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<title> Iranian Journal of Materials Science and Engineering </title>
<link>http:// ijmse.iust.ac.ir</link>
<description>Iranian Journal of Materials Science and Engineering - Journal articles for year 2026, Volume 23, Number 3</description>
<generator>Yektaweb Collection - https://yektaweb.com</generator>
<language>en</language>
<pubDate>2026/9/10</pubDate>

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						<title>Electrochemical Properties for BaSr1-xGdxCo2O5+δ and Ba0.5Sr0.5-xGdxCoO3-δ as a Cathode for Intermediate-Temperature Solid Oxide Fuel Cells</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4528&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;span style=&quot;font-size:12pt&quot;&gt;&lt;span style=&quot;line-height:200%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;&lt;span style=&quot;font-size:10.0pt&quot;&gt;&lt;span style=&quot;line-height:200%&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;The structural and electrochemical properties of Gd-doped perovskite oxides were investigated to improve the performance of solid oxide fuel cell (SOFC) cathodes. Ba&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;0.5&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;Sr&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;0.5-x&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;Gd&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;x&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;CoO&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;3-&amp;delta;&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; and BaSr&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;1-x&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;Gd&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;x&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;Co&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;2&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;O&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;5+&amp;delta;&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; (BSGC) compounds were synthesized via a &lt;/span&gt;&lt;strong&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;sol&amp;ndash;gel thermolysis&lt;/span&gt;&lt;/strong&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; method to elucidate the effects of Gd incorporation on crystal structure, microstructure, and electrochemical activity. &lt;/span&gt;&lt;strong&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;X-ray diffraction (XRD)&lt;/span&gt;&lt;/strong&gt;&lt;b&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; &lt;/span&gt;&lt;/b&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;and &lt;/span&gt;&lt;strong&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;scanning electron microscopy (SEM)&lt;/span&gt;&lt;/strong&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; confirmed the coexistence of simple and double perovskite phases, with Gd substitution leading to finer grains (down to 0.4 &lt;/span&gt;&lt;span style=&quot;background:yellow&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;&amp;plusmn; 0.14&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; &amp;mu;m) and improved phase homogeneity. &lt;/span&gt;&lt;strong&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;Area-specific resistance (ASR)&lt;/span&gt;&lt;/strong&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; and conductivity measurements revealed a strong structure&amp;ndash;performance relationship. The optimal composition, Ba&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;0.5&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;Sr&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;0.3&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;Gd&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;0.2&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;CoO&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;3-&amp;delta;&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;, exhibited &lt;/span&gt;&lt;span style=&quot;background:yellow&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;an exceptionally low ASR of &lt;/span&gt;&lt;strong&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;0.12 &amp;Omega; cm&amp;sup2;&lt;/span&gt;&lt;/strong&gt;&lt;b&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; &lt;/span&gt;&lt;/b&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;at 700 &amp;deg;C which further decreased to a minimum of 0.04 &lt;/span&gt;&lt;strong&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;&amp;Omega; cm&amp;sup2;&lt;/span&gt;&lt;/strong&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; at 850 &amp;deg;C, significantly&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; outperforming GdBaCo&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;2&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;O&lt;/span&gt;&lt;sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;5+&amp;delta;&lt;/span&gt;&lt;/sub&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; (GBCO), (1.76 &amp;Omega; cm&amp;sup2;). These findings demonstrate that rational structural design through rare-earth doping effectively enhances oxygen transport and electrochemical activity, providing a promising pathway for high-performance intermediate-temperature SOFC cathodes.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;</description>
						<author>Sara Tafaroji</author>
						<category></category>
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						<title>Thermomechanical Analysis and Optimization of Residual Stresses in SS316L Components Fabricated by Directed Energy Deposition</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4534&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;span style=&quot;font-size:12pt&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;The Directed Energy Deposition (DED) process is very sensitive to thermal environments, tends to produce residual stresses and geometric distortion. It is important to understand the influence of processing parameters on these effects in order to enhance build quality. The objective of this study is to control residual stress and distortion in the DED process by investigating baseplate thickness, &lt;a name=&quot;_Hlk202300610&quot;&gt;number of layers deposited before laser interruption&lt;/a&gt;, dwell time, and laser power by a full factorial experiment design. The numerical results were validated by experimental measurement of residual stress using the X-ray diffraction (XRD) technique. The optimized processing conditions resulted in a 43% reduction in residual stress and a 33% decrease in dimensional distortion compared to the baseline setup. Among the four factors, baseplate thickness had the most significant effect, whereas dwell time had the least impact. To the best of the authors&amp;rsquo; knowledge, the combined effect of baseplate thickness, dwell time, number of layers deposited before laser interruption, and laser power on residual stress and distortion in DED has not been previously investigated. The findings of this study provide a mathematical basis for future research aimed at optimizing process and material parameters in DED process.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br&gt;
&amp;nbsp;</description>
						<author>Farnoosh Turki</author>
						<category></category>
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						<title>Effect of Aging Duration on Mineral Composition, Microstructure, and Texture in a Malachite based Co precipitate and its Composite (Metallic) Oxidic Derivatives</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4548&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;span style=&quot;font-size:11pt&quot;&gt;&lt;span style=&quot;line-height:200%&quot;&gt;&lt;span style=&quot;font-family:Calibri,sans-serif&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;This study deals with the dependence of mineral, microstructural, and textural properties on the duration of the indispensable yet easily controlled step of aging. For this purpose, a set of Cu/Zn/Al precursors were synthesized using a conventional constant‑pH method. The precipitates were aged for three different durations of zero, two, and four hours. The obtained precipitates, after several washing cycles and overnight drying, were then calcined at 623 K. Precursor and calcined samples were studied in terms of elemental composition, mineral composition, microstructure, texture, porosity, and metallic copper surface area. The results suggest that the dependence of precursor surface area on aging is realized by its dependence on phase composition. In the precipitate aged for two hours, the relative dominance of malachite leads to the highest pre‑calcination surface area of 57 m&lt;sup&gt;2&lt;/sup&gt;/g. The individual thermal behaviors of the precursor phases and their pre‑calcination surface area values seem to conjointly determine the post‑calcination surface area of the samples. Such that a combination of ripened particle structure and susceptibility to calcination induced surface deterioration yields the lowest post‑calcination surface area after aging for four hours. The calcines derived from the unaged and the two‑hour‑aged precursors yield surface area values of approximately 57&amp;ndash;58 m&lt;sup&gt;2&lt;/sup&gt;/g, sensibly higher than that of the four‑hour‑aged sample. The Cu&lt;sup&gt;0&lt;/sup&gt; surface area values of the samples depend on aging duration through the effect it imparts on the Cu/Zn‑interdispersion of the precursor malachite phase. The highest Cu/Zn‑interdispersion is achieved in the two‑hour‑aged sample that finally exhibited a maximum Cu&lt;sup&gt;0&lt;/sup&gt; surface of 112 m&lt;sup&gt;2&lt;/sup&gt;/g&lt;sub&gt;Cu&lt;/sub&gt;.&lt;/span&gt;&lt;span lang=&quot;FA&quot; dir=&quot;RTL&quot; style=&quot;font-family:&quot;Times New Roman&quot;,serif&quot;&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br&gt;
&amp;nbsp;</description>
						<author>Hajar Ghanbari</author>
						<category></category>
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						<title>Effect of Temperature-Time on simultaneous hydrogen reduction of molybdenum and tungsten oxides</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4571&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;span style=&quot;font-size:12pt&quot;&gt;&lt;span style=&quot;text-justify:inter-ideograph&quot;&gt;&lt;span style=&quot;unicode-bidi:embed&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;The Mo-30 wt% W solid solution is a well-established molybdenum-based alloy. A recent approach to alloying Mo and W involves the simultaneous reduction of their oxides by hydrogen. Several studies have reported the production of Mo-W alloys via the reduction of mixed oxides.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; But the alloying mechanism and the effects of key reduction parameters on alloy formation remain uninvestigated&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;. In the present study, the simultaneous hydrogen reduction of MoO₃&amp;ndash;WO₃ mixed oxides was investigated as a potential route for producing pre-alloyed Mo&amp;ndash;W powders. In this study pre-alloyed Mo-30 wt% W is. The effects of reduction temperature and holding time on phase evolution, morphology, and alloy formation were systematically examined. The chosen temperature range is 600-1050&amp;deg;C. The influence of time on phase formation and morphology during the hydrogen reduction of molybdenum and tungsten oxides is examined over a 30-360 minute period. &lt;/span&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;Other parameters such as heating rate (&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;20&lt;/span&gt;&lt;/span&gt;&lt;m:omath&gt;&lt;m:f&gt;&lt;m:fpr&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span cambria=&quot;&quot; math=&quot;&quot; style=&quot;font-family:&quot;&gt;&lt;m:ctrlpr&gt;&lt;/m:ctrlpr&gt;&lt;/span&gt;&lt;/span&gt;&lt;/m:fpr&gt;&lt;m:num&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span cambria=&quot;&quot; math=&quot;&quot; style=&quot;font-family:&quot;&gt;&lt;m:r&gt;&lt;m:rpr&gt;&lt;m:scr m:val=&quot;roman&quot;&gt;&lt;m:sty m:val=&quot;p&quot;&gt;&lt;/m:sty&gt;&lt;/m:scr&gt;&lt;/m:rpr&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;℃&lt;/span&gt;&lt;/m:r&gt;&lt;/span&gt;&lt;/span&gt;&lt;/m:num&gt;&lt;m:den&gt;&lt;i&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span cambria=&quot;&quot; math=&quot;&quot; style=&quot;font-family:&quot;&gt;&lt;m:r&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;min&lt;/span&gt;&lt;/m:r&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/m:den&gt;&lt;/m:f&gt;&lt;/m:omath&gt;&lt;span style=&quot;font-size:12.0pt&quot;&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;&lt;span style=&quot;position:relative&quot;&gt;&lt;span style=&quot;top:13.0pt&quot;&gt;&lt;img alt=&quot;&quot; id=&quot;_x0000_i1025&quot; src=&quot;data:image/png;base64,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&quot; style=&quot;width:16.5pt; height:27.75pt&quot; &gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;), bed height (10mm), H₂ flow rate (&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;500&lt;/span&gt;&lt;/span&gt;&lt;m:omath&gt;&lt;m:f&gt;&lt;m:fpr&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span cambria=&quot;&quot; math=&quot;&quot; style=&quot;font-family:&quot;&gt;&lt;m:ctrlpr&gt;&lt;/m:ctrlpr&gt;&lt;/span&gt;&lt;/span&gt;&lt;/m:fpr&gt;&lt;m:num&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span cambria=&quot;&quot; math=&quot;&quot; style=&quot;font-family:&quot;&gt;&lt;m:r&gt;&lt;m:rpr&gt;&lt;m:scr m:val=&quot;roman&quot;&gt;&lt;m:sty m:val=&quot;p&quot;&gt;&lt;/m:sty&gt;&lt;/m:scr&gt;&lt;/m:rpr&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;ml&lt;/span&gt;&lt;/m:r&gt;&lt;/span&gt;&lt;/span&gt;&lt;/m:num&gt;&lt;m:den&gt;&lt;i&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span cambria=&quot;&quot; math=&quot;&quot; style=&quot;font-family:&quot;&gt;&lt;m:r&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;min&lt;/span&gt;&lt;/m:r&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/m:den&gt;&lt;/m:f&gt;&lt;/m:omath&gt;&lt;span style=&quot;font-size:12.0pt&quot;&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;&lt;span style=&quot;position:relative&quot;&gt;&lt;span style=&quot;top:13.0pt&quot;&gt;&lt;img alt=&quot;&quot; id=&quot;_x0000_i1025&quot; src=&quot;data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAABYAAAAlCAIAAADJOI5vAAAAAXNSR0IArs4c6QAAAAlwSFlzAAAOxAAADsQBlSsOGwAAARhJREFUSEvtVckNwjAQHFMMD0QF0AQvSoB24MuPDvgAHVACD6CXMOwkzhIUZBELIZEVipZ41nvYMwko0NEGHeMZ/uUt1kAAjq91cxbpvwlwaOKzN8IiWSoLnlY1L83h33fW6GIBrKxUPlm2VmlyUhsZWgyf46QTzzCL5/Fy2rJ4ZfmGrdHUYFx17Yd/vOBJ5/MRqB9nPbYMFzxtC5L91npaGU4EuJoKRBZJETydxDHyKiIFqNRk8FjYAhsTCOJOwMUxlVASdGQxEempXPKaIJ8nJhSjucRg+REpEbCXNs4zMLM8e2DuHOk9C6TJj8idhVBlyypUmKRRCZmNJr2neRH1APMznEgoiq7f5bSrpZZbrN+iHsxvzOIOFm57xwkMJ94AAAAASUVORK5CYII=&quot; style=&quot;width:16.5pt; height:27.75pt&quot; &gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;), and material weight (14.3g) were kept constant.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; The reduced samples are analyzed using X-ray diffraction (XRD) and scanning electron microscopy (SEM). The effects of temperature and time on the reduction processes are closely linked. Results indicate the formation of MoO₂ and WO₂ phases at 600&amp;deg;C after 60 minutes of hydrogen reduction. No Oxide phases were detected in XRD analysis of the sample that was reduced at 800&amp;deg;C for 180 minutes. Therefore, tungsten and molybdenum coexist in all particles of the samples.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; &lt;/span&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;Mass transfer between Mo and W takes place during the reduction of oxides to the metallic phase.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt; But isothermal reduction does not yield a homogeneous alloy. In these studies, for T &gt; 800&amp;deg;C, increasing time has minimal effect on alloying these elements. At T=800&amp;deg;C, a significant change in morphology occurs at t&gt;180 min. At T=800&amp;deg;C, a notable morphological change occurs after t&gt;180 min. These changes are caused by the CVT mechanism. The optimal conditions for achieving chemical homogeneity in the alloy powder particles after reduction were identified as: 600&amp;deg;C for 60 min, 600 to 1050 for 240 min, and 180 min at 1050&amp;deg;C. This cycle leads to the formation of homogeneous alloy powder particles. The achieved homogeneity is attributed to providing sufficient time for mass transport between molybdenum and tungsten oxide particles through gaseous chemical species formed within this temperature range.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br&gt;
&lt;br&gt;
&lt;span style=&quot;background-color:#ffffff;&quot;&gt;&amp;nbsp;&lt;/span&gt;</description>
						<author>Hossein Aghajani</author>
						<category></category>
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						<title>Design and Optimisation of Corrosion Behaviour of Mg-Zn-Ca Alloy System Using Thermodynamic and Statistical Simulation</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4603&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;span style=&quot;font-size:10pt&quot;&gt;&lt;span style=&quot;line-height:200%&quot;&gt;&lt;span linotype=&quot;&quot; palatino=&quot;&quot; style=&quot;font-family:&quot;&gt;&lt;span style=&quot;color:black&quot;&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;line-height:200%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;In recent years, Mg- based alloys have been considered as a biodegradable biomaterial for implant applications. However, the high corrosion rate and hydrogen gas evolution in an aqueous environment are the most important challenges for these alloys. This study has focused on optimizing the biocorrosion properties of &amp;nbsp;bioalloys in Mg-Zn-Ca system, using a combined approach of thermodynamic simulations, and response surface methodology (RSM). In, Mg&lt;sub&gt;2&lt;/sub&gt;Ca and Ca&lt;sub&gt;x&lt;/sub&gt;Mg&lt;sub&gt;y&lt;/sub&gt;Zn&lt;sub&gt;z&lt;/sub&gt; precipitates have a significant effect on corrosion mechanisms. It is believed that, in the Mg-Zn-Ca alloy system, the Mg&lt;sub&gt;2&lt;/sub&gt;Ca secondary phase usually enhances corrosion rate with microgalvanic coupling mechanisms. The ternary phases Ca&lt;sub&gt;x&lt;/sub&gt;Mg&lt;sub&gt;y&lt;/sub&gt;Zn&lt;sub&gt;z&lt;/sub&gt; have less detrimental effects on corrosion resistance. To minimize harmful phases, CompuTherm&amp;rsquo;s PANDAT software was utilized for phase evolution prediction, with outputs directly validated against experimental measurements. Potentiodynamic tafel polarization experiments and long-term immersion tests were conducted to evaluate the corrosion rate. In order to design an alloy with the least detrimental phase, a statistical model (RSM) was developed based on predicted results from thermodynamic model. The results showed that the ZX31 (Mg-2.6Zn-1Ca) exhibited the highest corrosion potential (-1.6336 V&lt;sub&gt;Ag/AgCl&lt;/sub&gt;) and the lowest corrosion current density (216 &amp;micro;A/cm&lt;sup&gt;2&lt;/sup&gt;), showing higher biocorrosion resistance compared to ZX24 (Mg-2.3Zn-4.0Ca) and ZX15 (Mg-1.3Zn-4.8Ca). &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br&gt;
&amp;nbsp;</description>
						<author>M. Reza Aboutalebi</author>
						<category></category>
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						<title>Enhancing Dielectric and Ferroelectric Properties in PFN–PT Ceramics via (Ca,Sr)ZrO3 Modification for Advanced Electronic Applications</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4601&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;span style=&quot;font-size:11pt&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span style=&quot;font-family:Calibri,sans-serif&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;&lt;span style=&quot;color:black&quot;&gt;The structural, dielectric, and ferroelectric properties of (1&amp;minus;x)PFN&amp;ndash;PT/x(Ca,Sr)ZrO₃ ceramics (x = 0&amp;ndash;0.08) were systematically investigated. X-ray diffraction analysis confirmed the formation of a single-phase perovskite structure, while Rietveld refinement revealed a gradual reduction in the monoclinic lattice distortion with increasing CZ and SZ contents, indicating structural evolution toward a pseudocubic-like state near the morphotropic phase boundary (MPB). Quantitative FE-SEM analysis showed dense microstructures with progressive grain refinement at higher modifier concentrations. Temperature-dependent dielectric measurements exhibited the highest dielectric constant for the x = 0.04 compositions, whereas the modified Curie&amp;ndash;Weiss analysis confirmed diffuse phase transition and relaxor behavior, with &amp;gamma; values of 1.94 and 1.68 for PFN&amp;ndash;PT:0.04CZ and PFN&amp;ndash;PT:0.04SZ, respectively. Room-temperature ferroelectric measurements yielded maximum remanent polarization (P&lt;sub&gt;r&lt;/sub&gt;) values of 24.32 and 34.26 &amp;mu;C cm⁻&amp;sup2; for the CZ- and SZ-modified ceramics at x = 0.04. The enhanced dielectric and ferroelectric properties are closely correlated with the reduced monoclinic distortion near the MPB, highlighting the crucial role of structural optimization in improving the functional performance of PFN&amp;ndash;PT-based ceramics.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br&gt;
&amp;nbsp;</description>
						<author>marjaneh jafari fesharaki</author>
						<category></category>
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						<title>Effect of Twin Boundary Density on Mechanical Response and Dislocation Evolution in a Nickel-Based Superalloy: A Molecular Dynamics Study</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4525&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;span style=&quot;font-size:10pt&quot;&gt;&lt;span style=&quot;line-height:normal&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;background:lime&quot;&gt;&lt;span style=&quot;color:black&quot;&gt;&lt;span style=&quot;background-color:#ffffff;&quot;&gt;Twin-boundary engineering provides an effective approach for tailoring the mechanical response of nickel-based superalloys; however, the density-dependent atomistic mechanisms remain insufficiently understood in explicit dual-phase &amp;gamma;/&amp;gamma;&amp;prime; microstructures. Molecular dynamics simulations were performed on a single-crystal model and models containing one, two, and eight twin boundaries oriented perpendicular to the loading direction. The tensile response was analyzed in conjunction with dislocation-density evolution, microstructural changes, and Constructed-surface-mesh analysis to characterize crack initiation and growth. The TB1 model exhibited higher yield stress and strain than the single-crystal model because the isolated twin boundary impeded dislocation motion. In contrast, TB2 and TB8 yielded at lower stresses and strains because the increased twin-boundary density introduced additional preferential nucleation sites at the twin boundaries and twin-boundary/&amp;gamma;&amp;ndash;&amp;gamma;&amp;prime; interface intersections. Despite its earlier yielding, TB2 exhibited the highest ultimate stress among all models and the highest ultimate strain among the twinned models. This behavior was attributed to deformation partitioning between two comparatively stable twin boundaries, which promoted distributed precipitate shearing, dislocation storage, and sustained strain hardening. TB8 exhibited the highest initial dislocation density, followed by a decrease during plastic deformation associated with twin-boundary migration, defect rearrangement, and strain localization. Constructed-surface-mesh analysis further showed that crack initiation was delayed to a strain of approximately 0.07356 in TB2, compared with approximately 0.066 in TB1 and TB8. Crack propagation occurred predominantly along the twin boundaries and &amp;gamma;/&amp;gamma;&amp;prime; phase interfaces. These findings reveal a non-monotonic, density-dependent transition from barrier-controlled strengthening in TB1 to deformation-partitioning-assisted hardening in TB2 and boundary-migration-assisted, localization-dominated softening in TB8.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;color:black&quot;&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br&gt;
&lt;br&gt;
&amp;nbsp;</description>
						<author>mojtaba zolfaghari</author>
						<category></category>
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						<title>Microstructural Investigation of Laser-Welded Anodized 6061 Aluminum Alloy</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4581&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;span style=&quot;font-size:10pt&quot;&gt;&lt;span style=&quot;unicode-bidi:embed&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;&lt;span style=&quot;font-size:12.0pt&quot;&gt;In this study, the feasibility of laser welding on anodized aluminum alloy has been investigated. There are many demands in the industry for the welding of anodized aluminium sheets. Firstly, the anodizing process was performed by changing the anodizing time and keeping the other anodizing parameters constant.&amp;nbsp;The anodizing process&amp;nbsp;was&amp;nbsp;performed&amp;nbsp;at three different anodizing times of 30, 45, and 60 minutes. Then, the sample with the largest oxide layer thickness, which was obtained at the higher anodizing time, was chosen for the laser welding. The welding process was performed at a laser power of 1500 watts and a welding speed of 300 mm/s on an anodized 6061-T6 aluminum alloy with an oxide layer thickness of 17 microns. The current investigation depicted that the sound joint occurred between two anodized aluminium sheets. Although the anodized layer acts as an inhibitor for the joining of aluminum sheets due to its high melting point, the results showed a homogeneous distribution of the elements within the weld zone. In the meantime, the growth of dendrites across the weldment shows the concentration of elements in the interdendritic regions of the weldment. &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br&gt;
&amp;nbsp;</description>
						<author>Seyed Reza Elmi Hosseini</author>
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						<title>Heat Treatment Effects on Microstructure, Hardness &amp; Corrosion of Al-12Si-Cu Alloy</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4421&amp;sid=1&amp;slc_lang=en</link>
						<description>The influence of different heat treatment parameters, namely solutionizing and artificial&lt;br&gt;
aging conditions, on the microstructure, mechanical hardness, and corrosion resistance of Al-&lt;br&gt;
12Si-Cu alloy are systematically explored in this work. Solution treatment was performed at&lt;br&gt;
two temperatures (500&amp;deg;C and 530&amp;deg;C) and two durations (0.5 and 3 hours), and artificial aging&lt;br&gt;
was made at two temperatures (180&amp;deg;C and 310&amp;deg;C) over two durations (2 and 5 hours).&lt;br&gt;
Optical microscopy also showed interesting microstructural changes with fine grain&lt;br&gt;
refinement and enhanced spheroidization of the coarse eutectic Si phase and a more uniform&lt;br&gt;
distribution of primary intermetallic grains. These structural adjustments were identified as&lt;br&gt;
direct determinants of properties of the material. Maximum microhardness (155 HV) was&lt;br&gt;
achieved at the temperatures of 500&amp;deg;C/3 h solutionizing and 180&amp;deg;C for 5 h aging (S3), which&lt;br&gt;
was ascribed to successful solid solution strengthening and fine precipitation hardening. In&lt;br&gt;
contrast, the lowest hardness (54 HV) was obtained at the values 530&amp;deg;C/3 h + 310&amp;deg;C/5 h (S8),&lt;br&gt;
showing the harmful impact of over-aging at higher temperatures. Analysis of&lt;br&gt;
electrochemical corrosion detected a significant correlation between the corrosion resistance&lt;br&gt;
and treated microstructure, where conditions favoring microstructural refinement resulted in a&lt;br&gt;
decrease in corrosion current density. A Design of Experiments (DOE) method by way of the&lt;br&gt;
Taguchi L8 orthogonal array was used to find out how each parameter contributed relative to&lt;br&gt;
the other variable. The analysis revealed that, whilst the aging temperature was the most&lt;br&gt;
influential factor to the microhardness, the solution time was the controlling factor on the&lt;br&gt;
surface roughness. The results demonstrate a robust determination of the main processing&lt;br&gt;
windows which are known to be crucial to enhance particular properties and verify the&lt;br&gt;
tremendous feasibility of temperature control in heat treatment process optimization in&lt;br&gt;
engineering the necessary trade-off between mechanical strength and corrosion performance&lt;br&gt;
in Al-12Si-Cu alloys.</description>
						<author>asaad Kadhim  eqal</author>
						<category></category>
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						<title>Evolution of Structural, Dielectric and Magnetic Properties of Cobalt Ferrite Nanoparticles Produced by Sol-Gel Technique During Sintering Treatment</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4451&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;span style=&quot;color:#000000;&quot;&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;line-height:107%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;This study investigates the effect of sintering temperature on the structural, dielectric and magnetic properties of cobalt ferrite nanoparticles (CoFe₂O₄ NPs) synthesized by the sol&amp;ndash;gel method. The samples were sintered at 400&amp;deg;C&amp;ndash;1000&amp;deg;C for 2 h and characterized using XRD, FTIR, SEM, AFM, dielectric and VSM measurements. XRD confirmed the formation of a stable cubic spinel structure, with crystallite size increasing from 10.71 to 16.09 nm and porosity decreasing with increasing sintering temperature. SEM and AFM showed progressive grain growth and improved grain connectivity, with the sample at 800&amp;deg;C exhibiting the most uniform morphology before excessive grain growth occurred at 1000&amp;deg;C. The dielectric response showed decreasing real and imaginary permittivity with increasing frequency, while the sample at 800&amp;deg;C exhibited the lowest dielectric loss (tan &amp;delta; &amp;asymp; 2 at 1 kHz). Magnetic measurements revealed ferrimagnetic behavior, with saturation magnetization increasing from 27.5 emu/g at 400&amp;deg;C to 68 emu/g at 1000&amp;deg;C, whereas coercivity reached a maximum of 715 Oe at 800&amp;deg;C. Overall, sintering at 800&amp;deg;C provided the best balance between microstructural uniformity, low dielectric loss and magnetic performance, making it a &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;font-size:12.0pt&quot;&gt;&lt;span style=&quot;line-height:107%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;strong&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;line-height:107%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt; candidate for further evaluation in high-frequency and multifunctional magnetic applications.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;</description>
						<author>Mohammed Alluaibi</author>
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						<title>Tribological, Mechanical and Electrochemical Characterization of GS-42CrMo4V Track Roller Steel for Mining Applications</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4652&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;div style=&quot;text-align: justify;&quot;&gt;&lt;span style=&quot;font-size:12pt&quot;&gt;&lt;span style=&quot;line-height:200%&quot;&gt;&lt;span style=&quot;font-family:Arial,sans-serif&quot;&gt;&lt;span style=&quot;font-size:11.0pt&quot;&gt;&lt;span style=&quot;line-height:200%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;Track rollers used in bucket wheel excavators are subjected to repeated mechanical loading in an environment where abrasive particles, moisture and corrosive contaminants can accelerate surface deterioration. The present study examines the mechanical, electrochemical and tribological behaviour of GS‑42CrMo4V cast steel used for this application. The material w::as char::acterized through chemical composition analysis, microhardness measurement, tensile testing and fractographic examination. Its corrosion behaviour was further evaluated in 3.5 wt.% NaCl and acidic HCl and H₂SO₄ solutions using potentiodynamic polarization and electrochemical impedance spectroscopy, while three-body abrasion and reciprocating wear tests were carried out to assess its resistance to material loss under different contact conditions. The bottom roller exhibited an average microhardness of 430 HV, compared with 314.2 HV for the roller pin. Tensile and fractographic observations indicated good mechanical performance, although localized damage features were observed on the fractured surfaces. The electrochemical results showed that the material performed better in the neutral chloride solution than in the acidic media. In 3.5 wt.% NaCl, the corrosion current density and corrosion rate were 1.597&amp;nbsp;&amp;mu;A cm⁻&amp;sup2; and 0.487 mpy, respectively, whereas the acidic solutions produced considerably higher corrosion activity. The wear tests confirmed that high hardness alone did not prevent material removal under abrasive and sliding contact. Abrasive action, plastic deformation and localized adhesive interactions contributed to surface degradation under the investigated conditions. The results therefore indicate that, despite its favourable hardness and mechanical characteristics, GS-42CrMo4V remains susceptible to degradation in aggressive acidic environments and under severe abrasive and sliding conditions. The observed behaviour points to the need for further improvement in material processing, surface condition, corrosion protection and the control of abrasive particle ingress. These findings provide a basis for understanding the service-related limitations of the material and for improving the durability of track rollers used in mining equipment.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;</description>
						<author>Krishnakumar K</author>
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						<title>Sol-Enhanced Electrodeposition of Ni-Co-CeO2 Nano-composite Electrodes for Improved Electrochemical Performance in an Alkaline Media</title>
						<link>http://ce.iust.ac.ir/ijmse/browse.php?a_id=4640&amp;sid=1&amp;slc_lang=en</link>
						<description>&lt;span style=&quot;font-size:12pt&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;&lt;span new=&quot;&quot; roman=&quot;&quot; style=&quot;font-family:&quot; times=&quot;&quot;&gt;&lt;span style=&quot;line-height:150%&quot;&gt;In this study, Ni-Co-CeO&lt;sub&gt;2&lt;/sub&gt; nanocomposite coatings were deposited on copper substrates via a sol-enhanced electrodeposition method. Cerium oxide nanoparticles were synthesized using cerium chloride precursor and HMTA as a precipitating agent at 70 &amp;deg;C and subsequently added to a Watts bath containing nickel and cobalt ions. An investigation of the effect of deposition current density (10 to 30 mA.cm&lt;sup&gt;-2&lt;/sup&gt;) revealed that increasing the deposition current density reduced the cerium oxide content in the coating from 12.2 to 7.1 wt%. SEM images confirmed a morphological transformation from an acicular structure to a fine-grained microstructure with surface heterogeneity in the presence of the nanoparticles. XRD results further demonstrated grain refinement induced by the CeO&lt;sub&gt;2&lt;/sub&gt; reinforcing phase. Electrochemical evaluations in 1 M KOH solution showed that the sample deposited at a current density of 20 mA.cm&lt;sup&gt;-2&lt;/sup&gt; exhibited the highest performance, with a discharge time of 92 seconds (a 77% improvement compared to the particle-free sample) and optimal charge transfer resistance. This enhanced performance is attributed to a favorable balance between the electrical conductivity of the metallic matrix and the catalytic activity of the cerium oxide nanoparticles. The findings of this investigation substantiate the efficacy of the sol-enhanced method in designing advanced electrodes for energy systems.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;</description>
						<author>Saeed rastegari</author>
						<category></category>
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