5 research outputs found
Highly Enhanced Gas Sorption Capacities of N‑Doped Porous Carbon Spheres by Hot NH<sub>3</sub> and CO<sub>2</sub> Treatments
Highly
enhanced CO<sub>2</sub> and H<sub>2</sub> adsorption properties
were achieved with a series of phenolic resin-based carbon spheres
(resorcinol–formaldehyde carbon (RFC) and phenol–formaldehyde
carbon (PFC)) by carbonization of RF and PF polymer (RFP and PFP)
spheres synthesized via a sol–gel reaction and subsequent activation
with hot CO<sub>2</sub> or NH<sub>3</sub> treatment. Monodisperse
and size-tunable (100–600 nm) RFC and PFC spheres had intrinsic
nitrogen contents (ca. 1.5 wt %), which are attributed to the synthesis
conditions that utilized NH<sub>3</sub> as a basic catalyst as well
as nitrogen precursor. A series of CO<sub>2</sub>-activated and N-doped
RFC and PFC spheres showed almost perfect correlation (<i>R</i><sup>2</sup> = 0.99) between CO<sub>2</sub> adsorption capacities
and accumulated pore volumes of fine micropores (ultramicropore <1
nm) obtained using the nonlocal density functional theory (NLDFT)
model. Interestingly, NH<sub>3</sub> activation served not only as
an effective method for heteroatom doping (i.e., nitrogen) into the
carbon framework but also as an excellent activation process to fine-tune
the surface area and pore size distribution (PSD). Increased nitrogen
doping levels up to ca. 2.8 wt % for NH<sub>3</sub>-activated RFC
spheres showed superior CO<sub>2</sub> adsorption capacities of 4.54
(1 bar) and 7.14 mmol g<sup>–1</sup> (1 bar) at 298 and 273
K, respectively. Compared to CO<sub>2</sub>-activated RFC spheres
with similar ultramicropore volume presenting CO<sub>2</sub> uptakes
of 4.41 (1 bar) and 6.86 mmol g<sup>–1</sup> (1 bar) at 298
and 273 K, respectively, NH<sub>3</sub>-activated nitrogen-enriched
RFC was found to have elevated chemisorption ability. Moreover, prolonged
activation of RFC and PFC spheres provided ultrahigh surface areas,
one of which reached 4079 m<sup>2</sup>g<sup>–1</sup> with
an unprecedented superb H<sub>2</sub> uptake capacity of 3.26 wt %
at 77 K (1 bar), representing one of the best H<sub>2</sub> storage
media among carbonaceous materials and metal–organic frameworks
(MOFs)
Variation in Crystalline Phases: Controlling the Selectivity between Silicon and Silicon Carbide via Magnesiothermic Reduction using Silica/Carbon Composites
Magnesiothermic
reduction of various types of silica/carbon (SiO<sub>2</sub>/C) composites
has been frequently used to synthesize silicon/carbon
(Si/C) composites and silicon carbide (SiC) materials, which are of
great interest in the research areas of lithium-ion batteries (LIBs)
and nonmetal oxide ceramics, respectively. Up to now, however, it
has not been comprehensively understood how totally different crystal
phases of Si or SiC can result from the compositionally identical
parent materials (SiO<sub>2</sub>/C) via magnesiothermic reduction.
In this article, we propose a formation mechanism of Si and SiC by
magnesiothermic reduction of SiO<sub>2</sub>/C; SiC is formed at the
interface between SiO<sub>2</sub> and carbon when silicon intermediates,
mainly <i>in situ</i>-formed Mg<sub>2</sub>Si, encounter
carbon through diffusion. Otherwise, Si is formed, which is supported
by an <i>ex situ</i> reaction between Mg<sub>2</sub>Si and
carbon nanosphere that results in SiC. In addition, the resultant
crystalline phase ratio between Si and SiC can be controlled by manipulating
the synthesis parameters such as the contact areas between silica
and carbon of parent materials, reaction temperatures, heating rates,
and amount of the reactant mixtures used. The reasons for the dependence
on these synthesis parameters could be attributed to the modulated
chance of an encounter between silicon intermediates and carbon, which
determines the destination of silicon intermediates, namely, either
thermodynamically preferred SiC or kinetic product of Si as a final
product. Such a finding was applied to design and synthesize the hollow
mesoporous shell (ca. 3–4 nm pore) SiC, which is particularly
of interest as a catalyst support under harsh environments
Bioinspired Synthesis of Melaninlike Nanoparticles for Highly N‑Doped Carbons Utilized as Enhanced CO<sub>2</sub> Adsorbents and Efficient Oxygen Reduction Catalysts
Highly
N-doped nanoporous carbons have been of great interest as
a high uptake CO<sub>2</sub> adsorbent and as an efficient metal-free
oxygen reduction reaction (ORR) catalyst. Therefore, it is essential
to produce porosity-tunable and highly N-doped carbons through cost-effective
means. Herein, we introduce the bioinspired synthesis of a monodisperse
and N-enriched melaninlike polymer (MP) resembling the sepia biopolymer (SP) from oceanic cuttlefish. These
polymers were subsequently utilized for highly N-doped synthetic carbon
(MC) and biomass carbon (SC) spheres. An adequate CO<sub>2</sub> activation
process fine-tunes the ultramicroporosity (<1 nm) of N-doped MC
and SC spheres, those with maximum ultramicroporosities of which show
remarkable CO<sub>2</sub> adsorption capacities. In addition, N-doped
MC and SC with ultrahigh surface areas of 2677 and 2506 m<sup>2</sup>/g, respectively, showed excellent ORR activities with a favored
four electron reduction pathway, long-term durability, and better
methanol tolerance, comparable to a commercial Pt-based catalyst
Elucidating Relationships between Structural Properties of Nanoporous Carbonaceous Shells and Electrochemical Performances of Si@Carbon Anodes for Lithium-Ion Batteries
The encapsulation
of silicon in hollow carbonaceous shells (Si@C)
is known to be a successful solution for silicon anodes in Li-ion
batteries, resulting in many efforts to manipulate the structural
properties of carbonaceous materials to improve their electrochemical
performance. In this regard, we demonstrate in this work how both
the shell thickness and pore size of nanoporous carbonaceous materials
containing silicon anodes influence the electrochemical performance.
Structurally well-defined Si@C materials with varying carbon-shell
thicknesses and pore sizes were synthesized by a nanocasting method
that manipulated the carbon shell and by a subsequent magnesiothermic
reduction that converted the amorphous silica cores into silicon nanocrystals.
When these materials were employed as anodes, it was verified that
two opposite effects occur with respect to the thickness of carbon
shell: The weight ratio of silicon and the electrical conductivity
are simultaneously affected, so that the best electrochemical performance
is not obtained from either the thickest or the thinnest carbon shell.
Such countervailing effects were carefully confirmed through a series
of electrochemical performance tests and the use of electrochemical
impedance spectroscopy. In addition, the effect of pore size was elucidated
by comparing Si@C samples with different pore sizes, revealing that
larger pores can further improve the electrochemical performance as
a result of enhanced Li-ion diffusion
Dynamic Nuclear Polarization of Selectively <sup>29</sup>Si-Enriched Core@shell Silica Nanoparticles
29Si silica nanoparticles (SiO2 NPs) are
promising magnetic resonance imaging (MRI) probes that possess advantageous
properties for in vivo applications, including suitable biocompatibility,
tailorable properties, and high water dispersibility. Dynamic nuclear
polarization (DNP) is used to enhance 29Si MR signals via
enhanced nuclear spin alignment; to date, there has been limited success
employing DNP for SiO2 NPs due to the lack of endogenous
electronic defects that are required for the process. To create opportunities
for SiO2-based 29Si MRI probes, we synthesized
variously featured SiO2 NPs with selective 29Si isotope enrichment on homogeneous and core@shell structures (shell
thickness: 10 nm, core size: 40 nm), and identified the critical factors
for optimal DNP signal enhancement as well as the effective hyperpolarization
depth when using an exogenous radical. Based on the synthetic design,
this critical factor is the proportion of 29Si in the shell
layer regardless of core enrichment. Furthermore, the effective depth
of hyperpolarization is less than 10 nm between the surface and core,
which demonstrates an approximately 40% elongated diffusion length
for the shell-enriched NPs compared to the natural abundance NPs.
This improved regulation of surface properties facilitates the development
of isotopically enriched SiO2 NPs as hyperpolarized contrast
agents for in vivo MRI