Lukas
Bauer
,
Maximilian
Benz‡
,
Thomas M.
Klapötke
*,
Cedric
Pignot
and
Jörg
Stierstorfer
Department of Chemistry, Ludwig-Maximilian University Munich, Butenandtstr. 5-13, 81377 Munich, Germany. Web: http://www.hedm.cup.uni-muenchen.deE-mail: tmk@cup.uni-muenchen.de
First published on 19th March 2022
With the synthesis of 5-(1-hydroxy-3-nitro-1,2,4-triazol-5-yl)-1-hydroxy-tetrazole (1) we can report the first successful production of a combined bis-heterocyclic system composed of 1-hydroxy-tetrazole and 1-hydroxy-1,2,4-triazole. The straightforward synthesis modifies the cyano group of the nitro-triazole starting material within four steps to the tetrazol-1-ol and finally oxidizes the triazole selectively to the 1-hydroxy-triazole, resulting in compound 1, which is a hybrid molecule of the two in energetic materials chemistry established bis-heterocyclic motifs 1,1′-dihydroxy-3,3′-dinitro-bis-1,2,4-triazole and 1,1′-dihydroxy-5,5′-bistetrazole. In order to tune and improve the performance parameters, several nitrogen rich bases were used to obtain the respective ionic derivatives. All compounds were characterized using multinuclear NMR and IR spectroscopy, differential thermal analysis (DTA) and elemental analysis. Several compounds could be further analyzed using X-ray diffraction measurements. The heats of formation for all investigated compounds were determined and the detonation properties (EXPLO5 V6.05.02) were calculated. These data, as well as the sensitivity values, were compared to related substances.
Of high potential for replacing the currently common secondary explosives are triazole-, tetrazole- and furazan-based compounds, especially in the form of bis-heterocycles. These scaffolds exhibit high densities, highly endothermic heats of formation and therefore good performance compared to several single ring systems.7,11–14
Since, in addition to a high heat of formation, density plays the major role in the calculation of detonation parameters, some recurring strategies are widely used to increase it, such as nitration of the molecular backbone, formation of a system consisting of π-stacking parts or the synthesis of ionic derivatives to maximize the packing coefficient.8,15,16
Another approach is to utilize N-oxidation, which not only has the advantage of increasing the oxygen balance but also boosting the density through the addition of a further heteroatom. Fig. 1 depicts some prominent molecular moieties containing bis-heterocyclic systems and N-oxides at the respective position 1.17–23 Among the most promising molecules developed with the aim of replacing RDX are the bis-hydroxylammonium derivatives of 3,3′-dinitro-bis-1,2,4-triazol-1,1′-diolate (MAD-X1)19 and 5,5′-bistetrazol-1,1′-diolate (TKX-50),18 which are attracting great attention in the international community.24–30
Combination of 1-hydroxy-tetrazole and 1-hydroxy-3-nitro-1,2,4-triazole yields the hybrid molecule 1-hydroxy-3-nitro-(1,2,4-triazol-5-yl)-1-hydroxy-tetrazole (1) with the aim to combine the positive properties of the fundamental symmetric bis-heterocycles in a new asymmetric molecule: preferrable the high heat of formation of 1,1′-dihydroxy-5,5′-bistetrazole (A) with the high density and insensitivity toward external stimuli of 1,1′-dihydroxy-3,3′-dinitro-bis-1,2,4-triazole (Fig. 2).
Oxidation of 5-(3-nitro-1,2,4-triazol-5-yl)-1-hydroxy-tetrazole at the triazole yielded 5-(1-hydroxy-3-nitro-1,2,4-triazol-5-yl)-1-hydroxy-tetrazole trihydrate (1) and was performed with Oxone® as an oxidant (Scheme 2). This has already been established as a suitable reagent in similar reactions.16,32,33 The reaction was buffered to pH = 7 in an aqueous medium using tri-sodium phosphate dodecahydrate. Other buffer reagents, such as sodium and potassium acetate and sodium hydrogen carbonate, as well as non-buffered conditions were examined but did not yield 1 at all. Maximal yields of 70% were achieved with a reaction time of 16 h at room temperature (25 °C). Due to the electron withdrawing effect of the nitro group of the triazole, the oxidation occurs selectively at the meta position to the nitro function. All attempts to dehydrate 1 failed, as it kept drawing and absorbing water from the air.
Ionic derivatives 2–7 were obtained by dissolving 1 in ethanol or ethanol/water mixtures and adding two equivalents of the respective base to the solution. For the ammonium salt 2, gaseous ammonia was bubbled through the solution for about 1 minute. Compounds 2–5 precipitated immediately as water free salts and were used for characterization without further purification after washing with a small amount of the respective solvent. For compounds 6 and 7 the solution had to be reduced to precipitate the solid. In the case of compounds 2–6, the double salts were obtained. Despite the use of two equivalents of the base, only the mono triaminoguanidinium derivative 7 could be obtained, which is known to happen from similar systems (Scheme 3).34
Compound 1 crystallizes as a trihydrate in the orthorhombic space group Cmca with a cell volume of 1969.5(7) Å3 and eight molecular units per unit cell. The cell constants are a = 6.239(12) Å, b = 7.842(16) Å and c = 40.259(8) Å while the density is 1.809 g cm−3 at 293 K. Compared to the room temperature densities of 1,1′-dihydroxy-5,5′-bistetrazole·2 H2O (1.778 g cm−3) and 1,1′-dihydroxy-3,3′-dinitro-bis-1,2,4-triazole·2 H2O (1.829 g cm−3), 1 lies in the middle of the two values as it is a chemical mixture of both of them.18,19 The crystal structure is depicted in Fig. 1a. The bond lengths in both azole rings are in the range of N–N (N5–N6, 1.332(3) Å; N2–N3, 1.309(4) Å) and N–C (N1–C1, 1.339(4) Å; N7–C2, 1.341(4) Å) single and double bonds, respectively. The bond lengths for the N-oxides are 1.339(3) Å (O1–N1) and 1.337(3) Å (O2–N5) which is a normal value for N-bonded hydroxides donating electron density into the aromatic system. The angles N1–O1–H1 (107(3)°) and N5–O2–H2 (102(3)°) are close to the ideal tetrahedral angle, yet deviate slightly from it, which can be explained by the hydrogen bridges that have formed. Due to the orthorhombic symmetry, the molecule itself is completely planar (N1–C1–C2–N5, 180.00°; O3–N8–C3–N7, 180.00°). Each bis-heterocycle is surrounded by eight water molecules. All heteroatoms with the exception of N2 and N8 are involved in the formation of a network consisting of strong to moderately strong hydrogen bonds, which cover a distance range of 1.57(4) Å (O2–H2_a⋯O6) to 2.63(6) Å (O6–H2_b⋯O4). This results in the layered stacking of 1 shown in Fig. 3b with a layer distance of 3.12 Å.
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Fig. 3 (a) Molecular structure of 1 as determined by X-ray diffraction with thermal ellipsoids drawn at the 50% probability level; (b) 2D layer structure of 1 viewed along the b axis. |
Bis-ammonium derivate 2 crystallizes in the monoclinic space group P21/n with a cell volume of 914.2 Å3 and four molecular units per unit cell. The cell constants are a = 4.3259(1) Å, b = 26.9849(8) Å and c = 7.9243(2) Å, while the density is 1.803 g cm−3 at 106 K. The two aromatic rings with their N-oxides form an almost planar configuration (O1–N1–C1–C2, 0.5(3)°; N4–C1–C2–N7, 170.00(5)°; O2–N5–C2–C1, 175.6(2)°). Only the nitro group of the triazole is twisted out of this plane 13.2(2)°(O3–N8–C3–N6). Every anionic bis-heterocycle is surrounded by nine ammonium cations, forming a large number of hydrogen bonds. 2 forms a wave like structure along the b axis (Fig. 4b). The change of orientation takes place after two formula units of the anion. The ammonium cations are located between the anion layers.
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Fig. 4 (a) Molecular structure of 2 as determined by low temperature X-ray diffraction with thermal ellipsoids drawn at the 50% probability level; (b) zig-zig pattern of 2 viewed along the ac plane. |
Compound 3 crystallizes in the triclinic space group P with a cell volume of 528.11(19) Å3 and two molecular units per cell. The constants are a = 3.6755(4) Å, b = 8.0751(9) Å and c = 17.8693(18) Å while the density is 1.750 g cm−3 at 173 K. The nearly planar anion (N5–C2–C1–N1, 175.4(3)°; O4–N8–C3–N6, 173.1(3)°; O1–N1–N2–N3, 179.3(3)°) forms a layer like structure along the bc plane, as depicted in Fig. 5b. The free spaces between the respective layers are filled by hydrazinium cations, which form a large number of hydrogen bonds to the double anion.
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Fig. 5 (a) Molecular structure of 3 as determined by low temperature X-ray diffraction with thermal ellipsoids drawn at the 50% probability level; (b) layer structure of 3 viewed along the a axis. |
Compound 4 crystallizes with the inclusion of one water molecule in the monoclinic space group P21/c with a cell volume of 1100.2(3) Å3 and four molecular units per cell. The cell constants are a = 7.3751(11) Å, b = 15.0961(19) Å and c = 10.4402(14) Å while the density is 1.800 g cm−3 at 298 K. The anionic moiety is presented in almost planar conformation (O1–N1–C1–C2, −1.0(4)°; O2–N5–C2–C1, 0.3(4)°; O3–N8–C3–N6, 0.0(4)°). No other anion structure features this kind of coplanar arrangement of the aromatic rings. Along the ac plane, the bis-heterocycle forms a zig-zag-like structure, which is due to the same space group very similar to the three-dimensional structure of 2. The cations and the crystal water form layers between the respective linear chains of anions (Fig. 6b).
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Fig. 6 (a) Molecular structure of 4·H2O as determined by X-ray diffraction with thermal ellipsoids drawn at the 50% probability level; (b) zig-zag pattern of 4 along the b axis. |
Bis-aminoguanidinium derivative 6 crystallizes in the monoclinic space group I2/a with a cell volume of 2835.0(1) Å3 and eight molecules per unit cell. The cell constants are a = 11.245(2) Å, b = 6.7268(15) Å and c = 37.486(8) Å while the density is 1.698 g cm−3 at 100 K. Compound 6 is the most twisted anion structure for double deprotonated anions compared in this study. The two azole rings are twisted by 148.9(4)°(N4–C1–C2–N7) toward each other. As shown in Fig. 7b, the maximum number and strength of hydrogen bonds with the aminoguanidinium cation is achieved by this twist of the anion. Along b, the formation of channels of anions and cations occurs. It can also be observed that the aminoguanidinium units are twisted in relation to each other. This also results from the maximization of the intermolecular bonds.
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Fig. 7 (a) Molecular structure of 6 as determined by low temperature X-ray diffraction with thermal ellipsoids drawn at the 50% probability level; (b) pattern of 6 viewed along the a axis. |
Compound 7 crystallizes in the triclinic space group P with a cell volume of 611.07(13) Å3 and two molecular units per cell. The constants are a = 7.5556(8) Å, b = 8.1499(8) Å and c = 11.4798(12) Å while the density is 1.730 g cm−3 at 102 K. It is the only compound that is preserved only as a single salt. Compared to the structures described above, this also results in the unique assembly of 7. The single deprotonation occurs at the triazole OH group, since the proton there has a lower pKa value than the proton at the tetrazole as a result of the nitro substituent. This deprotonation also leads to the rotation of the rings relative to each other into a sterically unfavorable position, so that both hydroxy units are on the same side (N7–C2–C1–N4, 15.3(2)°). This ring formation is stabilized by a strong intramolecular interaction formed between the two hydroxy groups and the remaining proton. H1 can be classified as a divided proton, since it is more likely to be bound to O1, but also has a very strong interaction with O2 (O1–H1, 1.05(4) Å; O2–H1, 1.47(4) Å; O1–H1–O2, 171(2)°). Compared to the neutral compound 1, the bonds O1–H1 and O2–H1 (O1–H1, 0.86(4) Å; O2–H2, 0.85(4) Å) are significantly prolonged. Viewed along the ab plane (Fig. 8b), the mono-anion forms an oblique cylindrical structure in which the heterocycles are alternately superimposed. This pattern is embedded by triaminoguanidinium cations. Along the space diagonal (Fig. 8c), anions and cations are arranged in pairs in a chessboard-like structure, with the respective orientation flipped by 90° toward each other.
Proton coupled 15N NMR measurements were measured for neutral compound 1 and bis-ammonium salt 2 as a representative for the anion moiety. For the two bis-heterocycles, eight different resonances were obtained. An additional signal is detectable in the spectrum of 2. This belongs to the resonance of the ammonium cation. By comparison with the spectra of the respective symmetric molecules 1,1-dihydroxy-5,5′-bistetrazole (A)17 and 1,1′-dihydroxy-3,3′-dinitro-bis-1,2,4-triazole (B)19 all signals could be assigned, as shown in Fig. 9. The double deprotonation results in a shift of some signals to lower fields. That is the case for the two oxygen-substituted nitrogen atoms N1 and N5 as well as N3. The nitrogen atoms N2, N4, N6, N7 and N8 remain almost unchanged by the deprotonation, with respect to the chemical shift.
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Fig. 9 Proton coupled 15N NMR spectra of 1 (top, (a)) and 2 (bottom, (b)) measured in DMSO-D6. Chemical shifts are given with respect to MeNO2. |
1 | 2 | 3 | 4 | 5 | 6 | 7 | TKX-50 | MAD-X1 | β-HMX | |
---|---|---|---|---|---|---|---|---|---|---|
a Impact sensitivity (BAM drophammer (1 of 6)). b Friction sensitivity (BAM friction tester (1 of 6)). c Electrostatic discharge device (OZM research). d From X-ray diffraction analysis recalculated to 298 K; * Density is based on gas pycnometer measurement at 25 °C. e Nitrogen content. f Oxygen balance with respect to the formation of CO2. g Decomposition temperature (DTA; β = 5 °C min−1). h Calculated enthalpy of formation. i Calculated energy of formation. j Energy of explosion. k Detonation temperature. l Volume of detonation products (assuming only gaseous products). m Detonation pressure at Chapman-Jouguet point. n Detonation velocity. | ||||||||||
Formula | C3H8N8O7 | C3H8N10O4 | C3H10N12O4 | C3H8N10O6 | C5H12N14O4 | C5H14N16O4 | C4H10N14O4 | C2H8N10O4 | C4H8N10O8 | C4H8N8O8 |
M [g mol−1] | 268.13 | 248.16 | 278.19 | 280.16 | 332.24 | 362.28 | 318.21 | 236.15 | 324.17 | 296.16 |
ISa [J] | >40 | >40 | 10 | 20 | >40 | 40 | 7 | 20 | >40 | 7 |
FSb [N] | >360 | >360 | 216 | 324 | >360 | >360 | 192 | 120 | >360 | 112 |
ESD [J]c | 0.50 | 0.37 | 0.10 | 0.20 | 0.25 | 0.25 | 0.10 | 0.10 | 0.50 | 0.20 |
P [g cm−3] | 1.808 | 1.753 | 1.718 | 1.885* | 1.707* | 1.649 | 1.681 | 1.877 | 1.90 | 1.904 |
N [%] | 44.8 | 56.4 | 60.4 | 50.0 | 59.0 | 61.9 | 61.6 | 59.3 | 43.2 | 37.84 |
Ω [%] | −19.2 | −38.7 | −40.3 | −22.8 | −57.8 | −57.4 | −45.3 | −27.1 | −19.7 | −21.6 |
T dec [°C] | 169 | 265 | 206 | 205 | 270 | 219 | 204 | 221 | 217 | 279 |
ΔfH0![]() |
−261.4 | 200.6 | 547.3 | 316.4 | 261.9 | 490.6 | 615.5 | 447.0 | 222.3 | 74.8 |
ΔfU0![]() |
−233.0 | 227.8 | 579.6 | 346.2 | 299.1 | 532.7 | 650.2 | 474.3 | 254.5 | 109.5 |
Explo5 V6.05.02 | ||||||||||
−ΔExU0![]() |
4587 | 4378 | 5825 | 5631 | 3557 | 3995 | 6383 | 5758 | 5670 | 5700 |
T
det![]() |
3126 | 2995 | 3353 | 3573 | 2518 | 2709 | 3978 | 3513 | 3670 | 3623 |
V
0![]() |
820 | 873 | 907 | 831 | 865 | 889 | 875 | 910 | 778 | 763 |
P
CJ![]() |
313 | 284 | 311 | 386 | 244 | 249 | 318 | 401 | 381 | 378 |
V
det![]() |
8666 | 8650 | 9052 | 9490 | 8271 | 8358 | 9058 | 9940 | 9270 | 9193 |
At least since the synthesis of TKX-50 and MAD-X1 and their establishment as green secondary explosive replacements, the benefit of introducing N-oxidation to nitrogen-rich azoles is undeniable.18,38–41 The advantages are not only the apparent increase of the oxygen balance, but also the increase of the respective densities as well as higher thermal robustness, since the introduction of an oxygen adds another site for the hydrogen bridge acceptor.
Hydroxylammonium, formally oxidized ammonium, is for several reasons of great interest in energetic materials chemistry. As for the oxidation of the heterocycles, the main advantages are the increased oxidation balance and the elevated density of the resulting salt. With the increasing numbers of N-oxides, a clear trend is visible of better performance parameters for a growing number of introduced oxygen atoms. Fig. 10 depicts the investigation on the effect of rising numbers of N-oxidations based on the heterocyclic motif 5-(3-nitro-1,2,4-triazol-5-yl)-tetrazole.42 Hydroxylammonium was chosen as the cation for this comparison, but similar trends can be seen for other salts. For the decomposition point, an increase of about 25 °C compared to the minor oxidized compounds G and H is observed for 4, even if this trend is not completely unambiguous. The densities were all determined through pycnometric measurements and are therefore easily comparable among themselves. The density of 4 is more than 0.1 g cm−3 higher than that of G, which is due to the double N-oxidation. The closely related detonation rate also increases with increasing N-oxidation. In general, it can be noted that the rise in density and detonation velocity from G to H is not as large as from H to 4. However, it can be stated that there is a clear improvement in all energetic parameters with increasing numbers of N-oxides.
Footnotes |
† Electronic supplementary information (ESI) available: A detailed Experimental and X-ray diffraction section, details and graphic illustrations of the thermal analysis and the computational methods. CCDC 2144424–2144432. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/d2ma00135g |
‡ First author. |
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