Buckling of an axisymmetric vesicle under compression: the effects of resistance to shear

We consider the axisymmetric deformation of an initially spherical, porous vesicle with incompressible membrane having finite resistance to in-plane shearing, as the vesicle is compressed between parallel plates. We adopt a thin-shell balance-of-forces formulation in which the mechanical properties...

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Bibliographic Details
Main Authors: Preston, S.P (Author), Jensen, O.E (Author), Richardson, Giles (Author)
Format: Article
Language:English
Published: 2007-12-01.
Subjects:
Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Preston, S.P.  |e author 
700 1 0 |a Jensen, O.E.  |e author 
700 1 0 |a Richardson, Giles  |e author 
245 0 0 |a Buckling of an axisymmetric vesicle under compression: the effects of resistance to shear 
260 |c 2007-12-01. 
856 |z Get fulltext  |u https://eprints.soton.ac.uk/156323/1/PUBLISHED.pdf 
520 |a We consider the axisymmetric deformation of an initially spherical, porous vesicle with incompressible membrane having finite resistance to in-plane shearing, as the vesicle is compressed between parallel plates. We adopt a thin-shell balance-of-forces formulation in which the mechanical properties of the membrane are described by a single dimensionless parameter, C, which is the ratio of the membrane's resistance to shearing to its resistance to bending. This results in a novel free-boundary problem which we solve numerically to obtain vesicle shapes as a function of plate separation, h. For small deformations, the vesicle contacts each plate over a small circular area. At a critical value of plate separation, hTC, there is a transcritical bifurcation from which a new branch of solutions emerges, representing buckled vesicles which contact each plate along a circular curve. For the values of C investigated, we find that the transcritical bifurcation is subcritical and that there is a further saddle-node bifurcation (fold) along the branch of buckled solutions at h = hSN (where hSN > hTC). The resulting bifurcation structure is commensurate with a hysteresis loop in which a sudden transition from an unbuckled solution to a buckled one occurs as h is decreased through hTC and a further sudden transition, this time from a buckled solution to an unbuckled one, occurs as h is increased through hSN. We find that hSN and hTC increase with C, that is, vesicles that resist shear are more prone to buckling.  
655 7 |a Article