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Oil solubilization:
→
loading lipid phases with hydrophobic component
→
increasing negative curvature
bicontinuous cub ic (V
2
)
→
reverse hexagonal (H
2
)
→
reverse microemulsion (L
2
)
Bulk systems:
Dispersed systems:
cubosomes
hexosomes
→
emulsified microemulsion
Tuning back:
addition of surfactant
decreasing negative curvature
cubosomes
hexosomes
emulsified microemulsion
Figure 5.14
Tuning back the curvature of oil-loaded self-assembled nanostructures.
1
β
= 100
β
= 75
β
= 25
= 0
β
0
1
2
3
4
q [nm
-1
]
Figure 5.15
Effect of DGMO content on the SAXS curves of TC-loaded aqueous
dispersions at 25°C for
values ranging from 0 to 100. The intensities
have been shifted by a constant arbitrary factor for the sake of visibility. [Reprinted
from Yaghmur et al. (2006b) .]
α
=
6, and with
β
DGMO, at
α
=
6, promoted a reversed transition (from hexosomes at
β
=
0
and 25 back to cubosomes at
50 and 100), thus rendering the spontaneous
curvature of the oil-loaded interior less negative. However, an amount of
DGMO (
β
=
50) higher than that of oil was needed to overcome the effect of
TC, which indicates that TC had a larger impact on the internal structure than
DGMO. At a higher content of solubilized TC [at
β
=
α
=
75 as presented in
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