9 research outputs found
Thermal expansion characteristics of high energy insensitive explosive α-NTO
Thermal expansion is an important structural parameter to evaluate the structural stability and performance reliability of energetic materials. In order to further understand the thermal expansion characteristics and mechanism of high-energy insensitive explosive 3-nitro-1, 2, 4-triazol-5-one (NTO), the thermal expansion characteristics of α-NTO were studied by in-situ X-ray diffraction (XRD) technique. Based on the Rietveld full-spectrum fitting structure refinement principle, the thermal expansion coefficient of α-NTO was obtained. The results show that α-NTO exhibits obvious reversible anisotropic thermal expansion under the action of thermal field. Based on infrared and Raman spectroscopy combined with theoretical calculation methods, the crystal packing structure of α-NTO at different temperatures and its correlation with thermal expansion characteristics were studied. It is believed that the functional groups that produce hydrogen bonds and hydrogen bond receptors in the crystal structure of α-NTO under thermal stimulation play a leading role. At the same time, compared with the thermal expansion characteristics of other explosive crystals, the influence of crystal packing on the thermal stability of explosive crystal structure was analyzed. The results show that the thermal expansion anisotropy of layered packing explosive crystals with strong hydrogen bonding is more obvious.</p
The Temperature-Dependent Thermal Expansion of 2,6-Diamino-3,5-dinitropyrazine-1-oxide Effected by Hydrogen Bond Network Relaxation
<div><p>The temperature-dependent thermal expansion of 2,6-diamino-3,5-dinitropyrazine-1-oxide (LLM-105) was investigated by using powder X-ray diffraction (PXRD) together with Rietveld refinement to estimate the dimension at a crystal lattice level. In the temperature range of 30–200°C, the coefficient of thermal expansion (CTE) of LLM-105 is temperature dependent, which is different from other explosives, such as hexahydro-1,3,5-trinitro-1,3,5-triazine (RDX), 2,2′,4,4′,6,6′-hexanitrostilbene (HNS) and octahydro-1,3,5,7-tetranitro-1,3,5,7-tetrazocine (HMX), with constant CTEs. The results of temperature-dependent infrared (IR) spectra indicated that the intermolecular hydrogen bond network relaxes with increasing temperature, which results in temperature-dependent thermal expansion. In this work, more accurate CTEs for LLM-105 crystals are obtained and the effects of the hydrogen bond network on the thermal expansion are further clarified. These results are beneficial to the design of materials with structural peculiarities and as-expected thermal expansion to satisfy different application requirements.</p></div
High-Yielding and Continuous Fabrication of Nanosized CL-20-Based Energetic Cocrystals via Electrospraying Deposition
Energetic
cocrystals, especially CL-20-based cocrystals, have attracted
a wide range of attention due to their low sensitivity and impressive
detonation performance. In this study, a series of nanosized CL-20-based
energetic cocrystals were successfully
fabricated by electrospray deposition. For CL-20/TNT nanococrystals,
the influence of different solvents on the morphology and crystal
structure of as-prepared cocrystals were investigated. The results
showed that all the electrosprayed CL-20/TNT samples were partial
formation of cocrystals and particles obtained from ketone had smaller
size than those obtained from ethyl solvents. In contrast, electrosprayed
CL-20/DNB nanococrystals had completely formed the cocrystal structure
proved by DSC and PXRD. Moreover, the terahertz (THz) result confirmed
the formation of intermolecular hydrogen bonds. Additionally, we have
fabricated the CL-20/TNB cocrystals for the first time by using electrospray
method. The PXRD and DSC results confirmed the formation of this novel
energetic cocrystal. Expectedly, all the electrosprayed nanosized
CL-20-based cocrystals exhibited visible reduced impact sensitivity
compared with raw CL-20. The electrospray can thus offer a flexible
and versatile approach for continuous and high-yielding synthesis
of nanosized energetic cocrystals with preferable safety performance,
and provide an efficient screening to quickly distinguish whether
two energetic materials can form a cocrystal
Occupancy Model for Predicting the Crystal Morphologies Influenced by Solvents and Temperature, and Its Application to Nitroamine Explosives
A new occupancy model for predicting the crystal morphologies
influenced by solvent and temperature is proposed. In the model, the
attachment energy is corrected by a relative occupancy, which is the
occupancy of a solute molecule relative to the total ones of a solute
molecule and a solvent molecule. The occupancy is defined proportional
to the averaged interaction energy between a solute or solvent molecule
and a crystal surface. The validity of the model is confirmed by its
successful applications to predict the crystal morphologies of a class
of well-known nitroamino explosives hexahydro-1,3,5-trinitro-1,3,5-
triazine, octahydro-1,3,5,7-tertranitro-1,3,5,7-tetrazocine and 2,4,6,8,10,12-hexanitrohexaaz-aisowurtzitane
grown in solution. Furthermore, the applications of this model regarding
concentration, molecular diffusion ability in solution, and mixed
solvents are prospected
Growth of 2D Plate-Like HMX Crystals on Hydrophilic Substrate
Two-dimensional
(2D) plate-like HMX crystals have been grown first
on hydrophilic substrate using an evaporation/solvent–nonsolvent
crystallization technique. As-grown crystals have been investigated
by X-ray diffraction (XRD), Fourier transform infrared (FT-IR) spectra,
scanning electron microscopy (SEM), confocal laser scanning microscope
(CLSM), and atomic force microscopy (AFM). The results unambiguously
indicate that the plate-like crystals with large (011) faces are β-HMX,
and the fluctuations in the smooth area of (011) face are monomolecular
or bimolecular HMX, which suggests the mechanism of monomolecular
stacking pattern and layer-by-layer growth. Furthermore, the distinct
recess consisting of hexagons parallel to each other is observed on
the center of the (011) face. The special growth morphology, which
is markedly different from that by the classical spiral growth, is
attributed mainly to the negative concentration gradient in the constrained
condition
From a Novel Energetic Coordination Polymer Precursor to Diverse Mn<sub>2</sub>O<sub>3</sub> Nanostructures: Control of Pyrolysis Products Morphology Achieved by Changing the Calcination Atmosphere
A novel
strategy to fabricate diverse α-Mn<sub>2</sub>O<sub>3</sub> nanostructures
from the nitrogen-rich energetic coordination
polymer (ECP) [MnÂ(BTO)Â(H<sub>2</sub>O)<sub>2</sub>]<sub><i>n</i></sub> (BTO = 1<i>H</i>,1′<i>H</i>-[5,5′-bitetrazole]-1,1′-bisÂ(olate))
has been developed by changing the pyrolysis atmosphere. The results
show that the energetic constituent and calcination environment are
vital factors to get quite different morphologies of pyrolysis products.
When the calcination reaction occurs under N<sub>2</sub> or O<sub>2</sub>, rod-shaped mesoporous α-Mn<sub>2</sub>O<sub>3</sub> with a large specific surface of 50.2 m<sup>2</sup>·g<sup>–1</sup> and monodispersed α-Mn<sub>2</sub>O<sub>3</sub> with a size
of 10–20 nm can be obtained, respectively, which provides a
new platform to prepare specific shapes and sizes of manganese oxides.
Inspired by the transformation of <b>1</b> under O<sub>2</sub> atmosphere, we applied an in situ generated ultrafine α-Mn<sub>2</sub>O<sub>3</sub> catalyst in the decomposition of ammonium perchlorate
(AP) using ECP <b>1</b> as a precursor. The catalytic process
of AP shows a remarkable decreased decomposition temperature (271
°C) and a narrower decomposition interval (from 253 to 275 °C).
To our best knowledge, with such a low metal loading (0.65 wt %),
the catalytic performance of in situ generated monodispersed ultrafine
α-Mn<sub>2</sub>O<sub>3</sub> is by far the best, which suggests
that this ultraefficient catalyst has great potential in AP-based
propellants
Evident Hydrogen Bonded Chains Building CL-20-Based Cocrystals
We
report two kinds of evident hydrogen bonded chains constructing two
binary cocrystals of 2,4,6,8,10,12-hexanitrohexaazaisowurtzitane (CL-20)
with <i>para</i>-benzoquinone (<b>1</b>) and 1,4-naphthoquinone
(<b>2</b>): one kind is the CL-20 molecule chains linked by <i>R</i><sub>2</sub><sup>2</sup>(6) hydrogen bonds, and the other is connected by CL-20 and coformer
(<b>1</b> or <b>2</b>) molecules alternately through <i>R</i><sub>2</sub><sup>1</sup>(5) hydrogen bonds. All chains extend to the entire cocrystals CL-20/<b>1</b> and CL-20/<b>2</b> with crossing points of CL-20 molecules.
In contrast to the unremarkable intermolecular interactions in observed
CL-20 polymorphs and cocrystals, these two kinds of chains in CL-20/<b>1</b> and CL-20/<b>2</b> are evident and can be readily
understood using the definition of supramolecular synthons. Moreover,
the thermal behaviors, impact sensitivity, and detonation properties
of these two energetic cocrystals are reported
Three Energetic 2,2′,4,4′,6,6′-Hexanitrostilbene Cocrystals Regularly Constructed by H‑bonding, π‑Stacking, and van der Waals Interactions
Three new energetic
2,2′,4,4′,6,6′-hexanitrostilbene
(HNS) cocrystals, HNS/4,4′-bipyridine, HNS/<i>trans</i>-1,2-bisÂ(4-pyridyl)Âethylene, and HNS/1,2-bisÂ(4-pyridyl)Âethane have
been synthesized. A good geometric match and rich H-bonds have been
observed between the selected coformer and HNS molecules in all three
cocrystals. According to similar configuration and arrangement of
HNS–coformer H-bonds, coformer–coformer π-stacking,
and HNS–HNS H-bonding interactions, the three cocrystals have
a common cocrystal architecture and show high thermal stability and
improved sensitivity. This study is helpful for understanding the
formation mechanism of energetic cocrystals and the design of new
energetic cocrystals
Five Energetic Cocrystals of BTF by Intermolecular Hydrogen Bond and π‑Stacking Interactions
Five novel BTF (benzotrifuroxan) cocrystals, possessing
a similar
density to RDX (1,3,5-trinitrohexahydro-1,3,5-triazine), have been
prepared and reported first. Their single-crystal structures are presented
and discussed. Interactions between cocrystal formers are discussed
with shifts in the IR spectra providing additional support for the
presence of various interactions. Hydrogen-bonding and π-stacking
interactions are found to be the most prominent. Especially, the interactions
between electron-poor π-systems of BTF and electron-rich groups
of other cocrystal formers such as nitro groups of TNB exist commonly
in all five novel cocrystals. This kind of interaction can be a more
potential driving force for energetic cocrystals, since explosives
with poor active hydrogen bonds are usually hard to form cocrystals
with other explosives for the lack of strong intermolecular interactions.
Because of the changes in structure, the physicochemical characteristics
including density and melting point together with energetic properties
of BTF altered after cocrystallization. All of the densities are between
both of the cocrystal formers. Cocrystals of BTF with TNT and TNB
have impact sensitivities between those of both cocrystal formers,
while the remaining three cocrystals (BTF/TNA, BTF/MATNB, and BTF/TNAZ)
all are more sensitive than either cocrystal former. It indicates
that a cocrystal with TNT or TNB can reduce the shock sensitivity
of BTF; especially, the cocrystal BTF/TNB not only has a lower sensitivity
than RDX but also equal energetic properties, which potentially improve
the viability of BTF in explosive applications. This paper owns an
important consideration in the design of future BTF and other explosive
cocrystals, and the result provides some feasibility to improve the
application of the high explosive BTF