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<title>Most recent issue published online for the International Journal of Materials and Product Technology.</title>
<description>International Journal of Materials and Product Technology</description>
<link>http://www.inderscience.com/browse/index.php?journalID=20&amp;year=2011&amp;vol=42&amp;issue=1/2</link>
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<title>International Journal of Materials and Product Technology</title>
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<link>http://www.inderscience.com/browse/index.php?journalID=20&amp;year=2011&amp;vol=42&amp;issue=1/2</link>
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<title>Pressureless sintering of silicon nitride ceramics with porous gradient structure for gas filter application</title>
<link>http://www.inderscience.com/link.php?id=44909</link>
<description>In the present study, Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics with high porosity and porous gradient structure are prepared by pressureless sintering technique. Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics with porosity of 34&#45;47&#37; are prepared by using ZrP&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;7 as a binder material and heat treated at 1000&#176;C in a nitrogen atmosphere. Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics with porosity of 50&#45;70&#37; are prepared by using ZrP&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;7 as a binder material, starch or naphthalene as a pore&#45;forming agent and then heat treated at 1000&#176;C in a nitrogen atmosphere. Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics with porous gradient structure are then formed by laminating the Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 porous ceramics with ordered porosity, followed by sintering at 1000&#176;C. The phase compositions are analysed by X&#45;ray diffraction &#40;XRD&#41;, and the microstructure of the sintered samples is observed by scanning electronic microscope &#40;SEM&#41;. The results show that the obtained Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics exhibit a good porous&#45;graded structure from high porosity to low porosity. The major phase of Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics is still &#945; phase.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44909"><b>Pressureless sintering of silicon nitride ceramics with porous gradient structure for gas filter application</b></A><br />Fei Chen; Lingling Ma; Qiang Shen; Chuanbin Wang; Lianmeng Zhang<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 3 - 11</i><br />In the present study, Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics with high porosity and porous gradient structure are prepared by pressureless sintering technique. Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics with porosity of 34&#45;47&#37; are prepared by using ZrP&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;7 as a binder material and heat treated at 1000&#176;C in a nitrogen atmosphere. Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics with porosity of 50&#45;70&#37; are prepared by using ZrP&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;7 as a binder material, starch or naphthalene as a pore&#45;forming agent and then heat treated at 1000&#176;C in a nitrogen atmosphere. Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics with porous gradient structure are then formed by laminating the Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 porous ceramics with ordered porosity, followed by sintering at 1000&#176;C. The phase compositions are analysed by X&#45;ray diffraction &#40;XRD&#41;, and the microstructure of the sintered samples is observed by scanning electronic microscope &#40;SEM&#41;. The results show that the obtained Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics exhibit a good porous&#45;graded structure from high porosity to low porosity. The major phase of Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 ceramics is still &#945; phase.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044909</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 3 - 11</dc:source>
<dc:creator>Fei Chen; Lingling Ma; Qiang Shen; Chuanbin Wang; Lianmeng Zhang</dc:creator>
<dc:contributor>Key Laboratory of Advanced Technology for Specially Functional Materials, Ministry of Education, Wuhan University of Technology, Wuhan 430070, China; State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; Key Laboratory of Advanced Technology for Specially Functional Materials, Ministry of Education, Wuhan University of Technology, Wuhan 430070, China; State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China</dc:contributor>
<dc:subject>silicon nitride</dc:subject>
<dc:subject>porous gradient structure</dc:subject>
<dc:subject>pressureless sintering</dc:subject>
<dc:subject>pore forming agents</dc:subject>
<dc:subject>porous ceramics</dc:subject>
<dc:subject>gas filters</dc:subject>
<dc:subject>porosity.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>3</prism:startingPage>
<prism:endingPage>11</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
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<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044910">
<title>Fabrication of Si3N4&#45;based seal coating on porous Si3N4 ceramics</title>
<link>http://www.inderscience.com/link.php?id=44910</link>
<description>In this study, Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4&#45;based seal coatings using MgO, Al&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3 and SiO&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2 as the sintering additives were prepared on the porous Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 substrates by room temperature spraying and pressureless sintering. The composition of the Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4&#45;based seal coatings was well designed, in order to both match the coefficient of thermal expansion with that of the porous Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 substrate and form the liquid phase at a relative low temperature. During the sintering process, the liquid phases promote the densification and homogenisation of the Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4&#45;based seal coatings. A good combination between Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4&#45;based seal coatings and substrate is achieved, as a result of the liquid&#45;phase penetration into the pores in the porous Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 substrate.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44910"><b>Fabrication of Si3N4&#45;based seal coating on porous Si3N4 ceramics</b></A><br />Qiang Shen; Ying Yang; Fei Chen; Lianmeng Zhang<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 12 - 20</i><br />In this study, Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4&#45;based seal coatings using MgO, Al&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3 and SiO&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2 as the sintering additives were prepared on the porous Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 substrates by room temperature spraying and pressureless sintering. The composition of the Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4&#45;based seal coatings was well designed, in order to both match the coefficient of thermal expansion with that of the porous Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 substrate and form the liquid phase at a relative low temperature. During the sintering process, the liquid phases promote the densification and homogenisation of the Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4&#45;based seal coatings. A good combination between Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4&#45;based seal coatings and substrate is achieved, as a result of the liquid&#45;phase penetration into the pores in the porous Si&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3N&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;4 substrate.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044910</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 12 - 20</dc:source>
<dc:creator>Qiang Shen; Ying Yang; Fei Chen; Lianmeng Zhang</dc:creator>
<dc:contributor>State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China; Key Laboratory of Advanced Technology for Specially Functional Materials, Ministry of Education, Wuhan University of Technology, Wuhan 430070, China. &#39; State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China; Key Laboratory of Advanced Technology for Specially Functional Materials, Ministry of Education, Wuhan University of Technology, Wuhan 430070, China</dc:contributor>
<dc:subject>silicon nitride</dc:subject>
<dc:subject>seal coatings</dc:subject>
<dc:subject>spraying</dc:subject>
<dc:subject>pressureless sintering</dc:subject>
<dc:subject>porous ceramics.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>12</prism:startingPage>
<prism:endingPage>20</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044911">
<title>Design and joining of graphite to copper by a simple direct casting technology</title>
<link>http://www.inderscience.com/link.php?id=44911</link>
<description>A simple low&#45;cost direct casting technology has been developed for joining graphite and copper. The direct casting of copper on graphite was possible through mixing transition metal &#40;Cr&#41; powders with Cu powders to decrease the contact angle between graphite and copper and form a carbide layer at high temperature &#40;&amp;gt;1100&#176;C&#41; in a vacuum furnace for 20&#45;80 min. For decreasing the coefficient of thermal expansion of copper alloy, refractory metal W powders were also added into the mixed powders. The reaction between the transition metal and graphite determined the formation of a thin carbide layer on the graphite surface, as detected by X&#45;ray diffraction analysis. The cross&#45;section of the joined samples was observed by SEM. The shear strength of the C&#45;Cu joints was measured at room temperature with a compression machine.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44911"><b>Design and joining of graphite to copper by a simple direct casting technology</b></A><br />Zhangjian Zhou; Zhihong Zhong; Dandan Qu; Changchun Ge<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 21 - 28</i><br />A simple low&#45;cost direct casting technology has been developed for joining graphite and copper. The direct casting of copper on graphite was possible through mixing transition metal &#40;Cr&#41; powders with Cu powders to decrease the contact angle between graphite and copper and form a carbide layer at high temperature &#40;&amp;gt;1100&#176;C&#41; in a vacuum furnace for 20&#45;80 min. For decreasing the coefficient of thermal expansion of copper alloy, refractory metal W powders were also added into the mixed powders. The reaction between the transition metal and graphite determined the formation of a thin carbide layer on the graphite surface, as detected by X&#45;ray diffraction analysis. The cross&#45;section of the joined samples was observed by SEM. The shear strength of the C&#45;Cu joints was measured at room temperature with a compression machine.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044911</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 21 - 28</dc:source>
<dc:creator>Zhangjian Zhou; Zhihong Zhong; Dandan Qu; Changchun Ge</dc:creator>
<dc:contributor>School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083, China. &#39; School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083, China. &#39; School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083, China. &#39; School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083, China</dc:contributor>
<dc:subject>graphite joining</dc:subject>
<dc:subject>copper joining direct casting</dc:subject>
<dc:subject>copper alloys</dc:subject>
<dc:subject>shear strength.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>21</prism:startingPage>
<prism:endingPage>28</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044912">
<title>Fabrication of functionally graded grinding wheel by a centrifugal mixed&#45;powder method for CFRP&#45;drilling applications</title>
<link>http://www.inderscience.com/link.php?id=44912</link>
<description>We are developing functionally graded grinding wheels fabricated by a centrifugal mixed&#45;powder method. As a first step of this fabrication method, a powder mixture of abrasive particles and metal matrix particles is inserted into a spinning mould. After that, a metal matrix ingot is melted and then the molten metal matrix is poured into the spinning mould with the powder mixture. As a result, the molten metal matrix penetrates into the space between the particles due to the pressure exerted by the centrifugal force. At the same time, the metal matrix powder is melted by the heat from molten matrix poured from the crucible. Finally, a ring&#45;shaped sample with abrasive particles distributed on its surface &#40;functionally graded grinding wheel&#41; can be obtained. In this study, functionally graded grinding wheel fabricated by the centrifugal mixed&#45;powder method will be reported.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44912"><b>Fabrication of functionally graded grinding wheel by a centrifugal mixed&#45;powder method for CFRP&#45;drilling applications</b></A><br />Yoshimi Watanabe; Eri Miura&#45;Fujiwara; Hisashi Sato; Kunio Takekoshi; Hideaki Tsuge; Tadashi Kaga; Naoyuki Bando; Shigemasa Yamagami; Kazumasa Kurachi; Hisanori Yokoyama<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 29 - 45</i><br />We are developing functionally graded grinding wheels fabricated by a centrifugal mixed&#45;powder method. As a first step of this fabrication method, a powder mixture of abrasive particles and metal matrix particles is inserted into a spinning mould. After that, a metal matrix ingot is melted and then the molten metal matrix is poured into the spinning mould with the powder mixture. As a result, the molten metal matrix penetrates into the space between the particles due to the pressure exerted by the centrifugal force. At the same time, the metal matrix powder is melted by the heat from molten matrix poured from the crucible. Finally, a ring&#45;shaped sample with abrasive particles distributed on its surface &#40;functionally graded grinding wheel&#41; can be obtained. In this study, functionally graded grinding wheel fabricated by the centrifugal mixed&#45;powder method will be reported.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044912</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 29 - 45</dc:source>
<dc:creator>Yoshimi Watanabe; Eri Miura&#45;Fujiwara; Hisashi Sato; Kunio Takekoshi; Hideaki Tsuge; Tadashi Kaga; Naoyuki Bando; Shigemasa Yamagami; Kazumasa Kurachi; Hisanori Yokoyama</dc:creator>
<dc:contributor>Omohi College, Graduate School of Engineering, Nagoya Institute of Technology, Gokiso&#45;cho, Showa&#45;ku, Nagoya 466&#45;8555, Japan. &#39; Omohi College, Graduate School of Engineering, Nagoya Institute of Technology, Gokiso&#45;cho, Showa&#45;ku, Nagoya 466&#45;8555, Japan. &#39; Omohi College, Graduate School of Engineering, Nagoya Institute of Technology, Gokiso&#45;cho, Showa&#45;ku, Nagoya 466&#45;8555, Japan. &#39; Gifu Economic and Industrial Promotion Center, 5&#45;14&#45;53 Yabuta Minami, Gifu 500&#45;8505, Japan; Research Institute for Machinery and Materials, Gifu Prefectural Government, 1288 Oze, Seki 501&#45;3265, Japan. &#39; Research Institute for Machinery and Materials, Gifu Prefectural Government, 1288 Oze, Seki 501&#45;3265, Japan. &#39; Research Institute for Machinery and Materials, Gifu Prefectural Government, 1288 Oze, Seki 501&#45;3265, Japan. &#39; Research Institute for Machinery and Materials, Gifu Prefectural Government, 1288 Oze, Seki 501&#45;3265, Japan. &#39; Research Institute for Machinery and Materials, Gifu Prefectural Government, 1288 Oze, Seki 501&#45;3265, Japan. &#39; Gifu Prefectural Ceramics Research Institute, 3&#45;11 Hoshigaoka, Tajimi 507&#45;0811, Japan. &#39; Gifu Prefectural Ceramics Research Institute, 3&#45;11 Hoshigaoka, Tajimi 507&#45;0811, Japan</dc:contributor>
<dc:subject>FGM</dc:subject>
<dc:subject>functionally graded materials</dc:subject>
<dc:subject>centrifugal force</dc:subject>
<dc:subject>casting</dc:subject>
<dc:subject>diamond particles</dc:subject>
<dc:subject>functionally graded grinding wheels</dc:subject>
<dc:subject>CFRP</dc:subject>
<dc:subject>carbon fibre reinforced plastics</dc:subject>
<dc:subject>gyro</dc:subject>
<dc:subject>nanoparticles</dc:subject>
<dc:subject>composite particles</dc:subject>
<dc:subject>nanotechnology.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>29</prism:startingPage>
<prism:endingPage>45</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044913">
<title>Study of strength and toughness in Japanese sword produced from Tamahagane steel by Tatara process</title>
<link>http://www.inderscience.com/link.php?id=44913</link>
<description>Several metallurgical properties of a traditional Japanese sword were investigated from sharp edge to core area in cross&#45;section and on surface. The microstructure is found to be lath martensite at the sharp edge and the prior austenite grain size is observed to be very fine. Towards the inside from the sharp edge in the cross&#45;section, the microstructure changes gradually from hard martensite to soft ferrite. Micro hardness along the centre line in the cross&#45;section was measured. The sharp edge is very hard and the hardness decreases drastically with the detachment from the sharp edge. The hardness gradient on the hardness distribution curve, tan &amp;theta; is defined here. The value of tan &amp;theta; is estimated as an important factor for the explanation of mechanical properties of Japanese swords. Furthermore, residual stress was measured with XRD. Large compressive stress is consequently found on the surface including the sharp edge, which is effective for strengthening the Japanese sword.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44913"><b>Study of strength and toughness in Japanese sword produced from Tamahagane steel by Tatara process</b></A><br />M. Yaso; T. Takaiwa; Y. Minagi; T. Kanaizumi; K. Kubota; Y. Noda; Ananda Kumar Das; S. Morito; T. Ohba<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 46 - 55</i><br />Several metallurgical properties of a traditional Japanese sword were investigated from sharp edge to core area in cross&#45;section and on surface. The microstructure is found to be lath martensite at the sharp edge and the prior austenite grain size is observed to be very fine. Towards the inside from the sharp edge in the cross&#45;section, the microstructure changes gradually from hard martensite to soft ferrite. Micro hardness along the centre line in the cross&#45;section was measured. The sharp edge is very hard and the hardness decreases drastically with the detachment from the sharp edge. The hardness gradient on the hardness distribution curve, tan &amp;theta; is defined here. The value of tan &amp;theta; is estimated as an important factor for the explanation of mechanical properties of Japanese swords. Furthermore, residual stress was measured with XRD. Large compressive stress is consequently found on the surface including the sharp edge, which is effective for strengthening the Japanese sword.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044913</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 46 - 55</dc:source>
<dc:creator>M. Yaso; T. Takaiwa; Y. Minagi; T. Kanaizumi; K. Kubota; Y. Noda; Ananda Kumar Das; S. Morito; T. Ohba</dc:creator>
<dc:contributor>Wakoh Museum, Yasugi&#45;cho 1058, Yasugi 692&#45;0011, Japan. &#39; Wakoh Museum, Yasugi&#45;cho 1058, Yasugi 692&#45;0011, Japan. &#39; Wakoh Museum, Yasugi&#45;cho 1058, Yasugi 692&#45;0011, Japan. &#39; Metallurgical Research Laboratory, Hitachi Metals, Ltd., Yasugi&#45;cho 2107&#45;2, Yasugi, Japan. &#39; Metallurgical Research Laboratory, Hitachi Metals, Ltd., Yasugi&#45;cho 2107&#45;2, Yasugi, Japan. &#39; Department of Materials Science, Shimane University, Nishikawatsu 1060, Matsue, Japan. &#39; Department of Materials Science, Shimane University, Nishikawatsu 1060, Matsue, Japan. &#39; Department of Materials Science, Shimane University, Nishikawatsu 1060, Matsue, Japan. &#39; Department of Materials Science, Shimane University, Nishikawatsu 1060, Matsue, Japan</dc:contributor>
<dc:subject>Japanese swords</dc:subject>
<dc:subject>Tatara process</dc:subject>
<dc:subject>steel strength</dc:subject>
<dc:subject>steel toughness</dc:subject>
<dc:subject>residual stress</dc:subject>
<dc:subject>hardness gradient</dc:subject>
<dc:subject>Japan</dc:subject>
<dc:subject>traditional swords</dc:subject>
<dc:subject>microstructure</dc:subject>
<dc:subject>martensite</dc:subject>
<dc:subject>austenite</dc:subject>
<dc:subject>mechanical properties.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>46</prism:startingPage>
<prism:endingPage>55</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044914">
<title>Impact performance of Al&#47;SiC functionally graded circular plates</title>
<link>http://www.inderscience.com/link.php?id=44914</link>
<description>This experimental study addresses the effect of ceramic reinforcement on the impact performance of functionally graded &#40;FG&#41; circular plates. The FG circular plates were produced from two different ceramic &#40;SiC or Al&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3&#41; and metal &#40;Al&#41; combinations using powder stacking&#45;hot pressing technique. The Al&#47;SiC FG circular plates exhibited better impact resistance than Al&#47;Al&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3 FG circular plates. The effect of ceramic particle size was also investigated on the impact performance of specimens with different composition variations. A ceramic particle size of 50 &amp;mu;m improved the impact performance. In addition, the material composition and impactor velocity also affected the impact performance. Thus, the contact force increases as the composition changes from metal&#45;rich to ceramic&#45;rich. The peak contact force increases with increasing the velocity of impactor.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44914"><b>Impact performance of Al&#47;SiC functionally graded circular plates</b></A><br />M. Kemal Apalak; Recep Gunes; Murat Aydin; J.N. Reddy<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 56 - 65</i><br />This experimental study addresses the effect of ceramic reinforcement on the impact performance of functionally graded &#40;FG&#41; circular plates. The FG circular plates were produced from two different ceramic &#40;SiC or Al&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3&#41; and metal &#40;Al&#41; combinations using powder stacking&#45;hot pressing technique. The Al&#47;SiC FG circular plates exhibited better impact resistance than Al&#47;Al&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3 FG circular plates. The effect of ceramic particle size was also investigated on the impact performance of specimens with different composition variations. A ceramic particle size of 50 &amp;mu;m improved the impact performance. In addition, the material composition and impactor velocity also affected the impact performance. Thus, the contact force increases as the composition changes from metal&#45;rich to ceramic&#45;rich. The peak contact force increases with increasing the velocity of impactor.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044914</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 56 - 65</dc:source>
<dc:creator>M. Kemal Apalak; Recep Gunes; Murat Aydin; J.N. Reddy</dc:creator>
<dc:contributor>Department of Mechanical Engineering, Erciyes University, Kayseri 38039, Turkey. &#39; Department of Mechanical Engineering, Erciyes University, Kayseri 38039, Turkey. &#39; School of Civil Aviation, Erciyes University, Kayseri 38039, Turkey. &#39; Department of Mechanical Engineering, Texas A&amp;amp;M University, College Station, TX 77843&#45;3123, USA</dc:contributor>
<dc:subject>functionally graded materials</dc:subject>
<dc:subject>impact performance</dc:subject>
<dc:subject>low velocity impact</dc:subject>
<dc:subject>circular plates</dc:subject>
<dc:subject>aluminium</dc:subject>
<dc:subject>silicon carbide</dc:subject>
<dc:subject>ceramic reinforcement</dc:subject>
<dc:subject>powder stacking</dc:subject>
<dc:subject>hot pressing</dc:subject>
<dc:subject>ceramic particles.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>56</prism:startingPage>
<prism:endingPage>65</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044915">
<title>Thermoelectric properties and conduction mechanism of conductive polythiophenes</title>
<link>http://www.inderscience.com/link.php?id=44915</link>
<description>In this study, we synthesised conductive polymers of polythiophene series and evaluated their thermoelectric properties in the temperature range from 88 K to 350 K. Poly&#45;hexylthiophenes showed a conduction mechanism of the nearest&#45;neighbour distance hopping &#40;NDH&#41; in the measured temperature range, while the main conduction mechanism of polythiophenes was the variable range hopping &#40;VRH&#41;. Only polythiophenes with low electrical conductivity &#40;such as 0.02 S&#47;cm&#41; presented NDH at temperatures of below 200 K. The conduction mechanism is changed by the distance between the thiophene main chains and the kinetic energy of carriers.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44915"><b>Thermoelectric properties and conduction mechanism of conductive polythiophenes</b></A><br />Yoshikazu Shinohara; Yukihiro Isoda; Kentaro Hiraishi; Akito Masuhara; Hidetoshi Oikawa<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 66 - 73</i><br />In this study, we synthesised conductive polymers of polythiophene series and evaluated their thermoelectric properties in the temperature range from 88 K to 350 K. Poly&#45;hexylthiophenes showed a conduction mechanism of the nearest&#45;neighbour distance hopping &#40;NDH&#41; in the measured temperature range, while the main conduction mechanism of polythiophenes was the variable range hopping &#40;VRH&#41;. Only polythiophenes with low electrical conductivity &#40;such as 0.02 S&#47;cm&#41; presented NDH at temperatures of below 200 K. The conduction mechanism is changed by the distance between the thiophene main chains and the kinetic energy of carriers.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044915</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 66 - 73</dc:source>
<dc:creator>Yoshikazu Shinohara; Yukihiro Isoda; Kentaro Hiraishi; Akito Masuhara; Hidetoshi Oikawa</dc:creator>
<dc:contributor>National Institute for Materials Science, I&#45;2&#45;1, Sengen, Tsukuba, Ibaraki 305&#45;0047, Japan. &#39; National Institute for Materials Science, I&#45;2&#45;1, Sengen, Tsukuba, Ibaraki 305&#45;0047, Japan. &#39; Precision Processing Materials Laboratories, JSR Corporation, 100, Kawajiri&#45;cho, Yokkaichi, Mie, 510&#45;8552 Japan. &#39; Graduate School of Science and Engineering, Department of Organic Device Engineering, Yamagata University, Yamagata 992&#45;8510, Japan. &#39; Institute of Multidisciplinary Research for Advanced Materials &#40;IMRAM&#41;, Tohoku University, Katahira 2&#45;1&#45;1, Aoba&#45;ku, Sendai 980&#45;8577 Japan</dc:contributor>
<dc:subject>thermoelectric materials</dc:subject>
<dc:subject>conductive polymers</dc:subject>
<dc:subject>conduction mechanisms</dc:subject>
<dc:subject>conductive polythiophenes</dc:subject>
<dc:subject>low electrical conductivity.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>66</prism:startingPage>
<prism:endingPage>73</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044916">
<title>Molecular dynamics study on the mechanical characteristics of Al&#45;terminated Al&#47;&amp;alpha;&#45;Al2O3 interface under tensile loading</title>
<link>http://www.inderscience.com/link.php?id=44916</link>
<description>Molecular dynamics simulation has been performed to study the mechanical properties and behaviour of the interface between Al and Al&#45;terminated &amp;alpha;&#45;Al&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3 under tension loading. The atomistic structures of the metal&#47;ceramic interface are first modelled according to experimental results. The interatomic potential utilised here is a multicomponent potential proposed by us. The results reveal that atomic rearrangement caused by lattice misfit occurs after relaxation, expressed as the stacking&#45;fault islands at the interface, which shows reasonable agreement with experiments. During the tension process, the system reaches its ultimate strength 7.89 GPa at strain 11.08&#37; when the crack nucleation emerges in the aluminium.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44916"><b>Molecular dynamics study on the mechanical characteristics of Al&#45;terminated Al&#47;&amp;alpha;&#45;Al2O3 interface under tensile loading</b></A><br />Xin Lai; Lisheng Liu; Hai Mei; Pengcheng Zhai<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 74 - 86</i><br />Molecular dynamics simulation has been performed to study the mechanical properties and behaviour of the interface between Al and Al&#45;terminated &amp;alpha;&#45;Al&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;2O&amp;lt;SUB align&#61;&#34;right&#34;&amp;gt;3 under tension loading. The atomistic structures of the metal&#47;ceramic interface are first modelled according to experimental results. The interatomic potential utilised here is a multicomponent potential proposed by us. The results reveal that atomic rearrangement caused by lattice misfit occurs after relaxation, expressed as the stacking&#45;fault islands at the interface, which shows reasonable agreement with experiments. During the tension process, the system reaches its ultimate strength 7.89 GPa at strain 11.08&#37; when the crack nucleation emerges in the aluminium.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044916</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 74 - 86</dc:source>
<dc:creator>Xin Lai; Lisheng Liu; Hai Mei; Pengcheng Zhai</dc:creator>
<dc:contributor>Department of Engineering Structure and Mechanics, Wuhan University of Technology, Wuhan 430070, China. &#39; Department of Engineering Structure and Mechanics, Wuhan University of Technology, Wuhan 430070, China. &#39; Department of Engineering Structure and Mechanics, Wuhan University of Technology, Wuhan 430070, China. &#39; Department of Engineering Structure and Mechanics, Wuhan University of Technology, Wuhan 430070, China</dc:contributor>
<dc:subject>molecular dynamics</dc:subject>
<dc:subject>interface tension</dc:subject>
<dc:subject>aluminium</dc:subject>
<dc:subject>aluminum oxide</dc:subject>
<dc:subject>Al&#45;Al2O3 interface</dc:subject>
<dc:subject>lattice misfit</dc:subject>
<dc:subject>lattice mismatch</dc:subject>
<dc:subject>atomic rearrangement</dc:subject>
<dc:subject>simulation</dc:subject>
<dc:subject>metal&#45;ceramic interface</dc:subject>
<dc:subject>crack nucleation.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>74</prism:startingPage>
<prism:endingPage>86</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044917">
<title>Numerical simulation on the impact resistance of functionally graded materials</title>
<link>http://www.inderscience.com/link.php?id=44917</link>
<description>The stress wave propagation and damage evolution within the sandwich structure of ceramic faceplate&#47;Functionally Graded Materials &#40;FGMs&#41; interlayer&#47;metal backplate are numerically studied in this paper. The microstructure models of FGM interlayer are constructed by introducing a new algorithm based on Voronoi discretisation. Four typical microstructure models of FGM interlayer with different composition gradient are constructed to analyse the effect of composition gradient of FGM interlayer on the stress wave propagation and damage evolution in the sandwich structures under impulse loading. The results demonstrate that the composition gradients of FGM interlayer significantly affect the stress propagation and damage evolution in the sandwich structures. The unidirectivity of stress wave in these models varies with the variation of composition gradient, and a slow variation of composition gradient is helpful for reducing the stress on the surface of backplate.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44917"><b>Numerical simulation on the impact resistance of functionally graded materials</b></A><br />Jiangtao Zhang; Mei Zhang; Pengcheng Zhai; Lisheng Liu; Huiji Shi<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 87 - 97</i><br />The stress wave propagation and damage evolution within the sandwich structure of ceramic faceplate&#47;Functionally Graded Materials &#40;FGMs&#41; interlayer&#47;metal backplate are numerically studied in this paper. The microstructure models of FGM interlayer are constructed by introducing a new algorithm based on Voronoi discretisation. Four typical microstructure models of FGM interlayer with different composition gradient are constructed to analyse the effect of composition gradient of FGM interlayer on the stress wave propagation and damage evolution in the sandwich structures under impulse loading. The results demonstrate that the composition gradients of FGM interlayer significantly affect the stress propagation and damage evolution in the sandwich structures. The unidirectivity of stress wave in these models varies with the variation of composition gradient, and a slow variation of composition gradient is helpful for reducing the stress on the surface of backplate.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044917</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 87 - 97</dc:source>
<dc:creator>Jiangtao Zhang; Mei Zhang; Pengcheng Zhai; Lisheng Liu; Huiji Shi</dc:creator>
<dc:contributor>Key Lab of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; Key Lab of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; Key Lab of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; Key Lab of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; Key Laboratory for Applied Mechanics of Ministrator of Education, Tsinghua University, Beijing 100084, China</dc:contributor>
<dc:subject>functionally graded materials</dc:subject>
<dc:subject>microstructure</dc:subject>
<dc:subject>impulse loading</dc:subject>
<dc:subject>stress waves</dc:subject>
<dc:subject>damage evolution</dc:subject>
<dc:subject>impact resistance</dc:subject>
<dc:subject>wave propagation</dc:subject>
<dc:subject>sandwich structures</dc:subject>
<dc:subject>ceramics.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>87</prism:startingPage>
<prism:endingPage>97</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044918">
<title>Numerical simulation on the interface debonding in solid propellant under large deformation by a cohesive zone model</title>
<link>http://www.inderscience.com/link.php?id=44918</link>
<description>A new algorithm based on the artificial interaction force between neighbouring particles are introduced to build microstructure models of solid propellant, and the numerical simulation on the non&#45;linear properties of solid propellants under large deformation are performed by using the remeshing technique based on the finite element code ANSYS. The binder&#47;particle interface debonding is modelled through cohesive zone models. The results show that the interface debonding of large particles precedes that of small particles. The overall strains at which interface debonding takes place and the predicted effective stresses of propellants decrease with the decreasing of interface strength. At large strains, the load is mainly carried by the binder network, which is formed due to severe interface debonding. The simulated microscopic deformation modes of solid propellants are well consistent with those of experiments.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44918"><b>Numerical simulation on the interface debonding in solid propellant under large deformation by a cohesive zone model</b></A><br />Mei Zhang; Jiangtao Zhang; Pengcheng Zhai; Lisheng Liu; Huiji Shi<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 98 - 109</i><br />A new algorithm based on the artificial interaction force between neighbouring particles are introduced to build microstructure models of solid propellant, and the numerical simulation on the non&#45;linear properties of solid propellants under large deformation are performed by using the remeshing technique based on the finite element code ANSYS. The binder&#47;particle interface debonding is modelled through cohesive zone models. The results show that the interface debonding of large particles precedes that of small particles. The overall strains at which interface debonding takes place and the predicted effective stresses of propellants decrease with the decreasing of interface strength. At large strains, the load is mainly carried by the binder network, which is formed due to severe interface debonding. The simulated microscopic deformation modes of solid propellants are well consistent with those of experiments.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044918</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 98 - 109</dc:source>
<dc:creator>Mei Zhang; Jiangtao Zhang; Pengcheng Zhai; Lisheng Liu; Huiji Shi</dc:creator>
<dc:contributor>Key Lab of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; Key Lab of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; Key Lab of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; Key Lab of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China. &#39; Key laboratory for Applied Mechanics of Ministrator of Education, Tsinghua University, Beijing 100084, China</dc:contributor>
<dc:subject>solid propellant</dc:subject>
<dc:subject>microstructure modelling</dc:subject>
<dc:subject>cohesive interface models</dc:subject>
<dc:subject>large deformation</dc:subject>
<dc:subject>interface debonding</dc:subject>
<dc:subject>finite element method</dc:subject>
<dc:subject>FEM</dc:subject>
<dc:subject>interface strength</dc:subject>
<dc:subject>simulation.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>98</prism:startingPage>
<prism:endingPage>109</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044888">
<title>Experimental study on cross&#45;section distortion of thin&#45;walled rectangular 3A21 aluminium alloy tube by rotary draw bending</title>
<link>http://www.inderscience.com/link.php?id=44888</link>
<description>The cross&#45;section distortion is inevitably produced in rotary draw bending process of thin&#45;walled rectangular 3A21 aluminium alloy tube, which severely affects the forming quality of the tube. To predict and control cross&#45;section distortion, the experiments with different process parameters are carried out. It is indicated that the effects of bending angle, core number and clearance between the pressure die and tube on the cross&#45;section distortion are significant, but the effects of clearance between wiper die and tube and the boost velocity of the pressure die can be neglected. The maximum cross&#45;section distortion is produced in the section of the angle 50&#176;, and the position does not change with the variation of the process parameters. The results are of significance in the determination of the process parameters for the rotary draw bending process of rectangular tube.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44888"><b>Experimental study on cross&#45;section distortion of thin&#45;walled rectangular 3A21 aluminium alloy tube by rotary draw bending</b></A><br />Kuanxin Liu; Yuli Liu; He Yang; Gangyao Zhao<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 110 - 120</i><br />The cross&#45;section distortion is inevitably produced in rotary draw bending process of thin&#45;walled rectangular 3A21 aluminium alloy tube, which severely affects the forming quality of the tube. To predict and control cross&#45;section distortion, the experiments with different process parameters are carried out. It is indicated that the effects of bending angle, core number and clearance between the pressure die and tube on the cross&#45;section distortion are significant, but the effects of clearance between wiper die and tube and the boost velocity of the pressure die can be neglected. The maximum cross&#45;section distortion is produced in the section of the angle 50&#176;, and the position does not change with the variation of the process parameters. The results are of significance in the determination of the process parameters for the rotary draw bending process of rectangular tube.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044888</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 110 - 120</dc:source>
<dc:creator>Kuanxin Liu; Yuli Liu; He Yang; Gangyao Zhao</dc:creator>
<dc:contributor>State Key Laboratory of Solidification Processing, School of Materials Science and Engineering, Northwestern Polytechnical University, Xi&#39;an 710072, China. &#39; State Key Laboratory of Solidification Processing, School of Materials Science and Engineering, Northwestern Polytechnical University, Xi&#39;an 710072, China. &#39; State Key Laboratory of Solidification Processing, School of Materials Science and Engineering, Northwestern Polytechnical University, Xi&#39;an 710072, China. &#39; School of Aeronautical Manufacturing Engineering, Nanchang Hangkong University, Nanchang, 330063, Jiangxi, China</dc:contributor>
<dc:subject>experimental study</dc:subject>
<dc:subject>thin&#45;walled tubes</dc:subject>
<dc:subject>rectangular tubes</dc:subject>
<dc:subject>rotary draw bending</dc:subject>
<dc:subject>cross&#45;section distortion</dc:subject>
<dc:subject>aluminium alloys</dc:subject>
<dc:subject>forming quality.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>110</prism:startingPage>
<prism:endingPage>120</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJMPT.2011.044884">
<title>Low&#45;voltage silicon chip&#47;glass ring anodic bonding for MEMS device packaging and experimental evaluation of bonding quality</title>
<link>http://www.inderscience.com/link.php?id=44884</link>
<description>Packaging technologies are a great issue in MEMS&#47;NEMS device fabrication. Silicon to glass anodic bonding is a common bonding technique for packaging. In this paper, we describe low voltage silicon chip&#47;glass ring anodic bonding to meet the need of MEMS device batch fabrication. The bonding voltage decreases to be 160 V and the bonding time is cut down from 30 minutes to be about two minutes. The anodic bonding quality of silicon chip&#47;glass ring, effects of thermal cycling and thermal shock, are evaluated in details. The bonding strength is measured using a tensile tester and the fracture mainly occurs inside the silicon chip rather than along the interface. The bonding surface has large adherence intension and can work under harsh environment.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=44884"><b>Low&#45;voltage silicon chip&#47;glass ring anodic bonding for MEMS device packaging and experimental evaluation of bonding quality</b></A><br />Quan Wang; Ran Hu; Xiaodan Yang; Jianning Ding<br /><i>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 121 - 129</i><br />Packaging technologies are a great issue in MEMS&#47;NEMS device fabrication. Silicon to glass anodic bonding is a common bonding technique for packaging. In this paper, we describe low voltage silicon chip&#47;glass ring anodic bonding to meet the need of MEMS device batch fabrication. The bonding voltage decreases to be 160 V and the bonding time is cut down from 30 minutes to be about two minutes. The anodic bonding quality of silicon chip&#47;glass ring, effects of thermal cycling and thermal shock, are evaluated in details. The bonding strength is measured using a tensile tester and the fracture mainly occurs inside the silicon chip rather than along the interface. The bonding surface has large adherence intension and can work under harsh environment.</p>]]></content:encoded>
<dc:identifier>10.1504/IJMPT.2011.044884</dc:identifier>
<dc:source>International Journal of Materials and Product Technology, Vol. 42, No. 1/2 (2011) pp. 121 - 129</dc:source>
<dc:creator>Quan Wang; Ran Hu; Xiaodan Yang; Jianning Ding</dc:creator>
<dc:contributor>Mechanical Engineering School, Jiangsu University, 301 Xuefu Road, Zhenjiang City, 212013, Jiangsu Province, China; State Key Laboratory of Transducer Technology, Chinese Academy of Sciences, 865 Changning Road, Shanghai City, 200050, China. &#39; Mechanical Engineering School, Jiangsu University, 301 Xuefu Road, Zhenjiang City, 212013, Jiangsu Province, China. &#39; Mechanical Engineering School, Jiangsu University, 301 Xuefu Road, Zhenjiang City, 212013, Jiangsu Province, China. &#39; Centre of Micro&#47;Nano Science and Technology, Jiangsu University, 301 Xuefu Road, Zhenjiang City, 212013, Jiangsu Province, China</dc:contributor>
<dc:subject>packaging</dc:subject>
<dc:subject>silicon chips</dc:subject>
<dc:subject>Pyrex7740</dc:subject>
<dc:subject>anodic bonding</dc:subject>
<dc:subject>bonding quality</dc:subject>
<dc:subject>glass bonding</dc:subject>
<dc:subject>silicon bonding</dc:subject>
<dc:subject>MEMS device</dc:subject>
<dc:subject>microelectromechanical devices</dc:subject>
<dc:subject>batch fabrication</dc:subject>
<dc:subject>thermal cycling</dc:subject>
<dc:subject>thermal shock</dc:subject>
<dc:subject>bond strength</dc:subject>
<dc:subject>tensile testing</dc:subject>
<dc:subject>fracture.</dc:subject>
<dc:date>2012-01-15T23:20:50-05:00</dc:date>
<prism:volume>42</prism:volume>
<prism:number>1/2</prism:number>
<prism:startingPage>121</prism:startingPage>
<prism:endingPage>129</prism:endingPage>
<prism:publicationDate>2012-01-15T23:20:50-05:00</prism:publicationDate>
</item>
</rdf:RDF>

