4 research outputs found
Spontaneous Thermoreversible Formation of Cationic Vesicles in a Protic Ionic Liquid
The search for stable vesicular structures is a long-standing
topic
of research because of the usefulness of these structures and the
scarcity of surfactant systems that spontaneously form vesicles in
true thermodynamic equilibrium. We report the first experimental evidence
of spontaneous formation of vesicles for a pure cationic double tail
surfactant (didodecyldimethylammonium bromide, DDAB) in a protic ionic
liquid (ethylammonium nitrate, EAN). Using small and ultra-small angle
neutron scattering, rheology and bright field microscopy, we identify
the coexistence of two vesicle containing phases in compositions ranging
from 2 to 68 wt %. A low density highly viscous solution containing
giant vesicles (<i>D</i> ā¼ 30 Ī¼m) and a sponge
(L<sub>3</sub>) phase coexists with a dilute high density phase containing
large vesicles (<i>D</i> ā¼ 2.5 Ī¼m). Vesicles
form spontaneously via different thermodynamic routes, with the same
size distribution, which strongly supports that they exist in a true
thermodynamic equilibrium. The formation of equilibrium vesicles and
the L<sub>3</sub> phase is facilitated by ion exchange between the
cationic surfactant and the ionic liquid, as well as the strength
of the solvophobic effect in the protic ionic liquid
Spontaneous Thermoreversible Formation of Cationic Vesicles in a Protic Ionic Liquid
The search for stable vesicular structures is a long-standing
topic
of research because of the usefulness of these structures and the
scarcity of surfactant systems that spontaneously form vesicles in
true thermodynamic equilibrium. We report the first experimental evidence
of spontaneous formation of vesicles for a pure cationic double tail
surfactant (didodecyldimethylammonium bromide, DDAB) in a protic ionic
liquid (ethylammonium nitrate, EAN). Using small and ultra-small angle
neutron scattering, rheology and bright field microscopy, we identify
the coexistence of two vesicle containing phases in compositions ranging
from 2 to 68 wt %. A low density highly viscous solution containing
giant vesicles (<i>D</i> ā¼ 30 Ī¼m) and a sponge
(L<sub>3</sub>) phase coexists with a dilute high density phase containing
large vesicles (<i>D</i> ā¼ 2.5 Ī¼m). Vesicles
form spontaneously via different thermodynamic routes, with the same
size distribution, which strongly supports that they exist in a true
thermodynamic equilibrium. The formation of equilibrium vesicles and
the L<sub>3</sub> phase is facilitated by ion exchange between the
cationic surfactant and the ionic liquid, as well as the strength
of the solvophobic effect in the protic ionic liquid
Spontaneous Thermoreversible Formation of Cationic Vesicles in a Protic Ionic Liquid
The search for stable vesicular structures is a long-standing
topic
of research because of the usefulness of these structures and the
scarcity of surfactant systems that spontaneously form vesicles in
true thermodynamic equilibrium. We report the first experimental evidence
of spontaneous formation of vesicles for a pure cationic double tail
surfactant (didodecyldimethylammonium bromide, DDAB) in a protic ionic
liquid (ethylammonium nitrate, EAN). Using small and ultra-small angle
neutron scattering, rheology and bright field microscopy, we identify
the coexistence of two vesicle containing phases in compositions ranging
from 2 to 68 wt %. A low density highly viscous solution containing
giant vesicles (<i>D</i> ā¼ 30 Ī¼m) and a sponge
(L<sub>3</sub>) phase coexists with a dilute high density phase containing
large vesicles (<i>D</i> ā¼ 2.5 Ī¼m). Vesicles
form spontaneously via different thermodynamic routes, with the same
size distribution, which strongly supports that they exist in a true
thermodynamic equilibrium. The formation of equilibrium vesicles and
the L<sub>3</sub> phase is facilitated by ion exchange between the
cationic surfactant and the ionic liquid, as well as the strength
of the solvophobic effect in the protic ionic liquid
Catalyst Architecture for Stable Single Atom Dispersion Enables Site-Specific Spectroscopic and Reactivity Measurements of CO Adsorbed to Pt Atoms, Oxidized Pt Clusters, and Metallic Pt Clusters on TiO<sub>2</sub>
Oxide-supported
precious metal nanoparticles are widely used industrial
catalysts. Due to expense and rarity, developing synthetic protocols
that reduce precious metal nanoparticle size and stabilize dispersed
species is essential. Supported atomically dispersed, single precious
metal atoms represent the most efficient metal utilization geometry,
although debate regarding the catalytic activity of supported single
precious atom species has arisen from difficulty in synthesizing homogeneous
and stable single atom dispersions, and a lack of site-specific characterization
approaches. We propose a catalyst architecture and characterization
approach to overcome these limitations, by depositing ā¼1 precious
metal atom per support particle and characterizing structures by correlating
scanning transmission electron microscopy imaging and CO probe molecule
infrared spectroscopy. This is demonstrated for Pt supported on anatase
TiO<sub>2</sub>. In these structures, isolated Pt atoms, Pt<sub>iso</sub>, remain stable through various conditions, and spectroscopic evidence
suggests Pt<sub>iso</sub> species exist in homogeneous local environments.
Comparing Pt<sub>iso</sub> to ā¼1 nm preoxidized (Pt<sub>ox</sub>) and prereduced (Pt<sub>metal</sub>) Pt clusters on TiO<sub>2</sub>, we identify unique spectroscopic signatures of CO bound to each
site and find CO adsorption energy is ordered: Pt<sub>iso</sub> āŖ
Pt<sub>metal</sub> < Pt<sub>ox</sub>. Pt<sub>iso</sub> species
exhibited a 2-fold greater turnover frequency for CO oxidation than
1 nm Pt<sub>metal</sub> clusters but share an identical reaction mechanism.
We propose the active catalytic sites are cationic interfacial Pt
atoms bonded to TiO<sub>2</sub> and that Pt<sub>iso</sub> exhibits
optimal reactivity because every atom is exposed for catalysis and
forms an interfacial site with TiO<sub>2</sub>. This approach should
be generally useful for studying the behavior of supported precious
metal atoms