Ajay Kumar
Chinnam
a,
Richard J.
Staples
b,
Gang
Zhao
a and
Jean'ne M.
Shreeve
*a
aDepartment of Chemistry, University of Idaho, Moscow, Idaho 83844-2343, USA. E-mail: jshreeve@uidaho.edu
bDepartment of Chemistry, Michigan State University East Lansing, MI 48824, USA
First published on 10th May 2022
Nitrogen-rich heterocycles are essential for designing novel energetic green materials with the combination of high explosive performance and acceptable mechanical sensitivities. In this work, two sets of high nitrogen-azoles, derived from tetrazoles and triazole assemblies with N-trinitromethane, 5,5′-(2-(trinitromethyl)-2H-1,2,3-triazole-4,5-diyl)bis(1H-tetrazole) (TBTN) and N-methylene tetrazole, 5,5′-(2-((1H-tetrazol-5-yl)methyl)-2H-1,2,3-triazole-4,5-diyl)bis(1H-tetrazole) (TBTT) are described. Their molecular structures were confirmed using multinuclear (1H, 13C, and 15N) NMR spectra and single-crystal X-ray diffraction analysis. These molecules are attention attracting results emanating from methodologies utilized to access a unique class of tri-ionic salts in reaction with nitrogen-rich bases. The thermostabilities, mechanical sensitivities, and detonation properties of all new compounds were determined. Surprisingly, the nitro-based tri-cationic salts, 5b (Dv = 9376 m s−1) and 5c (Dv = 9418 m s−1), have excellent detonation velocities relative to HMX (Dv = 9144 m s−1), while those of the nitro-free tri-cationic salts, 8b·H2O (Dv = 8998 m s−1) and 8c·0.5H2O (Dv = 9058 m s−1), are superior to that of RDX (Dv = 8795 m s−1) and approach HMX values. Additionally, nearly all new compounds are insensitive to mechanical stimuli because of the high percentage of hydrogen bond interactions (HBs) between the anions and cations, which are evaluated using two-dimensional (2D) fingerprint and Hirshfeld surface analyses. It is believed that the work presented here is the first example of high-performing and insensitive tri-cationic energetic salts, which may establish a discovery platform for the “green” synthesis of future energetic materials.
Various methods have been developed to enhance the thermostability and improve sensitivity by synthesizing salts through neutralization or metathesis reactions with various protonated cations or co-crystallization with a less sensitive material.18–21 The advantages of energetic salts include lower vapor pressure, larger positive heats of formation, higher thermostability, and lower sensitivity. Ammonium-based cations are essential in preparing energetic salts, frequently helping hydrogen bond (HB) formation with the corresponding anions.22,23 There are several energetic salts based on mono- and di-cationic salts. Not surprisingly, the latter shows higher detonation performances than mono-cationic salts.24 Also, it is often crucial to select a suitable anion such as one which is nitro-based for the preparation of high performing energetic salts. However, there are only few studies have focused on nitro-free anions based on nitrogen-rich anions or N-oxides in recent years,25,26 for instance, compounds A and B, which form di-cationic salts by a double deprotonation of tetrazole NH or N-hydroxide (Fig. 1).27 Compounds A and B are examples of energetic green materials with excellent positive heats of formation of 801.0 kJ mol−1 and 823 kJ mol−1, respectively. These derivatives have outstanding thermostabilities (>240 °C) but are highly sensitive to impact (<3 J), which makes handling them a challenge in practical applications.
Fig. 1 (a) Energetic materials, TNT, RDX, and HMX; (b) examples of nitrogen-rich green energetic materials; (c) and new molecules; red circle for accessing anions. |
Very recently, our group reported compound C with improved detonation properties and low sensitivity to impact by introducing a nitro-methyl group on the nitrogen scaffold of A.28 Although compound C meets the required sensitivity properties, the detonation properties are still relatively low compared with those of RDX. Because of our interest in the development of novel high performing, eco-friendly insensitive materials, we now report two sets of nitrogen-rich materials, based on the skeleton of compound A. These compounds contain the high performing explosophore, trinitromethane (–C(NO2)3) (4), and the nitrogen-rich stable and insensitive N-methylene-tetrazole (7). Compounds 4 and 7 are unusual with an advantage for preparing tri-cationic salts by neutralizing them with bases. All compounds are isolated in excellent yields and thoroughly characterized by advanced spectroscopy. The structures of 4, 5a, 5b, and 7 were analyzed by using single-crystal X-ray diffraction methods. Most of the compounds are highly thermostable and insensitive to impact and friction. All new compounds have high nitrogen–oxygen content (73.15 to 82.47%), which results in high positive heats of formation and detonation performances. Most new compounds have higher detonation properties than RDX, while the tri-cationic salts, 5b and 5c, have a superior performance relative to HMX. Furthermore, the syntheses of high nitrogen-rich derivative 7 and its energetic salts are achieved under “green reaction conditions,” which are highly desirable for the synthesis of future energetic materials.
Next nitro-free heterocycles were investigated by incorporating additional tetrazole rings on the triazole ring and neutralizing them with nitrogen-rich bases. Not surprisingly, N-substituted acetonitrile, 6, was obtained in various yields from the reaction of potassium salt, 1, with chloroacetonitrile in acetonitrile under reflux conditions (Scheme 2). With the trinitrile derivative 6 in hand, it was reacted with sodium azide using zinc chloride as a catalyst in an aqueous solution at reflux temperature to give a complex metal salt mixture, from which it was not possible to isolate pure 7. However, under mildly acidic conditions, with ammonium chloride as a catalyst, tri-tetrazole, 7, was formed in a high yield. Then, the three tetrazole rings of 7 were neutralized with aqueous bases, ammonia, hydroxylamine, and hydrazine, in acetonitrile to obtain nitrogen-rich tri-ionic salts 8a–c (Scheme 2).
The 15N NMR spectra of the nitro free energetic compound, 7, and its salts, 8a and 8b, in DMSO-d6 (Fig. 3) are similar to that of compound 4. One drop of D2O was added to compound 7 in order to control the proton exchange on the triazole rings. There are three tetrazole rings in compound 7 bonded to the triazole ring: two of them through a C–C bond, while the third via a N-methylene bridge. Since the molecular structure of 7 has C2-symmetry, six signals are found in the 15N NMR spectrum. The triazole ring atom signals were observed at δ = −125.5 (N2) and δ = −15.5 (N3), while the tetrazole ring resonances were observed between δ = −12.3 and −95.8. In the 15N NMR of both salts, 8a and 8b, seven signals were observed because of the tri-tetrazole anion framework (six signals) and cation (one signal). The signals for the corresponding cation of 8a (NH4+) are observed at δ = −356.6 (N7) and 8b (NH4OH+) at δ = −290.8 (N7). The nitrogen signals for the anion were found between δ = 8.3 and −127.1 (for 8a) and δ = 7.2 and −126.0 (for 8b), which are significantly different from those of the parent compound 7.
Fig. 4 (a) Thermal ellipsoid plot (50%) and labeling scheme for 4·MeOH. (b and c) HB system connects two molecules of 4·MeOH. |
The mono hydrated diammonium salt of 5a·H2O was obtained by slow evaporation in a mixture of water and methanol. It belongs to the monoclinic space group I2/a (Z = 8) with a calculated density of 1.753 g cm−3 at 99.99 K (Fig. 5a). Only one tetrazole molecule is deprotonated to form a tetrazole anion and eliminate one nitro group to form the dinitromethane anion, which is neutralized with two ammonium ions. Dianionic nitrogen-rich skeleton is neutralized with two ammonium ions. The anion ring system is nearly planar with torsion angles of C4–C2–C1–C4 = −5.0°(3), C2–C1–C4–N11 = −3.8°(3), and C1–C2–C3–N7 = 0.5°(3) and the two nitro groups together with the atom C5 form another plane. The angle between the two planes is 75.97°. The N–C bond lengths of N–C(NO2)2 and –C(NO2)2 are slightly lower than those in the molecular structure of 4·MeOH. There are several hydrogen bonds (N–H⋯N and N–H⋯O) which are observed in the three-dimensional packing network (Fig. 5b).
Fig. 5 (a) Thermal ellipsoid plot (50%) and labeling scheme for 5a·H2O. (b) A b axis view of the ball-and-stick packing diagram of 5a·H2O. |
Crystals of the hydroxylammonium salt, 5b, were obtained with one water molecule from the mixture of ethanol and water. The water molecule and one of the hydroxylammonium cations are found to have a disorder, which is removed for clarity (Fig. 6a). 5b·H2O crystallizes in the monoclinic space group Ia (Z = 8) with a crystal density of 1.759 g cm−3 at 100 K. Unlike 5a·H2O, both tetrazole rings were deprotonated and eliminated along with one nitro group to form a tri-anionic fragment, which coordinates with three hydroxylammonium ions. The tri-anionic structure is arranged very much like the molecular structure of 4·MeOH (with a twofold screw axis). All the atoms of the 1,2,3-triazole are coplanar while the dinitro methane group is found on the perpendicular plane at an angle of 85.59°. The bond lengths in the triazole and tetrazole rings are between typical single and double bonds. The N–C bond lengths of N–C(NO2)2 and –C(NO2)2 are nearly identical to those in the molecular structure of 5a. In the crystal packing of compound 5b·H2O, there are many strong intermolecular hydrogen bond interactions due to the hydroxylamine groups, nitro oxygen atoms, and nitrogen atoms in both the anions and cations (Fig. 6b).
Fig. 6 (a) Thermal ellipsoid plot (50%) and labeling scheme for 5b·H2O. (b) Hydrogen bonding interaction between hydroxylammonium cations and anions in the crystal structure of 5b·H2O. |
Crystals of 7 were obtained without water or solvent molecule from the mixture of acetonitrile and hydrochloric acid and crystallized in the monoclinic space group P21/c (Z = 4) with a crystal density of 1.772 g cm−3 at 100 K and a twofold axis passing through the center of the molecule (Fig. 7a). The bond lengths and angles within the azole rings are within the range of normal C–N, N–N, and C–C single and double bonds. The dihedral angle between the mean planes through the 1,2,3-triazole and N-methylene bridge tetrazole rings was found to be 67.83°. In the crystal packing diagram, there are several inter- and intramolecular bonds (N–H⋯N), which form a three-dimensional framework (Fig. 7b).
Fig. 7 (a) Thermal ellipsoid plot (50%) and labeling scheme for 7. (b) A b axis view of the ball-and-stick packing diagram of 7. |
Comp. | T d [°C] | ρ [g cm−3] | ΔHfc [kJ mol−1]/[kJ g−1] | V D [m s−1] | P [GPa] | ISf [J] | FSg [N] | N + Oh [%] |
---|---|---|---|---|---|---|---|---|
a Decomposition temperature (onset). b Density measured by a gas pycnometer at 25 °C. c Calculated molar enthalpy of formation. d Calculated detonation velocity. e Calculated detonation pressure. f Impact sensitivity. g Friction sensitivity. h Combined nitrogen and oxygen content. i Ref. 24. j Ref. 25. k Ref. 3. | ||||||||
4 | 157 | 1.84 | 982.4/2.77 | 9101 | 35.93 | 9 | 120 | 82.47 |
5a·H2O | 146 | 1.71 | 251.4/0.69 | 8176 | 24.78 | >60 | >360 | 80.30 |
5b | 196 | 1.76 | 1399.3/3.42 | 9376 | 37.25 | 38 | 360 | 82.32 |
5c | 169 | 1.74 | 1500.7/3.70 | 9418 | 34.68 | 35 | 360 | 81.45 |
7 | 284 | 1.75 | 1228.8/4.27 | 8362 | 26.14 | 55 | >360 | 73.15 |
8a·H2O | 256 | 1.57 | 1559.4/4.37 | 8598 | 26.11 | >60 | >360 | 75.25 |
8b·H2O | 245 | 1.64 | 1637.2/4.05 | 8998 | 30.74 | >60 | >360 | 78.42 |
8c·0.5H2O | 265 | 1.63 | 1858.6/4.73 | 9058 | 29.43 | >60 | >360 | 77.14 |
A | 277 | 1.69 | 823.0/3.46 | 8360 | 26.00 | 2 | 240 | 78.46 |
B | 246 | 1.67 | 801.0/3.90 | 8277 | 24.80 | 1 | 240 | 75.11 |
C | 281 | 1.79 | 945.8/3.35 | 8636 | 29.50 | 10 | 240 | 76.58 |
RDX | 204 | 1.80 | 70.7/0.32 | 8795 | 34.90 | 7.5 | 120 | 81.06 |
HMX | 280 | 1.90 | 74.8/0.25 | 9144 | 39.20 | 7.4 | 120 | 81.06 |
Fig. 8 Calculated heats of formation, experimental densities (a), calculated detonation velocities, and detonation pressures (b) of 4, 5a–c, 7, 8a–c, and compared with those of A, B, C, RDX, and HMX. |
Using the experimental density and calculated heats of formation, detonation properties were obtained using the EXPLO5 (Version 6.01) computer code.31 Because of high densities and positive heats of formation, detonation velocities (VD) and detonation pressures (P) of the new energetic compounds have excellent performance. Except for the polytetrazole compound, 7 (8362 m s−1), ammonium salt, 8a (8176 m s−1), and ammonium salts, 5a·H2O (8176 m s−1), all other compounds especially, the nitro free energetic salts, 8b·H2O (8998 m s−1) and 8c·0.5H2O (9058 m s−1), display outstanding performances compared with RDX (8795 m s−1). Among all these compounds, the detonation properties of the trinitro compound, 4 (9101 m s−1), and its tri-cationic salts, 5b (9376 m s−1) and 5c (9418 m s−1), are superior to those of HMX (9144 m s−1) (Fig. 8b).
The impact sensitivity experiments were measured according to STANAG 4489 using a BAM drop hammer for the safety and handling of these new materials.32,33 The friction sensitivity experiments were measured according to STANAG 4487 using a BAM friction tester (Fig. 9).34 The trinitromethane compound 4, is sensitive to mechanical stimuli (impact sensitivity (IS) = 9 J; friction sensitivity (FS) = 120 N), while the other new compounds are much less sensitive (IS = 35–65 J; FS = 360 N). Most importantly, the high performing tri-cationic salts, 5b (IS = 38 J; FS = 360 N), 5c (IS = 35 J; FS = 360 N), 8b·H2O (IS = 65 J; FS > 360 N), and 8b·0.5H2O (IS = 65 J; FS > 360 N), have better mechanical stabilities than the high energy explosives, RDX (IS = 7.5 J; FS = 120 N) and HMX (IS = 7.4 J; FS = 120 N).
Fig. 9 Experimental impact and friction sensitivity of 4, 5a–c, 7, 8a–c, and compared with those of reference compounds, A, B, C, RDX, and HMX. |
The Hirshfeld electrostatic surfaces and two-dimensional (2D) fingerprint of the crystals were used to understand the inert- and intramolecular interactions (Fig. 10).35 In the Hirshfeld surface analysis, red dots indicate the close contact intermolecular hydrogen bonds (HBs). The blue area is the O–C, C–C, and C–N interactions, which tell the high energy and sensitivity features of an energetic material. In Fig. 10e–h, 2D fingerprint plots, the spikes indicate the strong O⋯H and N⋯H hydrogen bonding interactions. Based on the crystal structures, 5a has large O⋯H (31.9%) and N⋯H (30.0%) interactions, while these HB interactions decreased in 7 (N⋯H, 43.9%), 5b (O⋯H, 35.6%; N⋯H, 7.8%), and 4 (O⋯H, 16.4%; N⋯H, 20.7%), respectively. As a result of the HB-interactions, compounds 5a, 5b, and 7 are more stable and less sensitive than compound 4, which are comparable with experimental results (Fig. 10).
Footnote |
† Electronic supplementary information (ESI) available. CCDC 2160564–2160567. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d2ma00406b |
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