TY - CHAP
T1 - An Extended Kirchhoff–Love Shell Model with Out-of-Plane Normal Stress
T2 - Out-of-Plane Deformation
AU - Taniguchi, Yasutoshi
AU - Takizawa, Kenji
AU - Otoguro, Yuto
AU - Tezduyar, Tayfun E.
N1 - Publisher Copyright:
© The Author(s), under exclusive license to Springer Nature Switzerland AG 2023.
PY - 2023
Y1 - 2023
N2 - In this chapter on a hyperelastic extended Kirchhoff–Love shell model with out-of-plane normal stress, we present the derivation of the new model, with focus on the mechanics of the out-of-plane deformation. Accounting for the out-of-plane normal stress distribution in the out-of-plane direction affects the accuracy in calculating the deformed-configuration out-of-plane position, and consequently the nonlinear response of the shell. The improvement is beyond what we get from accounting for the out-of-plane deformation mapping. By accounting for the out-of-plane normal stress, the traction acting on the shell can be specified on the upper and lower surfaces separately. With that, the new model is free from the “midsurface” location in terms of specifying the traction. We also present derivations related to the variation of the kinetic energy and the form of specifying the traction and moment acting on the upper and lower surfaces and along the edges. We present test computations for unidirectional plate bending. We use the neo-Hookean and Fung’s material models, for the compressible- and incompressible-material cases, and with the out-of-plane normal stress and without, which is the plane-stress case.
AB - In this chapter on a hyperelastic extended Kirchhoff–Love shell model with out-of-plane normal stress, we present the derivation of the new model, with focus on the mechanics of the out-of-plane deformation. Accounting for the out-of-plane normal stress distribution in the out-of-plane direction affects the accuracy in calculating the deformed-configuration out-of-plane position, and consequently the nonlinear response of the shell. The improvement is beyond what we get from accounting for the out-of-plane deformation mapping. By accounting for the out-of-plane normal stress, the traction acting on the shell can be specified on the upper and lower surfaces separately. With that, the new model is free from the “midsurface” location in terms of specifying the traction. We also present derivations related to the variation of the kinetic energy and the form of specifying the traction and moment acting on the upper and lower surfaces and along the edges. We present test computations for unidirectional plate bending. We use the neo-Hookean and Fung’s material models, for the compressible- and incompressible-material cases, and with the out-of-plane normal stress and without, which is the plane-stress case.
UR - http://www.scopus.com/inward/record.url?scp=85177657476&partnerID=8YFLogxK
U2 - 10.1007/978-3-031-36942-1_12
DO - 10.1007/978-3-031-36942-1_12
M3 - Chapter
AN - SCOPUS:85177657476
T3 - Modeling and Simulation in Science, Engineering and Technology
SP - 389
EP - 435
BT - Modeling and Simulation in Science, Engineering and Technology
PB - Birkhauser
ER -