| نویسندگان | محمد عارفی,سینا کیانی مقدم,الیاس محمدرضایی بیدگلی,مسعود کیانی,Omer Civalek |
| نشریه | COMPOS STRUCT |
| شماره صفحات | 112924 |
| شماره مجلد | 255 |
| ضریب تاثیر (IF) | 5.407 |
| نوع مقاله | Full Paper |
| تاریخ انتشار | 2021-01-01 |
| رتبه نشریه | علمی - پژوهشی |
| نوع نشریه | الکترونیکی |
| کشور محل چاپ | ایران |
| نمایه نشریه | JCR ,SCOPUS |
| کلید واژه ها | Thermo‐elastic analysis Halpin‐Tsai model First‐order shear deformation theory Graphene nanoplatelets (GPLs) Functionally graded materials |
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چکیده مقاله
Analysis of graphene nanoplatelets (GPLs) reinforced cylindrical shell subjected to thermo‐mechanical loads is
studied in this paper based on shear deformation theory. Halpin‐Tsai micromechanical model and rule of mix-
tures are used for calculation of effective material properties of composite materials with different distributions
of reinforcements including uniform symmetric and asymmetric distributions for nanoplatelet material. The
various distributions are included UD (uniform distribution of GPLs along the thickness direction), FG‐O
(linear variation of GPLs, where highest amount is locates at middle layer) and FG‐X(linear variation of
GPLs, where highest amount is locates at top and bottom layers). The shear strains especially at both ends
of cylindrical shell are included in our formulation using the two‐dimensional first‐order shear deformation
theory (FSDT). Minimum total potential energy principle is used to derive the governing equations using
Hooke’s law and application of Euler equations using the functional of the system. Eigenvalue and eigenvector
method is used for solution of the governing equations. The radial and axial displacements and various com-
ponents of stress are calculated in terms of number of layers, GPLs weight fraction, thermal loading, various
distributions of reinforcement and coefficient of the elastic foundation. The numerical results indicate that
maximum and minimum stresses are obtained for FG‐O and FG‐X distributions. Also, the biggest and lowest
radial displacements are obtained for UD and FG‐X distributions, respectively.