A Linear, First-order Shell Model for Transverse Isotropic Material under a Uniform Change of Temperature

Author(s):  
Andreas Pomp
2021 ◽  
pp. 108128652097848
Author(s):  
GY Zhang ◽  
X-L Gao

A new non-classical model for first-order shear deformation circular cylindrical thin shells is developed by using a modified couple stress theory and a surface elasticity theory. Through a variational formulation based on Hamilton’s principle, the equations of motion and boundary conditions are simultaneously obtained, and the microstructure and surface energy effects are treated in a unified manner. The newly developed non-classical shell model contains one material length-scale parameter to account for the microstructure effect and three surface elastic constants to capture the surface energy effect. The new model includes shell models considering the microstructure effect only or the surface energy effect alone as special cases and recovers the first-order shear deformation circular cylindrical thin shell model based on classical elasticity as a limiting case. In addition, the current shell model reduces to the non-classical model for Mindlin plates incorporating the microstructure and surface energy effects when the thin shell radius tends to infinity. To illustrate the new model, the static bending and free vibration problems of a simply supported circular cylindrical thin shell are analytically solved. The numerical results reveal that the inclusion of the microstructure and surface energy effects leads to reduced shell deflections and rotation angles and increased natural frequencies. The differences are significant when the shell is very thin, but they diminish as the shell thickness increases. These predicted size effects at the micron scale agree with the general trends observed in experiments.


First-order perturbation theory is used to derive the equations governing the normal inodes of vibrations of a crystal in which the atoms are polarizable. The method is based on the harmonic, electrostatic and adiabatic approximations, it is thus assumed that all phonon frequencies are much lower than the frequencies of electron transitions; the results therefore do not apply to metals. In the dipolar approximation the equations derived are found to be identical with those which have been obtained for the `shell model ’ of a crystal, and which are known to give results in rather good agreement with the measured dispersion relations for phonons in germanium and sodium iodide. The method is extended to include the interaction of quadrupole and higher moments of the electron distribution of anatom or ion.


2008 ◽  
Vol 23 (27n30) ◽  
pp. 2604-2607
Author(s):  
ATSUSHI UMEYA ◽  
GOUKI KANEKO ◽  
KAZUO MUTO

In a shell-model calculation with traditional effective charges, theoretical B(E2) values are larger than experimental values for neutron-rich carbon isotopes 16 C and 18 C . Using the shell-model with 2ħw excitations in the first order perturbation theory, we investigate the B(E2) values and the effective charges for stable and neutron-rich carbon isotopes.


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