Abstract
The solution is based on small deflection theory, and it is assumed that the stresses are always below the proportional limit. The material for both the faces and the core is considered isotropic. Three equations of equilibrium, derived by means of the principle of virtual displacements, form the starting point of the theory. The equilibrium equations are partial linear differential equations with constant coefficients—two are of the second order, and the third is of the fourth order. Both the equations of equilibrium and 16 boundary conditions are satisfied identically.
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
