Abstract

Self-assembly of biomembranes results from the intricate interactions between water and the lipids’ hydrophilic head groups. Therefore, the lipid–water interplay strongly contributes to modulating membrane architecture, lipid diffusion, and chemical activity. Here, we introduce a new method of obtaining dehydrated, phase-separated, supported lipid bilayers (SLBs) solely by controlling the decrease of their environment’s relative humidity. This facilitates the study of the structure and dynamics of SLBs over a wide range of hydration states. We show that the lipid domain structure of phase-separated SLBs is largely insensitive to the presence of the hydration layer. In stark contrast, lipid mobility is drastically affected by dehydration, showing a 6-fold decrease in lateral diffusion. At the same time, the diffusion activation energy increases approximately 2-fold for the dehydrated membrane. The obtained results, correlated with the hydration structure of a lipid molecule, revealed that about six to seven water molecules directly hydrating the phosphocholine moiety play a pivotal role in modulating lipid diffusion. These findings could provide deeper insights into the fundamental reactions where local dehydration occurs, for instance during cell–cell fusion, and help us better understand the survivability of anhydrobiotic organisms. Finally, the strong dependence of lipid mobility on the number of hydrating water molecules opens up an application potential for SLBs as very precise, nanoscale hydration sensors.

Highlights

  • Biological cell membranes are dynamic barriers composed of a large variety of lipids and embedded with various proteins

  • In the experiments we considered three levels of membrane hydration, described in detail in the Experimental Section and schematically depicted in Figure 1B: (i) fully hydrated supported lipid bilayers (SLBs), where the membrane is submerged in bulk water, (ii) SLB for which most of the bulk water was pipetted out and the sample was left open to equilibrate to room humidity (∼30% RH), and (iii) SLB for which bulk water was removed to the highest extent and the sample was immediately exposed to a N2 atmosphere with ∼90% RH

  • The domain size, distribution, and shape are typical of liquid disordered (Ld)/liquid ordered (Lo) phaseseparated SLBs prepared in such conditions, in full agreement with previous reports.[58]

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Summary

Introduction

Biological cell membranes are dynamic barriers composed of a large variety of lipids and embedded with various proteins. Hydrophobic mismatch is considered to be one of the key physicochemical mechanisms that regulate membrane organization and promotes nanoscopic and microscopic separation of liquid ordered (Lo) and liquid disordered (Ld) phases It determines the position and orientation of transmembrane proteins in both model and living cell membranes.[6] The thin layer of water that directly hydrates the membrane, commonly referred to as biological water,[11,12] has been proven to actively participate in the biological functioning of DNA.[13] biological water is inherently connected with the process of protein folding,[14] aggregation,[15,16] and stabilization of the structure even in extreme thermodynamic conditions.[17] Numerous experiments aimed at understanding the properties of biological water, using nuclear magnetic resonance,[18] X-ray

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