4 research outputs found
Coating Graphene Oxide with Lipid Bilayers Greatly Decreases Its Hemolytic Properties
Toxicity evaluation for the proper
use of graphene oxide (GO) in
biomedical applications involving intravenous injections is crucial,
but the GO circulation time and blood interactions are largely unknown.
It is thought that GO may cause physical disruption (hemolysis) of
red blood cells. The aim of this work is to characterize the interaction
of GO with model and cell membranes and use this knowledge to improve
GO hemocompatibility. We have found that GO interacts with both neutral
and negatively charged lipid membranes; binding is decreased beyond
a certain concentration of negatively charged lipids and favored in
high-salt buffers. After this binding occurs, some of the vesicles
remain intact, while others are disrupted and spread over the GO surface.
Neutral membrane vesicles tend to break down and extend over the GO,
while vesicles with negatively charged membranes are mainly bound
to the GO without disruption. GO also interacts with red blood cells
and causes hemolysis; hemolysis is decreased when GO is previously
coated with lipid membranes, particularly with pure phosphatidylcholine
vesicles
Homoleptic Organocobalt(III) Compounds with Intermediate Spin
Homoleptic
organocobalt(III) compounds with formula [NBu<sub>4</sub>][Co<sup>III</sup>(C<sub>6</sub>X<sub>5</sub>)<sub>4</sub>] [X = F (<b>3</b>), Cl (<b>4</b>)] were obtained in reasonable yields
by chemical oxidation of the corresponding divalent species [NBu<sub>4</sub>]<sub>2</sub>[Co<sup>II</sup>(C<sub>6</sub>X<sub>5</sub>)<sub>4</sub>] [X = F (<b>1</b>), Cl (<b>2</b>)]. The
[Co<sup>III</sup>(C<sub>6</sub>X<sub>5</sub>)<sub>4</sub>]<sup>−</sup>/[Co<sup>II</sup>(C<sub>6</sub>X<sub>5</sub>)<sub>4</sub>]<sup>2–</sup> couples are electrochemically related by quasi-reversible, one-electron
exchange processes at moderate potential: <i>E</i>
<sub>1/2</sub> = −0.29 (X = F) and −0.36 V (X = Cl) versus saturated
calomel electrode. The [Co<sup>III</sup>(C<sub>6</sub>X<sub>5</sub>)<sub>4</sub>]<sup>−</sup> anions in salts <b>3</b> and <b>4</b> show an unusual square-planar geometry as established by
single-crystal X-ray diffraction methods. According to their stereochemistry,
these Co<sup>III</sup> derivatives (d<sup>6</sup>) are paramagnetic
non-Kramers systems with a large zero-field splitting contribution
and no observable electron paramagnetic resonance (EPR) spectrum.
The thermal dependence of their magnetic susceptibilities can be explained
in terms of a spin-Hamiltonian formalism with <i>S</i> =
1 ground state (intermediate spin) and substantial spin–orbit
contribution. The magnetic properties of the square-planar d<sup>7</sup> parent species [NBu<sub>4</sub>]<sub>2</sub>[Co<sup>II</sup>(C<sub>6</sub>X<sub>5</sub>)<sub>4</sub>] were also thoroughly studied
both at microscopic (EPR) and macroscopic levels (alternating current
and direct current magnetization measurements). They behave as <i>S</i> = 1/2 (low spin) systems with mainly (d<sub><i>z</i><sup>2</sup></sub>)<sup>1</sup> electron configuration and a certain
degree of s-orbital admixture that has been quantified. The electronic
structures of all four open-shell [Co(C<sub>6</sub>X<sub>5</sub>)<sub>4</sub>]<sup><i>q</i>−</sup> compounds (<i>q</i> = 1, 2) accounting for their respective magnetic properties
are based on a common orbital energy-level diagram