TY - JOUR
T1 - Dynamic stability of non‐linear shells of revolution under consideration of the fluid–soil–structure interaction
AU - Wunderlich, W.
AU - Schäpertöns, B.
AU - Temme, C.
PY - 1994/8/15
Y1 - 1994/8/15
N2 - The dynamic behaviour of liquid‐filled shells of revolution is investigated considering the soil–structure interaction and the fluid–structure interaction, respectively. In the circumferential direction the loads and variables are approximated by Fourier series. The shell is modelled through shell ring elements including non‐linear behaviour, coupled with isoparametric continuum ring elements and special infinite elements for the soil and isoparametric pressure ring elements for the fluid. Transient loadings like earthquake excitation and the non‐linearities of the shell and the soil require an analysis in the time domain. To reduce the size of the problem, linear parts of the system are condensed by the substructure technique. The soil region is divided into two parts, a near field permitting non‐linearities like plastification or uplifting of the shell, and a far field for the treatment of radiation of energy. The boundary conditions for the shell footing have a strong influence on the distribution of the axial membrane forces and, hence, on the stability limit, which is mostly governed by plastic collapse and caused by the dynamically activated pressure acting on the tank wall. It is shown how the soil properties influence the dynamic stability of the shell under harmonic excitation and under realistic earthquake motion.
AB - The dynamic behaviour of liquid‐filled shells of revolution is investigated considering the soil–structure interaction and the fluid–structure interaction, respectively. In the circumferential direction the loads and variables are approximated by Fourier series. The shell is modelled through shell ring elements including non‐linear behaviour, coupled with isoparametric continuum ring elements and special infinite elements for the soil and isoparametric pressure ring elements for the fluid. Transient loadings like earthquake excitation and the non‐linearities of the shell and the soil require an analysis in the time domain. To reduce the size of the problem, linear parts of the system are condensed by the substructure technique. The soil region is divided into two parts, a near field permitting non‐linearities like plastification or uplifting of the shell, and a far field for the treatment of radiation of energy. The boundary conditions for the shell footing have a strong influence on the distribution of the axial membrane forces and, hence, on the stability limit, which is mostly governed by plastic collapse and caused by the dynamically activated pressure acting on the tank wall. It is shown how the soil properties influence the dynamic stability of the shell under harmonic excitation and under realistic earthquake motion.
UR - http://www.scopus.com/inward/record.url?scp=0028486517&partnerID=8YFLogxK
U2 - 10.1002/nme.1620371510
DO - 10.1002/nme.1620371510
M3 - Article
AN - SCOPUS:0028486517
SN - 0029-5981
VL - 37
SP - 2679
EP - 2697
JO - International Journal for Numerical Methods in Engineering
JF - International Journal for Numerical Methods in Engineering
IS - 15
ER -