Biophysical studies of membrane proteins/peptides. Interaction with ...
Biophysical studies of membrane proteins/peptides. Interaction with ...
Biophysical studies of membrane proteins/peptides. Interaction with ...
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signal for neighbouring cells to phagocytose the dead cell and digest it (Alberts et al.,<br />
2002).<br />
1.4. Lipid structure and curvature<br />
Lipids in hydrated conditions exhibit polymorphic behaviour as they can assemble<br />
in different structures. The structure adopted by a lipid aggregate can be influenced by<br />
the molecular structure <strong>of</strong> the lipid itself and a myriad <strong>of</strong> environmental conditions,<br />
such as water content, pH, ionic strength, temperature and pressure. Lipid molecules can<br />
assemble in an aqueous environment either in a lamellar structure (as in a lipid bilayer)<br />
or in non-lamellar phases (micelle, hexagonal, inverted hexagonal phases, and the cubic<br />
phase (see Fig. I.4)). Because phase transitions between these different aggregates can<br />
be activated by changes in water content, these phases are called lyotropic.<br />
The different possibilities for organizations <strong>of</strong> lipids are the result <strong>of</strong> the intrinsic<br />
shape <strong>of</strong> the lipid molecule. When the headgroup <strong>of</strong> a lipid occupies the same area than<br />
the area occupied by its hydrophobic section, the leaflets or monolayers formed by<br />
association <strong>of</strong> molecules <strong>of</strong> this lipid will present zero spontaneous curvature, forming a<br />
planar <strong>membrane</strong> for which both leaflets (or monolayers) present null curvature. A lipid<br />
bilayer composed <strong>of</strong> this lipid <strong>with</strong> the same number <strong>of</strong> molecules in each monolayer<br />
should be flat. However, in order to eliminate the aqueous exposure <strong>of</strong> the hydrophobic<br />
edges <strong>of</strong> the bilayer, the bilayer can unite the edges and form a curved vesicle. In this<br />
aggregate the exterior monolayer must present a concave (or positive) curvature and the<br />
interior monolayer must present a curvature <strong>with</strong> opposite direction. In this way,<br />
spontaneous curvature <strong>of</strong> a lipid monolayer refers to the curvature observed in the<br />
absence <strong>of</strong> edge conditions (Zimmerberg, 2000).<br />
For monolayers composed <strong>of</strong> lipids presenting headgroups <strong>with</strong> a cross-section<br />
different to that <strong>of</strong> the hydrophobic tails, a spontaneous curvature will be present, and<br />
the packing <strong>of</strong> these lipids in a lipid bilayer <strong>with</strong> a lamellar structure will result in<br />
curvature stress, that can be supported by the lamellar structure only up to a certain<br />
extent. In case the lipid bilayer cannot sustain this curvature stress, the lamellar<br />
structure (L) will be broken and non-lamellar phases will arise. The basic structural<br />
phase <strong>of</strong> biological <strong>membrane</strong>s is nevertheless a lamellar phospholipid bilayer matrix,<br />
and deviations from a lamellar arrangement are generally not desirable in the plasma<br />
<strong>membrane</strong>. The inclusion <strong>of</strong> lipids <strong>with</strong> propensity to non-lamellar structure leads to a<br />
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