Abstract

Reaction-diffusion systems encapsulated within giant unilamellar vesicles (GUVs) can lead to shape oscillations of these vesicles as recently observed for the bacterial Min protein system. This system contains two Min proteins, MinD and MinE, which periodically attach to and detach from the GUV membranes, with the detachment being driven by ATP hydrolysis. Here, we address these shape oscillations within the theoretical framework of curvature elasticity and show that they can be understood in terms of a spontaneous curvature that changes periodically with time. We focus on the simplest case provided by a attachment-detachment kinetics that is laterally uniform along the membrane. During each oscillation cycle, the vesicle shape is transformed from a symmetric dumbbell with two subcompartments of equal size to an asymmetric dumbbell with two subcompartments of different size, followed by the reverse, symmetry-restoring transformation. This sequence of shapes is first analyzed within the spontaneous curvature model which is then extended to the area-difference-elasticity model by decomposing the spontaneous curvature into a local and nonlocal component. For both symmetric and asymmetric dumbbells, the two subcompartments are connected by a narrow membrane neck with a circular waistline. The radius of this waistline undergoes periodic oscillations, the time dependence of which can be reasonably well fitted by a single Fourier mode with an average time period of 56 s.

Highlights

  • In a recent experimental study, the Min protein system was encapsulated within giant unilamellar vesicles (GUVs) which were observed to undergo cyclic shape oscillations.[6]

  • We first focus on the spontaneous curvature model[10,11,12] and show that the vesicle shape oscillations can be understood in terms of a preferred or spontaneous membrane curvature that changes periodically in time

  • The simplest model is provided by the spontaneous curvature model in which the shape of a uniform vesicle membrane depends on two dimensionless parameters, the volume-toarea ratio v, see eqn (4), and the rescaled spontaneous curvature m% = mRve

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Summary

Introduction

In a recent experimental study, the Min protein system was encapsulated within GUVs which were observed to undergo cyclic shape oscillations.[6]. For this v-value, we study the possible vesicle shapes as we vary the spontaneous curvature m% and find both symmetric and asymmetric dumbbells for a certain range of m% -values. In these two figures, the symmetric and asymmetric dumbbells are displayed in blue and red color, respectively. We will first use the spontaneous curvature model, for which the GUV shapes are solely determined

Min proteins enclosed by GUVs
Spontaneous curvature model
Two independent shape parameters
Computational methods for stable vesicle shapes
Theoretical analysis of GUV shapes
Two branches of stable dumbbells
Two branches of the bending energy
Closing and opening of membrane necks
Time dependence of active shape oscillations
Modifications arising from area-difference-elasticity
Discussion

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