4.7 Article

Multispherical shapes of vesicles highlight the curvature elasticity of biomembranes

Journal

ADVANCES IN COLLOID AND INTERFACE SCIENCE
Volume 301, Issue -, Pages -

Publisher

ELSEVIER
DOI: 10.1016/j.cis.2022.102613

Keywords

Synthetic biosystems; Lipid bilayers; Giant vesicles; Transbilayer asymmetry; Spontaneous curvature; Multispherical patterns

Funding

  1. German Federal Ministry of Education and Research (BMBF)
  2. Max Planck Society the Max Planck Institute of Colloids and Interfaces

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This review article summarizes previous studies and presents a comprehensive theory for the unusual multispherical shapes formed by giant lipid vesicles. The multispheres consist of large and small spheres and can be built up from variable numbers of these spheres depending on the sign of their spontaneous curvature. The geometry of the multispheres is governed by curvature elasticity and stability conditions. Future studies could investigate the response of multispheres to external forces, membrane fusion between spheres, and the morphological complexity arising from lipid phase separation.
Giant lipid vesicles form unusual multispherical or multi-balloon shapes consisting of several spheres that are connected by membrane necks. Such multispherical shapes have been recently observed when the two sides of the membranes were exposed to different sugar solutions. This sugar asymmetry induced a spontaneous curvature, the sign of which could be reversed by swapping the interior with the exterior solution. Here, previous studies of multispherical shapes are reviewed and extended to develop a comprehensive theory for these shapes. Each multisphere consists of large and small spheres, characterized by two radii, the large-sphere radius, R-l, and the small-sphere radius, R-s. For positive spontaneous curvature, the multisphere can be built up from variable numbers N-l and N-s of large and small spheres. In addition, multispheres consisting of N* = N-l + N-s equally sized spheres are also possible and provide examples for constant-mean-curvature surfaces. For negative spontaneous curvature, all multispheres consist of one large sphere that encloses a variable number Ns of small spheres. These general features of multispheres arise from two basic properties of curvature elasticity: the local shape equation for spherical membrane segments and the stability conditions for closed membrane necks. In addition, the (N-l + N-s)-multispheres can form several (N-l + N-s)-patterns that differ in the way, in which the spheres are mutually connected. These patterns may involve multispherical junctions consisting of individual spheres that are connected to more than two neighboring spheres. The geometry of the multispheres is governed by two polynomial equations which imply that (N-l + N-s)-multispheres can only be formed within a certain restricted range of vesicle volumes. Each (N-l + N-s)-pattern can be characterized by a certain stability regime that depends both on the stability of the closed necks and on the multispherical geometry. Interesting and challenging topics for future studies include the response of multispheres to locally applied external forces, membrane fusion between spheres to create multispherical shapes of higher-genus topology, and the enlarged morphological complexity of multispheres arising from lipid phase separation and intramembrane domains.

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