TY - JOUR
T1 - Hamiltonian system and post buckling of elastic cylindrical shells under the heat shock
AU - Yang, Chang-Yu
AU - Xu, Xin-Sheng
AU - Lim, Chee-Wah
PY - 2013/12
Y1 - 2013/12
N2 - Based on the Donnell theory, thermal elasticity, large deflection theory and energy principle, a Hamiltonian system was presented for the buckling of shells under thermal shock. The buckling problem was divided into two stages, namely, pre-buckling and post-buckling. In the Hamiltonian system, generalized eigenvalues and symplectic eigensolution correspond to critical temperatures and buckling modes, respectively. Based on symplectic eigensolutions, computational formulas for post-buckling of shells under thermal shock were derived using adjoint symplectic orthogonality and symplectic expansion theorem. Thus, a numerical method is formed. The numerical results describe the whole process of buckling development for cylindrical shells. The results show that the post buckling evolvement depends highly on the source location, distribution, boundary conditions, intensity of heat source, material parameters, and geometrical shape of shells. Besides, the buckling mode is developing from lower to higher order and finally tends to vibration mode.
AB - Based on the Donnell theory, thermal elasticity, large deflection theory and energy principle, a Hamiltonian system was presented for the buckling of shells under thermal shock. The buckling problem was divided into two stages, namely, pre-buckling and post-buckling. In the Hamiltonian system, generalized eigenvalues and symplectic eigensolution correspond to critical temperatures and buckling modes, respectively. Based on symplectic eigensolutions, computational formulas for post-buckling of shells under thermal shock were derived using adjoint symplectic orthogonality and symplectic expansion theorem. Thus, a numerical method is formed. The numerical results describe the whole process of buckling development for cylindrical shells. The results show that the post buckling evolvement depends highly on the source location, distribution, boundary conditions, intensity of heat source, material parameters, and geometrical shape of shells. Besides, the buckling mode is developing from lower to higher order and finally tends to vibration mode.
KW - Buckling mode
KW - Cylindrical shell
KW - Hamiltonian system
KW - Post buckling
KW - Thermal shock
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M3 - RGC 22 - Publication in policy or professional journal
SN - 1005-3026
VL - 34
SP - 179
EP - 183
JO - Dongbei Daxue Xuebao/Journal of Northeastern University
JF - Dongbei Daxue Xuebao/Journal of Northeastern University
IS - SUPPL.2
ER -