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Cellular dewetting refers to the process of
nucleation In thermodynamics, nucleation is the first step in the formation of either a new thermodynamic phase or structure via self-assembly or self-organization within a substance or mixture. Nucleation is typically defined to be the process that de ...
and enlargement of transendothelial cell macroaperture (TEM) tunnels in
endothelial cells The endothelium is a single layer of squamous endothelial cells that line the interior surface of blood vessels and lymphatic vessels. The endothelium forms an interface between circulating blood or lymph in the lumen and the rest of the ves ...
(Figure 1). This phenomenon is analogous to the nucleation and growth of dry patches in viscous liquids spreading on a non-wettable substrate (Figure 2). Cellular dewetting is triggered by several protein toxins from
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, notably the EDIN-like factors from ''Staphylococcus aureus'' and from ''Clostridium botulinum'', as well as edema toxin from ''Bacillus anthracis''. TEMs form in response to the rupture of
cytoskeleton The cytoskeleton is a complex, dynamic network of interlinking protein filaments present in the cytoplasm of all cells, including those of bacteria and archaea. In eukaryotes, it extends from the cell nucleus to the cell membrane and is comp ...
physical connections through the
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due to inhibition of the RhoA/ROCK pathway or to induction of the flux of cyclic-AMP ( cAMP) broad
signaling molecule In biology, cell signaling (cell signalling in British English) or cell communication is the ability of a cell to receive, process, and transmit signals with its environment and with itself. Cell signaling is a fundamental property of all cellula ...
.


Physics behind cellular dewetting

The phenomenon of cellular dewetting can be interpreted by physical modeling (Figure 2). The driving force responsible for the spontaneous formation of TEM tunnels and their opening is the membrane tension that results from the spreading of cells due to actomyosin relaxation. Opposite to liquid dewetting, TEMs reach a maximum diameter, at which the driving force is balanced by a resisting force that develops along TEM edges (Figure 2). This resisting force is referred to as line tension and is uncharacterized at the molecular level.


Physical parameters

Driving forces pulling on a tunnel of radius ''R'', as depicted in Figure 2. Here, pulling is due to the tensioning of the
cell membrane The cell membrane (also known as the plasma membrane (PM) or cytoplasmic membrane, and historically referred to as the plasmalemma) is a biological membrane that separates and protects the interior of all cells from the outside environment (the ...
(σ) that is partly counteracted by a line tension around the tunnel (''T''). In these conditions, the net driving force (''FD'') consists of two contributions: F_D = \sigma - \frac{R} Dewetting proceeds if ''FD''>0. Membrane tension (''σ'') depends on the tunnel radius ''R''. A tunnel increase in size relaxes the
membrane A membrane is a selective barrier; it allows some things to pass through but stops others. Such things may be molecules, ions, or other small particles. Membranes can be generally classified into synthetic membranes and biological membranes. ...
, inducing a decrease in membrane tension, as described by Helfrich’s law. Line tension (''T'') corresponds to the resisting force along the edge of the tunnel that opposes membrane tension and limits dewetting. This line tension can have physical and molecular components.


References

Cell biology Biophysics