Abstract

AbstractThe present investigation deals with the two-dimensional deformation in a thermoelastic micropolar solid with cubic symmetry at the interface of the semi-infinite semiconducting medium under photothermal theory. A mechanical force is applied along the interface. The analytic expressions for the components of normal displacement, temperature distribution, normal force stress, and tangential couple stress for a thermoelastic micropolar solid with cubic symmetry have been obtained using normal mode analysis technique. The effect of anisotropy, microrotation, and thermoelasticity on the derived components have been depicted graphically.

Highlights

  • A micropolar continuum is a collection of inter-connected particles in the form of small rigid bodies in which materials’ deformation is determined by both translational and rotational motion

  • Discussions, and conclusions For numerical computations, we consider the values of physical constants as, (1) For micropolar solid with cubic symmetry as (Kumar & Partap, 2010): A1 = 19.6 × 1010 N/m2, A2 = 11.7 × 1010 N/m2, A3 = 5.6 × 1010 N/m2, A4 = 4.3 × 1010 N/m2, B3 = 0.98 × 10−9N

  • The variations of numerical values for normal displacement, temperature distribution, normal force stress, and tangential couple stress are shown in Figures (2)–(5) for G-L theory by taking n0 = 0, the mechanical force with magnitude, P1 = 1.0, ω = ω0 + ιξ, ω0 = - 0.3, ξ = 0.1, and a = 0.9 for, Figure 2

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Summary

Introduction

A micropolar continuum is a collection of inter-connected particles in the form of small rigid bodies in which materials’ deformation is determined by both translational and rotational motion. Othman, Abo-Dahab, and Alosaimi (2016) investigated the two-dimensional problem of micropolar thermoelastic rotating medium possessing cubic symmetry under the effect of inclined load in the context of Green Naghdi theory of type-III. The effect of initial hydrostatic stress on the reflection of generalized thermoelastic waves from a solid half-space was studied by Singh, Kumar, and Singh (2006). The field equations and constitutive relations in the absence of body forces, body couples, and heat sources for medium I and medium II are given by, For medium I i.e. micropolar thermoelastic medium with cubic symmetry is given by Lord and Shulman (1967), Green and Lindsay (1972), and Minagawa et al (1981) as, P1 semi-infinite semiconducting medium (medium-II). Using above non-dimensional variables and dropping superscripts the Equations (1–7) becomes, h1

Solution of the problem
Boundary conditions
Conclusion
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