Fully localized post-buckling states of cylindrical shells under axial compression

We compute nonlinear force equilibrium solutions for a clamped thin cylindrical shell under axial compression. The equilibrium solutions are dynamically unstable and located on the stability boundary of the unbuckled state. A fully localized single dimple deformation is identified as the edge state—the attractor for the dynamics restricted to the stability boundary. Under variation of the axial load, the single dimple undergoes homoclinic snaking in the azimuthal direction, creating states with multiple dimples arranged around the central circumference. Once the circumference is completely filled with a ring of dimples, snaking in the axial direction leads to further growth of the dimple pattern. These fully nonlinear solutions embedded in the stability boundary of the unbuckled state constitute critical shape deformations. The solutions may thus be a step towards explaining when the buckling and subsequent collapse of an axially loaded cylinder shell is triggered.

[1]  T. Schneider,et al.  Homoclinic snaking in plane Couette flow: bending, skewing and finite-size effects , 2015, Journal of Fluid Mechanics.

[2]  J. Michael T. Thompson,et al.  Shock-Sensitivity in Shell-Like Structures: With Simulations of Spherical Shell Buckling , 2015, Int. J. Bifurc. Chaos.

[3]  Edgar Knobloch,et al.  Spatial Localization in Dissipative Systems , 2015 .

[4]  J. Thompson Advances in Shell Buckling: Theory and Experiments , 2014, Int. J. Bifurc. Chaos.

[5]  E. Knobloch,et al.  Convectons and secondary snaking in three-dimensional natural doubly diffusive convection , 2013 .

[6]  S. Residori,et al.  Homoclinic snaking of localized patterns in a spatially forced system. , 2011, Physical review letters.

[7]  John W. Hutchinson,et al.  Knockdown factors for buckling of cylindrical and spherical shells subject to reduced biaxial membrane stress , 2010 .

[8]  T. Schneider,et al.  Snakes and ladders: localized solutions of plane Couette flow. , 2009, Physical review letters.

[9]  E. Knobloch,et al.  Eckhaus instability and homoclinic snaking. , 2008, Physical review. E, Statistical, nonlinear, and soft matter physics.

[10]  Alan R. Champneys,et al.  Localized Hexagon Patterns of the Planar Swift-Hohenberg Equation , 2008, SIAM J. Appl. Dyn. Syst..

[11]  Mark A. Peletier,et al.  Numerical Variational Methods Applied to Cylinder Buckling , 2008, SIAM J. Sci. Comput..

[12]  T. Schneider State Space Properties of Transitional Pipe Flow , 2007 .

[13]  B. Eckhardt,et al.  Edge of chaos in pipe flow. , 2006, Chaos.

[14]  Edgar Knobloch,et al.  Spatially localized binary-fluid convection , 2006, Journal of Fluid Mechanics.

[15]  J. Yorke,et al.  Edge of chaos in a parallel shear flow. , 2006, Physical review letters.

[16]  M. Peletier,et al.  Cylinder Buckling: The Mountain Pass as an Organizing Center , 2005, SIAM J. Appl. Math..

[17]  G. Hunt Buckling in Space and Time , 2006 .

[18]  W. E,et al.  Finite temperature string method for the study of rare events. , 2002, The journal of physical chemistry. B.

[19]  Tomoaki Itano,et al.  A periodic-like solution in channel flow , 2003, Journal of Fluid Mechanics.

[20]  Mark A. Peletier,et al.  Cylindrical shell buckling: a characterization of localization and periodicity , 2003 .

[21]  G. W. Hunt,et al.  Cellular Buckling in Long Structures , 2000 .

[22]  Alan R. Champneys,et al.  Computation of Homoclinic Orbits in Partial Differential Equations: An Application to Cylindrical Shell Buckling , 1999, SIAM J. Sci. Comput..

[23]  Alan R. Champneys,et al.  Homoclinic and Heteroclinic Orbits Underlying the Post-Buckling of axially Compressed Cylindrical Shells , 1999 .

[24]  Bengt Fornberg,et al.  Classroom Note: Calculation of Weights in Finite Difference Formulas , 1998, SIAM Rev..

[25]  B. Fornberg CALCULATION OF WEIGHTS IN FINITE DIFFERENCE FORMULAS∗ , 1998 .

[26]  Alan R. Champneys,et al.  Computation of localized post buckling in long axially compressed cylindrical shells , 1997, Philosophical Transactions of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[27]  Steven J. Ruuth,et al.  Implicit-explicit methods for time-dependent partial differential equations , 1995 .

[28]  Y. Choi,et al.  A mountain pass method for the numerical solution of semilinear elliptic problems , 1993 .

[29]  G. Simitses,et al.  Elastic stability of circular cylindrical shells , 1984 .

[30]  John E. Dennis,et al.  Numerical methods for unconstrained optimization and nonlinear equations , 1983, Prentice Hall series in computational mathematics.

[31]  Martin Golubitsky,et al.  Boundary conditions and mode jumping in the buckling of a rectangular plate , 1979 .

[32]  J. Swift,et al.  Hydrodynamic fluctuations at the convective instability , 1977 .

[33]  W. T. Koiter THE STABILITY OF ELASTIC EQUILIBRIUM , 1970 .

[34]  Johann Arbocz,et al.  The effect of general imperfections on the buckling of cylindrical shells , 1968 .