The analysis of structurally orthotropic shells by means of the compliance method
Structurally orthotropic shells analyzed by compliance method
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Structurally orthotropic shells analyzed by compliance method
Membrane stresses and equilibrium of orthotropic cylindrical shells with large deformations
Analysis of linear elastic thin shells of revolution subjected to arbitrary temperatures and loads - computer program users manual
Fatigue and fracture in elastic cylindrical shells with circumferential crack under axial tension, noting precracked specimens
Liquid instability of vibrating partially filled elastic tank emphasizing resonant breathing mode and frequency response
Linear shell theory elastic constant instability conditions for symmetrically loaded shells of revolution
A method is developed to compute frequency response and acoustic radiation of a complex shell. The axisymmetric geometry of the shell includes cylindrical, conical, and spherical segments stiffened by discrete rings and bulkheads. The shell is coupled to internal masses and elastic frames. Shell segments are treated by transfer matrices. Rings, bulkheads, frames, and concentrated masses are treated by impedances at junctions of segments. The shell is coupled to an external acoustic fluid treated by Green's function and curved surface elements. A major issue facing the method's treatment of the fluid would be lack of existence or uniqueness encountered in the uncoupled, external acoustic problem at characteristic wavenumbers. By using a simple spherical shell, without internal structures, this potential hindrance is shown not to arise. A fuller application of the method awaits subsequent results.
Buckling and initial postbuckling behavior of thin elastic cylindrical shells of elliptical cross section
Elastic stability of clamped shallow spherical shells under concentrated load, noting buckling modes
Cylindrical shell stability under axisymmetric moving loads
Linear shell theory for nonlinear transverse coupled vibrations of partially filled circular cylindrical elastic tank
Computer program for determining static and dynamic response of symmetrically loaded elastic orthotropic shells of revolution
Linear shell theory for nonlinear transverse coupled vibrations of partially filled circular cylindrical elastic tank
Users manual on static and dynamic computer programs on linear elastic thin shell theory - Apollo command module water impact
Elastic stability of clamped shallow spherical shells under concentrated load, noting buckling modes
A model of Io is presented that consists of an elastic inner core, a low strength asthenosphere, and a thin elastic outer shell. The middle layer is ssumed to posses negligible shear strength and to be characterized by a Newtonian viscosity. The fluid in the viscous layer is forced to circulate mainly by the tidal distortion in the outer shell, modeled here as a variation in the distortion amplitude. As a result, heat is generated in the fluid by viscous dissipation. There are three important unconstrained parameters in the model: the fluid viscosity, the thickness of the fluid layer, and the degree to which the distortion of the outer shell is affected by the fluid viscosity. For a wide range of these model parameters viscous heating can generate just as much or even more heat than does elastic dissipation is the outer shell. The model suggests that much of Io's heat flow may be generated below the outer shell and could provide a source of energy for any silicate volcanism on the satellite.
Nonlinear theory for equilibrium deformation of shells compared with classical three-dimensional theory of elasticity
Conical shell theory and piston theory aerodynamics are used to study the aeroelastic stability of the thermal protection system (TPS) on the NASA Hypersonic Inflatable Aerodynamic Decelerator (HIAD). Structural models of the TPS consist of single or multiple orthotropic conical shell systems resting on several circumferential linear elastic supports. The shells in each model may have pinned (simply-supported) or elastically-supported edges. The Lagrangian is formulated in terms of the generalized coordinates for all displacements and the Rayleigh-Ritz method is used to derive the equations of motion. The natural modes of vibration and aeroelastic stability boundaries are found by calculating the eigenvalues and eigenvectors of a large coefficient matrix. When the in-flight configuration of the TPS is approximated as a single shell without elastic supports, asymmetric flutter in many circumferential waves is observed. When the elastic supports are included, the shell flutters symmetrically in zero circumferential waves. Structural damping is found to be important in this case. Aeroelastic models that consider the individual TPS layers as separate shells tend to flutter asymmetrically at high dynamic pressures relative to the single shell models. Several parameter studies also examine the effects of tension, orthotropicity, and elastic support stiffness.