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<ArticleSet>
<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Analysis of Non-Darcy Flow in Rock Fill Materials Using Gradually Varied Flow Method</ArticleTitle>
<VernacularTitle>Analysis of Non-Darcy Flow in Rock Fill Materials Using Gradually Varied Flow Method</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20773</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Jalal</FirstName>
					<LastName>Bazargan</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>S. Mohammad</FirstName>
					<LastName>Shoaei</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>Analysis of flow through rockfill materials is usually carried out by solving the differential equation which is a combination of nonlinear [i=mvn] and continuity equations. However, solving this differential equation either by means of finite difference method or similar procedures is relatively time consuming, and with uncertainty involved in water surface profile this becomes even more difficult. To analyze flow through rockfill materials an alternative method which is based on gradually varied flow theory may be applied that is comparatively simpler and less time consuming. To apply this alternative method it is necessary to examine the validity of assumptions on which gradually varied flow method are based. Moreover, the involved parameters in gradually varied flow equation should be reverted to porous media condition. In this research by conducting a vast number of experiments on various types of materials the acceptability of assumptions of gradually varied flow method for analysis of flow through coarse porous media is investigated and the effect of physical characters of porous medium such as void ratio, uniformity coefficient Cu, gradation coefficient Cc and viscosity of fluid as well as certain features of flow such as velocity and hydraulic gradient are also examined. Findings indicate that: 1). by accepting some degrees of discrepancies, one may use the gradually varied flow method for analysis of flow through coarse porous media. 2). the permeability parameters of coarse porous media may be successfully related to the physical characters of granular materials. 3). A Comparison between observed and computed flow profiles through media indicates accuracy and applicability of equations that are derived by authors of this paper.</Abstract>
			<OtherAbstract Language="FA">Analysis of flow through rockfill materials is usually carried out by solving the differential equation which is a combination of nonlinear [i=mvn] and continuity equations. However, solving this differential equation either by means of finite difference method or similar procedures is relatively time consuming, and with uncertainty involved in water surface profile this becomes even more difficult. To analyze flow through rockfill materials an alternative method which is based on gradually varied flow theory may be applied that is comparatively simpler and less time consuming. To apply this alternative method it is necessary to examine the validity of assumptions on which gradually varied flow method are based. Moreover, the involved parameters in gradually varied flow equation should be reverted to porous media condition. In this research by conducting a vast number of experiments on various types of materials the acceptability of assumptions of gradually varied flow method for analysis of flow through coarse porous media is investigated and the effect of physical characters of porous medium such as void ratio, uniformity coefficient Cu, gradation coefficient Cc and viscosity of fluid as well as certain features of flow such as velocity and hydraulic gradient are also examined. Findings indicate that: 1). by accepting some degrees of discrepancies, one may use the gradually varied flow method for analysis of flow through coarse porous media. 2). the permeability parameters of coarse porous media may be successfully related to the physical characters of granular materials. 3). A Comparison between observed and computed flow profiles through media indicates accuracy and applicability of equations that are derived by authors of this paper.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Course Porous Media</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Gradually Varied Flow Method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Nondarcy Flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Physical Characters of Materials</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Rock Fill Materials</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20773_a37ee573dc5f403e1d1d1da6eee65aa3.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Dynamic Analysis of High-Speed Railway Bridges with Application to Vehicle-Bridges Interaction</ArticleTitle>
<VernacularTitle>Dynamic Analysis of High-Speed Railway Bridges with Application to Vehicle-Bridges Interaction</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20774</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Khosro</FirstName>
					<LastName>Bargi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Alireza</FirstName>
					<LastName>Aghabozorgi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>Dynamic effects of high speed trains on railway bridges have been analyzed in many research works. Two major approaches have been used widely: in the first approach represented by a constant load that crosses the bridges and thus dynamic properties of the vehicle itself are ignored. There are also more complex methods that incorporate dynamic properties of both the structure and the vehicle. In these models primary and secondary suspension systems the bogie and the wheels are incorporated into the model by their individual &amp; commercial ad mechanical properties. In this paper, two and three dimensional finite element models of a high speed trains crossing bridges susceptible to resonance effects are developed. In order to model dynamic interaction of the vehicle and the bridge, differential equation of second order is solved for both the vehicle and the bridge. The equating differential equations of the 2 systems are coupled by forces exerted on the vehicle and on the structure in rail wheel contacts. An explicit time advancement scheme is used to drive the model in time. It was necessary to regenerate reprehensive matrixes of the system in each time step, resulting it considerable computational cost.
Using the developed numerical model, a parametric study is done, revealing importance of damping and stiffness of primary suspension system, damping and stiffness of secondary suspension systems, damping and stiffness of ballast, interaction effects of vehicle and bridge simultaneously on dynamic behavior of bridge-vehicle system for high speed trains. The range of parameters for which a full dynamic model of the vehicle would be necessary is derived on the parametric study.</Abstract>
			<OtherAbstract Language="FA">Dynamic effects of high speed trains on railway bridges have been analyzed in many research works. Two major approaches have been used widely: in the first approach represented by a constant load that crosses the bridges and thus dynamic properties of the vehicle itself are ignored. There are also more complex methods that incorporate dynamic properties of both the structure and the vehicle. In these models primary and secondary suspension systems the bogie and the wheels are incorporated into the model by their individual &amp; commercial ad mechanical properties. In this paper, two and three dimensional finite element models of a high speed trains crossing bridges susceptible to resonance effects are developed. In order to model dynamic interaction of the vehicle and the bridge, differential equation of second order is solved for both the vehicle and the bridge. The equating differential equations of the 2 systems are coupled by forces exerted on the vehicle and on the structure in rail wheel contacts. An explicit time advancement scheme is used to drive the model in time. It was necessary to regenerate reprehensive matrixes of the system in each time step, resulting it considerable computational cost.
Using the developed numerical model, a parametric study is done, revealing importance of damping and stiffness of primary suspension system, damping and stiffness of secondary suspension systems, damping and stiffness of ballast, interaction effects of vehicle and bridge simultaneously on dynamic behavior of bridge-vehicle system for high speed trains. The range of parameters for which a full dynamic model of the vehicle would be necessary is derived on the parametric study.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Bridge</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">dynamic analysis</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">High-Speed Railways</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Vehicle-Bridge Interaction</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20774_30044db06dbe640aafcffa8b3be983d4.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Study of the Cyclic Behavior of Saturated Sand Considering the Effect of Induced Anisotropy</ArticleTitle>
<VernacularTitle>Study of the Cyclic Behavior of Saturated Sand Considering the Effect of Induced Anisotropy</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20775</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Hadi</FirstName>
					<LastName>Bahadori</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Abbas</FirstName>
					<LastName>Ghalandarzadeh</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>The cyclic behavior of saturated sand is studied in this paper using Firouzkooh sand. In order to evaluate the effect of induced anisotropy total number of 30 cyclic triaxial tests were programmed such that in addition to the occurrence of different types of liquefaction, investigation of the anisotropy effect after consolidation and stress reversal could be studied. Induced anisotropy extent is analysed by its effect on the liquefaction potential using Cyclic Stress method. The results show that the sand exhibits much more softening behavior in extensional mode which shows the importance of this phenomenon in the liquefaction susceptibility assessment of saturated sands. Finally, the reversal coeffitient index (rc) is introduced in this paper which indicates that in addition to anisotropy, the deviator stress reversal affects the soil behavior.</Abstract>
			<OtherAbstract Language="FA">The cyclic behavior of saturated sand is studied in this paper using Firouzkooh sand. In order to evaluate the effect of induced anisotropy total number of 30 cyclic triaxial tests were programmed such that in addition to the occurrence of different types of liquefaction, investigation of the anisotropy effect after consolidation and stress reversal could be studied. Induced anisotropy extent is analysed by its effect on the liquefaction potential using Cyclic Stress method. The results show that the sand exhibits much more softening behavior in extensional mode which shows the importance of this phenomenon in the liquefaction susceptibility assessment of saturated sands. Finally, the reversal coeffitient index (rc) is introduced in this paper which indicates that in addition to anisotropy, the deviator stress reversal affects the soil behavior.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Cyclic Behavior</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Extensional Mode</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Firouzkooh Sand</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Induced Anisotropy</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20775_52419be694c985bf235d328209e1b69d.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Modeling of Generation and Propagation of Tsunami Waves along the Southern Coast of Iran</ArticleTitle>
<VernacularTitle>Numerical Modeling of Generation and Propagation of Tsunami Waves along the Southern Coast of Iran</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20776</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mohammad</FirstName>
					<LastName>Heydarzadeh</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Moharram</FirstName>
					<LastName>Pirooz</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Naser</FirstName>
					<LastName>Hajizadeh</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract></Abstract>
			<OtherAbstract Language="FA"></OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Makran Subduction Zone</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Numerical Modeling</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Tsunami</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">tsunami generation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Tsunami Propagation</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20776_edb65f6808cc2364f908a0a6bb37f1d7.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigation on Hydraulic Fracturing in Embankment Dams</ArticleTitle>
<VernacularTitle>Investigation on Hydraulic Fracturing in Embankment Dams</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20777</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>S. Omid</FirstName>
					<LastName>Khamesi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Ali Asghar</FirstName>
					<LastName>Mirghasemi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>One of the most dangerous threats which embankment dams face with is hydraulic fracture. This phenomenon usually happens during first water impounding when the water pressure increases instantly in dam’s core. There are different methods to study hydraulic fracturing in embankment dams. In this paper Hyttejuvet Dam, a rock fill dam in Norway, which has been damaged by hydraulic fracture, is selected to evaluate the efficiency of these methods. Behavior of the dam during construction and first water impounding is modeled using finite element method. Afterwards using different methods, hydraulic fracturing is investigated for the Hyttejuvet Dam. In the next step using relations which correctly predicted fracturing in Hyttejuvet dam, the risk of this phenomenon is studied for Galabar Dam in Zanjan Province, Iran. Therefore coupled pore fluid-displacement analysis has been conducted for the dam during construction and first water impounding stage. These investigations showed that hydraulic fracture in the Hyttejuvet dam is correctly predicted by Komakpanah and Ghambari relations.  Also hydraulic fracturing of Glabar Dam is judged unlikely.</Abstract>
			<OtherAbstract Language="FA">One of the most dangerous threats which embankment dams face with is hydraulic fracture. This phenomenon usually happens during first water impounding when the water pressure increases instantly in dam’s core. There are different methods to study hydraulic fracturing in embankment dams. In this paper Hyttejuvet Dam, a rock fill dam in Norway, which has been damaged by hydraulic fracture, is selected to evaluate the efficiency of these methods. Behavior of the dam during construction and first water impounding is modeled using finite element method. Afterwards using different methods, hydraulic fracturing is investigated for the Hyttejuvet Dam. In the next step using relations which correctly predicted fracturing in Hyttejuvet dam, the risk of this phenomenon is studied for Galabar Dam in Zanjan Province, Iran. Therefore coupled pore fluid-displacement analysis has been conducted for the dam during construction and first water impounding stage. These investigations showed that hydraulic fracture in the Hyttejuvet dam is correctly predicted by Komakpanah and Ghambari relations.  Also hydraulic fracturing of Glabar Dam is judged unlikely.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">ABAQUS</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Embankment Dam</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">FEM</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Galabar Dam</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Hydraulic fracturing</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Hyttejuvet Dam</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Stress Arching</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20777_85c24da710157de708c65b00d8f2575f.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Comparing X-Braces Acceptance Criteria of Steel Building code, Quick and Comprehensive Seismic Evaluation Procedures</ArticleTitle>
<VernacularTitle>Comparing X-Braces Acceptance Criteria of Steel Building code, Quick and Comprehensive Seismic Evaluation Procedures</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20778</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Habib</FirstName>
					<LastName>Sami</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>S Mehdi</FirstName>
					<LastName>Zahraei</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, acceptance criteria of steel building code, comprehensive and quick evaluation procedures for X-bracing, are compared to each other parametrically and numerically. For this purpose, it is assumed first that the sample building is designed to meet steel building code and then by introducing transform parameters and using stress ratio of the designed components, acceptance of the designed building for life safety performance level is investigated. X-bracing acceptance criteria are studied using the new method and a list of differences for 2, 4, 6 &amp; 8 story buildings is prepared in details. Results show that almost 5% of X-braced samples designed based on steel building code are rejected by comprehensive and quick seismic evaluation. On the other hand, some rejected components based on steel building code, meet comprehensive and quick evaluation procedures. Furthermore, by using a similar method and assuming that building components meet quick evaluation, their acceptance possibility by comprehensive evaluation is investigated. Based on acquired results, almost 50% of X-braces meeting quick evaluation, are rejected by comprehensive evaluation. In contrast, some rejected samples by quick evaluation meet comprehensive evaluation procedure.</Abstract>
			<OtherAbstract Language="FA">In this paper, acceptance criteria of steel building code, comprehensive and quick evaluation procedures for X-bracing, are compared to each other parametrically and numerically. For this purpose, it is assumed first that the sample building is designed to meet steel building code and then by introducing transform parameters and using stress ratio of the designed components, acceptance of the designed building for life safety performance level is investigated. X-bracing acceptance criteria are studied using the new method and a list of differences for 2, 4, 6 &amp; 8 story buildings is prepared in details. Results show that almost 5% of X-braced samples designed based on steel building code are rejected by comprehensive and quick seismic evaluation. On the other hand, some rejected components based on steel building code, meet comprehensive and quick evaluation procedures. Furthermore, by using a similar method and assuming that building components meet quick evaluation, their acceptance possibility by comprehensive evaluation is investigated. Based on acquired results, almost 50% of X-braces meeting quick evaluation, are rejected by comprehensive evaluation. In contrast, some rejected samples by quick evaluation meet comprehensive evaluation procedure.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Acceptance Criteria</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Comprehensive Evaluation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Life Safety Performance Level</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Quick Evaluation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">X-Braces</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20778_82412905ecf24c9240ff4c120f0c66fe.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Seepage Analysis with Discrete Singular Convolution Method</ArticleTitle>
<VernacularTitle>Seepage Analysis with Discrete Singular Convolution Method</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20779</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Reza</FirstName>
					<LastName>Attarnejad</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Mahmood</FirstName>
					<LastName>Rabbanee</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, seepage analysis in isotropic environment is presented by discrete singular convolution (DSC) method. This method has been used for solving numerical problems since 1999. The theoretical basis of the method is distribution and wavelet theory. DSC exhibits accuracy for integration of global methods and flexibility for handling complex geometries and boundary conditions of local methods. At first, a simple case governed by Laplace equation and regularized Shannon’s kernel is considered to show the accuracy and efficiency of DSC method through L? and L2 errors. Seepage under concrete dam with or without sheet-pile is then solved through two different case studies. The results of this method against finite difference results are considered. The results show that this method is more accurate than finite difference method with reception of more operation value and optimization of R parameter.</Abstract>
			<OtherAbstract Language="FA">In this paper, seepage analysis in isotropic environment is presented by discrete singular convolution (DSC) method. This method has been used for solving numerical problems since 1999. The theoretical basis of the method is distribution and wavelet theory. DSC exhibits accuracy for integration of global methods and flexibility for handling complex geometries and boundary conditions of local methods. At first, a simple case governed by Laplace equation and regularized Shannon’s kernel is considered to show the accuracy and efficiency of DSC method through L? and L2 errors. Seepage under concrete dam with or without sheet-pile is then solved through two different case studies. The results of this method against finite difference results are considered. The results show that this method is more accurate than finite difference method with reception of more operation value and optimization of R parameter.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Discrete Singular Convolution</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Distribution Theory</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Laplace Equation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Regularized Shannon’s Kernel</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Seepage</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Wavelet Theory</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20779_df664228fa6c7bf82c5b1f05c304d8ad.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Bearing Capacity of Foundations Located on Concave Slopes in Plan View Using Upper Bound Theorem</ArticleTitle>
<VernacularTitle>Bearing Capacity of Foundations Located on Concave Slopes in Plan View Using Upper Bound Theorem</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20780</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Orang</FirstName>
					<LastName>Farzaneh</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Farajollah</FirstName>
					<LastName>Askari</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Reza</FirstName>
					<LastName>Yeganeh Khaksar</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>Bearing Capacity of concave slopes is such a three-dimensional problem that two-dimensional assumptions do not result in satisfactory and acceptable results. Presented in this article is an algorithm to calculate the bearing capacity of foundations located on such slopes based on the upper bound theorem of the limit analysis approach.
Limit analysis method is based on the extensions of maximum work principle derived by Hill, and was given in the form of theorems by Drucker, Prager and Greenberg. Using this approach, the true solution from a lower bound to an upper bound would be bracketed. Applicability of this theorem requires that the soil’s behavior be perfectly plastic and the deformation be governed by the normality rule. Considering the theorem of kinematic approach (upper-bound), the rate of work done by traction and body forces would be less than or equal to the energy dissipation rate in any assumed kinematically admissible failure mechanism. In this algorithm, initially the collapse mechanism is assumed as a set of five or six-face rigid blocks slipping on each other with enrgy dissipation taking place along planar velocity discontinuities. and then, during an optimizing process the minimum result would be considered as the ultimate load of the slope. This approach can be considered as an extension of the procedure proposed by Farzaneh and Askari in 1999. The numerical results indicate that the bearing capacity of a shallow foundation on concave slope is more than that of the same foundation on linear slope and also fewer is the ratio of slope radius to its height, more would be the bearing capacity of the foundation located on it.  In addition, unloaded slopes are more stable when they are concave comparing with linear slopes. In bearing capacity, the curvature effect in concave slopes is more considerable for frictional soils than cohesive ones. The results are presented in the form of applicable charts to evaluate the bearing capacity of a foundation located on a concave slope.</Abstract>
			<OtherAbstract Language="FA">Bearing Capacity of concave slopes is such a three-dimensional problem that two-dimensional assumptions do not result in satisfactory and acceptable results. Presented in this article is an algorithm to calculate the bearing capacity of foundations located on such slopes based on the upper bound theorem of the limit analysis approach.
Limit analysis method is based on the extensions of maximum work principle derived by Hill, and was given in the form of theorems by Drucker, Prager and Greenberg. Using this approach, the true solution from a lower bound to an upper bound would be bracketed. Applicability of this theorem requires that the soil’s behavior be perfectly plastic and the deformation be governed by the normality rule. Considering the theorem of kinematic approach (upper-bound), the rate of work done by traction and body forces would be less than or equal to the energy dissipation rate in any assumed kinematically admissible failure mechanism. In this algorithm, initially the collapse mechanism is assumed as a set of five or six-face rigid blocks slipping on each other with enrgy dissipation taking place along planar velocity discontinuities. and then, during an optimizing process the minimum result would be considered as the ultimate load of the slope. This approach can be considered as an extension of the procedure proposed by Farzaneh and Askari in 1999. The numerical results indicate that the bearing capacity of a shallow foundation on concave slope is more than that of the same foundation on linear slope and also fewer is the ratio of slope radius to its height, more would be the bearing capacity of the foundation located on it.  In addition, unloaded slopes are more stable when they are concave comparing with linear slopes. In bearing capacity, the curvature effect in concave slopes is more considerable for frictional soils than cohesive ones. The results are presented in the form of applicable charts to evaluate the bearing capacity of a foundation located on a concave slope.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Bearing Capacity</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Concave slope in Plan View</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Limit Analysis Approach</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Three-Dimensional Analysis</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Upper Bound Theorem</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20780_e4371ded8ccf1c3eca4036849e571ad3.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Effect of Turbulent Modeling on Computed Wind Pressure Load over Cooling Towers with Base Structures and Comparison with VGB Guide-line</ArticleTitle>
<VernacularTitle>Effect of Turbulent Modeling on Computed Wind Pressure Load over Cooling Towers with Base Structures and Comparison with VGB Guide-line</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20781</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mohammad Ali</FirstName>
					<LastName>Goudarzi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Saeid Reza</FirstName>
					<LastName>Sabbagh Yazdi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>The wind pressure is one of the important loads on cooling towers which can be computed via numerical solution of the wind flow. In this paper, the effects of turbulent modeling on accurate computations of wind pressure on a cooling tower with base structure are investigated. For this propose, the results of a finite element flow solver using various commonly used turbulence models are compared with the reported laboratory measurements on a small scale physical. Having chosen the most suitable turbulence model, the effect of considering the geometrical features of the base structures supporting the louvers on formation of pressure fields over the external surface of a cooling tower in actual scale (designed for the KAZERUN combined cycle power plant) is investigated. The computed results of this case with and without base attachments are compared with the wind loads which are suggested by the VGB guidelines. The comparison of the results shows that, the pressure distribution trend (particularly in the rear side) slightly differs for various elevations. Furthermore, considering the effects of base structures of the cooling towers ends up with computed pressure distribution different from the pressure distribution suggested VGB guidelines, particularly in lower parts of the tower.</Abstract>
			<OtherAbstract Language="FA">The wind pressure is one of the important loads on cooling towers which can be computed via numerical solution of the wind flow. In this paper, the effects of turbulent modeling on accurate computations of wind pressure on a cooling tower with base structure are investigated. For this propose, the results of a finite element flow solver using various commonly used turbulence models are compared with the reported laboratory measurements on a small scale physical. Having chosen the most suitable turbulence model, the effect of considering the geometrical features of the base structures supporting the louvers on formation of pressure fields over the external surface of a cooling tower in actual scale (designed for the KAZERUN combined cycle power plant) is investigated. The computed results of this case with and without base attachments are compared with the wind loads which are suggested by the VGB guidelines. The comparison of the results shows that, the pressure distribution trend (particularly in the rear side) slightly differs for various elevations. Furthermore, considering the effects of base structures of the cooling towers ends up with computed pressure distribution different from the pressure distribution suggested VGB guidelines, particularly in lower parts of the tower.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Cooling Tower with Base Structures</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">finite element method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Turbulence Modeling</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Wind Pressure</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20781_0937d18a8fa6e60deb95aec1e5a9abff.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>A Study on the Behavior of Beam to Boxed Column Connections with Peripheral Diaphragms</ArticleTitle>
<VernacularTitle>A Study on the Behavior of Beam to Boxed Column Connections with Peripheral Diaphragms</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20782</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Shahrokh</FirstName>
					<LastName>Malek</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Morteza</FirstName>
					<LastName>Hajifathali</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract></Abstract>
			<OtherAbstract Language="FA"></OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Beam to Column Connections</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Boxed Columns</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Connection Rotation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Continuity Plate</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Dog Bone Beam Flange</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Ductility</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Moment-Curvature Relationship</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Peripheral Plates</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20782_4eefbacb2ab197be05558d91bf2840b0.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Uniformity Effect on Scour hole Dimensions due to Free Falling Jets</ArticleTitle>
<VernacularTitle>Uniformity Effect on Scour hole Dimensions due to Free Falling Jets</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20783</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mojtaba</FirstName>
					<LastName>Mehraein</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Masoud</FirstName>
					<LastName>Ghodsian</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Hamidreza</FirstName>
					<LastName>Ranjbar</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract></Abstract>
			<OtherAbstract Language="FA"></OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Experimental Equations</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Experimental study</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Free Falling Jets</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Laboratory Model</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">prototype</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">scour</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20783_0b28f511d5c936f11cb254cee564494e.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Experimental Study on Flow Field and Scour Pattern around T Shaped Spur Dike in a 90 Degree Bend</ArticleTitle>
<VernacularTitle>Experimental Study on Flow Field and Scour Pattern around T Shaped Spur Dike in a 90 Degree Bend</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20784</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mohammad</FirstName>
					<LastName>Vaghefi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Masoud</FirstName>
					<LastName>Ghodsian</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>Spur dike is a hydraulic structure used for protection of river banks. In the past few decades, the use of spur dikes for stability of the outer banks of rivers has attracted the attention of hydraulic engineers. Setting spur dikes in the flow’s direction leads to local scour around the spur dike and changes the topography of the bed. This study experimentally measures the flow field and scour around T-shaped spur dike install in 90 degree bend. The experiments were carried out in a channel with a 90 degrees bend and with a mild curvature. Uniform sediments having an average diameter of 1.28mm were used under clear water condition. The three-dimensional Acoustic Doppler Velocimeter (ADV) and point gage were used for measuring the flow field and bed topography. For this purpose, scour test was done at the beginning of the experiment and the topography of the bed with the scour hole around the sour dike installed at the 75 degree was measured. And the three-dimensional time-averaged velocity was measured. Then the comparison of the three dimensional components of speed was made in different sections and the differences of the flow pattern along the bend was analyzed. The observations showed the effect of the spur dike and the bed’s topography in distorting the secondary flow pattern and in the formation of the subsequent secondary flow. In addition, the secondary flows are formed along the scour hole slope development. In the downstream sections of the spur dike, the power of the secondary flow increases.  At the end of the bend, this changes the flow direction from the external bank towards the internal bank. In the plans, some horizontal vortices with a counter-clock-wise direction can also be observed in the upstream of the spur dike in different layers.</Abstract>
			<OtherAbstract Language="FA">Spur dike is a hydraulic structure used for protection of river banks. In the past few decades, the use of spur dikes for stability of the outer banks of rivers has attracted the attention of hydraulic engineers. Setting spur dikes in the flow’s direction leads to local scour around the spur dike and changes the topography of the bed. This study experimentally measures the flow field and scour around T-shaped spur dike install in 90 degree bend. The experiments were carried out in a channel with a 90 degrees bend and with a mild curvature. Uniform sediments having an average diameter of 1.28mm were used under clear water condition. The three-dimensional Acoustic Doppler Velocimeter (ADV) and point gage were used for measuring the flow field and bed topography. For this purpose, scour test was done at the beginning of the experiment and the topography of the bed with the scour hole around the sour dike installed at the 75 degree was measured. And the three-dimensional time-averaged velocity was measured. Then the comparison of the three dimensional components of speed was made in different sections and the differences of the flow pattern along the bend was analyzed. The observations showed the effect of the spur dike and the bed’s topography in distorting the secondary flow pattern and in the formation of the subsequent secondary flow. In addition, the secondary flows are formed along the scour hole slope development. In the downstream sections of the spur dike, the power of the secondary flow increases.  At the end of the bend, this changes the flow direction from the external bank towards the internal bank. In the plans, some horizontal vortices with a counter-clock-wise direction can also be observed in the upstream of the spur dike in different layers.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">90 degree bend</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Flow pattern</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Scour Pattern</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">secondary flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">T Shape Spur Dike</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20784_c67076202cbd4595038d03e65fa57227.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Nonlinear Vibration Analysis of Rubber Springs in Suspension Systems of Passenger Trains</ArticleTitle>
<VernacularTitle>Nonlinear Vibration Analysis of Rubber Springs in Suspension Systems of Passenger Trains</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20785</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Davood</FirstName>
					<LastName>Younesian</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Hasan</FirstName>
					<LastName>Shokrollahi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>Rubber springs could perform the same function of the steel springs in railway vehicle suspension systems and they have benefits of having no wear and rust. They are now successfully being used in both primary and secondary suspension systems of passenger trains. Nonlinear vibration of rubber springs used in suspension systems of passenger trains is studied in this paper. The rubber spring model mainly aims at representing the mechanical behavior of rubber springs for the frequency range of 0±20 Hz. The model is one-dimensional with a relationship between force and motion based on a superposition of elastic, friction and Maxwell visco-elastic forces. Inclusion of a friction force means that increased stiffness at small displacement amplitudes as well as rate-independent damping (hysteresis) can be considered. The validity of the model experimentally has been verified in the literature. A parametric study shows that the rubber spring equivalent stiffness has softening behavior with respect to both amplitude and frequency and its equivalent damping has hardening behavior with respect to both amplitude and the excitation frequency. The nonlinear rubber model is used in a dynamic ride model consists of body, bogies and wheelsets. The excitation here is the surface roughness of the rail which arises from the rail corrugation. The rail roughness is generated randomly by its Power Spectral Density (PSD) for 5 classes of rails according to USA rail classification. Classes 1 to 5 are considered and a dynamic simulation is carried out in order to more identify the rubber spring behavior in suspension systems. The numerical simulation is carried out using MATLAB software and all nonlinearities are exactly modeled. The simulation output here is the level of comfort index obtained by Sperling Comfort Index. A comprehensive parametric study is carried out and the effects of train speed as well as the rubber mechanical properties and the rail class on the comfort indexes and also the equivalent stiffness and damping of the rubber elements are studied.
A new linearization technique namely Weighted-Linearization Method (WLM) is proposed in this paper in order to simplify full-nonlinear model. In this method the behavior of nonlinear rubber spring is more magnified in vicinity of the frequency range of 4-6 Hz in which all filter gains are in their highest value (close to 1.0).  The aim here is to enhance correlation between the linear and nonlinear model to get similar results for the Comfort Index. The weighting frequency function which is utilized in linearization procedure is the Sperling filter transfer function. Very good correlation is achieved between the results obtained for linear and nonlinear model. It is also found that the classical linearization procedure results in considerable error in calculating comfort indicators.</Abstract>
			<OtherAbstract Language="FA">Rubber springs could perform the same function of the steel springs in railway vehicle suspension systems and they have benefits of having no wear and rust. They are now successfully being used in both primary and secondary suspension systems of passenger trains. Nonlinear vibration of rubber springs used in suspension systems of passenger trains is studied in this paper. The rubber spring model mainly aims at representing the mechanical behavior of rubber springs for the frequency range of 0±20 Hz. The model is one-dimensional with a relationship between force and motion based on a superposition of elastic, friction and Maxwell visco-elastic forces. Inclusion of a friction force means that increased stiffness at small displacement amplitudes as well as rate-independent damping (hysteresis) can be considered. The validity of the model experimentally has been verified in the literature. A parametric study shows that the rubber spring equivalent stiffness has softening behavior with respect to both amplitude and frequency and its equivalent damping has hardening behavior with respect to both amplitude and the excitation frequency. The nonlinear rubber model is used in a dynamic ride model consists of body, bogies and wheelsets. The excitation here is the surface roughness of the rail which arises from the rail corrugation. The rail roughness is generated randomly by its Power Spectral Density (PSD) for 5 classes of rails according to USA rail classification. Classes 1 to 5 are considered and a dynamic simulation is carried out in order to more identify the rubber spring behavior in suspension systems. The numerical simulation is carried out using MATLAB software and all nonlinearities are exactly modeled. The simulation output here is the level of comfort index obtained by Sperling Comfort Index. A comprehensive parametric study is carried out and the effects of train speed as well as the rubber mechanical properties and the rail class on the comfort indexes and also the equivalent stiffness and damping of the rubber elements are studied.
A new linearization technique namely Weighted-Linearization Method (WLM) is proposed in this paper in order to simplify full-nonlinear model. In this method the behavior of nonlinear rubber spring is more magnified in vicinity of the frequency range of 4-6 Hz in which all filter gains are in their highest value (close to 1.0).  The aim here is to enhance correlation between the linear and nonlinear model to get similar results for the Comfort Index. The weighting frequency function which is utilized in linearization procedure is the Sperling filter transfer function. Very good correlation is achieved between the results obtained for linear and nonlinear model. It is also found that the classical linearization procedure results in considerable error in calculating comfort indicators.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">comfort index</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Nonlinear Vibration Analysis</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Passenger Trains</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Rubber</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Suspension Systems</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcse.ut.ac.ir/article_20785_47846a2d7b4ea07e7ee1b3d50fb6528a.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName></PublisherName>
				<JournalTitle>Journal of Civil and Surveying Engineering</JournalTitle>
				<Issn></Issn>
				<Volume>44</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2010</Year>
					<Month>06</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>The Third Generation Spectral Wave Model, WAVEWATACH-III, Enhanced for use in Nearshore Regions</ArticleTitle>
<VernacularTitle>The Third Generation Spectral Wave Model, WAVEWATACH-III, Enhanced for use in Nearshore Regions</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">20786</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Peyman</FirstName>
					<LastName>Badiei</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>S. Mostafa</FirstName>
					<LastName>Siadat Mousavi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>1970</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>WAVEWATCH-III is a third generation spectral wave model, developed originally for deep water in Ocean Modeling Branch of NOAA. By adding nearshore processes and removing some restriction from its code, the model can be applied to a full range of water depths from offshore to coastal regions. Depth induced wave breaking, surf zone energy dissipation and Triad wave-wave interactions are the important physical processes considered in shallow waters. The restrictions on time steps and minimum water depth in the original code have been relaxed to make the model applicable to coastal areas with high spatial resolution. The simulation results of the modified model have been compared with another third generation and widely tested spectral model, SWAN, in addition to some laboratory and field data.</Abstract>
			<OtherAbstract Language="FA">WAVEWATCH-III is a third generation spectral wave model, developed originally for deep water in Ocean Modeling Branch of NOAA. By adding nearshore processes and removing some restriction from its code, the model can be applied to a full range of water depths from offshore to coastal regions. Depth induced wave breaking, surf zone energy dissipation and Triad wave-wave interactions are the important physical processes considered in shallow waters. The restrictions on time steps and minimum water depth in the original code have been relaxed to make the model applicable to coastal areas with high spatial resolution. The simulation results of the modified model have been compared with another third generation and widely tested spectral model, SWAN, in addition to some laboratory and field data.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">energy dissipation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Spectral Wave Models</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">SWAN</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Triad Wave-Wave Interaction</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">wave breaking</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">WAVEWATCH-III</Param>
			</Object>
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