11 research outputs found
Thermal Activation of a Pure Montmorillonite Clay and Its Reactivity in Cementitious Systems
Clay
minerals are potential candidates as raw materials for new
supplementary cementitious materials (SCMs) that can partly replace
Portland cement and thereby significantly reduce CO<sub>2</sub> emissions
associated with cement production. We present the characterization
of the complex, disordered structure of a pure montmorillonite clay
heated at various temperatures (110–1100 °C), by solid-state <sup>27</sup>Al and <sup>29</sup>Si MAS NMR methods. The SiO<sub>4</sub> tetrahedra and AlO<sub>6</sub> octahedral sites become progressively
more distorted, exhibit a significant degree of disorder upon dehydroxylation
(600–800 °C), and do not lead to the formation of any
metastable phase. At high temperatures (1000–1100 °C),
the layer structure of the clay breaks down, forming stable crystalline
phases. The chemical reactivity, measured as the degree of dissolution/precipitation
in an alkaline solution, is found to be proportional to the degree
of disorder/dehydroxylation. The maximum reactivity as a function
of the heating temperature is achieved at 800 °C prior to the
formation of inert, condensed Q<sup>4</sup>-type phases in the material.
At maximum reactivity the calcium silicate hydrate (C-S-H) phase contains
silicate chains with the highest aluminum incorporation, leading to
blended cements containing a C-S-H phase with longer chain lengths.
Most importantly, by exploiting the differential spin–lattice
relaxation behavior of the <sup>29</sup>Si spins, evidence of multiple
sites and components in both the naturally occurring and heated montmorillonite
is being reported for the first time
Structural Investigation of Ye’elimite, Ca<sub>4</sub>Al<sub>6</sub>O<sub>12</sub>SO<sub>4</sub>, by <sup>27</sup>Al MAS and MQMAS NMR at Different Magnetic Fields
Ye’elimite
is the principal component in calcium sulfoaluminate
cement, which currently attracts significant attention, since it can
be produced with lower CO<sub>2</sub> emissions compared to conventional
portland cement. The crystal structure of ye’elimite is not
well-established, and it has been proposed to exhibit cubic, tetragonal,
and orthorhombic structures. The present work reports a comprehensive <sup>27</sup>Al magic-angle spinning (MAS) and multiple-quantum (MQ) MAS
NMR study of ye’elimite, utilizing six magnetic fields from
4.7 to 22.3 T. These spectra are only compatible with the orthorhombic <i>Pcc</i>2 structure of ye’elimite, implying the presence
of eight distinct AlO<sub>4</sub> sites. The <sup>27</sup>Al NMR spectra
are convincingly simulated by eight distinct sites, and <sup>27</sup>Al quadrupole coupling parameters and isotropic chemical shifts are
reported for the first time for ye’elimite. These parameters
are a prerequisite for a reliable interpretation and quantification
of ye’elimite in <sup>27</sup>Al NMR spectra of ye’elimite-based
cements. Density functional theory (DFT) calculations are used in
the assignment of the specific Al sites in ye’elimite. Structural
relaxations by DFT, using two proposed <i>Pcc</i>2 structures
as starting points, result virtually in the same set of optimized
fractional atomic coordinates, which is proposed as a new refined
structure for ye’elimite. The refined structure gives the best
agreement between experimental and calculated <sup>27</sup>Al quadrupole
tensor elements for the eight Al sites. Finally, the <sup>33</sup>S MAS NMR spectra for ye’elimite, monosulfate, and anhydrite
are reported
Resolution of the Two Aluminum Sites in Ettringite by <sup>27</sup>Al MAS and MQMAS NMR at Very High Magnetic Field (22.3 T)
Ettringite (Ca<sub>6</sub>[Al(OH)<sub>6</sub>]<sub>2</sub>(SO<sub>4</sub>)<sub>3</sub>·26H<sub>2</sub>O) is the first hydration
product formed during Portland cement hydration. <sup>27</sup>Al MAS
NMR has been used in a wide number of studies to detect and quantify
ettringite in hydrated cement blends by the observation of a single,
narrow resonance at 13–14 ppm. This work reports the first
observation of resonances from two distinct Al sites in octahedral
coordination for ettringite, employing <sup>27</sup>Al MAS and MQMAS
NMR at an ultrahigh magnetic field (22.3 T). Thereby, the <sup>27</sup>Al NMR spectra are in agreement with the most accepted trigonal model
for the ettringite structure. <sup>27</sup>Al quadrupole coupling
parameters and isotropic chemical shifts for the two Al sites are
determined from simulations and least-squares optimization of slow-speed <sup>27</sup>Al MAS NMR spectra of the satellite transitions. These data
reveal that the local environments for the two octahedral Al sites
are very similar, in accord with the most recent XRD refinements of
the ettringite structure. Finally, the significant improvement in
spectral resolution by the application of an ultrahigh magnetic field
is illustrated by the detection of the two Al sites from ettringite
in a hydrated cement mimicking the composition of a calcium sulfoaluminate
cement
Dynamic Solid-State NMR Experiments Reveal Structural Changes for a Methyl Silicate Nanostructure on Deuterium Substitution
Structural characterizations
of three different solid–gas reaction products, recently obtained
from abraded solid-state silicate free radicals reacting with two
isotopically enriched methane gases, <sup>13</sup>CH<sub>4</sub> and
CD<sub>4</sub> (a possible sink for methane on MARS) and with <sup>13</sup>CO<sub>2</sub>, are derived from various dynamic solid-state
NMR experiments. These include cross-polarization/depolarization zero-cross
times (ZCTs), variable temperature (VT) NMR to study 3-site jump CH<sub>3</sub>/CD<sub>3</sub> activation energies (<i>E</i><sub>a</sub>), and <sup>13</sup>CO<sub>2</sub>/<sup>13</sup>CH<sub>3</sub> molecular species as a spy to determine the approximate diameters
for the channel structures for some of these structures. Literature <i>E</i><sub>a</sub> data indicate that l-alanine and
4-CH<sub>3</sub>-phenanthrene exhibit the highest known <i>E</i><sub>a</sub> values (= 20–22.6 kJ/mol) for CH<sub>3</sub> 3-site
jump motions. The ZCTs for these two compounds are 120 and 162 μs,
respectively, indicative of the high <i>E</i><sub>a</sub> values for CH<sub>3</sub>/CD<sub>3</sub> groups. Determination of <i>E</i><sub>a</sub> for 4-CD<sub>3</sub>-phenanthrene by low-temperature <sup>2</sup>H MAS NMR experiments supplemented the previously reported
liquid-state <i>E</i><sub>a</sub> value (<i>E</i><sub>a</sub> = 21 kJ/mol) for 4-CH<sub>3</sub>-phenanthrene. Finally,
such experiments also revealed the structural difference for the free-radical
reaction products with <sup>13</sup>CH<sub>4</sub> and CD<sub>4</sub>, i.e, a change from helical to chain structure
Hydrogen Storage Capacity Loss in a LiBH<sub>4</sub>–Al Composite
A detailed investigation of the decomposition
reactions and decay
in the hydrogen storage capacity during repeated hydrogen release
and uptake cycles for the reactive composite LiBH<sub>4</sub>–Al
(2:3) is presented. Furthermore, the influence of a titanium boride,
TiB<sub>2</sub>, additive is investigated. The study combines information
from multiple techniques: in situ synchrotron radiation powder X-ray
diffraction, Sieverts measurements, simultaneous thermogravimetric
analysis, differential scanning calorimetry and mass spectroscopy,
solid-state magic-angle spinning nuclear magnetic resonance (MAS NMR),
and Raman spectroscopy. The decomposition of LiBH<sub>4</sub>–Al
results in the formation of LiAl, AlB<sub>2</sub>, and Li<sub>2</sub>B<sub>12</sub>H<sub>12</sub> via several reactions and intermediate
compounds. The TiB<sub>2</sub> additive appears to have a limited
effect on the decomposition pathway of the samples, but seems to facilitate
formation of intermediate species at lower temperatures compared to
the sample without additive. Solid solutions of Li<sub><i>x</i></sub>Al<sub>1–<i>x</i></sub>B<sub>2</sub> or Al<sub>1–<i>x</i></sub>B<sub>2</sub> are observed during
decomposition and from Rietveld refinement the composition of the
solid solution is estimated to be Li<sub>0.22</sub>Al<sub>0.78</sub>B<sub>2</sub>. The intercalation of Li in the AlB<sub>2</sub> structure
is further investigated by <sup>11</sup>B and <sup>27</sup>Al MAS
NMR spectra of the LiH-AlB<sub>2</sub> and AlB<sub>2</sub> samples
(presented in Supporting Information).
Hydrogen release and uptake for LiBH<sub>4</sub>–Al reveals
a significant loss in the hydrogen storage capacity, that is, after
four cycles a capacity of about 45% remains, and after 10 cycles,
the capacity is degraded to approximately 15% of the theoretically
available hydrogen content. This capacity loss may be due to the formation
of Li<sub>2</sub>B<sub>12</sub>H<sub>12</sub>, as observed by <sup>11</sup>B MAS NMR and Raman spectroscopy. Formation of Li<sub>2</sub>B<sub>12</sub>H<sub>12</sub> has previously been observed during
the decomposition of LiBH<sub>4</sub>, but it has not been reported
earlier in the LiBH<sub>4</sub>–Al (2:3) system
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У статті окреслено необхідність реформування діючого законодавства України в сфері функціонування страхового ринку, запропоновані основні заходи щодо покращення його стану.In the article outlined necessity of reformation of current legislation of Ukraine for the sphere of functioning of insurance market, basic measures are offered on the improvement of his state
Synthesis, Crystal Structure, Thermal Decomposition, and <sup>11</sup>B MAS NMR Characterization of Mg(BH<sub>4</sub>)<sub>2</sub>(NH<sub>3</sub>BH<sub>3</sub>)<sub>2</sub>
A metal borohydride–ammonia
borane complex, Mg(BH<sub>4</sub>)<sub>2</sub>(NH<sub>3</sub>BH<sub>3</sub>)<sub>2</sub> was synthesized via a solid-state reaction between
Mg(BH<sub>4</sub>)<sub>2</sub> and NH<sub>3</sub>BH<sub>3</sub>. Different
mechanochemical reaction mechanisms are observed, since Mg(BH<sub>4</sub>)<sub>2</sub>(NH<sub>3</sub>BH<sub>3</sub>)<sub>2</sub> is
obtained from α-Mg(BH<sub>4</sub>)<sub>2</sub>, whereas a mixture
of Mg(BH<sub>4</sub>)<sub>2</sub>(NH<sub>3</sub>BH<sub>3</sub>)<sub>2</sub>, NH<sub>3</sub>BH<sub>3</sub>, and amorphous Mg(BH<sub>4</sub>)<sub>2</sub> is obtained from γ-Mg(BH<sub>4</sub>)<sub>2</sub>. The crystal structure of Mg(BH<sub>4</sub>)<sub>2</sub>(NH<sub>3</sub>BH<sub>3</sub>)<sub>2</sub> has been determined by powder
X-ray diffraction and optimized by first-principles calculations.
The borohydride groups act as terminal ligands, and molecular complexes
are linked via strong dihydrogen bonds (<2.0 Å), which may
contribute to the high melting point of Mg(BH<sub>4</sub>)<sub>2</sub>(NH<sub>3</sub>BH<sub>3</sub>)<sub>2</sub> found to be ∼48
°C in contrast to those for other molecular metal borohydrides.
Precise values for the <sup>11</sup>B quadrupole coupling parameters
and isotropic chemical shifts are reported for the two NH<sub>3</sub>BH<sub>3</sub> sites and two BH<sub>4</sub><sup>–</sup> sites
in Mg(BH<sub>4</sub>)<sub>2</sub>(NH<sub>3</sub>BH<sub>3</sub>)<sub>2</sub> from <sup>11</sup>B MAS NMR spectra of the central and satellite
transitions and MQMAS NMR. The <sup>11</sup>B quadrupole coupling
parameters agree excellently with the electric field gradients for
the <sup>11</sup>B sites from the DFT calculations and suggest that
a more detailed structural model is obtained by DFT optimization,
which allows evaluation of the dihydrogen bonding scheme
Trends in Syntheses, Structures, and Properties for Three Series of Ammine Rare-Earth Metal Borohydrides, M(BH<sub>4</sub>)<sub>3</sub>·<i>n</i>NH<sub>3</sub> (M = Y, Gd, and Dy)
Fourteen
solvent- and halide-free ammine rare-earth metal borohydrides M(BH<sub>4</sub>)<sub>3</sub>·<i>n</i>NH<sub>3</sub>, M = Y,
Gd, Dy, <i>n</i> = 7, 6, 5, 4, 2, and 1, have been synthesized
by a new approach, and their structures as well as chemical and physical
properties are characterized. Extensive series of coordination complexes
with systematic variation in the number of ligands are presented,
as prepared by combined mechanochemistry, solvent-based methods, solid–gas
reactions, and thermal treatment. This new synthesis approach may
have a significant impact within inorganic coordination chemistry.
Halide-free metal borohydrides have been synthesized by solvent-based
metathesis reactions of LiBH<sub>4</sub> and MCl<sub>3</sub> (3:1),
followed by reactions of M(BH<sub>4</sub>)<sub>3</sub> with an excess
of NH<sub>3</sub> gas, yielding M(BH<sub>4</sub>)<sub>3</sub>·7NH<sub>3</sub> (M = Y, Gd, and Dy). Crystal structure models for M(BH<sub>4</sub>)<sub>3</sub>·<i>n</i>NH<sub>3</sub> are derived
from a combination of powder X-ray diffraction (PXD), <sup>11</sup>B magic-angle spinning NMR, and density functional theory (DFT) calculations.
The structures vary from two-dimensional layers (<i>n</i> = 1), one-dimensional chains (<i>n</i> = 2), molecular
compounds (<i>n</i> = 4 and 5), to contain complex ions
(<i>n</i> = 6 and 7). NH<sub>3</sub> coordinates to the
metal in all compounds, while BH<sub>4</sub><sup>–</sup> has
a flexible coordination, i.e., either as a terminal or bridging ligand
or as a counterion. M(BH<sub>4</sub>)<sub>3</sub>·7NH<sub>3</sub> releases ammonia stepwise by thermal treatment producing M(BH<sub>4</sub>)<sub>3</sub>·<i>n</i>NH<sub>3</sub> (6, 5,
and 4), whereas hydrogen is released for <i>n</i> ≤
4. Detailed analysis of the dihydrogen bonds reveals new insight about
the hydrogen elimination mechanism, which contradicts current hypotheses.
Overall, the present work provides new general knowledge toward rational
materials design and preparation along with limitations of PXD and
DFT for analysis of structures with a significant degree of dynamics
in the structures
(NH<sub>4</sub>)<sub>4</sub>Sn<sub>2</sub>S<sub>6</sub>·3H<sub>2</sub>O: Crystal Structure, Thermal Decomposition, and Precursor for Textured Thin Film
Understanding
the condensation of the dimeric thiostannate(IV)
[Sn<sub>2</sub>S<sub>6</sub>]<sup>4–</sup> to SnS<sub>2</sub> is of key importance for the development of solution processing
of advanced tin(IV) sulfide based electronic devices such as photovoltaics
(e.g., Cu<sub>2</sub>ZnSnS<sub>4</sub>, CZTSSe) and thin-film transistors.
Here, we report the crystal structure of tetraammonium thiostannate(IV)
trihydrate ((NH<sub>4</sub>)<sub>4</sub>Sn<sub>2</sub>S<sub>6</sub>·3H<sub>2</sub>O), which can be used as a more environmentally
friendly alternative to the hydrazinium analogue in solution processed
advanced tin(IV) sulfide based electronic devices, e.g., CZTSSe. Hirshfeld
surface analysis shows that crystal bound water molecules play a significant
role in the structure and interact strongly with the sulfur atoms
in the dimeric thiostannate(IV) complex [Sn<sub>2</sub>S<sub>6</sub>]<sup>4–</sup>. The thermal decomposition and corresponding
condensation of ((NH<sub>4</sub>)<sub>4</sub>Sn<sub>2</sub>S<sub>6</sub>·3H<sub>2</sub>O) to SnS<sub>2</sub> have been studied by TG/DSC-MS
and solid-state <sup>119</sup>Sn MAS NMR. It involves the formation
of the relatively more condensed thiostannate(IV) complex [Sn<sub>4</sub>S<sub>10</sub>]<sup>4–</sup> at 90 °C via evaporation
of ammonia, hydrogen sulfide, and water from the structure. With increasing
temperature, more tin is transformed from tetrahedral to octahedral
coordination, and at 220 °C, crystalline SnS<sub>2</sub> is formed.
In an aqueous ammonium sulfide based solution, the structure of dimeric
[Sn<sub>2</sub>S<sub>6</sub>]<sup>4–</sup> is retained, and
aqueous solutions of (NH<sub>4</sub>)<sub>4</sub>Sn<sub>2</sub>S<sub>6</sub>·3H<sub>2</sub>O can be spin coated and thermally decomposed
to form crystalline SnS<sub>2</sub> thin films. X-ray scattering techniques
show that the solution processed SnS<sub>2</sub> thin film is highly
textured with the <i>ab</i> plane parallel to the substrate.
Furthermore, AFM and TEM reveal that the thin film is continuous and
with an inherent porous surface structure from the gaseous formation
byproducts