6 research outputs found
Роль нових форм організації наукових досліджень у підвищенні інноваційного потенціалу НАН України
Здійснено порівняльний аналіз інноваційних розробок учених НАН України, частина яких перевершує показники зарубіжних або не має відповідних аналогів у світі, а також розглянуто значення нових форм організації наукових досліджень. Запропоновано першочергові заходи для підвищення ролі науки в інноваційному розвитку суспільства.Осуществлен сравнительный анализ инновационных разработок ученых НАН Украины, часть которых превосходит показатели зарубежных или не имеет соответствующих аналогов в мире, а также рассмотрено значение новых форм организации научных исследований. Предложены первоочередные меры по повышению роли науки в инновационном развитии общества.The comparative analysis of innovative developments of scientists of NAS of Ukraine, part of which excels foreign indexes or does not have proper analogues in the world is carried out. Value of new forms of scientific researche organization is determined. Primary measures are offered for the increase of science role in innovative development of society
Coverage and Disruption of Phospholipid Membranes by Oxide Nanoparticles
We
studied the interactions of silica and titanium dioxide nanoparticles
with phospholipid membranes and show how electrostatics plays an important
role. For this, we systematically varied the charge density of both
the membranes by changing their lipid composition and the oxide particles
by changing the pH. For the silica nanoparticles, results from our
recently presented fluorescence vesicle leakage assay are combined
with data on particle adsorption onto supported lipid bilayers obtained
by optical reflectometry. Because of the strong tendency of the TiO<sub>2</sub> nanoparticles to aggregate, the interaction of these particles
with the bilayer was studied only in the leakage assay. Self-consistent
field (SCF) modeling was applied to interpret the results on a molecular
level. At low charge densities of either the silica nanoparticles
or the lipid bilayers, no electrostatic barrier to adsorption exists.
However, the adsorption rate and adsorbed amounts drop with increasing
(negative) charge densities on particles and membranes because of
electric double-layer repulsion, which is confirmed by the effect
of the ionic strength. SCF calculations show that charged particles
change the structure of lipid bilayers by a reorientation of a fraction
of the zwitterionic phosphatidylcholine (PC) headgroups. This explains
the affinity of the silica particles for pure PC lipid layers, even
at relatively high particle charge densities. Particle adsorption
does not always lead to the disruption of the membrane integrity,
as is clear from a comparison of the leakage and adsorption data for
the silica particles. The attraction should be strong enough, and
in line with this, we found that for positively charged TiO<sub>2</sub> particles vesicle disruption increases with increasing negative
charge density on the membranes. Our results may be extrapolated to
a broader range of oxide nanoparticles and ultimately may be used
for establishing more accurate nanoparticle toxicity assessments and
drug-delivery systems
Interfacial Tension and Wettability in Water–Carbon Dioxide Systems: Experiments and Self-consistent Field Modeling
This paper presents experimental
and modeling results on water–CO<sub>2</sub> interfacial tension
(IFT) together with wettability studies
of water on both hydrophilic and hydrophobic surfaces immersed in
CO<sub>2</sub>. CO<sub>2</sub>–water interfacial tension (IFT)
measurements showed that the IFT decreased with increasing pressure
and the negative slopes of IFT–pressure isotherms decreased
with increasing temperature. Water contact angle on a cellulose surface
(hydrophilic) immersed in CO<sub>2</sub> increased with pressure,
whereas the water contact angle on a hydrophobic surface such as hexamethyl
disilazane (HMDS) coated silicon surface was almost independent of
pressure. These experimental findings were augmented by modeling using
the self-consistent field theory. The theory applies the lattice discretization
scheme of Scheutjens and Fleer, with a discretization length close
to the size of the molecules. In line with this we have implemented
a primitive molecular model, with just small variations in the molar
volume. The theory makes use of the Bragg-Williams approximation and
has binary Flory–Huggins interaction parameters (FH) between
CO<sub>2</sub>, water, and free volume. Using this model, we generated
the complete IFT–pressure isotherms at various temperatures,
which coincided well with the trends reported in literature, that
is, the water–CO<sub>2</sub> interfacial tension decreased
with increasing pressure for pressures ≤100 bar and became
independent of pressure >100 bar. The transition point occurred
at
higher pressures with increasing temperature. At three-phase coexistence
(water–CO<sub>2</sub>–free volume) and at the water–vapor
interface (water–free volume), we always found the CO<sub>2</sub> phase in between the water-rich and free volume-rich phases. This
means that for the conditions studied, the water–vapor interface
is always wet by CO<sub>2</sub> and there are no signs of a nearby
wetting transition. Calculation of the water contact angle on a solid
surface was based on the computed adsorption isotherms of water from
a vapor or from a pressurized CO<sub>2</sub>-rich phase and analysis
of surface pressures at water–vapor or water–CO<sub>2</sub> coexistence. The results matched reasonably well with the
experimental contact angle data. Besides, we also computed the volume
fraction profiles of the CO<sub>2</sub>, H<sub>2</sub>O, and the <i>V</i> phase, from which the preferential adsorption of CO<sub>2</sub> near the hydrophilic surface was deduced
Impact of Macromolecular Architecture on Bending Rigidity of Dendronized Surfaces
Nanomechanical
properties of natural and artificial nanomembranes
can be strongly affected by anchored or tethered macromolecules. The
intermolecular interactions in polymeric layers give rise to so-called
induced bending rigidity which complements the bare rigidity of the
membrane. Using analytical mean-field theory, we explore how macromolecular
architecture of tethered polymers affects the bending rigidities of
the polymer-decorated membranes. The developed theory enables us to
consider explicitly various polymer architectures including regular
dendrons, Ψ-shaped, star- and comblike macromolecules as well
as macrocycles. Numerical self-consistent field computations for selected
(regular dendritic) topology complement the analytical theory and
support its predictions. We consider both cases of (i) quenched symmetric
distribution of tethered molecules on both sides of the membrane and
(ii) annealing distribution in which the tethered polymers can relocate
from the concave to the convex side of the membrane upon bending.
We demonstrate that at a given surface coverage an increase in the
degree of branching or cyclization leads to the decrease in the induced
bending rigidity. Relocation of the tethered molecules from concave
to convex surfaces leads to the additional decrease in polymer contribution
to the membrane bending rigidity. In the latter case, a decrease in
configurational entropy due to this redistributions substantially
contributes to the bending rigidity
Adhesion and Friction Properties of Polymer Brushes: Fluoro versus Nonfluoro Polymer Brushes at Varying Thickness
A series
of different thicknesses of fluoro poly(2,2,2-trifluoroethyl
methacrylate) and its analogous nonfluoro poly(ethyl methacrylate)
polymer brushes were prepared via surface-initiated ATRP (SI-ATRP)
on Si(111) surfaces. The thiol-yne click reaction was used to immobilize
the SI-ATRP initiator with a high surface coverage, in order to achieve
denser polymer brushes (grafting density from ∼0.1 to 0.8 chains/nm<sup>2</sup>). All polymer brushes were characterized by static water
contact angle measurements, infrared absorption reflection spectroscopy,
and X-ray photoelectron spectroscopy. Adhesion and friction force
measurements were conducted with silica colloidal probe atomic force
microscopy (CP-AFM) under ambient and dry (argon) conditions. The
fluoro poly(2,2,2-trifluoroethyl methacrylate) polymer showed a decrease
in adhesion and friction with increasing thickness. The analogous
nonfluoro poly(ethyl methacrylate) polymer brushes showed high adhesion
and friction under ambient conditions. Friction coefficients down
to 0.0057 (ambient conditions) and 0.0031 (dry argon) were obtained
for poly(2,2,2-trifluoroethyl methacrylate) polymer brushes with 140
nm thickness, which are the lowest among these types of polymer brushes
Impact of Macromolecular Architecture on Bending Rigidity of Dendronized Surfaces
Nanomechanical
properties of natural and artificial nanomembranes
can be strongly affected by anchored or tethered macromolecules. The
intermolecular interactions in polymeric layers give rise to so-called
induced bending rigidity which complements the bare rigidity of the
membrane. Using analytical mean-field theory, we explore how macromolecular
architecture of tethered polymers affects the bending rigidities of
the polymer-decorated membranes. The developed theory enables us to
consider explicitly various polymer architectures including regular
dendrons, Ψ-shaped, star- and comblike macromolecules as well
as macrocycles. Numerical self-consistent field computations for selected
(regular dendritic) topology complement the analytical theory and
support its predictions. We consider both cases of (i) quenched symmetric
distribution of tethered molecules on both sides of the membrane and
(ii) annealing distribution in which the tethered polymers can relocate
from the concave to the convex side of the membrane upon bending.
We demonstrate that at a given surface coverage an increase in the
degree of branching or cyclization leads to the decrease in the induced
bending rigidity. Relocation of the tethered molecules from concave
to convex surfaces leads to the additional decrease in polymer contribution
to the membrane bending rigidity. In the latter case, a decrease in
configurational entropy due to this redistributions substantially
contributes to the bending rigidity