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                <text>Faculty Publications</text>
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    <name>Book Chapter</name>
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              <text>Myson, Shruthy</text>
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          <name>Title</name>
          <description>A name given to the resource</description>
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              <text>Optimization procedure for multilayer heat transfer in nanoliquid with Joule heating using response surface methodology</text>
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              <text>01-01-2025</text>
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              <text>Methods of Mathematical Modeling: Advances and Applications;pp.103-134</text>
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              <text>&lt;a href="https://doi.org/10.1016/B978-0-44-313317-6.00010-X" target="_blank" rel="noreferrer noopener"&gt;https://doi.org/10.1016/B978-0-44-313317-6.00010-X&lt;/a&gt; &lt;br /&gt;&lt;br /&gt;&lt;a href="https://www.scopus.com/pages/publications/105019743830?origin=resultslist" target="_blank" rel="noreferrer noopener"&gt;https://www.scopus.com/pages/publications/105019743830?origin=resultslist&lt;/a&gt;</text>
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              <text>Myson S., Center for Mathematical Needs, Department of Mathematics, CHRIST (Deemed to be University), Karnataka, Bengaluru, India</text>
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              <text>In this chapter, magnetohydrodynamic flow (MHD) and heat transfer in a multilayer vertical channel are studied with one phase containing pure water and the other phase containing oil-based Cu nanofluid. The effects of viscous dissipation and Joule heating are included in the energy equation. The modeled equations are coupled and nonlinear; they are solved using the regular perturbation method (RPM) and the differential transform method (DTM). The analysis examines the impact of the Hartmann number, thermal Grashof number, nanoparticle volume fraction (NVF), and Brinkman number on the Nusselt number, velocity, and temperature distributions. Furthermore, an optimization of the Nusselt number is performed for three different levels of the Hartmann number (5?M?6), the Brinkman number (0.1?Br?0.3), and the NVF (1%???3%) using the Response Surface Methodology (RSM). The Hartmann number and NVF were found to suppress flow, while the thermal Grashof number and the Brinkman number increase the flow field. Sensitivity computations reveal that the Nusselt number on the left wall is more sensitive to the Hartmann number and the NVF, while the Nusselt number of the right wall is more sensitive to the Brinkman number and NVF.  2025 Elsevier Inc. All rights are reserved, including those for text and data mining, AI training, and similar technologies.</text>
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              <text>Differential transform method; Heat transfer; Multilayer flow; Nanofluid; Response surface methodology; Sensitivity analysis</text>
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              <text>ISBN: 978-044313317-6; 978-044313316-9;</text>
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              <text>Restricted Access; Hardcopy may be available in the library</text>
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