Ordering of lipid A-monophosphate clusters in aqueous solutions
In this investigation, a study of the self-assembly of electrostatically stabilized aqueous dispersions of nanometric lipid A-monophosphate clusters from Escherichia coli was carried out in three different volume-fraction regimes. The experimental techniques used in the investigation were osmotic pr...
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Veröffentlicht in: | The Journal of chemical physics 2007-09, Vol.127 (11), p.115103-115103-22 |
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Zusammenfassung: | In this investigation, a study of the self-assembly of electrostatically stabilized aqueous dispersions of nanometric lipid A-monophosphate clusters from
Escherichia coli
was carried out in three different volume-fraction regimes. The experimental techniques used in the investigation were osmotic pressure, static and quasielastic light scattering, scanning electron microscopy and transmission electron microscopy, and small-angle x-ray scattering. Experiments were carried out at low ionic strength (
I
=
0.1
-
5.0
mM
NaCl) at
25
°
C
. At volume fractions between
1.5
×
10
−
4
⩽
ϕ
⩽
5.4
×
10
−
4
, the lipid A-monophosphate clusters had an average rms hydrodynamic diameter of
d
¯
=
7.5
nm
, and a weighted-average molecular weight of
(
1.78
±
0.23
)
×
10
5
g
mol
−
1
. Quasielastic light scattering (LS) experiments yield similar values for the particle size and particle size distribution compared to electron microscopy, small-angle x-ray scattering, and LS experiments. When the volume fraction was increased to a higher regime
5.4
×
10
−
4
⩽
ϕ
⩽
9.50
×
10
−
4
, much larger clusters of lipid A monophosphate formed. The clusters detected in this volume-fraction range were assembled from between 8 and 52 of the
d
¯
=
7.5
nm
clusters and the assemblies are densely packed in such a way that colloidal crystals composed of the monodisperse microspheres are in physical contact with their nearest neighbors. Clusters that formed in volume fractions between
10.0
×
10
−
4
⩽
ϕ
⩽
40.0
×
10
−
4
revealed a weighted-average molecular weight of
(
10.15
±
0.17
)
×
10
6
g
mol
−
1
and a hydrodynamic diameter of
∼
d
¯
=
70.6
nm
. The crossover volume fraction between the small and the large clusters appeared at
ϕ
cr
=
5.05
×
10
−
4
. In the intermediate volume-fraction range, the scattered intensity
I
(
Q
)
vs
Q
curves (light and x rays) showed asymptotic behavior. From the asymptotic curves, the scattered intensity, the relationship between the average mass and radius, and the fractal dimension
d
f
were determined. The
d
f
value, which was evaluated from the expression
I
(
Q
)
∝
R
G
d
f
, was found to be
1.67
±
0.03
, a value that was virtually independent of the ionic strength (
0.1
-
5.0
mM
NaCl) at
25
°
C
. Even at a very low ionic strength (
I
=
0.10
mM
NaCl), lipid A monophosphate formed a number of differently shaped clusters. Electron microscope images showed that two types of self-assembled clusters existed at the lowest volume-fraction range studied and also dominated the ima |
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ISSN: | 0021-9606 1089-7690 |
DOI: | 10.1063/1.2768524 |