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<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University (SRTTU)</PublisherName>
				<JournalTitle>Journal of Computational &amp; Applied Research in Mechanical Engineering (JCARME)</JournalTitle>
				<Issn>2228-7922</Issn>
				<Volume>12</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Assessment of particle size distribution and tensile properties of hybrid epoxy composite reinforced with functionalized graphene and CNT nanofillers</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>1</FirstPage>
			<LastPage>12</LastPage>
			<ELocationID EIdType="pii">1689</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jcarme.2022.5312.1656</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>Manoj Kumar</FirstName>
					<LastName>Shukla</LastName>
<Affiliation>Department of Mechanical Engineering, Institute of Engineering &amp; Technology, GLA University, Mathura 281406, India,  
Department of Mechanical Engineering, Institute of Engineering &amp; Technology, GLA University, Mathura 281406, India</Affiliation>

</Author>
<Author>
					<FirstName>Kamal</FirstName>
					<LastName>Sharma</LastName>
<Affiliation>Kalaniketan Polytechnic College, Jabalpur 482001, Jabalpur, Affiliated to Rajiv Gandhi Technical University, Bhopal, India</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>05</Month>
					<Day>22</Day>
				</PubDate>
			</History>
		<Abstract>The synergetic effect of amine functionalized multiple graphene layers (AMGL) and multi-walled carbon nanotube (AMWCNT) nano-fillers mixed with epoxy resin is investigated on the particle size distribution (PSD) and tensile properties of hybrid composites. The hybrid composites with an equal ratio of nano-fillers at a weight percent of 0.25, 0.50, 1, and 2 wt % are fabricated. The particle size analysis (PSA) is performed by the dynamic light scattering (DLS) technique and image analysis (IA) method; both verify PSD for composites. This is further verified by the analyses of scanning electron microscopy (SEM) images using Image J software. The optimum composite particle size of 6.8 µm and homogeneous mixture with a poly-dispersity index (PI) of 0.74 is investigated for a sample having filler content of 0.5 wt %. Tensile stress and elastic modulus is also found to be maximum at 0.5 wt %, which is 49.91 MPa of 2302 Mpa, respectively. The chemical composition of composite affecting its PSD is characterized by energy dispersive X-ray (EDX) process. Dimensional analysis of particle size in the domain of epoxy matrix provides deep insights to the researchers and may also provide them a direction for selecting an appropriate material for a particular application.  </Abstract>
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			<Object Type="keyword">
			<Param Name="value">Graphene</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Carbon nanotube (CNT)</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Particle size distribution (PSD)</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Hybrid composite</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Image Analysis (IA)</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Tensile strength</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Elastic modulus</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcarme.sru.ac.ir/article_1689_ac888a7651181b71ce514a6d6496d666.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University (SRTTU)</PublisherName>
				<JournalTitle>Journal of Computational &amp; Applied Research in Mechanical Engineering (JCARME)</JournalTitle>
				<Issn>2228-7922</Issn>
				<Volume>12</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical prediction of the drag coefficient of bluff bodies in three-dimensional pipe flow</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>13</FirstPage>
			<LastPage>29</LastPage>
			<ELocationID EIdType="pii">1622</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jcarme.2021.7114.1931</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>A.</FirstName>
					<LastName>Tamil Chandran</LastName>
<Affiliation>Fluid Control Research Institute, Palakkad, Kerala- 678623, India</Affiliation>

</Author>
<Author>
					<FirstName>T.</FirstName>
					<LastName>Suthakar</LastName>
<Affiliation>Mechanical Engineering department, National Institute of Technology- Trichirapallai, Tamil Nadu, India</Affiliation>

</Author>
<Author>
					<FirstName>K. R.</FirstName>
					<LastName>Balasubramanian</LastName>
<Affiliation>Mechanical Engineering department, National Institute of Technology- Trichirapallai, Tamil Nadu, India</Affiliation>

</Author>
<Author>
					<FirstName>S.</FirstName>
					<LastName>Rammohan</LastName>
<Affiliation>Fluid Control Research Institute, Palakkad, Kerala- 678623, India</Affiliation>

</Author>
<Author>
					<FirstName>Jacob</FirstName>
					<LastName>Chandapillai</LastName>
<Affiliation>Fluid Control Research Institute, Palakkad, Kerala- 678623, India</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2020</Year>
					<Month>07</Month>
					<Day>13</Day>
				</PubDate>
			</History>
		<Abstract>Numerical analysis of drag coefficient of three-dimensional bluff bodies such as flat plates, cylinder, triangular prism, semicircular profiles located in the flow path of the pipe was performed. Bluff bodies of various lengths are analysed using a turbulence model. The effect of bluff body thickness on drag coefficient was analysed. A significant observation of the study is the reduction in drag coefficient with an increase in thickness. Effect of pressure coefficient on drag coefficient was evaluated. The study confirms that frictional coefficient has negligible effect on drag coefficient in the studied Reynolds number range. Change in drag coefficient over a wide range of Reynolds number was studied and is reported. Irrespective of geometry and length, the study indicates that there is a significant difference in drag coefficient between two dimensional and three dimensional simulation studies. It is also concluded that the length  of a bluff body in a confined domain  has a significant effect on its drag coefficient.</Abstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Drag coefficient</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Pressure coefficient</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Turbulence model</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Computational Fluid Dynamics</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Bluff body</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Friction coefficient</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcarme.sru.ac.ir/article_1622_371408b0954b53888523f96e2a465cde.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University (SRTTU)</PublisherName>
				<JournalTitle>Journal of Computational &amp; Applied Research in Mechanical Engineering (JCARME)</JournalTitle>
				<Issn>2228-7922</Issn>
				<Volume>12</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Experimental study of melting of composite phase change materials used in honeycomb energy storage system</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>31</FirstPage>
			<LastPage>40</LastPage>
			<ELocationID EIdType="pii">1698</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jcarme.2022.8741.2175</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>Ahmed F.</FirstName>
					<LastName>Hasan</LastName>
<Affiliation>Department of Materials Engineering, University of Diyala, Baquba 32001, Iraq</Affiliation>

</Author>
<Author>
					<FirstName>Salah N.</FirstName>
					<LastName>Farhan</LastName>
<Affiliation>Department of Chemical Engineering, University of Diyala, Baquba 32001, Iraq</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2022</Year>
					<Month>01</Month>
					<Day>09</Day>
				</PubDate>
			</History>
		<Abstract>Phase change materials have attracted a considerable attention in thermal energy storage research recently due to their thermal characteristic. Composite materials have great potential as one of the best alternative approach that would be utilized to increase the thermal performance of this sort of materials. This work aims to improve the Latent Heat energy Storage Unit (LHSU) in terms of thermal performance during the melting process by utilizing honeycomb metal structures conﬁguration. An experimental study has been carried out to examine the thermal behavior of this particular material in honeycomb LHSU. The thermal performance evaluation in terms of melting time of the proposed honeycomb LHSU was conducted in comparison with the normal LHSU. The influences of using different heat transfer fluid temperature on the charging power are considered for the enhanced geometrical conﬁguration.  The results showed significant enhancement in the melting time which reached 87%. Also, the melting range in the lower part of the storage unit was improved compared with the normal one from 190 to 24 min in case of using honeycomb. For the propose of configuration, by increasing the fluid temperature, charging power was accelerated, which in turn reduces the charging time from 14% to 16.</Abstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Composite honeycomb</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">storage unit</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Phase change materials</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">latent heat</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Honeycomb structure</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcarme.sru.ac.ir/article_1698_dd988d9732b108c145298c9198054810.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University (SRTTU)</PublisherName>
				<JournalTitle>Journal of Computational &amp; Applied Research in Mechanical Engineering (JCARME)</JournalTitle>
				<Issn>2228-7922</Issn>
				<Volume>12</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Surface finish characteristics of distinct materials using extrusion honing process</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>41</FirstPage>
			<LastPage>50</LastPage>
			<ELocationID EIdType="pii">1621</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jcarme.2021.7797.2042</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>S. L. N.</FirstName>
					<LastName>Jayasimha</LastName>
<Affiliation>Department of Mechanical Engineering, P.E.S College of Engineering, Mandya-571401, India</Affiliation>

</Author>
<Author>
					<FirstName>Ganapathy</FirstName>
					<LastName>Bawge</LastName>
<Affiliation>Department of Mechanical Engineering, P.E.S College of Engineering, Mandya-571401, India</Affiliation>

</Author>
<Author>
					<FirstName>H. P.</FirstName>
					<LastName>Raju</LastName>
<Affiliation>Department of Mechanical Engineering, P.E.S College of Engineering, Mandya-571401, India</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>02</Month>
					<Day>17</Day>
				</PubDate>
			</History>
		<Abstract>Traditional methods of finishing like grinding, lapping, and honing are limited to finishing of vital shapes such as flat and circular. These conventional methods are lagging for processing components that are fabricated by hard materials, involving complicated profiles in particular. Hence, it is essential to explore a finishing process, which addresses wide applications, better accuracy, higher efficiency, consistent quality and economy in finishing complex shaped parts. So, a new precision finishing process like extrusion honing has been implemented for polishing from several microns to the nano level. This work aims to assess the influence of a number of abrasive media passes on the surface integrity of aluminum, copper, and titanium grade-2 materials. The study has been performed by adopting an abrasive 36 mesh size with a concentration of 40% followed by 10 abrasive media passes. The influence of these process parameters has been studied in analyzing the roughness characteristics R&lt;sub&gt;a&lt;/sub&gt;, R&lt;sub&gt;max,&lt;/sub&gt; R&lt;sub&gt;z&lt;/sub&gt;, and R&lt;sub&gt;max&lt;/sub&gt;/R&lt;sub&gt;a&lt;/sub&gt; and the nature of surface induced by SEM characterization for the metals of consideration using the extrusion honing process.</Abstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Extrusion honing</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Surface finish</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Material removal</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Abrasives</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcarme.sru.ac.ir/article_1621_1b48e60c9403d6abd51133cfe3955528.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University (SRTTU)</PublisherName>
				<JournalTitle>Journal of Computational &amp; Applied Research in Mechanical Engineering (JCARME)</JournalTitle>
				<Issn>2228-7922</Issn>
				<Volume>12</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Large eddy simulation of non-reactive flow in burners</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>51</FirstPage>
			<LastPage>62</LastPage>
			<ELocationID EIdType="pii">1646</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jcarme.2022.8470.2139</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Zakyani</LastName>
<Affiliation>Aerospace Research Institute (ARI), Tehran, 1465774111, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>10</Month>
					<Day>12</Day>
				</PubDate>
			</History>
		<Abstract>Large eddy simulations of non-reactive Delft II and Sydney bluff body flow are performed using different sub-grid scale models. Simulation of non-reactive burners is useful when studying flow characteristics inside reactive burners. As turbulent combustion simulation is rather an intricate task, it is helpful to study cold air flow inside the combustion chamber before igniting the chamber. In order to study the flow inside the mentioned test cases, different sub-grid scale models, i.e., constant Smagorinsky, dynamic Smagorinsky and dynamic WALE model are used to model the unresolved small scales. For the numerical simulations, a finite volume in-house code is used. The code adopts the projection method to solve the fluid flow equations. A second-order accurate scheme is used for spatial discretization. The time integration is done using a second-order accurate predictor-corrector scheme. For solving the resultant pressure Poisson equation, TDMA (Tridiagonal Matrix Algorithm) is used with multi-grid convergence acceleration. Generally, the results show good agreement with available experimental data. As expected, the dynamic WALE model performs better than the other models. To further improve the results, a rather realistic type of velocity inlet boundary conditions are applied to Sydney bluff body flow, i.e., digital filter velocity inflow boundary conditions. The results show drastic improvement using digital filter inflow, which is mainly due to the turbulent nature of the flow field.</Abstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Large Eddy Simulation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Sub-Grid Scale Models</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Constant Smagorinsky Model</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Dynamic Smagorinsky Model</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Dynamic WALE Model</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcarme.sru.ac.ir/article_1646_fd40affb920e734cdd58df5e242ec53f.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University (SRTTU)</PublisherName>
				<JournalTitle>Journal of Computational &amp; Applied Research in Mechanical Engineering (JCARME)</JournalTitle>
				<Issn>2228-7922</Issn>
				<Volume>12</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Modeling of dynamic cutting forces and cutting characteristics based on the analyzed results of average force-feed rate relationship in milling process</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>63</FirstPage>
			<LastPage>75</LastPage>
			<ELocationID EIdType="pii">1620</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jcarme.2021.8011.2070</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>Nhu-Tung</FirstName>
					<LastName>Nguyen</LastName>
<Affiliation>HaUI Institute of Technology – HIT, Hanoi University of Industry, Hanoi city, 100000, Vietnam</Affiliation>

</Author>
<Author>
					<FirstName>Dong Van</FirstName>
					<LastName>Pham</LastName>
<Affiliation>Science and Technology Department, Hanoi University of Industry, Hanoi city, 100000, Vietnam</Affiliation>

</Author>
<Author>
					<FirstName>Cuong Duc</FirstName>
					<LastName>Pham</LastName>
<Affiliation>HaUI Institute of Technology – HIT, Hanoi University of Industry, Hanoi city, 100000, Vietnam</Affiliation>

</Author>
<Author>
					<FirstName>Dung Hoang</FirstName>
					<LastName>Tien</LastName>
<Affiliation>Mechanical Engineering Faculty, Hanoi University of Industry, Hanoi city, 100000, Vietnam</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>04</Month>
					<Day>20</Day>
				</PubDate>
			</History>
		<Abstract>Cutting force coefficients (CFCs) are the most important factors in the prediction of CFs (CFs) and other machining characteristics (MCs). This study was conducted to model the CFs and MCs in the milling process based on the calculated values of CFCs. From the relationship of average values of CFs and feed rate, CFCs were determined and used to predict dynamic CFs (DCFs) in the flat milling process. In static models, the average values of CFs were presented as a linear regression of feed rate. The DCFs and other MCs were modeled depending on the cutting parameters, cutter geometry, CFCs, and structure parameters of the machine-tool system. By performing the flat-milling process of gray cast iron GG25 using HSS-Co solid tool, the average CFs were modeled as the linear regression of feed rate with large determination coefficients (R&lt;sup&gt;2&lt;/sup&gt; &gt; 93%). Besides, all CFCs of a pairs of tool and workpiece for each cutting type were successfully determined based on the measured data of CFs from the experimental process. Moreover, the proposed models of DCFs were successfully verified based on the compared results between the predicted CFs and measured CFs in several cutting tests with different cutting parameters. The proposed models of cutting force in this study were successfully used to predict the DCFs and several MCs in milling processes using a flat milling tool. And can be used to design and develop tools and machine in industrial manufacturing.</Abstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Dynamic cutting force</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Average cutting force</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Cutting characteristics</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Flat-milling process</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcarme.sru.ac.ir/article_1620_891c02bb472ef4deb1c2295c7a6178c5.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University (SRTTU)</PublisherName>
				<JournalTitle>Journal of Computational &amp; Applied Research in Mechanical Engineering (JCARME)</JournalTitle>
				<Issn>2228-7922</Issn>
				<Volume>12</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Performance analysis of a combined cooling, heating and power system based on micro gas turbine from the point of view of exergy</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>77</FirstPage>
			<LastPage>93</LastPage>
			<ELocationID EIdType="pii">1643</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jcarme.2021.7514.1999</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>J.</FirstName>
					<LastName>Pirkandi</LastName>
<Affiliation>Faculty of Aerospace, Malek Ashtar University of Technology, 15875-1774, Iran</Affiliation>

</Author>
<Author>
					<FirstName>A.</FirstName>
					<LastName>Amiralaei</LastName>
<Affiliation>Department of Mechanical Engineering, Azad University, West Tehran Branch, 1468763785, Iran</Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Omian</LastName>
<Affiliation>Faculty of Aerospace, Malek Ashtar University of Technology, 15875-1774, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2020</Year>
					<Month>11</Month>
					<Day>15</Day>
				</PubDate>
			</History>
		<Abstract>In this research, a combined cooling, heating and power system (CCHP) has been analyzed from the perspective of entropy and exergy. The primary driver and the cooling system for this combined system consist of a micro gas turbine and a hot water lithium bromide single-effect absorption chiller, respectively. The effects of compressor pressure ratio, micro turbine inlet gas temperature and chiller cooling capacity on important system efficiencies and other operational parameters (e.g., electrical efficiency, thermal efficiency, combined heating and power cogeneration efficiency, and combined cooling, heating and power cogeneration efficiency) have been investigated. The findings indicate that the system has its highest electrical efficiency at a compressor pressure ratio of 5. Also at this pressure ratio, the cogeneration efficiency (combined heating, cooling and power) and the exergy efficiency are about 48% and 24%, respectively. Moreover, the increase of the turbine inlet gas temperature has had a positive effect on the investigated parameters. The results show that the increase of cooling capacity reduces the cogeneration efficiencies, but has no effect on the exergy efficiency. Also, by considering specific values for the studied parameters, the amounts of generated entropy and destroyed exergy in various parts of the system have been calculated. The results indicate that the highest amounts of entropy and exergy have been generated and destroyed in the combustion chamber. Parts of the results indicate a system state in which the overall efficiency (combined heating, cooling and power cogeneration efficiency) of the system has increased 13% relative to the system’s initial state.</Abstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">CCHP system</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Microturbine</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Absorption chiller</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Thermodynamic</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://jcarme.sru.ac.ir/article_1643_d9214c03b41f00c3db498054109a8669.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University (SRTTU)</PublisherName>
				<JournalTitle>Journal of Computational &amp; Applied Research in Mechanical Engineering (JCARME)</JournalTitle>
				<Issn>2228-7922</Issn>
				<Volume>12</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Analysis and implementation of the solar tree by determining the optimal angle in Shiraz-Iran</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>95</FirstPage>
			<LastPage>107</LastPage>
			<ELocationID EIdType="pii">1598</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jcarme.2021.8079.2076</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>Meraj</FirstName>
					<LastName>Rajaee</LastName>
<Affiliation>Department of Electrical Engineering, Technical and Vocational University (TVU), Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Mina</FirstName>
					<LastName>Jalali</LastName>
<Affiliation>Department of Electrical Engineering, Technical and Vocational University (TVU), Tehran, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>05</Month>
					<Day>16</Day>
				</PubDate>
			</History>
		<Abstract>The solar tree is a combination of technology and art that is considered as the application of solar energy in the art of urban architecture. This study aims to combine solar technology with architectural style and art, to help urban beautification and investigate the increase in solar panels&#039; efficiency by focusing on the optimal slope and no shading in the form of a new solar tree structure. In this paper, the best angle for placing panels on tree branches to increase Shiraz&#039;s maximum efficiency has been calculated. The best angle is done with the help of the NRI mathematical model. Also, the Fibonacci sequence, which originates from nature and real trees, has been used to minimize shadows on this tree. The panels&#039; optimal slope calculations are performed using MATLAB software. Also, the monthly efficiency changes resulting from the optimal slope have been calculated and displayed. By analyzing the computational relationships and their implementation by PVsyst simulator, the optimal annual slope of solar panels obtained 30 degrees. By implementing it in the solar tree structure, the proposed  annual efficiency of the model has increased by 12% compared to the fixed state. This article examines the technical methods of using solar systems in urban architecture with emphasis on integration methods. In the proposed and implemented solar tree model with the ability to adjust the optimal angle and beautify passages, parks and recreation centers, it is possible to charge electronic equipment such as mobile phones, tablets, and electric bicycles through clean solar energy.</Abstract>
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			<Param Name="value">solar tree</Param>
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			<Object Type="keyword">
			<Param Name="value">optimized slope</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">shadow effect</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">solar charger</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Solar energy</Param>
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</Article>

<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University (SRTTU)</PublisherName>
				<JournalTitle>Journal of Computational &amp; Applied Research in Mechanical Engineering (JCARME)</JournalTitle>
				<Issn>2228-7922</Issn>
				<Volume>12</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Study of the effect of the boundary layer excitation in the nanofluids flow inside the tube on increasing the heat transfer coefficient</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>109</FirstPage>
			<LastPage>119</LastPage>
			<ELocationID EIdType="pii">1601</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jcarme.2021.6252.1795</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>J.</FirstName>
					<LastName>Zareei</LastName>
<Affiliation>Department of Biosystem Engineering, Ferdowsi University of Mashhad, Mashad, Iran</Affiliation>

</Author>
<Author>
					<FirstName>S. H.</FirstName>
					<LastName>Hoseyni</LastName>
<Affiliation>Department of Mechanical Engineering, Islamic Azad University, Kashmar branch, Kashmar, Iran</Affiliation>

</Author>
<Author>
					<FirstName>M.</FirstName>
					<LastName>Elveny</LastName>
<Affiliation>DS &amp; CI Research group, Universitas Sumatera Utara, Medan, Indonesia</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>29</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, the effect of boundary layer excitation on increasing the heat transfer coefficient of water/carbon nanotube (CNT) nanofluid and water/aluminum oxide (Al&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt;) nanoparticles has been investigated. The turbulent flow equations inside the pipe with RNG K-ε turbulence model are solved employing fluent software. The results show that the use of water/CNT nanofluid significantly increases the heat transfer coefficient of the convection. There is no such increase for water-aluminum oxide nanoparticles. If the volumetric percentage of the carbon nanotube increases, the rate of increase in the heat transfer coefficient and the flow pressure drop will increase. Therefore, the use of water/CNT nanofluid with lower volumetric percentages is better for improving the convective heat transfer. Also, by placing the barrier on the inner wall of the tube and stimulating the boundary layer, the heat transfer coefficient  thereafter increases in the excitement area. In the present study, the use of three obstacles behind each other has increased the average heat transfer coefficient by 16.7%.</Abstract>
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			<Object Type="keyword">
			<Param Name="value">nanoparticles</Param>
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			<Object Type="keyword">
			<Param Name="value">Carbon nanotube</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Aluminumoxide nanoparticles</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Heat transfer coefficient</Param>
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<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University (SRTTU)</PublisherName>
				<JournalTitle>Journal of Computational &amp; Applied Research in Mechanical Engineering (JCARME)</JournalTitle>
				<Issn>2228-7922</Issn>
				<Volume>12</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Bearing fault prognostics using Takagi-Sugeno of extended fuzzy with recursive least square algorithms</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>121</FirstPage>
			<LastPage>132</LastPage>
			<ELocationID EIdType="pii">1623</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jcarme.2021.6760.1869</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>H. O.</FirstName>
					<LastName>Omoregbee</LastName>
<Affiliation>Department of Mechanical Engineering, University of Lagos, Akoka, Lagos, Nigeria</Affiliation>

</Author>
<Author>
					<FirstName>M. U.</FirstName>
					<LastName>Olanipekun</LastName>
<Affiliation>Electrical Engineering Department, Tshwane University of Technology, eMalahleni Campus, South Africa</Affiliation>

</Author>
<Author>
					<FirstName>M. O.</FirstName>
					<LastName>Okwu</LastName>
<Affiliation>Mechanical Engineering Department, Federal University of Petroleum Resources, Effurun. Nigeria</Affiliation>

</Author>
<Author>
					<FirstName>B. A.</FirstName>
					<LastName>Edward</LastName>
<Affiliation>Mechanical Engineering Department, Federal University of Petroleum Resources, Effurun. Nigeria</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2020</Year>
					<Month>04</Month>
					<Day>15</Day>
				</PubDate>
			</History>
		<Abstract>This paper presents the detection of fault prognostics in bearings with the application of extended Takagi-Sugeno fuzzy recursive least square algorithms (exTSFRLSA). The nonlinear system is decomposed into a multi-model structure, consisting of linear models that are not inherently independent, due to the fuzzy regions defined in exTSFRLSA. The exTSFRLSA was developed to tune, adjust and adapt the parameters involved in the propagation model, as it tends to update itself with the availability of new data. This method is suitable for the online identification of systems because of its unsupervised learning pattern which dwells on a mechanism cantered on rule-based evolution. Scenarios considered for the rule-based modification and upgrade are quite diverse, thereby ensuring effective comparison of measured and predicted defect size. An estimation of the remaining useful life was determined successfully with the proposed method, showing that the system performance health indicator reflects bearing degradation, and it was concluded that exTSFRLSA can be used for fault prediction of bearing where rolling element  are involved, especially while its operation is associated with fluctuating speed and load conditions.</Abstract>
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			<Param Name="value">Prognostics</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Rolling element bearing</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Remaining useful life</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Extended Takagi Sugeno</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Fuzzy</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Recursive least squares method</Param>
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</Article>
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