Abstract
The main aim of this article is to study the effect of gravity on piezo-thermoelasticity in the context of three phase lag (TPL) model with two-temperature. The governing equations of piezo-thermoelasticity in TPL model with two-temperature in the presence of gravity are solved by Normal mode analysis in half space and we calculate the stress, strain and displacement components. A cadmium selenide material has been considered for the numerical simulation and the result has been plotted graphically. The results obtained for both Lord Shulman (L–S) and TPL thermoelastic models are almost coincident to each other in case of strain, stress tensors and components of displacement but results differ in the case of one components of electric potentials due to the presence of gravity.
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Appendices
Appendix A
\({\text{A}}_{1} = \frac{{\left( {{\rho c}^{2} - {\text{C}}_{11} } \right){\upalpha }^{2} }}{{{\text{C}}_{44} }}\) | \({\text{A}}_{2} = \frac{{\left( {{\text{C}}_{13} + {\text{C}}_{14} } \right){\text{i}}\upalpha }}{{{\text{C}}_{44} }}\) | \({\text{A}}_{3} = \frac{{\uprho {\text{gi}}\upalpha }}{{{\text{C}}_{44} }}\) | \({\text{ A}}_{4} = \frac{{\left( {e_{31} + e_{15} } \right)i\alpha }}{{C_{44} }}\) |
\({\text{A}}_{5} = \frac{{\upbeta _{1} \left( {1 + {\text{a}}^{*} \upalpha ^{2} } \right){\text{i}}\upalpha }}{{{\text{C}}_{44} }}\) | \({\text{A}}_{6} = \frac{{{\text{a}}^{*}\upbeta _{1} {\text{i}}\upalpha }}{{{\text{C}}_{44} }} \) | \({\text{A}}_{7} = \left( {{\text{C}}_{44} + {\text{C}}_{13} } \right){\text{i}}\upalpha \) | \(A_{8} = \rho gi\alpha\) |
\(A_{9} = C_{33}\) | \(A_{10} = \left( {\rho c^{2} - C_{44} } \right)\alpha^{2}\) | \({\text{A}}_{11} = {\text{e}}_{33}\) | \(A_{12} = e_{15} \alpha^{2}\) |
\(A_{13} = \beta_{3} \left( {1 + a^{*} \alpha^{2} } \right)\) | \({\text{A}}_{14} = {\upbeta }_{3} {\text{a}}^{*}\) | \({\text{A}}_{15} = \left( {{\text{e}}_{15} + {\text{e}}_{31} } \right){\text{i}}\upalpha \) | \(A_{16} = \epsilon_{11} \alpha^{2}\) |
\(A_{17} = \epsilon_{33}\) | \(A_{18} = P_{3} (1 + a^{*} \alpha^{2}\)) | \(A_{19} = P_{3} a^{*}\) | \( A_{20} = i\alpha^{3} cK_{1} l_{1} - \alpha^{2} l_{2} K_{1}^{*}\) |
\({\text{A}}_{21} =\uprho {\text{c}}_{{\text{e}}} \left( {1 + {\text{a}}^{*} \upalpha ^{2} } \right)\upalpha ^{2} {\text{c}}^{2 }\) | \(A_{22} = \rho c_{e} a^{*} \alpha^{2} c^{2}\) | \({\text{A}}_{23} = {\text{K}}_{3}^{*} {\text{l}}_{2} - {\text{iK}}_{3} \upalpha {\text{cl}}_{1}\) | \({\text{A}}_{24} = {\text{T}}_{0}\upbeta _{1} {\text{i}}\upalpha ^{3} {\text{c}}^{2}\) |
\(A_{25} = T_{0} \beta_{3} \alpha^{2} c^{2}\) | \( A_{26} = P_{3} \alpha^{2} c^{2}\) |
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Appendix B
Appendix C
Appendix D
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Appendix E
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Kumari, S., Singh, M. & Sharma, S. Gravitational Effect on Piezo-Thermoelasiticity in the Context of Three Phase Lag Model with Two Temperature. Int. J. Appl. Comput. Math 9, 139 (2023). https://doi.org/10.1007/s40819-023-01617-0
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DOI: https://doi.org/10.1007/s40819-023-01617-0