295 research outputs found
Ligand Effects of Thiolate-Protected Au<sub>102</sub> Nanoclusters
The
Au<sub>102</sub>(<i>p</i>-MBA)<sub>44</sub> (<i>p</i>-MBA = <i>para</i>-mercaptobenzoic acid) nanocluster
is an ideal model to study the structures of gold nanoclusters, the
motifs of the monolayer ligand groups, and the crystal formation of
Au nanoparticles. Based on the partially exchanged Au<sub>102</sub>(<i>p</i>-MBA)<sub>40</sub>(<i>p</i>-BBT)<sub>4</sub> (<i>p</i>-BBT = <i>para</i>-bromobenzene
thiol) crystal structure (<i>J. Am. Chem. Soc.</i> <b>2012</b>, <i>134</i>, 13316–13322), we employed
density functional theory to investigate the ligand effects for different
thiolate substitutions. It was found that the intermolecular π–π
stacking plays an important role for the crystal’s stability
in addition to the increased intrinsic stability from the substituent
monomer. Furthermore, we suggested <i>para</i>-(dimethylamino)
benzenethiol (N(CH<sub>3</sub>)<sub>2</sub>–C<sub>6</sub>H<sub>4</sub>–SH) and <i>para</i>-amino benzenethiol (NH<sub>2</sub>–C<sub>6</sub>H<sub>4</sub>–SH) would be more
favorable than <i>p</i>-BBT for the stabilities of partially
exchanged Au<sub>102</sub>(<i>p</i>-MBA)<sub>44</sub> crystal
structures due to their stronger intermolecular π–π
stacking. This study provides a theoretical template for surface chemical
engineering
H<sub>2</sub> + H<sub>2</sub>O → H<sub>4</sub>O: Synthesizing Hyperhydrogenated Water in Small-Sized Fullerenes?
Nanoscale confinement provides an ideal platform to rouse
some
exceptional reactions which cannot happen in the open space. Intuitively,
H2 and H2O cannot react. Herein, through utilizing
small-sized fullerenes (C24, C26, C28, and C30) as nanoreactors, we demonstrate that a hyperhydrogenated
water species, H4O, can be easily formed using H2 and H2O under ambient conditions by ab initio molecular dynamics simulations. The H4O molecule rotates
freely in the cavity of the cages and maintains its structure during
the simulations. Further theoretical analysis indicates that H4O in the fullerene possesses high stability thermodynamically
and chemically, which can be rationalized by the electron transfer
between H4O and the fullerene. This work highlights the
possibility of utilizing fullerene as a nanoreactor to provide confinement
constraints for unexpected chemistry
Au<sub>42</sub>: An Alternative Icosahedral Golden Fullerene Cage
We present a new icosahedral gold fullerene, Au42, based on density functional theory calculations. The Au42 fullerene has a nanoscale hollow space that can hold up to 13 Au atoms. The Au42 fullerene also has a larger HOMO−LUMO gap compared to the compact-filling geometries. However, unlike the known gold fullerene Au32, the Au42 fullerene does not satisfy the 2(N + 1)2 aromatic rule and has a positive NICS value at the center of the cage. These two nanometer-sized gold fullerenes can be used as golden cages to accommodate other atoms or molecules for the purpose of studying fundamental chemistry because of their apparently dissimilar chemical characteristics, or they can be used as structural motifs to build highly stable core−shell nanoclusters or novel cluster-assembled materials
Water-Promoted O<sub>2</sub> Dissociation on Small-Sized Anionic Gold Clusters
Although thermodynamically O<sub>2</sub> favors dissociative
adsorption
over molecular adsorption on small-sized anionic gold clusters (except
Au<sub>2</sub><sup>–</sup>), O<sub>2</sub> dissociation is
unlikely to proceed under ambient conditions because of the high activation
energy barrier (>2.0 eV). Here, we present a systematic theoretical
study of reaction pathways for the O<sub>2</sub> dissociation on small-sized
anionic gold nanoclusters Au<sub><i>n</i></sub><sup>–</sup> (<i>n</i> = 1–6) with and without involvement of
a water molecule. The density functional theory calculations indicate
that the activation barriers from the molecular adsorption state of
O<sub>2</sub> to dissociative adsorption can be significantly lowered
with the involvement of a H<sub>2</sub>O molecule. Once the O<sub>2</sub> dissociates on small-size gold clusters, atomic oxygen is
readily available for other reactions, such as the CO oxidation, on
the surface of gold clusters. This theoretical study supports previous
experimental evidence that H<sub>2</sub>O can be used to activate
O<sub>2</sub>, which suggests an alternative way to exploit catalytic
capability of gold clusters for oxidation applications
Unraveling the Atomic Structures of the Au<sub>68</sub>(SR)<sub>34</sub> Nanoparticles
The atomic structure prediction of
thiolate-protected gold nanoparticle
(RS-AuNP) Au<sub>68</sub>(SH)<sub>34</sub> is performed based on the
“divide and protect” concept and experimental studies
on 14 kDa RS-AuNPs. Four low-lying energy isomers, <b>Iso1</b>–<b>Iso4</b>, were identified by the density-functional
theory. Our results indicate the most stable structure <b>Iso2</b> adopts the <i>C</i><sub>2<i>v</i></sub> Au<sub>50</sub> core with Marks-decahedral (m-Dh) Au<sub>18</sub> inner
core. The calculated HOMO–LUMO gap is 0.74 eV, which is very
close to that of Au<sub>67</sub>(SR)<sub>35</sub><sup>2–</sup>. Further analysis suggests the 14 kDa RS-AuNPs might be not only
the turn point between the fused core structure and the compact core
structure but also the turn point between the one-shell inner core
structure and the multishell inner core structure. The threshold number
of Au atoms in bulk-like RS-AuNPs is evaluated as ∼263 based
on the linear fitting of the HOMO–LUMO gaps of various RS-AuNPs
including Au<sub>68</sub>(SR)<sub>34</sub>. The research on the medium-sized
Au<sub>68</sub>(SR)<sub>34</sub> establishes a bridge between smaller
and larger RS-AuNPs, which is beneficial for us to better understand
the structures of the RS-AuNPs
Fig 9 -
Compression test of mud film of naturally weathered red-bed soil (A) Mud film; (B) Application of 100 N pressure to mud film; (C) Application of 200 N pressure to mud film; (D) Application of 400 N pressure to mud film; (E) Application of 800 N pressure to mud film.</p
Effects of mud viscosity, water content and particle content smaller than 1 mm on the infiltration distance of a mud film.
Effects of mud viscosity, water content and particle content smaller than 1 mm on the infiltration distance of a mud film.</p
Fig 14 -
Infiltration of 8 mm thick naturally weathered red-bed soil films after dropping water (A) Water dropped on an 8 mm thick naturally weathered red-bed soil film for 3 m; (B) Water dropped on an 8 mm thick naturally weathered red-bed soil film for 6 min; (C) Water dropped on an 8 mm thick naturally weathered red-bed soil film for 9 min; (D) Water dropped on an 8 mm thick naturally weathered red-bed soil film for 12 min.</p
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