38 research outputs found
Rhodium(II)-Catalyzed N–H Insertions of Carbenes under Mechanochemical Conditions
Under mechanochemical conditions in a mixer mill, Rh2(OAc)4 catalyzes the reaction between aryldiazoesters
and anilines to give α-amino esters. The process proceeds under
mild conditions and is insensitive to air. It is solvent-free and
scalable. A broad substrate scope, short reaction times, operational
simplicity, and good functional group tolerance are additional salient
features of this protocol
Tuning Electromagnetic Interference Shielding Performance through Controlled Alignment of Ni Nanowires in Soft PDMS Composites
Efficient
dispersion of nanostructured fillers in thermoplastic
polymers and elastomers remains an open challenge, and unless it is
addressed, the potential utilization of conducting and magnetic fillers
influencing the electronic properties of soft nanocomposites could
not be properly assessed. Herein, we present a unique approach to
address this challenge by constructing a microstructural fence using
aligned magnetic networks of Ni nanowires in the direction of the
applied external magnetic field, followed by flow-induced secondary
in-planar alignment of multiwalled carbon nanotubes during the curing
of the soft poly(dimethylsiloxane) (PDMS) elastomer. This mutually
perpendicular arrangement offers unique magnetoconducting features
to the soft elastomer matrix with moderately high conductivity, which
is the key to superior electromagnetic shielding performance. The
unique conformation of mutually perpendicular positions of both nanofillers
in the bulk PDMS composites results in enhanced electromagnetic interference
shielding performance (−28 dB) primarily through an absorption
(80%) mechanism, driven primarily by the maximized interaction with
incident electromagnetic waves inside the soft elastomer. Fundamental
insights into the governing viscoelastic responses of these elastomer
composites were gained through oscillatory rheological studies that
investigate interparticle attraction within a quasi-solid network
Tuning the Shape Anisotropy and Electromagnetic Screening Ability of Ultrahigh Magnetic Polymer and Surfactant-Capped FeCo Nanorods and Nanocubes in Soft Conducting Composites
Herein,
we demonstrate that very high electromagnetic (EM) shielding
efficiency can be achieved by dispersing nanoengineered FeCo anisometric
nanostructures in a poly(vinylidene difluoride) matrix in the presence
of conductive nanofillers (multiwall carbon nanotubes, MWCNTs). The
FeCo nanorods (∼800 nm) and nanocubes (∼100 nm) were
fabricated by a facile surfactant and polymer-assisted one-pot borohydride
reduction method. The growth mechanism depicted a two-directional
growth for cubes, whereas for nanorods, a unidirectional growth pattern
across the (110) plane was evident. A total shielding effectiveness
(SE<sub>T</sub>) of −44 dB at 18 GHz was achieved for a particular
combination of FeCo nanorods and MWCNT, and for nanocube-based composites,
it was found to be −39 dB at 18 GHz. It was observed from zero
field cooled-field cooled curves that the samples displayed room temperature
ferromagnetism. An excellent correlation between high aspect ratio
FeCo nanorod and superior EM absorption (89%) was explored, pertaining
to the fact that nanorods possessed higher magnetic saturation (177.1
emu/g) and coercivity (550 Oe) in contrast to the nanocubes with similar
composition. Furthermore, theoretical insight into the mechanism revealed
a high degree of interface scattering between conductive MWCNT and
magnetic loss components, giving rise to an excellent synergy between
magnetic and dielectric parts
Wool-Ball-Type Core-Dual-Shell FeCo@SiO<sub>2</sub>@MWCNTs Microcubes for Screening Electromagnetic Interference
Engineered nanostructure-reinforced
lightweight polymer composites
with superior electromagnetic (EM) shielding effectiveness (SE<sub>T</sub>) are widely employed in high-end applications such as aerospace
and microelectronic devices. Recently, carbon nanotube-based three-dimensional
nanostructures have shown enormous potential due to unmatched processability,
mechanical, and electronic properties. In this study, we present for
the first time, highly permeable FeCo-based core-double shell <i>wool-ball</i>-type microcubes chemically enclosed by dielectric
silica and conducting multiwalled carbon nanotubes (MWCNTs) sequentially;
the resulting reinforced nanocomposites with low filler loading produced
superior SE<sub>T</sub> of −35 dB at 18 GHz for a specimen
of 3 mm thickness. The excellent dispersion of microstructures in
the soft matrix owing to the encapsulation of hard FeCo magnets by
MWCNTs ensures low density and excellent flexibility for high-precision
applications. The nanoengineered core-dual shell strategy for fabricating
magnetic-dielectric-conducting microcubes ensures strong magnetic
loss, coupled with dielectric and conduction loss, respectively, from
SiO<sub>2</sub> and MWCNT shells. This approach, being unique in terms
of nanofabrication and subsequent formulation of lightweight flexible
composites, demonstrates a highly efficient way toward designing advanced
nanocomposites for cutting-edge shielding application
Stabilizing the [RSn(μ<sub>2</sub>‑O)SnR] Motif through Intramolecular N→Sn Coordination. Synthesis and Characterization of [(RSn)<sub>2</sub>(μ<sub>2</sub>‑O)(μ<sub>2</sub>‑FcCOO)<sub>2</sub>(η-FcCOO)<sub>2</sub>]·THF and {(RSn)<sub>2</sub>(μ<sub>2</sub>‑O)[(<i>t-</i>BuO)<sub>2</sub>PO<sub>2</sub>]<sub>2</sub>Cl<sub>2</sub>}·THF·2H<sub>2</sub>O (R = 2‑(Phenylazo)phenyl)
The reactions of RSnCl<sub>3</sub> (<b>1</b>; R = 2-(phenylazo)phenyl)
with FcCOOH or di-<i>tert</i>-butyl phosphate in refluxing
THF afforded the monoorganodistannoxanes [(RSn)<sub>2</sub>(μ<sub>2</sub>-O)(μ<sub>2</sub>-FcCOO)<sub>2</sub>(η-FcCOO)<sub>2</sub>]·THF (<b>2</b>) and {(RSn)<sub>2</sub>(μ<sub>2</sub>-O)[(<i>t-</i>BuO)<sub>2</sub>PO<sub>2</sub>]<sub>2</sub>Cl<sub>2</sub>}·THF·2H<sub>2</sub>O (<b>3</b>). The molecular structure of <b>2</b> contains seven-coordinate
tin centers in a distorted-pentagonal-bipyramidal geometry, while <b>3</b> contains six-coordinate tin centers in a distorted-octahedral
geometry. In the dinuclear compounds <b>2</b> and <b>3</b> the two tin centers are bridged by a μ<sub>2</sub>-O unit,
affording a rare Sn–O–Sn motif among monoorganostannoxanes.
In addition, each tin is also intramolecularly coordinated to the
nitrogen atom of the 2-phenylazophenyl substituent (N→Sn).
Further, in <b>2</b>, the two tin centers are bridged by two
isobidentate ferrocenecarboxylate ligands; each tin center also is
bound to a chelating ferrocenecarboxylate ligand. On the other hand,
in <b>3</b>, while the two tin centers are bridged by two isobidentate
di-<i>tert</i>-butyl phosphate ligands, each tin center
also has a terminal chloride ligand
Stabilizing the [RSn(μ<sub>2</sub>‑O)SnR] Motif through Intramolecular N→Sn Coordination. Synthesis and Characterization of [(RSn)<sub>2</sub>(μ<sub>2</sub>‑O)(μ<sub>2</sub>‑FcCOO)<sub>2</sub>(η-FcCOO)<sub>2</sub>]·THF and {(RSn)<sub>2</sub>(μ<sub>2</sub>‑O)[(<i>t-</i>BuO)<sub>2</sub>PO<sub>2</sub>]<sub>2</sub>Cl<sub>2</sub>}·THF·2H<sub>2</sub>O (R = 2‑(Phenylazo)phenyl)
The reactions of RSnCl<sub>3</sub> (<b>1</b>; R = 2-(phenylazo)phenyl)
with FcCOOH or di-<i>tert</i>-butyl phosphate in refluxing
THF afforded the monoorganodistannoxanes [(RSn)<sub>2</sub>(μ<sub>2</sub>-O)(μ<sub>2</sub>-FcCOO)<sub>2</sub>(η-FcCOO)<sub>2</sub>]·THF (<b>2</b>) and {(RSn)<sub>2</sub>(μ<sub>2</sub>-O)[(<i>t-</i>BuO)<sub>2</sub>PO<sub>2</sub>]<sub>2</sub>Cl<sub>2</sub>}·THF·2H<sub>2</sub>O (<b>3</b>). The molecular structure of <b>2</b> contains seven-coordinate
tin centers in a distorted-pentagonal-bipyramidal geometry, while <b>3</b> contains six-coordinate tin centers in a distorted-octahedral
geometry. In the dinuclear compounds <b>2</b> and <b>3</b> the two tin centers are bridged by a μ<sub>2</sub>-O unit,
affording a rare Sn–O–Sn motif among monoorganostannoxanes.
In addition, each tin is also intramolecularly coordinated to the
nitrogen atom of the 2-phenylazophenyl substituent (N→Sn).
Further, in <b>2</b>, the two tin centers are bridged by two
isobidentate ferrocenecarboxylate ligands; each tin center also is
bound to a chelating ferrocenecarboxylate ligand. On the other hand,
in <b>3</b>, while the two tin centers are bridged by two isobidentate
di-<i>tert</i>-butyl phosphate ligands, each tin center
also has a terminal chloride ligand
Absorption-Dominated Electromagnetic Wave Suppressor Derived from Ferrite-Doped Cross-Linked Graphene Framework and Conducting Carbon
To
minimize electromagnetic (EM) pollution, two key parameters, namely,
intrinsic wave impedance matching and intense absorption of incoming
EM radiation, must satisfy the utmost requirements. To target these
requirements, soft conducting composites consisting of binary blends
of polycarbonate (PC) and poly(vinylidene fluoride) (PVDF) were designed
with doped multiwalled carbon nanotubes (MWCNTs) and a three-dimensional
cross-linked graphene oxide (GO) framework doped with ferrite nanoparticles.
The doping of α-MnO<sub>2</sub> onto the MWCNTs ensured intrinsic
wave impedance matching in addition to providing conducting pathways,
and the ferrite-doped cross-linked GO facilitated the enhanced attenuation
of the incoming EM radiation. This unique combination of magnetodielectric
coupling led to a very high electromagnetic shielding efficiency (SE)
of −37 dB at 18 GHz, dominated by absorption-driven shielding.
The promising results from the composites further motivated us to
rationally stack individual composites into a multilayer architecture
following an absorption–multiple reflection–absorption
pathway. This resulted in an impressive SE of −57 dB for a
thin shield of 0.9-mm thickness. Such a high SE indicates >99.999%
attenuation of the incoming EM radiation, which, together with the
improvement in structural properties, validates the potential of these
materials in terms of applications in cost-effective and tunable solutions