Steel and Composite Structures

Volume 24, Number 2, 2017, pages 151-176

DOI: 10.12989/scs.2017.24.2.151

General equations for free vibrations of thick doubly curved sandwich panels with compressible and incompressible core using higher order shear deformation theory

M. Nasihatgozar, S.M.R. Khalili and K. Malekzadeh Fard

Abstract

This paper deals with general equations of motion for free vibration analysis response of thick three-layer doubly curved sandwich panels (DCSP) under simply supported boundary conditions (BCs) using higher order shear deformation theory. In this model, the face sheets are orthotropic laminated composite that follow the first order shear deformation theory (FSDT) based on Rissners-Mindlin (RM) kinematics field. The core is made of orthotropic material and its in-plane transverse displacements are modeled using the third order of the Taylor&#39;s series extension. It provides the potentiality for considering both compressible and incompressible cores. To find these equations and boundary conditions, Hamilton&#39;s principle is used. Also, the effect of trapezoidal shape factor for cross-section of curved panel element (1 &#177; <i>z/R</i>) is considered. The natural frequency parameters of DCSP are obtained using Galerkin Method. Convergence studies are performed with the appropriate formulas in general form for three-layer sandwich plate, cylindrical and spherical shells (both deep and shallow). The influences of core stiffness, ratio of core to face sheets thickness and radii of curvatures are investigated. Finally, for the first time, an optimum range for the core to face sheet stiffness ratio by considering the existence of in-plane stress which significantly affects the natural frequencies of DCSP are presented.

Key Words

sandwich panel; natural frequency; doubly curved; compressible core; incompressible core

Address

(1) M. Nasihatgozar: Department of Mechanical and Aerospace Engineering, Science and Research Branch, Islamic Azad University, Tehran, Iran;<br>(2) S.M.R. Khalili: Faculty of Mechanical Engineering, K.N. Toosi University of Technology, Tehran, Iran;<br>(3) S.M.R. Khalili: Department of Applied Mechanics, Indian Institute of Technolog Delhi, New Delhi, 110016, India;<br>(4) K. Malekzadeh Fard: Department of Structural Analysis and Simulation, Space Research Institute, Tehran, Iran.