameters, required for numerical analysis, are geometry, center of mass and velocity of underwater vehicle. Using numerical analysis, hydrodynamic forces and moments have been ploted as functions of time. Hydrodynamic coefficients in relevant to the desired geometry is derived by investigation on the equations of motion in sinusoidal maneuver at specific points such as zero lateral velocity or zero acceleration points. The results of the present procedure have been compared with the experimental results that reported in the literature and a good agreement between analytical and experimental results has been observed.</Abstract>
			<OtherAbstract Language="FA">This article describes how to extract some hydrodynamic coefficients of an underwater vehicle using computational fluid dynamics, and has been implemented on DARPA Suboff geometric model. In this article, a procedure has been provided to efficiently extract hydrodynamic coefficients, without using mesh regeneration for each maneuver. In this method by using simulation of some standard dynamic maneuvers, such as pure yaw and pure sway, a number of hydrodynamic coefficients have been obtained such as Y_v , Y_v ̇ , N_v , N_v ̇ and Y_r , Y_r ̇ , N_r, N_r ̇ . The parameters, required for numerical analysis, are geometry, center of mass and velocity of underwater vehicle. Using numerical analysis, hydrodynamic forces and moments have been ploted as functions of time. Hydrodynamic coefficients in relevant to the desired geometry is derived by investigation on the equations of motion in sinusoidal maneuver at specific points such as zero lateral velocity or zero acceleration points. The results of the present procedure have been compared with the experimental results that reported in the literature and a good agreement between analytical and experimental results has been observed.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Underwater Vehicle</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Hydrodynamic Coefficients</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Dynamic Maneuvers</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Computational Fluid dynamics</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1198_9e05887900345416e0ad40ae1d874436.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>2D and 3D Numerical Investigation of the Super Cavitation Phenomena in the case of Injection and No Injection of the Air and Water vapour on the Under Water Vehicle</ArticleTitle>
<VernacularTitle>2D and 3D Numerical Investigation of the Super Cavitation Phenomena in the case of Injection and No Injection of the Air and Water vapour on the Under Water Vehicle</VernacularTitle>
			<FirstPage>229</FirstPage>
			<LastPage>240</LastPage>
			<ELocationID EIdType="pii">1237</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.5280.2301</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>R.</FirstName>
					<LastName>Shamsoddini</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>S.R.</FirstName>
					<LastName>Ghodsi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>01</Month>
					<Day>11</Day>
				</PubDate>
			</History>
		<Abstract>In the present study, the super cavitation phenomenon with gas injection is investigated. The cavitation phenomena is one of the most complex problems of fluid dynamic. Cavitation usually creates problems in the some application and should be prevented. However, it is useful for some application. One of the advantages of the cavitation is drag reduction on the surface of underwater vehicles. However, it should be controlled. In the present study, the super cavitation phenomena is modeled and investigated using the RSM turbulence method. The main aim of the present study is to investigate the gas injection for stabilization this phenomena for drag reduction. Whereas the investigation on the exact dimension is a time consuming process, a scaled model was used for numerical modeling. The results shows that vapor injection don’t reduce the drag forces. However, the air injection by creation a thin layer of flow around the under vehicle reduces considerably the drag force.</Abstract>
			<OtherAbstract Language="FA">In the present study, the super cavitation phenomenon with gas injection is investigated. The cavitation phenomena is one of the most complex problems of fluid dynamic. Cavitation usually creates problems in the some application and should be prevented. However, it is useful for some application. One of the advantages of the cavitation is drag reduction on the surface of underwater vehicles. However, it should be controlled. In the present study, the super cavitation phenomena is modeled and investigated using the RSM turbulence method. The main aim of the present study is to investigate the gas injection for stabilization this phenomena for drag reduction. Whereas the investigation on the exact dimension is a time consuming process, a scaled model was used for numerical modeling. The results shows that vapor injection don’t reduce the drag forces. However, the air injection by creation a thin layer of flow around the under vehicle reduces considerably the drag force.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Super cavitation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">RSM model</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Gas injection</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Under water vehicle</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1237_7b87aea19b20a28403fbaf6aaf684939.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahrood University of Technology</PublisherName>
				<JournalTitle>Journal of Solid and Fluid Mechanics</JournalTitle>
				<Issn>2251-9475</Issn>
				<Volume>8</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2018</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical simulation of wave-floating bodies interaction using a truly incompressible SPH method with artificial compressibility approach</ArticleTitle>
<VernacularTitle>Numerical simulation of wave-floating bodies interaction using a truly incompressible SPH method with artificial compressibility approach</VernacularTitle>
			<FirstPage>241</FirstPage>
			<LastPage>252</LastPage>
			<ELocationID EIdType="pii">1238</ELocationID>
			
<ELocationID EIdType="doi">10.22044/jsfm.2018.6346.2498</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>F.</FirstName>
					<LastName>Rouzbahani</LastName>
<Affiliation>Department of mechanical engineering, Engineering Faculty, Isalamic Azad University, Hamedan, Iran</Affiliation>

</Author>
<Author>
					<FirstName>K.</FirstName>
					<LastName>Hejranfar</LastName>
<Affiliation>Department of Aerospace Engineering, Sharif University of Technology, Tehran, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2017</Year>
					<Month>10</Month>
					<Day>24</Day>
				</PubDate>
			</History>
		<Abstract>In the present study, the numerical simulation of free-surface flow and wave-floating bodies interaction is performed by a truly incompressible smoothed particle hydrodynamics based on the artificial compressibility method (ACISPH). The two-dimensional governing equations in the primitive variables formulation using Chorin&#039;s artificial compressibility method are written in the Lagrangian reference frame to provide an appropriate incompressible SPH algorithm for computing the incompressible flows. An implicit dual-time stepping scheme is used for the time integration to be capable of time accurate analysis of unsteady flows. Unlike the weakly compressible SPH (WCSPH) method, the ACISPH method does not involve any approximate enforcement of the incompressibility condition that usually implies time step restrictions and spurious oscillations in the flow field. Unlike the projection SPH algorithm, the ACISPH method does not involve an iterative solution of the pressure Poisson equation and the pressure field is efficiently computed locally through the solution of the governing equations. The accuracy of the ACISPH method is demonstrated by solving the incompressible flow in a 2-D Hydrostatics tank. Then, the wave-floating bodies interaction is simulated and the results obtained are compared with the available experimental and numerical results. The study shows that the artificial compressibility-based ISPH (ACISPH) method applied is accurate and robust for simulating the wave-floating bodies’ interaction.</Abstract>
			<OtherAbstract Language="FA">In the present study, the numerical simulation of free-surface flow and wave-floating bodies interaction is performed by a truly incompressible smoothed particle hydrodynamics based on the artificial compressibility method (ACISPH). The two-dimensional governing equations in the primitive variables formulation using Chorin&#039;s artificial compressibility method are written in the Lagrangian reference frame to provide an appropriate incompressible SPH algorithm for computing the incompressible flows. An implicit dual-time stepping scheme is used for the time integration to be capable of time accurate analysis of unsteady flows. Unlike the weakly compressible SPH (WCSPH) method, the ACISPH method does not involve any approximate enforcement of the incompressibility condition that usually implies time step restrictions and spurious oscillations in the flow field. Unlike the projection SPH algorithm, the ACISPH method does not involve an iterative solution of the pressure Poisson equation and the pressure field is efficiently computed locally through the solution of the governing equations. The accuracy of the ACISPH method is demonstrated by solving the incompressible flow in a 2-D Hydrostatics tank. Then, the wave-floating bodies interaction is simulated and the results obtained are compared with the available experimental and numerical results. The study shows that the artificial compressibility-based ISPH (ACISPH) method applied is accurate and robust for simulating the wave-floating bodies’ interaction.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Smoothed particle hydrodynamics (SPH)</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Incompressible Flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Artificial compressibility approach</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Dual-time stepping scheme</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">wave-floating bodies interaction</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jsfm.shahroodut.ac.ir/article_1238_755ba4e321bfb017110d11be98c4c0e4.pdf</ArchiveCopySource>
</Article>
</ArticleSet>
