Jatinder
Singh
a,
Richard J.
Staples
b 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, Michigan 48824, USA
First published on 23rd June 2022
Energetic properties of bistetrazole derivatives are improved by the step-by-step introduction of functionalities which improve heat of formation, density, and oxygen content. The incorporation of unsaturation between bis(1H-tetrazol-5-yl) and bis(1H-tetrazol-1-ol) derivatives leads to planarity which enhances the density of the final product. In this manuscript, we have synthesized compounds 1,2-di(1H-tetrazol-5-yl)ethane (4), (E)-1,2-di(1H-tetrazol-5-yl)ethene (5), and (E)-5,5′-(ethene-1,2-diyl)bis(1H-tetrazol-1-ol), (6) using readily available starting materials. Their corresponding dihydroxylammonium salts 7, 8 and 9 are obtained by reacting two equivalents of hydroxylamine (50% in water). New compounds are analyzed using IR, EA, DSC and multinuclear NMR spectroscopy (1H, 13C and 15N). The solid-state structures of compounds 6, 7, 8 and 9 are confirmed by single-crystal X-ray diffraction. The energetic performances are calculated using the EXPLO5 (v6.06.02) code and the sensitivities towards external stimuli such as friction and impact are determined according to BAM standard. Compound 6 {(E)-5,5′-(ethene-1,2-diyl)bis(1H-tetrazol-1-ol)} exhibits a surprisingly high density of 1.91 g cm−3 at 100 K (1.86 g cm−3 at 298 K). Its detonation velocity (9017 m s−1) is considerably superior to those of RDX (8795 m s−1), which suggests it is a competitive high-energy-density material.
The use of tetrazole-based compounds rather than nitro or nitroamino compounds RDX (1,3,5-trinitro-1,3,5-triazinane) and HMX (1,3,5,7-tetranitro-1,3,5,7-tetrazocane) has the advantage of high personal and ecological safety.19–22 RDX is a potential carcinogen known to be toxic to humans and organisms in the soil. However, the lack of oxygen content in tetrazole derivatives limits their detonation performance and practical applicability in comparison to nitro- or nitroamino-based compounds.23–27 Replacing the tetrazole ring with 1H-tetrazol-1-ol is known to enhance the density, oxygen balance, thermal stability, insensitivity, and detonation power.28 Notable examples include, 5,5′-bistetrazole-1,1′-diol (1,1-BTO) and dihydroxylammonium 5,5′-bistetrazole-1,1′-diolate (TKX-50) as high-performing high-energy-density materials (HEDMs) (Fig. 1(a)).29–31
The introduction of planarity through conjugation is an important strategy for realizing high-performance materials.32 Planarity in a molecule facilitates efficient packing and maximizes weak non-covalent interactions (π-stacking, anion-π, cation/π, H-bonding, etc.), which play vital roles in improving density and thermal stability.33 In addition, planar stacked layers absorb mechanical energy, which helps in reducing sensitivity toward external stimuli.34 Attempts to design conjugated planar HEDMs have been made by many researchers. For example, fused tetrazolo 1,2,4,5-tetrazine N-oxides, 4-amino-3,7-dinitro-[1,2,4]-triazolo[5,1-c][1,2,4]triazine, and nitroamino-functionalized 1,2,4-triazolo[4,3-b][1,2,4,5]tetrazine are planar conjugated structures reported as high-performance materials.35–37 Recently it was demonstrated that tetrazole or triazole ring substituted FOX-7-like molecules exhibit good thermal stability and improved sensitivity due to the planar conjugated structures.38–40 Inspired by the good performance of conjugated planar energetic compounds, we speculated that the introduction of a planar conjugated ethene link between tetrazole rings would improve the density, heat of formation and insensitivity.
Now we have synthesized ethane and ethene linked bistetrazole derivatives: 1,2-di(1H-tetrazol-5-yl)ethane (4), (E)-1,2-di(1H-tetrazol-5-yl)ethene (5), and the ethene-linked bis(1H-tetrazol-1-ol) derivative, (E)-5,5′-(ethene-1,2-diyl)bis(1H-tetrazol-1-ol), (6) using readily available starting materials. Dihydroxylammonium salts 7, 8 and 9 are obtained by reacting two equivalents of hydroxylamine (50% in water) with compounds 4, 5 and 6. Compound 6 exhibits the highest density and detonation properties.
All compounds are characterized by NMR (1H and 13C), and infrared (IR) spectroscopy as well as elemental analysis. In the 1H NMR spectrum of compound 6, the ethene group protons are shifted upfield (7.62 ppm) relative to compound 5 (7.67 ppm) (ESI†). In the 13C{1H} NMR spectrum, signals corresponding to the ethene group carbon atoms in 6 are observed at 116.8 ppm and the tetrazole at 144.0 ppm (ESI†). The 15N NMR spectra of 6 and 9 are given in Fig. 2. In the spectrum of 6, four signals are seen for the nitrogen atoms of the tetrazole ring at δ = −115.9, −54.2, −17.7 and −1.2, while nitrogen atoms corresponding to compound 9 are seen at δ = −85.1, −57.9, −17.1 and −11.8. The nitrogen atoms of the hydroxylamine cations in 9 are observed at δ = −296.9.
The structures of 6, 7, 8 and 9 were further confirmed by single-crystal X-ray diffraction (SC-XRD). Crystals suitable for SC-XRD analysis were obtained through the slow evaporation of a saturated solution in a methanol/water or ethanol/water mixture at room temperature. Crystal structures are given in Fig. 3–6. Crystallographic data and data collection parameters, bond lengths, and bond angles are given in the ESI.† Compound 6 crystallizes in the tetragonal space group I41cd with eight chemical formula units per unit cell (Fig. (3a)). The calculated crystal density for compound 6 is 1.905 g cm−3 at 100 K. Interestingly, the 1H-tetrazol-1-ol rings and the ethene bridge are nearly coplanar. In the crystal packing of 6, strong intermolecular hydrogen bonds and π–π stacking interactions are observed, which make a positive contribution to its density (Fig. 3b and c). The length of the hydrogen bond (O–H⋯N) is 1.927 Å and the distances of the π–π interactions between the stacked rings range from 3.038 to 3.203 Å.
Compound 7 crystallizes in the orthorhombic space group Ima2 with four chemical formula units per unit cell (Fig. (4)). The calculated crystal density for compound 7 is 1.506 g cm−3 at 100 K. In the crystal packing of 7, intermolecular interactions are between the hydroxylamine cations and the bistetrazole anion. The two tetrazole rings are perpendicular to each other. The compound is nonplanar which reduces its crystal density significantly.
Compound 8 crystallizes in the triclinic space group P with one chemical formula unit per unit cell (Fig. (5)). The calculated crystal density for compound 8 is 1.585 g cm−3 at 100 K. Relative to compound 7, compound 8 exhibits higher density due to the planar bistetrazole anions.
All atoms of the ethene-linked bistetrazole rings are coplanar. In addition, intermolecular hydrogen bonding and π–π stacking interactions are observed, which also make a positive contribution to the density. The distance of π–π interactions between the stacked rings is 3.195 Å.
Compound 9 crystallizes in monoclinic space group P21/c with four chemical formula units per unit cell (Fig. (6)). The calculated crystal density for compound 9 is 1.668 g cm−3 at 100 K. In the crystal packing of 9, intermolecular interactions are observed between the hydroxylammonium cations and the bis(1H-tetrazol-1-olate) anion.
Since crystal packing strongly influences physical properties of energetic compounds, two-dimensional (2D) fingerprints and the associated Hirshfeld surfaces41,42 are employed by using Crystalexplorer17.5 to understand structure–properties and intermolecular interactions in 6 (Fig. 7a and b). Red and blue dots on the Hirshfeld surface represent high and low close contacts, respectively. Strong stabilizing intermolecular (N⋯H) interactions are observed which contribute to high density and good thermal stability. In addition, high percentages (22.9%) of N⋯N, and N⋯C interactions are observed which denote π–π stacking between the molecules. This is also supported by noncovalent interaction (NCI) plots of gradient isosurfaces for 6 (Fig. c). The green surface is seen clearly in Fig. 7c due to the presence of π–π interactions.43–45 The combination of N⋯H and π–π interactions leads to the good molecular stability of compound 6.
Fig. 7 (a and b) Hirshfeld surface graphs and 2D fingerprint plots of 6. (c) Non-covalent interaction plots of gradient isosurfaces 6. |
Additionally, planar molecules with layered packing and π–π stacking interactions tend to exhibit reduced sensitivity by converting mechanical energy into electrostatic attraction between layers. Specifically, parallel planar-layered packing of molecules can effectively reduce the friction sensitivity (FS). As shown in Fig. 8a and b, FS of compound 6 is significantly larger in comparison to (E)-5,5′-(diazene-1,2-diyl)bis(1H-tetrazol-1-ol) (V). In comparison to V, the stabilizing interactions in compound 6 also ensure the safe compression of the molecule during impact. The IS and FS of compound 6 is also found to be superior to 5,5′-(hydrazine-1,2-diyl)bis(1H-tetrazol-1-ol) (IV) (Table 1).
Fig. 8 Comparison of sensitivity properties of compound 6 with (E)-5,5′-(diazene-1,2-diyl)bis(1H-tetrazol-1-ol) (V). |
T d (°C) | ρ (g cm−3) | ΔHfd (kJ mol−1)/kJ g−1 | P (GPa) | D v (m s−1) | ISg (J) | FSh (N) | |
---|---|---|---|---|---|---|---|
a Temperature of decomposition (onset). b Density – gas pycnometer at 298 K. c Crystal density at 100 K. d Calculated molar enthalpy of formation. e Calculated detonation pressure. f Calculated detonation velocity. g Impact sensitivity (IS). h Friction sensitivity (FS). i Ref. 47. j Ref. 48. k Ref. 49. All compounds were obtained as anhydrous powders to determine the properties in Table 1. | |||||||
4 | 253 | 1.50 | 584.2/3.52 | 17.6 | 7267 | >40 | >360 |
5 | 275 | 1.72 | 790.9/4.82 | 24.6 | 8229 | >20 | >240 |
6 | 226 | 1.86/1.91c | 776.9/3.96 | 32.6 | 9017 | >10 | >120 |
7 | 255 | 1.47/1.51c | 369.2/1.59 | 20.1 | 7771 | >40 | >360 |
8 | 288 | 1.56/1.59c | 597.7/2.60 | 23.6 | 8183 | >40 | >360 |
9 | 230 | 1.63/1.69c | 553.3/2.11 | 26.8 | 8462 | >40 | >360 |
IVi | 120 | 1.71 | 390.1 | 31.2 | 8711 | 1 | <5 |
Vi | 170 | 1.90 | 883.2 | 42.4 | 9548 | <1 | <5 |
TNTj | 295 | 1.65 | −59.4/−0.26 | 19.4 | 6824 | 15 | >353 |
RDXk | 204 | 1.80 | 92.6/0.42 | 34.9 | 8795 | 7.5 | 120 |
The thermal behavior of compounds 4–9 was explored using differential scanning calorimetry (DSC) at a heating rate of 5 °C min−1. The decomposition temperatures (onset) for all the compounds occur between 226 (6) and 288 (8) °C (Table 1). Densities which were measured using a gas pycnometer at 25 °C, range between 1.47 (7) to 1.86 (6) g cm−3 (Table 1). To study the energetic properties of compounds 4–9, the molar enthalpies of formation are calculated by using isodesmic reactions with the Gaussian 03 (revision D.01) suite of programs.
All the compounds have positive heats of formation (ΔHf) which fall between 369.2 to 790.9 kJ mol−1. Using the calculated HOFs and pycnometer densities, the detonation properties of compounds 4–9 are calculated with the EXPLO5 (version 6.06.02) code.46 (Table 1). The detonation velocities (calculated) are between 7267 and 9017 m s−1, and detonation pressures (calculated) range from 17.6 to 32.6 GPa, respectively. The detonation velocity (9017 m s−1) of compound 6 is superior to RDX (8795 m s−1). For comparison, we have also calculated the detonation properties of compounds 4–9 using the earlier EXPLO5 (version 6.01) code. The results are given in the ESI† (Table S1). The impact sensitivity and FS for compounds 4–9 are determined by using BAM standard methods. In comparison to RDX, compound 6 is less sensitive. In addition, the thermal stability and sensitivity properties of compound 6 are also found to be superior to compounds IV and V (Fig. 1 and Table 1).
Footnote |
† Electronic supplementary information (ESI) available: Isodesmic reactions, synthesis of compounds 3–9, DSC analysis, 1H, 13C and 14N NMR data, X-ray crystal structure parameters of 6, 7, 8 and 9. CCDC 2160643–2160646. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d2ma00664b |
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