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<title>Most recent issue published online for the International Journal of Theoretical and Applied Multiscale Mechanics.</title>
<description>International Journal of Theoretical and Applied Multiscale Mechanics</description>
<link>http://www.inderscience.com/browse/index.php?journalID=293&amp;year=2011&amp;vol=2&amp;issue=2</link>
<dc:publisher>Inderscience Publishers Ltd</dc:publisher>
<dc:language>en-uk</dc:language>
<prism:publicationName>International Journal of Theoretical and Applied Multiscale Mechanics</prism:publicationName>
<prism:issn>1755-9995</prism:issn>
<prism:eIssn>1756-0004</prism:eIssn>
<prism:copyright>&#169; 2011 Inderscience Publishers Ltd</prism:copyright>
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<rdf:li rdf:resource="http://dx.doi.org/10.1504/IJTAMM.2011.043533" />
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<rdf:li rdf:resource="http://dx.doi.org/10.1504/IJTAMM.2011.043535" />
<rdf:li rdf:resource="http://dx.doi.org/10.1504/IJTAMM.2011.043536" />
<rdf:li rdf:resource="http://dx.doi.org/10.1504/IJTAMM.2011.043537" />
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<title>International Journal of Theoretical and Applied Multiscale Mechanics</title>
<url>https://www.inderscience.com/images/files/coverImgs/ijtamm_scoverijtamm.jpg</url>
<link>http://www.inderscience.com/browse/index.php?journalID=293&amp;year=2011&amp;vol=2&amp;issue=2</link>
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<item rdf:about="http://dx.doi.org/10.1504/IJTAMM.2011.043533">
<title>Modelling dislocations in a polycrystal using the Generalised Finite Element Method</title>
<link>http://www.inderscience.com/link.php?id=43533</link>
<description>Modelling the interaction of dislocations with internal boundaries and free surfaces is essential to understanding the effect of microstructure on dislocation motion. However, dislocation dynamics methods rely on infinite domain solutions of dislocation fields which makes modelling of heterogeneous materials difficult. A finite domain dislocation dynamics capability is presented that resolves both the dislocation array and polycrystalline structure in a compatible manner so that free surfaces and material interfaces are easily treated. In this approach the polycrystalline structure is accommodated using the Generalised Finite Element Method &#40;GFEM&#41; &#40;Simone et al., 2006&#41; and the displacement due to dislocations is added to the displacement approximation.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=43533"><b>Modelling dislocations in a polycrystal using the Generalised Finite Element Method</b></A><br />J. Robbins; T.E. Voth<br /><i>International Journal of Theoretical and Applied Multiscale Mechanics, Vol. 2, No. 2 (2011) pp. 95 - 110</i><br />Modelling the interaction of dislocations with internal boundaries and free surfaces is essential to understanding the effect of microstructure on dislocation motion. However, dislocation dynamics methods rely on infinite domain solutions of dislocation fields which makes modelling of heterogeneous materials difficult. A finite domain dislocation dynamics capability is presented that resolves both the dislocation array and polycrystalline structure in a compatible manner so that free surfaces and material interfaces are easily treated. In this approach the polycrystalline structure is accommodated using the Generalised Finite Element Method &#40;GFEM&#41; &#40;Simone et al., 2006&#41; and the displacement due to dislocations is added to the displacement approximation.</p>]]></content:encoded>
<dc:identifier>10.1504/IJTAMM.2011.043533</dc:identifier>
<dc:source>International Journal of Theoretical and Applied Multiscale Mechanics, Vol. 2, No. 2 (2011) pp. 95 - 110</dc:source>
<dc:creator>J. Robbins; T.E. Voth</dc:creator>
<dc:contributor>Dynamic Material Properties, Sandia National Laboratories, Albuquerque, New Mexico 87185, USA. &#39; Exploratory Simulation Technologies, Sandia National Laboratories, Albuquerque, New Mexico 87185, USA</dc:contributor>
<dc:subject>dislocation modelling</dc:subject>
<dc:subject>polycrystals</dc:subject>
<dc:subject>GFEM</dc:subject>
<dc:subject>generalised FEM</dc:subject>
<dc:subject>&#63;nite element method</dc:subject>
<dc:subject>internal boundaries</dc:subject>
<dc:subject>free surfaces</dc:subject>
<dc:subject>microstructure</dc:subject>
<dc:subject>nickel</dc:subject>
<dc:subject>dislocations</dc:subject>
<dc:subject>dislocation motion</dc:subject>
<dc:subject>dislocation dynamics</dc:subject>
<dc:subject>displacement.</dc:subject>
<dc:date>2011-11-04T23:20:50-05:00</dc:date>
<prism:volume>2</prism:volume>
<prism:number>2</prism:number>
<prism:startingPage>95</prism:startingPage>
<prism:endingPage>110</prism:endingPage>
<prism:publicationDate>2011-11-04T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJTAMM.2011.043534">
<title>Simulation and design of exposed anchor bolts in shear</title>
<link>http://www.inderscience.com/link.php?id=43534</link>
<description>This paper describes a study of exposed anchors in shear such as those in a typical column footing connection with a grout leveling pad. Two groups of double&#45;shear tests of threaded rods &#40;ASTM A193 Grade B7&#41; were conducted along with finite element analyses to simulate the behaviour of exposed anchors in shear. The study indicated that the exposed length and boundary conditions of exposed anchors significantly affects the load&#45;carrying capacities and the corresponding failure modes because the anchors are subjected to combined bending, shear, and tension. Design equations were proposed for exposed anchors based on the experimental and numerical results.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=43534"><b>Simulation and design of exposed anchor bolts in shear</b></A><br />Zhibin Lin; Derek Petersen; Jian Zhao; Ying Tian<br /><i>International Journal of Theoretical and Applied Multiscale Mechanics, Vol. 2, No. 2 (2011) pp. 111 - 129</i><br />This paper describes a study of exposed anchors in shear such as those in a typical column footing connection with a grout leveling pad. Two groups of double&#45;shear tests of threaded rods &#40;ASTM A193 Grade B7&#41; were conducted along with finite element analyses to simulate the behaviour of exposed anchors in shear. The study indicated that the exposed length and boundary conditions of exposed anchors significantly affects the load&#45;carrying capacities and the corresponding failure modes because the anchors are subjected to combined bending, shear, and tension. Design equations were proposed for exposed anchors based on the experimental and numerical results.</p>]]></content:encoded>
<dc:identifier>10.1504/IJTAMM.2011.043534</dc:identifier>
<dc:source>International Journal of Theoretical and Applied Multiscale Mechanics, Vol. 2, No. 2 (2011) pp. 111 - 129</dc:source>
<dc:creator>Zhibin Lin; Derek Petersen; Jian Zhao; Ying Tian</dc:creator>
<dc:contributor>Department of Civil Engineering and Mechanics, University of Wisconsin&#45;Milwaukee, Milwaukee, WI 53201, USA. &#39; Osmose Railroad Services Inc., Madison, WI 53716, USA. &#39; Department of Civil Engineering and Mechanics, University of Wisconsin&#45;Milwaukee, Milwaukee, WI 53201, USA. &#39; Department of Civil and Environmental Engineering, University of Nevada, Las Vegas, NV 89154, USA</dc:contributor>
<dc:subject>concrete anchors</dc:subject>
<dc:subject>anchor connections</dc:subject>
<dc:subject>fastening to concrete</dc:subject>
<dc:subject>composite construction</dc:subject>
<dc:subject>exposed anchor bolts</dc:subject>
<dc:subject>shear tests</dc:subject>
<dc:subject>design</dc:subject>
<dc:subject>threaded rods</dc:subject>
<dc:subject>finite element analysis</dc:subject>
<dc:subject>FEA</dc:subject>
<dc:subject>simulation</dc:subject>
<dc:subject>load carrying</dc:subject>
<dc:subject>failure modes</dc:subject>
<dc:subject>bending</dc:subject>
<dc:subject>tension.</dc:subject>
<dc:date>2011-11-04T23:20:50-05:00</dc:date>
<prism:volume>2</prism:volume>
<prism:number>2</prism:number>
<prism:startingPage>111</prism:startingPage>
<prism:endingPage>129</prism:endingPage>
<prism:publicationDate>2011-11-04T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJTAMM.2011.043535">
<title>Viscous contribution to the pressure for electroviscous potential flow analysis of capillary instability</title>
<link>http://www.inderscience.com/link.php?id=43535</link>
<description>Viscous contribution for the Viscous Potential Flow &#40;VPF&#41; analysis of capillary instability with axial electric field at the interface of two viscous fluids has been analysed. In VPF, viscosity enters through normal stress balance and the effects of shearing stresses are completely ignored. To include the effect of shearing stresses, viscous pressure is included in normal stress balance along with irrotational pressure and it is assumed that the viscous contribution to the irrotational pressure will resolve the discrepancy between the tangential stresses at the interface. Stability criterion is given in terms of critical value of electric field. Various graphs have been drawn to show the effect of the parameters, such as electric field, inner fluid fraction, Ohnesorge number, conductivity ratio and permittivity ratio.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=43535"><b>Viscous contribution to the pressure for electroviscous potential flow analysis of capillary instability</b></A><br />M.K. Awasthi; G.S. Agrawal<br /><i>International Journal of Theoretical and Applied Multiscale Mechanics, Vol. 2, No. 2 (2011) pp. 130 - 145</i><br />Viscous contribution for the Viscous Potential Flow &#40;VPF&#41; analysis of capillary instability with axial electric field at the interface of two viscous fluids has been analysed. In VPF, viscosity enters through normal stress balance and the effects of shearing stresses are completely ignored. To include the effect of shearing stresses, viscous pressure is included in normal stress balance along with irrotational pressure and it is assumed that the viscous contribution to the irrotational pressure will resolve the discrepancy between the tangential stresses at the interface. Stability criterion is given in terms of critical value of electric field. Various graphs have been drawn to show the effect of the parameters, such as electric field, inner fluid fraction, Ohnesorge number, conductivity ratio and permittivity ratio.</p>]]></content:encoded>
<dc:identifier>10.1504/IJTAMM.2011.043535</dc:identifier>
<dc:source>International Journal of Theoretical and Applied Multiscale Mechanics, Vol. 2, No. 2 (2011) pp. 130 - 145</dc:source>
<dc:creator>M.K. Awasthi; G.S. Agrawal</dc:creator>
<dc:contributor>Department of Mathematics, Indian Institute of Technology Roorkee, Roorkee 247667, India. &#39; Department of Mathematics, Indian Institute of Technology Roorkee, Roorkee 247667, India</dc:contributor>
<dc:subject>viscous contribution</dc:subject>
<dc:subject>viscous potential flow</dc:subject>
<dc:subject>capillary instability</dc:subject>
<dc:subject>interfacial flows</dc:subject>
<dc:subject>axial electric field</dc:subject>
<dc:subject>electroviscous flow</dc:subject>
<dc:subject>viscous fluids</dc:subject>
<dc:subject>viscosity</dc:subject>
<dc:subject>shearing stress.</dc:subject>
<dc:date>2011-11-04T23:20:50-05:00</dc:date>
<prism:volume>2</prism:volume>
<prism:number>2</prism:number>
<prism:startingPage>130</prism:startingPage>
<prism:endingPage>145</prism:endingPage>
<prism:publicationDate>2011-11-04T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJTAMM.2011.043536">
<title>Nonlinear buckling of built&#45;up cold&#45;formed sections</title>
<link>http://www.inderscience.com/link.php?id=43536</link>
<description>An extensive numerical analysis was conducted to investigate the nonlinear buckling of built&#45;up cold&#45;formed sections. This paper presents the calibration of nonlinear finite element models to handle nonlinear buckling behaviour of cold&#45;formed steel sections with geometrically unstable configurations. The two nonlinear finite element packages ANSYS and ABAQUS were used to validate 265 experimental tests. Two different numerical schemes &#40;implicit static and explicit dynamic&#41; under various iterative and non&#45;iterative solution techniques, including Newton&#45;Raphson, Arc&#45;Length, Riks, and Central&#45;Difference integration methods, were adopted to produce reliable solutions. Overall, the numerical analysis estimated the experimental results reasonably well with an adjustment factor of 0.88.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=43536"><b>Nonlinear buckling of built&#45;up cold&#45;formed sections</b></A><br />Krisda Piyawat; Chris Ramseyer; Thomas H&#45;K. Kang<br /><i>International Journal of Theoretical and Applied Multiscale Mechanics, Vol. 2, No. 2 (2011) pp. 146 - 164</i><br />An extensive numerical analysis was conducted to investigate the nonlinear buckling of built&#45;up cold&#45;formed sections. This paper presents the calibration of nonlinear finite element models to handle nonlinear buckling behaviour of cold&#45;formed steel sections with geometrically unstable configurations. The two nonlinear finite element packages ANSYS and ABAQUS were used to validate 265 experimental tests. Two different numerical schemes &#40;implicit static and explicit dynamic&#41; under various iterative and non&#45;iterative solution techniques, including Newton&#45;Raphson, Arc&#45;Length, Riks, and Central&#45;Difference integration methods, were adopted to produce reliable solutions. Overall, the numerical analysis estimated the experimental results reasonably well with an adjustment factor of 0.88.</p>]]></content:encoded>
<dc:identifier>10.1504/IJTAMM.2011.043536</dc:identifier>
<dc:source>International Journal of Theoretical and Applied Multiscale Mechanics, Vol. 2, No. 2 (2011) pp. 146 - 164</dc:source>
<dc:creator>Krisda Piyawat; Chris Ramseyer; Thomas H&#45;K. Kang</dc:creator>
<dc:contributor>Donald G. Fears Structural Engineering Laboratory, School of Civil Engineering and Environmental Science, The University of Oklahoma, Norman, OK 73019, USA. &#39; Donald G. Fears Structural Engineering Laboratory, School of Civil Engineering and Environmental Science, The University of Oklahoma, Norman, OK 73019, USA. &#39; Donald G. Fears Structural Engineering Laboratory, School of Civil Engineering and Environmental Science, The University of Oklahoma, Norman, OK 73019, USA</dc:contributor>
<dc:subject>nonlinear FEA</dc:subject>
<dc:subject>finite element analysis</dc:subject>
<dc:subject>axial load capacity</dc:subject>
<dc:subject>distortional 
buckling</dc:subject>
<dc:subject>built&#45;up sections</dc:subject>
<dc:subject>cold&#45;formed steel sections</dc:subject>
<dc:subject>cold forming</dc:subject>
<dc:subject>modelling.</dc:subject>
<dc:date>2011-11-04T23:20:50-05:00</dc:date>
<prism:volume>2</prism:volume>
<prism:number>2</prism:number>
<prism:startingPage>146</prism:startingPage>
<prism:endingPage>164</prism:endingPage>
<prism:publicationDate>2011-11-04T23:20:50-05:00</prism:publicationDate>
</item>
<item rdf:about="http://dx.doi.org/10.1504/IJTAMM.2011.043537">
<title>Effects of surface charge density and distribution on the nanochannel electro&#45;osmotic flow</title>
<link>http://www.inderscience.com/link.php?id=43537</link>
<description>Surface charge density and distribution dependence of a nanochannel electro&#45;osmotic flow was examined using a Molecular Dynamics &#40;MD&#41; model. Systems consisting of Na&amp;lt;SUP align&#61;right&amp;gt;&#43;&amp;lt;&#47;SUP&amp;gt; and Cl&amp;lt;SUP align&#61;right&amp;gt;&#63;&amp;lt;&#47;SUP&amp;gt; ions in water confined between crystalline walls with varying negative charge on inner surfaces in an external electric field were investigated. At low surface charge densities, water flows as expected by common interpretations of electro&#45;osmosis. At intermediate surface charge density, the flow exhibits a maximum. Strongly charged surfaces cause adsorption of counterions, immobilisation of the near&#45;wall fluid layers, and subsequent flow reversal. An effect of increase in the viscosity of water near the strongly charged surface was demonstrated. When the discrete  1 e charge was distributed on a subgrid of surface atoms, the flow deteriorated and reversed at much lower surface charge densities than when all the surface atoms carried equal partial charge.</description>
<content:encoded><![CDATA[<p><a href="http://www.inderscience.com/link.php?id=43537"><b>Effects of surface charge density and distribution on the nanochannel electro&#45;osmotic flow</b></A><br />Bohumir Jelinek; Sergio D. Felicelli; Paul F. Mlakar; John F. Peters<br /><i>International Journal of Theoretical and Applied Multiscale Mechanics, Vol. 2, No. 2 (2011) pp. 165 - 183</i><br />Surface charge density and distribution dependence of a nanochannel electro&#45;osmotic flow was examined using a Molecular Dynamics &#40;MD&#41; model. Systems consisting of Na&amp;lt;SUP align&#61;right&amp;gt;&#43;&amp;lt;&#47;SUP&amp;gt; and Cl&amp;lt;SUP align&#61;right&amp;gt;&#63;&amp;lt;&#47;SUP&amp;gt; ions in water confined between crystalline walls with varying negative charge on inner surfaces in an external electric field were investigated. At low surface charge densities, water flows as expected by common interpretations of electro&#45;osmosis. At intermediate surface charge density, the flow exhibits a maximum. Strongly charged surfaces cause adsorption of counterions, immobilisation of the near&#45;wall fluid layers, and subsequent flow reversal. An effect of increase in the viscosity of water near the strongly charged surface was demonstrated. When the discrete  1 e charge was distributed on a subgrid of surface atoms, the flow deteriorated and reversed at much lower surface charge densities than when all the surface atoms carried equal partial charge.</p>]]></content:encoded>
<dc:identifier>10.1504/IJTAMM.2011.043537</dc:identifier>
<dc:source>International Journal of Theoretical and Applied Multiscale Mechanics, Vol. 2, No. 2 (2011) pp. 165 - 183</dc:source>
<dc:creator>Bohumir Jelinek; Sergio D. Felicelli; Paul F. Mlakar; John F. Peters</dc:creator>
<dc:contributor>Center for Advanced Vehicular Systems, Mississippi State University, 200 Research Boulevard, Starkville, Mississippi 39759, USA. &#39; Mechanical Engineering Department, Mississippi State University, Mail Stop 9552, 210 Carpenter Building, Mississippi State, Mississippi 39762, USA. &#39; US Army ERDC, 3909 Halls Ferry Rd., Vicksburg, Mississippi 39180, USA. &#39; US Army ERDC, 3909 Halls Ferry Rd., Vicksburg, Mississippi 39180, USA</dc:contributor>
<dc:subject>nanochannels</dc:subject>
<dc:subject>electrokinetic &#63;ow</dc:subject>
<dc:subject>electro&#45;osmosis</dc:subject>
<dc:subject>&#63;ow reversal</dc:subject>
<dc:subject>surface charge</dc:subject>
<dc:subject>charge density</dc:subject>
<dc:subject>charge distribution</dc:subject>
<dc:subject>density effects</dc:subject>
<dc:subject>viscosity</dc:subject>
<dc:subject>molecular dynamics.</dc:subject>
<dc:date>2011-11-04T23:20:50-05:00</dc:date>
<prism:volume>2</prism:volume>
<prism:number>2</prism:number>
<prism:startingPage>165</prism:startingPage>
<prism:endingPage>183</prism:endingPage>
<prism:publicationDate>2011-11-04T23:20:50-05:00</prism:publicationDate>
</item>
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