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<ArticleSet>
<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Modeling of Diaphragm Dosing Pumps with Fluid-Structure Interaction Analysis</ArticleTitle>
<VernacularTitle>Numerical Modeling of Diaphragm Dosing Pumps with Fluid-Structure Interaction Analysis</VernacularTitle>
			<FirstPage>1461</FirstPage>
			<LastPage>1480</LastPage>
			<ELocationID EIdType="pii">4784</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.20658.7288</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Rafat</FirstName>
					<LastName>Mohammadi</LastName>
<Affiliation>Department of Mechanical Engineering, Faculty of Engineering, Arak University, Arak, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Arefe</FirstName>
					<LastName>Rabiee Kerahrudib</LastName>
<Affiliation>Department of Mechanical Engineering, Faculty of Engineering, Arak University, Arak, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Amiir</FirstName>
					<LastName>Ahmadi</LastName>
<Affiliation>Department of Mechanical Engineering, Faculty of Engineering, Arak University, Arak, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>10</Month>
					<Day>11</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, the performance of a diaphragm dosing pump of the injection odorizers is simulated with the fluid-structure interaction analysis. The simulation results are validated with experimental data and the largest relative error is 16% for the average flow rate. Performance simulation of the diaphragm pump for the diaphragm oscillation period of 1 second and three different diaphragm displacement amplitudes of 0.8, 0.5, and 0.2 mm, shows that as the amplitude increases, the fluid velocity and consequently the flow rate of the pump increases. The average flow rate of the pump in the mentioned amplitudes is equal to 0.002, 0.0013, and 0.0005 kg/s, respectively. As the amplitude increases from 0.2 to 0.8 mm, the maximum stress applied to the diaphragm increases from 32.2 to 99.2 MPa (equivalent to 208%). Also, the effect of diaphragm oscillation frequency on pump performance is investigated. The results show that the pump&#039;s flow rate directly and linearly relates to the diaphragm oscillation frequency. In contrast, the applied stress on the diaphragm is not frequency-dependent and in the same ratios of the period, the applied stress is almost constant. According to the results, if the pump amplitude is set to 0.5 mm and the frequency is 1.6 Hz, instead of operating at a diaphragm amplitude of 0.8 mm and a frequency of 1 Hz, the pump&#039;s flow rate will be the same. While the maximum amount of stress in the diaphragm will be reduced by about 30% and the probability of damage will be reduced.</Abstract>
			<OtherAbstract Language="FA">In this paper, the performance of a diaphragm dosing pump of the injection odorizers is simulated with the fluid-structure interaction analysis. The simulation results are validated with experimental data and the largest relative error is 16% for the average flow rate. Performance simulation of the diaphragm pump for the diaphragm oscillation period of 1 second and three different diaphragm displacement amplitudes of 0.8, 0.5, and 0.2 mm, shows that as the amplitude increases, the fluid velocity and consequently the flow rate of the pump increases. The average flow rate of the pump in the mentioned amplitudes is equal to 0.002, 0.0013, and 0.0005 kg/s, respectively. As the amplitude increases from 0.2 to 0.8 mm, the maximum stress applied to the diaphragm increases from 32.2 to 99.2 MPa (equivalent to 208%). Also, the effect of diaphragm oscillation frequency on pump performance is investigated. The results show that the pump&#039;s flow rate directly and linearly relates to the diaphragm oscillation frequency. In contrast, the applied stress on the diaphragm is not frequency-dependent and in the same ratios of the period, the applied stress is almost constant. According to the results, if the pump amplitude is set to 0.5 mm and the frequency is 1.6 Hz, instead of operating at a diaphragm amplitude of 0.8 mm and a frequency of 1 Hz, the pump&#039;s flow rate will be the same. While the maximum amount of stress in the diaphragm will be reduced by about 30% and the probability of damage will be reduced.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Diaphragm pumps</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Numerical modeling</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Fluid-Structure Interaction</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Dosing pumps</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4784_5dedb42b34e50082065a783265ce28a8.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Simulation of the Role of the Anti-Angiogenic Therapy in Fluid Flow Behavior and Macromolecule Transport into a Heterogeneous Solid Tumor</ArticleTitle>
<VernacularTitle>Simulation of the Role of the Anti-Angiogenic Therapy in Fluid Flow Behavior and Macromolecule Transport into a Heterogeneous Solid Tumor</VernacularTitle>
			<FirstPage>1481</FirstPage>
			<LastPage>1512</LastPage>
			<ELocationID EIdType="pii">4800</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.20938.7343</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mahya</FirstName>
					<LastName>Mohammadi</LastName>
<Affiliation>Department of Mechanical Engineering, K. N. Toosi University of Technology, Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Cyrus</FirstName>
					<LastName>Aghanajafi</LastName>
<Affiliation>Department of Mechanical Engineering, K. N. Toosi University of Technology, Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Majid</FirstName>
					<LastName>Soltani</LastName>
<Affiliation>Department of Mechanical Engineering, K. N. Toosi University of Technology, Tehran, Iran</Affiliation>
<Identifier Source="ORCID">0000-0003-0878-6274</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>12</Month>
					<Day>31</Day>
				</PubDate>
			</History>
		<Abstract>The present study develops a numerical approach based on the mathematical models governing the behavior of fluid flow and drug transport in tumors to investigate the delivery of a macromolecule under the effect of the vascular normalization into a non-uniform tumor, including different parts of a real solid tumor. In this study, different tumor sizes in the range of  are considered. The area under the curves of the drug average distribution and its deviation in the tumor site over time is studied as the amount of drug delivered and the uniformity of delivered drug to assess the quality of drug delivery. Results show that before and after normalization, the behaviors of interstitial fluid flow and the distribution of therapeutic agent concentration depend on tumor size. Normalization in all sizes reduces the interstitial fluid pressure, which this pressure drop increases as the tumor size reduces. Normalization improves antibody concentration distribution at different times depending on tumor size. However, from the point of view of the average spatiotemporal criterion, vascular normalization improves macromolecule delivery into the tumor site in  by increasing the distribution uniformity. This research, by discussing the mechanisms affecting normalization efficiency, can provide insights for in vivo and in vitro studies that address the combination of anti-angiogenic therapy and chemotherapy.</Abstract>
			<OtherAbstract Language="FA">The present study develops a numerical approach based on the mathematical models governing the behavior of fluid flow and drug transport in tumors to investigate the delivery of a macromolecule under the effect of the vascular normalization into a non-uniform tumor, including different parts of a real solid tumor. In this study, different tumor sizes in the range of  are considered. The area under the curves of the drug average distribution and its deviation in the tumor site over time is studied as the amount of drug delivered and the uniformity of delivered drug to assess the quality of drug delivery. Results show that before and after normalization, the behaviors of interstitial fluid flow and the distribution of therapeutic agent concentration depend on tumor size. Normalization in all sizes reduces the interstitial fluid pressure, which this pressure drop increases as the tumor size reduces. Normalization improves antibody concentration distribution at different times depending on tumor size. However, from the point of view of the average spatiotemporal criterion, vascular normalization improves macromolecule delivery into the tumor site in  by increasing the distribution uniformity. This research, by discussing the mechanisms affecting normalization efficiency, can provide insights for in vivo and in vitro studies that address the combination of anti-angiogenic therapy and chemotherapy.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Fluid flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Drug transport</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Non-uniform tumor</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Vascular normalization</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Combo-therapy</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4800_0c4a4df48a930b56e7d71ec5a34b8257.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Acoustic Simulation of Hot and Cold Flow mixing by a Lobed Mixer in a High Bypass Ratio Turbofan Engine</ArticleTitle>
<VernacularTitle>Acoustic Simulation of Hot and Cold Flow mixing by a Lobed Mixer in a High Bypass Ratio Turbofan Engine</VernacularTitle>
			<FirstPage>1513</FirstPage>
			<LastPage>1532</LastPage>
			<ELocationID EIdType="pii">4823</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.20701.7296</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Sadegh</FirstName>
					<LastName>Fazeli</LastName>
<Affiliation>Malek Ashtar University</Affiliation>

</Author>
<Author>
					<FirstName>Rouhollah</FirstName>
					<LastName>Khoshkhoo</LastName>
<Affiliation>Faculty of Mechanical Engineering, MUT</Affiliation>

</Author>
<Author>
					<FirstName>Alireza</FirstName>
					<LastName>Khoeini Poor Far</LastName>
<Affiliation>PhD of Mechanical Engineering, Maintenance Engineering Department, Mapna Turbine 
Engineering and Manufacturing Company (TOGA)</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>10</Month>
					<Day>23</Day>
				</PubDate>
			</History>
		<Abstract>Noise reduction laws for turbofan engines require effective configurations to reduce jet engine noise. Lobed mixers are known to be effective for noise reduction in high bypass ratio turbofan engines. In this study, a mixture of hot and cold flow is simulated in a lobed mixer for a high bypass ratio turbofan engine. Navier-Stokes equations are considered three-dimensional, compressible, steady, and turbulent. To solve the turbulent flow, the turbulent model has been used; besides, to investigate the acoustic power, the Broadband noise source model was applied. In this research, first, the simulation method was validated and the results were compared with the experimental data of previous studies. Then, the impact of the lobed mixer was investigated on mixing hot and cold flow and noise reduction in a high-bypass ratio turbofan engine. The results of this study show that the maximum acoustic power was obtained at about 72 dB at a distance of 14 meters from the nozzle, decreasing by moving away from the engine nozzle; also, the maximum amount of acoustic power in the central body at nozzle exit has decreased from about 90 dB to 72 dB. The maximum acoustic power was observed at about 95 dB on the mixer surface next to the central body flow. Finally, we can conclude that a mixture of flow reduces the acoustic power and improves its uniformity at the nozzle exit while increasing the acoustic power near the central body.</Abstract>
			<OtherAbstract Language="FA">Noise reduction laws for turbofan engines require effective configurations to reduce jet engine noise. Lobed mixers are known to be effective for noise reduction in high bypass ratio turbofan engines. In this study, a mixture of hot and cold flow is simulated in a lobed mixer for a high bypass ratio turbofan engine. Navier-Stokes equations are considered three-dimensional, compressible, steady, and turbulent. To solve the turbulent flow, the turbulent model has been used; besides, to investigate the acoustic power, the Broadband noise source model was applied. In this research, first, the simulation method was validated and the results were compared with the experimental data of previous studies. Then, the impact of the lobed mixer was investigated on mixing hot and cold flow and noise reduction in a high-bypass ratio turbofan engine. The results of this study show that the maximum acoustic power was obtained at about 72 dB at a distance of 14 meters from the nozzle, decreasing by moving away from the engine nozzle; also, the maximum amount of acoustic power in the central body at nozzle exit has decreased from about 90 dB to 72 dB. The maximum acoustic power was observed at about 95 dB on the mixer surface next to the central body flow. Finally, we can conclude that a mixture of flow reduces the acoustic power and improves its uniformity at the nozzle exit while increasing the acoustic power near the central body.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Lobed Mixer</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Turbofan Engine with High Bypass Ratio</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">numerical simulation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Acoustic</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4823_0f089a3bcf38d052f7882d12b3923a82.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Investigation of Internal Flow Transition Using Modified γ-Reθ Model</ArticleTitle>
<VernacularTitle>Numerical Investigation of Internal Flow Transition Using Modified γ-Reθ Model</VernacularTitle>
			<FirstPage>1533</FirstPage>
			<LastPage>1552</LastPage>
			<ELocationID EIdType="pii">4818</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.21138.7383</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mohamad Ali</FirstName>
					<LastName>Modaresi</LastName>
<Affiliation>Tarbiat Modares University, Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Ghassem</FirstName>
					<LastName>Heidarinejad</LastName>
<Affiliation>Faculty of Mechanical Engineering, Tarbiat Modares University, Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Reza</FirstName>
					<LastName>Maddahian</LastName>
<Affiliation>Faculty of Mechanical Engineering, Tarbiat Modares University, Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Bahar</FirstName>
					<LastName>Firoozabadi</LastName>
<Affiliation>Sharif University of Technology</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2022</Year>
					<Month>02</Month>
					<Day>22</Day>
				</PubDate>
			</History>
		<Abstract>The numerical investigation of Transition is one of the challenging issues in turbulence modeling. In the present study, the coefficients of the &lt;em&gt;γ&lt;/em&gt;-&lt;em&gt;Re&lt;sub&gt;θ&lt;/sub&gt;&lt;/em&gt; model are modified based on the physics of internal flow transition to capture the entrance length properly. To validate the model, the internal flow is simulated using six test cases. A 3D duct, two smooth axisymmetric pipes, a 3D stenosis pipe, two parallel plates, and the backward-facing step configurations are considered at different Reynolds numbers from 2´10&lt;sup&gt;3&lt;/sup&gt; to 3´10&lt;sup&gt;5&lt;/sup&gt;. The flow variables, including the average velocity field, friction factor, fully developed friction factor, and the reattachment length are compared against the experimental, theoretical and large eddy simulation results. By comparing the results of average velocity against the semi-empirical relations and experimental data using new coefficients, it is observed the model can estimate the entrance length in accordance with experiments. The earlier coefficients lead to a reduction of entrance length by increasing the Reynolds number. Furthermore, the error percentages reduce by more than 7.6 and 26.7 percent using new coefficients rather than earlier models for fully developed friction factor and reattachment length, respectively.</Abstract>
			<OtherAbstract Language="FA">The numerical investigation of Transition is one of the challenging issues in turbulence modeling. In the present study, the coefficients of the &lt;em&gt;γ&lt;/em&gt;-&lt;em&gt;Re&lt;sub&gt;θ&lt;/sub&gt;&lt;/em&gt; model are modified based on the physics of internal flow transition to capture the entrance length properly. To validate the model, the internal flow is simulated using six test cases. A 3D duct, two smooth axisymmetric pipes, a 3D stenosis pipe, two parallel plates, and the backward-facing step configurations are considered at different Reynolds numbers from 2´10&lt;sup&gt;3&lt;/sup&gt; to 3´10&lt;sup&gt;5&lt;/sup&gt;. The flow variables, including the average velocity field, friction factor, fully developed friction factor, and the reattachment length are compared against the experimental, theoretical and large eddy simulation results. By comparing the results of average velocity against the semi-empirical relations and experimental data using new coefficients, it is observed the model can estimate the entrance length in accordance with experiments. The earlier coefficients lead to a reduction of entrance length by increasing the Reynolds number. Furthermore, the error percentages reduce by more than 7.6 and 26.7 percent using new coefficients rather than earlier models for fully developed friction factor and reattachment length, respectively.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Internal Flow</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">γ-Reθ transitional model</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Reynolds-averaged Navier–Stokes equations</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">numerical simulation</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4818_e88f243bf341ded9b4ced444795c3f17.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Advanced Exergy Investigation of Combined Cycle of Helium Reactor Gas Turbine with Organic Rankine Cycle</ArticleTitle>
<VernacularTitle>Advanced Exergy Investigation of Combined Cycle of Helium Reactor Gas Turbine with Organic Rankine Cycle</VernacularTitle>
			<FirstPage>1553</FirstPage>
			<LastPage>1574</LastPage>
			<ELocationID EIdType="pii">4795</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.20637.7284</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mohsen</FirstName>
					<LastName>Fallah</LastName>
<Affiliation>Mechanical engineering group, Azarbaijan Shahid Madani University</Affiliation>

</Author>
<Author>
					<FirstName>Zahra</FirstName>
					<LastName>Mohammadi</LastName>
<Affiliation>Tabriz university</Affiliation>

</Author>
<Author>
					<FirstName>Seyed Mohammad</FirstName>
					<LastName>Seyed Mahmoudi</LastName>
<Affiliation>Tabriz university</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>10</Month>
					<Day>06</Day>
				</PubDate>
			</History>
		<Abstract>&lt;span style=&quot;letter-spacing: .05pt;&quot;&gt;In this work, the combined cycle of a helium reactor gas turbine with an organic Rankine cycle is studied and compared from the perspective of conventional and advanced exergy analysis. Using Equation solving engineering software, modeling of this cycle has been done and the results of conventional energy and exergy analysis have been obtained. Then, to determine the appropriate prioritization of cycle component improvement from the perspective of advanced exergy analysis has been studied. In fact, advanced exergy analysis provides accurate information about the real potential for system performance improvement by dividing the exergy destruction of each component into endogenous, exogenous, avoidable, and unavoidable components. The results of advanced exergy analysis show that by modifying and upgrading the components of the system, 19.1% of the total exergy destruction of the system can be reduced. According to the advanced exergy analysis, the improvement priority belongs to the compressor and then to the reactor and gas turbine. However, from the conventional exergy analysis, the reactor&#039;s exergy destruction is greater than that of the compressor and the priority is on the reactor. In addition, based on the prioritization of advanced exergy analysis, it is possible to increase the cycle exergy efficiency from 75.21% to 82.51% and the cycle energy efficiency from 51% to 56.22%.&lt;/span&gt;</Abstract>
			<OtherAbstract Language="FA">&lt;span style=&quot;letter-spacing: .05pt;&quot;&gt;In this work, the combined cycle of a helium reactor gas turbine with an organic Rankine cycle is studied and compared from the perspective of conventional and advanced exergy analysis. Using Equation solving engineering software, modeling of this cycle has been done and the results of conventional energy and exergy analysis have been obtained. Then, to determine the appropriate prioritization of cycle component improvement from the perspective of advanced exergy analysis has been studied. In fact, advanced exergy analysis provides accurate information about the real potential for system performance improvement by dividing the exergy destruction of each component into endogenous, exogenous, avoidable, and unavoidable components. The results of advanced exergy analysis show that by modifying and upgrading the components of the system, 19.1% of the total exergy destruction of the system can be reduced. According to the advanced exergy analysis, the improvement priority belongs to the compressor and then to the reactor and gas turbine. However, from the conventional exergy analysis, the reactor&#039;s exergy destruction is greater than that of the compressor and the priority is on the reactor. In addition, based on the prioritization of advanced exergy analysis, it is possible to increase the cycle exergy efficiency from 75.21% to 82.51% and the cycle energy efficiency from 51% to 56.22%.&lt;/span&gt;</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">advanced exergy analysis</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Endogenous/exogenous exergy destruction</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">avoidable/unavoidable exergy destruction</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4795_adf7ee2dcf142b0e11888e72b43fcb75.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigating the Effect of Mesh Structure and Mesh Retaining Module on the Rate of Fog Harvesting</ArticleTitle>
<VernacularTitle>Investigating the Effect of Mesh Structure and Mesh Retaining Module on the Rate of Fog Harvesting</VernacularTitle>
			<FirstPage>1575</FirstPage>
			<LastPage>1586</LastPage>
			<ELocationID EIdType="pii">4799</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.20812.7320</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Amir Reza</FirstName>
					<LastName>Mohebi</LastName>
<Affiliation>Faculty of Chemical Engineering, Amirkabir University of Technology, Tehran, Iran.</Affiliation>

</Author>
<Author>
					<FirstName>Mehrdad</FirstName>
					<LastName>Mozaffarian</LastName>
<Affiliation>Faculty of Chemical Engineering, Amirkabir University of Technology, Tehran, Iran.</Affiliation>
<Identifier Source="ORCID">0000-0003-1030-2953</Identifier>

</Author>
<Author>
					<FirstName>Mohammad</FirstName>
					<LastName>Karimi</LastName>
<Affiliation>Faculty of Textile Engineering, Amirkabir University of Technology, Tehran, Iran.</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>11</Month>
					<Day>24</Day>
				</PubDate>
			</History>
		<Abstract>Nowadays, the impact of water scarcity is felt more than ever due to population growth, environmental changes, and increased industrial as well as agricultural developments.  Thus, it is imperative to harvest water from every available source such as fog. The process of harvesting water from fog which is a cost-effective method has attracted the attention of many researchers trying to increase the efficiency of this method in various ways. In this research, a practical test system is presented to investigate the influence of the mesh and the mesh retaining module on the rate of fog harvesting. 6 sets of modules and meshes were exposed to the fog flow and after taking the results, the most effective factor between the meshes and the module was determined. All factors affecting fog harvesting were kept constant during the test, and only the effects of the mesh and module were examined. Teflon yarns mesh which increased the fog harvesting by 23 to 77%, was chosen as the best mesh, while the Modular Funnel-Large Fog Collector module which increased the rate of fog collection by 7 to 9 times was considered as the best module. This unique effectiveness should be attributed to the aerodynamic property of the MF-LFC module, which uses the rate of fog flow effectively in order to increase water harvesting.</Abstract>
			<OtherAbstract Language="FA">Nowadays, the impact of water scarcity is felt more than ever due to population growth, environmental changes, and increased industrial as well as agricultural developments.  Thus, it is imperative to harvest water from every available source such as fog. The process of harvesting water from fog which is a cost-effective method has attracted the attention of many researchers trying to increase the efficiency of this method in various ways. In this research, a practical test system is presented to investigate the influence of the mesh and the mesh retaining module on the rate of fog harvesting. 6 sets of modules and meshes were exposed to the fog flow and after taking the results, the most effective factor between the meshes and the module was determined. All factors affecting fog harvesting were kept constant during the test, and only the effects of the mesh and module were examined. Teflon yarns mesh which increased the fog harvesting by 23 to 77%, was chosen as the best mesh, while the Modular Funnel-Large Fog Collector module which increased the rate of fog collection by 7 to 9 times was considered as the best module. This unique effectiveness should be attributed to the aerodynamic property of the MF-LFC module, which uses the rate of fog flow effectively in order to increase water harvesting.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Fog Harvesting</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Hexagonal Mesh</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Rachel Mesh</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Double Cylinderical Module</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Modular Funnel-Large Fog Collector Module</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4799_fecc3a370a23d13b1cf91ac3c1e1ca92.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Investigation of Steam Methane Reforming over Ni- and Rh-based Catalysts to Produce Hydrogen, Syngas and Reduce Surface Coverage</ArticleTitle>
<VernacularTitle>Numerical Investigation of Steam Methane Reforming over Ni- and Rh-based Catalysts to Produce Hydrogen, Syngas and Reduce Surface Coverage</VernacularTitle>
			<FirstPage>1587</FirstPage>
			<LastPage>1606</LastPage>
			<ELocationID EIdType="pii">4851</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.20851.7331</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Ali</FirstName>
					<LastName>Saeedi</LastName>
<Affiliation>University of Birjand</Affiliation>
<Identifier Source="ORCID">0000-0003-1950-6098</Identifier>

</Author>
<Author>
					<FirstName>Fatemeh</FirstName>
					<LastName>Zangooei</LastName>
<Affiliation>Department of Mechanical Engineering, University of Birjand</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>12</Month>
					<Day>15</Day>
				</PubDate>
			</History>
		<Abstract>&lt;span style=&quot;letter-spacing: .05pt;&quot;&gt;Steam methane reforming has the highest efficiency compared with other hydrogen production ways. Temperature, pressure, steam to methane ratio, and catalyst play essential roles in the Steam methane reforming process. In this paper, a numerical simulation method is performed using Cantera software in Python programming language to produce syngas and hydrogen in the Steam methane reforming process over Nickel- and Rhodium-based catalysts. The simulation is done in 600-1300K, steam to methane ratio of 2-4, and pressure of 0.25-4 bars to determine a suitable catalyst and the best range to produce hydrogen and syngas and to reduce Carbone surface coverage. The results demonstrate that the preferred ranges for hydrogen production over Nickel and Rhodium are temperature between 1000 to 1100K, pressure 1 to 2 bars, and steam to methane ratio 2.5 to 3 and 3 to 3.5 for each, respectively. The appropriate ranges to produce syngas over Nickel and Rhodium are temperature 1200-1300K and 1100-1300K, steam to methane ratio 2.5-3 and 3-3.5, respectively, and the pressure is suggested between 1-2 bars. However, Rhodium in the same condition is more active than Nickel, while the surface coverage formation is lower over Nickel than Rhodium. Therefore, Nickel is proposed to produce hydrogen via Steam Methane Reforming.&lt;/span&gt;</Abstract>
			<OtherAbstract Language="FA">&lt;span style=&quot;letter-spacing: .05pt;&quot;&gt;Steam methane reforming has the highest efficiency compared with other hydrogen production ways. Temperature, pressure, steam to methane ratio, and catalyst play essential roles in the Steam methane reforming process. In this paper, a numerical simulation method is performed using Cantera software in Python programming language to produce syngas and hydrogen in the Steam methane reforming process over Nickel- and Rhodium-based catalysts. The simulation is done in 600-1300K, steam to methane ratio of 2-4, and pressure of 0.25-4 bars to determine a suitable catalyst and the best range to produce hydrogen and syngas and to reduce Carbone surface coverage. The results demonstrate that the preferred ranges for hydrogen production over Nickel and Rhodium are temperature between 1000 to 1100K, pressure 1 to 2 bars, and steam to methane ratio 2.5 to 3 and 3 to 3.5 for each, respectively. The appropriate ranges to produce syngas over Nickel and Rhodium are temperature 1200-1300K and 1100-1300K, steam to methane ratio 2.5-3 and 3-3.5, respectively, and the pressure is suggested between 1-2 bars. However, Rhodium in the same condition is more active than Nickel, while the surface coverage formation is lower over Nickel than Rhodium. Therefore, Nickel is proposed to produce hydrogen via Steam Methane Reforming.&lt;/span&gt;</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Hydrogen Production</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Steam Methane Reforming</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">numerical simulation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Catalysts</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4851_5d40954183d62a82257835477ccad3d2.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Study of Catalyst Bed Performance of a Monopropellant Thruster Under Influence of Porosity Coefficient</ArticleTitle>
<VernacularTitle>Numerical Study of Catalyst Bed Performance of a Monopropellant Thruster Under Influence of Porosity Coefficient</VernacularTitle>
			<FirstPage>1607</FirstPage>
			<LastPage>1622</LastPage>
			<ELocationID EIdType="pii">4837</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.20741.7305</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Mohammadreza</FirstName>
					<LastName>Salimi</LastName>
<Affiliation>Ari</Affiliation>

</Author>
<Author>
					<FirstName>Hadiseh</FirstName>
					<LastName>Karimaei</LastName>
<Affiliation>Ari</Affiliation>

</Author>
<Author>
					<FirstName>Mostafa</FirstName>
					<LastName>Gholampour Yazdi</LastName>
<Affiliation>Ari</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>11</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>Hydrazine monopropellant thrusters are commonly used in the situation control and orbital transmission systems of satellites and space crafts. In these thrusters, hydrazine is decomposed into a hot gas product after passing through the catalyst bed during an exothermic reaction. The decomposition chamber of a monopropellant thruster is numerically modeled at the pore scale. Then the effect of catalyst bed porosity coefficient, which is the most important parameter affecting the performance of the decomposition chamber, is investigated. Simulations were performed in two-dimensional axial symmetry as the steady flow in the gas phase. Catalyst granules with an average diameter of 1 mm with three porosity coefficients of 0.4, 0.55, and 0.65 have been considered and the inlet pressure of the decomposition chamber has been considered to 15 bar. The results showed that the porosity coefficient has a very significant effect on the performance of the catalyst bed so that by decreasing this coefficient, the decomposition of hydrazine increases, the bed temperature, and outer wall temperature increase, and the mass flow rate decreases. Reducing the bed porosity coefficient from 0.65 to 0.4 causes about a 40% drop in the bed pressure compared to the initial inlet pressure and also about a 40% reduction in the mass flow rate through the bed. Therefore, the study of this parameter can greatly help the researchers in determining and optimizing the efficiency of the decomposition chamber.</Abstract>
			<OtherAbstract Language="FA">Hydrazine monopropellant thrusters are commonly used in the situation control and orbital transmission systems of satellites and space crafts. In these thrusters, hydrazine is decomposed into a hot gas product after passing through the catalyst bed during an exothermic reaction. The decomposition chamber of a monopropellant thruster is numerically modeled at the pore scale. Then the effect of catalyst bed porosity coefficient, which is the most important parameter affecting the performance of the decomposition chamber, is investigated. Simulations were performed in two-dimensional axial symmetry as the steady flow in the gas phase. Catalyst granules with an average diameter of 1 mm with three porosity coefficients of 0.4, 0.55, and 0.65 have been considered and the inlet pressure of the decomposition chamber has been considered to 15 bar. The results showed that the porosity coefficient has a very significant effect on the performance of the catalyst bed so that by decreasing this coefficient, the decomposition of hydrazine increases, the bed temperature, and outer wall temperature increase, and the mass flow rate decreases. Reducing the bed porosity coefficient from 0.65 to 0.4 causes about a 40% drop in the bed pressure compared to the initial inlet pressure and also about a 40% reduction in the mass flow rate through the bed. Therefore, the study of this parameter can greatly help the researchers in determining and optimizing the efficiency of the decomposition chamber.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Hydrazine thruster</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Catalyst bed</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Decomposition chamber</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Porosity coefficient</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Pore Scale</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4837_274a10ffa06e434f2a94df765cac6bf4.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigation of Unsteady Thermal Performance of Multi-Effect Desalination with Thermal Vapor Compression</ArticleTitle>
<VernacularTitle>Investigation of Unsteady Thermal Performance of Multi-Effect Desalination with Thermal Vapor Compression</VernacularTitle>
			<FirstPage>1623</FirstPage>
			<LastPage>1646</LastPage>
			<ELocationID EIdType="pii">4831</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.20921.7337</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Sobhan</FirstName>
					<LastName>Khajehnamaghi</LastName>
<Affiliation>Shahroud University of Technology, Shahroud, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Mohsen</FirstName>
					<LastName>Nazari</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Mostafa</FirstName>
					<LastName>Nazari</LastName>
<Affiliation>Shahrood Univ.</Affiliation>

</Author>
<Author>
					<FirstName>Omid</FirstName>
					<LastName>Pilevar</LastName>
<Affiliation>SUT</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>12</Month>
					<Day>24</Day>
				</PubDate>
			</History>
		<Abstract>Due to the high use of thermal desalination plants, there is a great tendency to simulate their behavior. Most of the research is focused on modeling steady behavior, but to design control systems and evaluate their performance, we also need to study unsteady behavior. Also, few researchers have studied the system shutdown. In this paper, steady and unsteady modeling of an industrial multi-effect desalination plant with four effects, one condenser, and a Thermo compressor has been studied. The variable-step, variable-order method has been used to solve differential equations. Each evaporator is divided into three phases of vapor, tubes, and brine then the equations of mass and energy conservation are used. Results have been validated with real plant data. The variables of temperature, vapor flow rate, brine flow rate and brine level were studied in unsteady modeling in starting, shutting down, and steady-state conditions. It was found that the largest change in the brine flow rate after shutting down is in the last effect, which increases by 42%. Also, the biggest change in the level of the brine is in the first effect, which after 800 seconds will reach 11 times the steady state that will cause the flooding phenomenon.</Abstract>
			<OtherAbstract Language="FA">Due to the high use of thermal desalination plants, there is a great tendency to simulate their behavior. Most of the research is focused on modeling steady behavior, but to design control systems and evaluate their performance, we also need to study unsteady behavior. Also, few researchers have studied the system shutdown. In this paper, steady and unsteady modeling of an industrial multi-effect desalination plant with four effects, one condenser, and a Thermo compressor has been studied. The variable-step, variable-order method has been used to solve differential equations. Each evaporator is divided into three phases of vapor, tubes, and brine then the equations of mass and energy conservation are used. Results have been validated with real plant data. The variables of temperature, vapor flow rate, brine flow rate and brine level were studied in unsteady modeling in starting, shutting down, and steady-state conditions. It was found that the largest change in the brine flow rate after shutting down is in the last effect, which increases by 42%. Also, the biggest change in the level of the brine is in the first effect, which after 800 seconds will reach 11 times the steady state that will cause the flooding phenomenon.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Desalination plants</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Unsteady behavior</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Shut down</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Variable-step and variable-order</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Flooding phenomenon</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4831_f720ec3e5486f090fd382b68e230b435.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Numerical Investigation of Effective Parameters in Radiant Heat Transfer of Oxyfuel Combustion Process of Swirling Gas Furnaces</ArticleTitle>
<VernacularTitle>Numerical Investigation of Effective Parameters in Radiant Heat Transfer of Oxyfuel Combustion Process of Swirling Gas Furnaces</VernacularTitle>
			<FirstPage>1647</FirstPage>
			<LastPage>1672</LastPage>
			<ELocationID EIdType="pii">4824</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.20957.7347</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Saman</FirstName>
					<LastName>Kasmaiee</LastName>
<Affiliation>Turbulence and Two Phase Flow Laboratory, 
Amirkabir University of Technology (Tehran Polytechnic) Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Sahar</FirstName>
					<LastName>Noori</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>Siroos</FirstName>
					<LastName>Kasmaiee</LastName>
<Affiliation>Turbulence and Two Phase Flow Laboratory, 
Amirkabir University of Technology (Tehran Polytechnic) Tehran, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2022</Year>
					<Month>01</Month>
					<Day>04</Day>
				</PubDate>
			</History>
		<Abstract>&lt;span style=&quot;letter-spacing: .05pt;&quot;&gt;In gas furnaces based on oxyfuel combustion, radiative heat transfer is an important part of the heat flux and plays an important role in the flame temperature distribution. Different parameters affect the radiant heat transfer of furnaces. In this study, the effect of wall emissivity coefficient, oxidizer compound, and inlet flow swirl number in a Harwell gas furnace was investigated.&lt;/span&gt; &lt;span style=&quot;letter-spacing: .05pt;&quot;&gt;k-ε standard, discrete ordinate, and eddy dissipation model were utilized to model turbulence, radiation, and combustion process, respectively. The radiative properties of the gaseous medium were determined using the weighted-sum-of-gray-gases model. The results showed that with increasing the swirl number, the maximum flame temperature moves upwards and approaches the inlet. This causes the heat flux of the walls to increase and the axial heat flux to decrease. By changing the oxidizer composition, the radiant activity of the gaseous medium changes. This causes a change in the temperature distribution in the whole field and axial and wall heat fluxes. The use of nitrogen in the oxidizer causes the maximum temperature to move towards the walls, while the use of carbon dioxide causes the flame to concentrate in the central axis, although the increase of the mass percentage of oxygen in the oxidizer improves flame diffusion. Increasing the wall emissivity coefficient causes the flame to become more concentrated and its maximum temperature to move upwards.&lt;/span&gt;</Abstract>
			<OtherAbstract Language="FA">&lt;span style=&quot;letter-spacing: .05pt;&quot;&gt;In gas furnaces based on oxyfuel combustion, radiative heat transfer is an important part of the heat flux and plays an important role in the flame temperature distribution. Different parameters affect the radiant heat transfer of furnaces. In this study, the effect of wall emissivity coefficient, oxidizer compound, and inlet flow swirl number in a Harwell gas furnace was investigated.&lt;/span&gt; &lt;span style=&quot;letter-spacing: .05pt;&quot;&gt;k-ε standard, discrete ordinate, and eddy dissipation model were utilized to model turbulence, radiation, and combustion process, respectively. The radiative properties of the gaseous medium were determined using the weighted-sum-of-gray-gases model. The results showed that with increasing the swirl number, the maximum flame temperature moves upwards and approaches the inlet. This causes the heat flux of the walls to increase and the axial heat flux to decrease. By changing the oxidizer composition, the radiant activity of the gaseous medium changes. This causes a change in the temperature distribution in the whole field and axial and wall heat fluxes. The use of nitrogen in the oxidizer causes the maximum temperature to move towards the walls, while the use of carbon dioxide causes the flame to concentrate in the central axis, although the increase of the mass percentage of oxygen in the oxidizer improves flame diffusion. Increasing the wall emissivity coefficient causes the flame to become more concentrated and its maximum temperature to move upwards.&lt;/span&gt;</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Combustion</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Gas furnace</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Oxidyfuel</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Radiation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Swirl number</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4824_2edfeadfe636973b42d7b6ac315b896c.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Development and Analysis of a Novel Multi-Generation System Fueled by Biogas with Smart Heat Recovery</ArticleTitle>
<VernacularTitle>Development and Analysis of a Novel Multi-Generation System Fueled by Biogas with Smart Heat Recovery</VernacularTitle>
			<FirstPage>1673</FirstPage>
			<LastPage>1700</LastPage>
			<ELocationID EIdType="pii">4820</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.20600.7269</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Maryam</FirstName>
					<LastName>Hassanzadeh</LastName>
<Affiliation>UMA</Affiliation>

</Author>
<Author>
					<FirstName>Hadi</FirstName>
					<LastName>Ghaebi</LastName>
<Affiliation>محقق اردبیلی-فنی و مهندسی- مهندسی مکانیک</Affiliation>

</Author>
<Author>
					<FirstName>Milad</FirstName>
					<LastName>Fili</LastName>
<Affiliation>Mechanical Engineering Department</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2021</Year>
					<Month>09</Month>
					<Day>27</Day>
				</PubDate>
			</History>
		<Abstract>This paper presents a novel multi-generation system based on biogas fuel for simultaneous production of goods such as electricity, cooling, freshwater, and hydrogen using smart heat recovery of combustion gases. The performance of the proposed system is investigated in terms of the first and second laws of thermodynamics. Also, to acquire a comprehensive evaluation of operation costs, an exergoeconomic analysis has been performed. Furthermore, a comprehensive parametric study has been conducted to understand the behavior of the system performance parameters with the design parameters. In the following, to show the superiority of using a Stirling engine, the investigation of the present study is performed under two different scenarios. The proposed system could produce 986 kW, 137.5 kW, 8.39 m&lt;sup&gt;3&lt;/sup&gt;/h, and 2.96 kg/h, net output electricity, cooling load, distilled water, and hydrogen while working with the Stirling engine. In this case, the energy and exergy efficiencies of the proposed system are obtained at 37.3% and 32.08%, which are improved by about 2.96% and 7.89%, respectively. In terms of cost metrics, the total unit cost of the products is about 0.1086$/kWh which has increased by 8.1% compared to the non-sterling engine mode.</Abstract>
			<OtherAbstract Language="FA">This paper presents a novel multi-generation system based on biogas fuel for simultaneous production of goods such as electricity, cooling, freshwater, and hydrogen using smart heat recovery of combustion gases. The performance of the proposed system is investigated in terms of the first and second laws of thermodynamics. Also, to acquire a comprehensive evaluation of operation costs, an exergoeconomic analysis has been performed. Furthermore, a comprehensive parametric study has been conducted to understand the behavior of the system performance parameters with the design parameters. In the following, to show the superiority of using a Stirling engine, the investigation of the present study is performed under two different scenarios. The proposed system could produce 986 kW, 137.5 kW, 8.39 m&lt;sup&gt;3&lt;/sup&gt;/h, and 2.96 kg/h, net output electricity, cooling load, distilled water, and hydrogen while working with the Stirling engine. In this case, the energy and exergy efficiencies of the proposed system are obtained at 37.3% and 32.08%, which are improved by about 2.96% and 7.89%, respectively. In terms of cost metrics, the total unit cost of the products is about 0.1086$/kWh which has increased by 8.1% compared to the non-sterling engine mode.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Gas turbine</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Biogas</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">west heat recovery</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">multi-generation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Stirling Engine</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4820_79cc30c73507cfc25d20fe7f7bcfd91b.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>Amirkabir University of Technology</PublisherName>
				<JournalTitle>Amirkabir Journal of Mechanical Engineering</JournalTitle>
				<Issn>2008-6032</Issn>
				<Volume>54</Volume>
				<Issue>7</Issue>
				<PubDate PubStatus="epublish">
					<Year>2022</Year>
					<Month>09</Month>
					<Day>23</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Energy Harvesting from Pool Boiling Using Electromagnetic Induction: Experimental Study and Numerical Simulation</ArticleTitle>
<VernacularTitle>Energy Harvesting from Pool Boiling Using Electromagnetic Induction: Experimental Study and Numerical Simulation</VernacularTitle>
			<FirstPage>1701</FirstPage>
			<LastPage>1716</LastPage>
			<ELocationID EIdType="pii">4856</ELocationID>
			
<ELocationID EIdType="doi">10.22060/mej.2022.21002.7358</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Rasool</FirstName>
					<LastName>Maroofiazar</LastName>
<Affiliation>Department of Mechanical Engineering, Faculty of Engineering, University of Maragheh, Maragheh, Iran</Affiliation>
<Identifier Source="ORCID">0000-0002-0746-4612</Identifier>

</Author>
<Author>
					<FirstName>Maziar</FirstName>
					<LastName>Fahimi Farzam</LastName>
<Affiliation>Department of Civil Engineering, Faculty of Engineering, University of Maragheh, Maragheh, Iran.</Affiliation>
<Identifier Source="ORCID">0000-0001-9635-8186</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2022</Year>
					<Month>01</Month>
					<Day>17</Day>
				</PubDate>
			</History>
		<Abstract>&lt;span style=&quot;letter-spacing: .05pt;&quot;&gt;In this study, a method has been proposed for energy harvesting from waste heat. A magnet was floated on the liquid in the coiled container and the system was placed on the heat source. By pool boiling of the liquid and according to Faraday&#039;s induction law, the voltage was induced in the coil by the movement of the magnet. Excess temperature, dimensions of the container, liquid height in the container, and the frame shape and diameter have been selected as effective parameters. Effects of these parameters on peak-to-peak voltage and root mean square voltage have been investigated experimentally. Obtained results showed that the maximum energy was harvested at higher values of excess temperature, liquid height, coil turn, and frame diameter with a spherical frame shape. The highest measured parameters were 532 mV and 95.65 mV for &lt;em&gt;Vpp&lt;/em&gt; and &lt;em&gt;Vrms&lt;/em&gt;, respectively. In the second part, the numerical method is used to simulate the proposed system. The effect of various parameters on interface characteristics has been investigated. The results showed that the trend of changes in the interface parameters, including its pressure and height, were consistent with experimental data. Therefore, this method can be used to design and predict the performance of the energy harvester.&lt;/span&gt;</Abstract>
			<OtherAbstract Language="FA">&lt;span style=&quot;letter-spacing: .05pt;&quot;&gt;In this study, a method has been proposed for energy harvesting from waste heat. A magnet was floated on the liquid in the coiled container and the system was placed on the heat source. By pool boiling of the liquid and according to Faraday&#039;s induction law, the voltage was induced in the coil by the movement of the magnet. Excess temperature, dimensions of the container, liquid height in the container, and the frame shape and diameter have been selected as effective parameters. Effects of these parameters on peak-to-peak voltage and root mean square voltage have been investigated experimentally. Obtained results showed that the maximum energy was harvested at higher values of excess temperature, liquid height, coil turn, and frame diameter with a spherical frame shape. The highest measured parameters were 532 mV and 95.65 mV for &lt;em&gt;Vpp&lt;/em&gt; and &lt;em&gt;Vrms&lt;/em&gt;, respectively. In the second part, the numerical method is used to simulate the proposed system. The effect of various parameters on interface characteristics has been investigated. The results showed that the trend of changes in the interface parameters, including its pressure and height, were consistent with experimental data. Therefore, this method can be used to design and predict the performance of the energy harvester.&lt;/span&gt;</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Energy harvesting</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Boiling</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Faraday's induction law</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Magnet</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">coil</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://mej.aut.ac.ir/article_4856_06f7c042b76e4b04f698c75b7b2777ea.pdf</ArchiveCopySource>
</Article>
</ArticleSet>
