Agata N.
Kuznetsova
ab,
Nikita E.
Leonov
a,
Oleg V.
Anikin
a,
Michael S.
Klenov
*a,
Aleksandr M.
Churakov
*a,
Yurii A.
Strelenko
a,
Roman A.
Novikov
a,
Ivan V.
Fedyanin
c,
Alla N.
Pivkina
d,
Tatiana S.
Kon’kova
d,
Valery P.
Sinditskii
e,
Anastasia D.
Smirnova
e and
Vladimir A.
Tartakovsky
a
aN. D. Zelinsky Institute of Organic Chemistry Russian Academy of Sciences, 47 Leninsky prospect, Moscow, 119991, Russian Federation. E-mail: klenov@ioc.ac.ru; churakov@ioc.ac.ru
bDepartment of Chemistry, Lomonosov Moscow State University, 1 Leninskie Gory, Moscow, 119991, Russian Federation
cA. N. Nesmeyanov Institute of Organoelement Compounds Russian Academy of Sciences, 28 Vavilova st., Moscow, 119991, Russian Federation
dN. N. Semenov Federal Research Center for Chemical Physics Russian Academy of Sciences, 4 Kosygin st., Moscow, 119991, Russian Federation
eMendeleev University of Chemical Technology, 9 Miusskaya Square, Moscow, 125047, Russian Federation
First published on 26th November 2024
The design of novel high energy density materials (HEDMs) is still one of the significant challenges in the field of applied chemistry. Newly discovered scaffolds are rare, but they open up new possibilities for HEDM design. Herein, a simple and effective two-step approach to previously unknown 1,4-dihydro-[1,2,3]triazolo[4,5-d][1,2,3]triazole (1) is presented. This compound is an individual energetic material (d = 1.84 g cm−3, , Tonset = 193 °C (all experimental values), D = 8.5 km s−1, P = 34 GPa (calculated ones)), but may also serve as a scaffold for the synthesis of structurally diversified related compounds. The precursors of triazolo–triazole 1 are previously unknown 5-amino-4-diazo-4H-1,2,3-triazolium chloride (4) and 5-amino-4-diazo-4H-1,2,3-triazole (5), which can also serve as starting materials for the synthesis of a variety of novel heterocycles. For example, the diazo compound 5 was used for the regioselective synthesis of a 2,5-disubstituted triazolo–triazole 10 bearing an N4-tripoid fragment. Overall, the developed approach to triazolo–triazole 1, 5-amino-4-diazo-4H-1,2,3-triazolium chloride (4) and 5-amino-4-diazo-4H-1,2,3-triazole (5) is expected to make these high nitrogen systems more accessible and affordable for the design of nitrogen containing fused heterocycles.
These advantages can be used to improve the energetic performance of target molecules.2 For a long time, a limited number of available fused heterocyclic backbones for the synthesis of structurally diverse energetic compounds have hindered the progress of the area of HEDMs. Over recent years, there have been several achievements that encouraged the dynamic development of this field of energetic materials. A variety of fused-ring-based high-energy materials have been elaborated by various research teams.9–14
[5,5]-Bicyclic heterocyclic EMs are at the forefront of high-energy research due to their high enthalpy of formation, good thermal stability and high density.
Pyrazolo[4,3-c]pyrazole (type A), pyrazolo[3,4-d][1,2,3]triazole (type B), [1,2,4]triazolo[4,3-b][1,2,4]triazole (type C), pyrazolo[3,4-c][1,2,5]oxadiazole 5-oxide (type D) and [1,2,3]triazolo[4,5-c][1,2,5]oxadiazole (type E) are promising polynitrogen scaffolds for the construction of novel high-energy materials (Fig. 1). In the last few years these heterocyclic systems made up the backbone of a number of modern EMs synthesized by the research teams led by Shreeve, Klapötke and others.15–31
One of the promising [5,5]-bicyclic heterocyclic scaffolds for perspective HEDMs is the [1,2,3]triazolo[4,5-d][1,2,3]triazole (TT) core.21 At the same time, known [1,2,3]triazolo[4,5-d]-[1,2,3]triazoles are limited to a number of examples bearing non-energetic aliphatic or aryl substituents at the 1,5- or 2,5-positions (Fig. 2).32–38 The parent unsubstituted 1,4-dihydro-[1,2,3]triazolo[4,5-d][1,2,3]triazole 1 has not been previously described.
![]() | ||
Fig. 2 The previously known non-energetic triazolo–triazoles, triazolo–triazole TT 1 synthesized here, and the future prospects of the functionalization of the triazolo–triazole framework. |
Here, we report the first synthesis and properties of parent 1,4-dihydro-[1,2,3]triazolo[4,5-d][1,2,3]triazole (1), which is a potential precursor for novel highly functionalized energetic triazolo–triazoles. TT 1 has several positions for functionalization, and there is the possibility of introducing various substituents which could subsequently be transformed into explosophore groups (Fig. 3).
Diazotization of aminotriazole 2 with NaNO2 in AcOH led to the formation of an intermediate diazonium salt, which, after dilution of the reaction mixture with ethanol, precipitated from the solution as diazo compound 3 in 35% yield. The replacement of AcOH with CF3CO2H resulted in an increase in the yield of diazotriazole 3 to 85%.
The formyl group of compound 3 was removed with concentrated HCl to afford diazonium salt 4. The latter is the first unsubstituted 1,2,3-triazole bearing an adjacent diazonium group and unsubstituted amino group.
Treatment of diazonium salt 4 with one equivalent of NaOH afforded 5-amino-4-diazo-4H-1,2,3-triazole (5) (Scheme 2a). The reaction was accompanied by a change in colour from yellowish to dark red. Compound 5 is the first heterocyclic diazo compound bearing adjacent diazo and amino groups. In the solid state it decomposed slowly at room temperature, but we were able to obtain good 13C and 14N NMR spectra in D2O solution recorded at 10 °C, which confirm its structure (for details, see the ESI†).
Treatment of diazonium salt 4 with 3 equiv. of NaOH followed by heating under reflux for 15 min was accompanied by a color change from dark-red to colorless, indicating completion of the cyclization process with the formation of sodium salt 6a. Subsequent neutralization of the solution with 3 equiv. of HCl gave target TT 1, which precipitated from the reaction mixture in 61% yield (see Scheme 2a). It was demonstrated that a three-fold excess of HCl led to the opening one of the triazole rings of TT 1, returning diazonium salt 4 in quantitative yield.
The optimization of the synthetic route provided a more convenient procedure for preparing TT 1 (Scheme 2b). Heating under reflux diazo compound 3 with 3 equiv. of NaOH led to removal of the N-formyl group. Subsequent acidification of the reaction mixture with 3 equiv. of HCl gave TT 1 in 92% yield. This one-pot conversion of compound 3 into TT 1 is a convenient and efficient method for the preparation of the latter in gram scale quantities.
TT 1 on treatment with aqueous bases (NaOH, KOH or 25% aqueous solution of tetraethylammonium hydroxide) afforded the corresponding disodium (6a), dipotassium (6b) and di tetraethylammonium (6c) salts in quantitative yields (Scheme 3a). Sodium salt 6a exists in a form of dihydrate, which is confirmed by elemental analysis and DSC/TGA. Salt 6c is a stable heptahydrate and its structure and molecular composition were confirmed by single crystal X-ray diffraction analysis and elemental analysis.
To gain insight into the regioselectivity of alkylation of TT 1 and its anion, we used methylation and tert-butylation reactions (see Scheme 3). Methylation of salts 6a–c with MeI resulted in four possible isomers 7a–d. The major products were 1,5-dimethyl TT 7a (57%) and 2,5-dimethyl TT 7b (25%), while 1,6- and 1,4-isomers 7c and 7d were minor products. The highest total yield of 7a–d (96%) was achieved from salt 6c·7H2O in MeCN at room temperature for 3 days (for details, see the ESI,† Table TS1). Replacing MeI with Me2SO4 resulted in a significantly lower overall yield of methylated isomers (34%).
tert-Butylation of TT 1 with excess tBuOH in the presence of 70% aqueous HClO4 for 3 h at room temperature yielded 1,5-disubstituted TT 8 (53%) and salt 9 (26%) (Scheme 3b). Increasing the reaction time to 24 h resulted in exhaustive tert-butylation of TT 8 to form salt 9 in 63% yield.
It should be noted that 1,6-isomer 7c and 1,4-isomer 7d are representatives of a hitherto unknown class of disubstituted triazolo–triazoles. Salts of 1,3,5-trisubstituted triazolo–triazole, such as salt 9, have also not been described previously.
Among dimethyl substituted triazoles, 2,5-disubstituted TT 7b is the most thermally stable isomer (Tonset >278 °C) (for more details, see the section ‘Physicochemical and energetic properties’). This is probably due to the lack of the possibility of ring-chain tautomerism in this isomer. Accordingly, it is 2,5-disubstituted triazolo–triazoles that are the most promising isomers for obtaining energetic compounds. The search for a regioselective method for the synthesis of such compounds is a challenging task.
As a model compound for developing a new synthetic protocol, we chose TT 10 bearing methyl and morpholine substituents at the 2,5-positions (Scheme 4). One of the reasons for choosing this particular compound is that we plan to create a convenient method for the synthesis of amino-substituted triazolo–triazoles, which could be converted into energetic compounds containing a tripoid N4-fragment.22
The starting compound in our synthetic protocol was diazonium salt 4 (see Scheme 4). After adding two-fold excess of morpholine to the MeCN solution of this salt, the color of the reaction mixture immediately changed to red-brown, indicating the formation of the intermediate diazo compound 5. Subsequent holding of the reaction mixture for 3 days at room temperature afforded triazole 11 in a 53% yield. Reaction of the latter with diazomethane gave methylated triazole 12 in a 65% yield (other isomers were obtained in trace amounts). Diazotization of triazole 12 followed by reaction with NaN3 resulted in azido-substituted triazole 13 (78% yield). Heating the latter under reflux in PhMe for 5 h resulted in cyclization to afford TT 10. Note that this synthetic approach has analogies in the literature.33–35
The use of the developed regioselective approach for the synthesis of energetic 2,5-disubstituted triazolotriazoles will be described in the following papers.
The crystal (space group P21/n, Z′ = 0.5) contains only half of the molecule in the asymmetric unit, as the molecule is located at an inversion center. Thus, the molecule's inherent symmetry allows for two potential isomeric configurations: a C2h symmetric isomer with protonated N1 and N4 atoms, or a D2h symmetric isomer with protonated N2 and N5 atoms.
Analysis of H-bonding patterns is also inconclusive due to the presence of multiple potential donor–acceptor pairs with similar interatomic distances (ca. 2.9–3.0 Å), including a shortened N1⋯N2 contact.
To resolve this ambiguity, periodic DFT calculations (PBE0-D3/POB-TZVP) were performed on both potential isomers. The calculations employed experimental unit cell parameters and symmetry, with initial non-H atomic coordinates derived from the PXRD solution. Comparative analysis of the optimized structures favored the 1,4-disubstituted isomer, as evidenced by its superior fit to the experimental PXRD pattern without refinement (see the ESI,† Fig. S2–S4), higher calculated lattice and cohesive energies (32.5 and 31.3 vs. 26.0 and 24.2 kcal mol−1), and a more reasonable hydrogen bonding network. The 1,4-hydrogen atom positions are also consistent with solid-state NMR data (see below). The final refined structure was obtained through restrained refinement of the PXRD pattern using the DFT-optimized 1,4-disubstituted isomer as a starting point.
While a detailed discussion of the molecular geometry is not feasible due to the data source, some general observations can be made. Notably, the refinement with weak restraints yields reasonable bond lengths and angles, consistent with a virtually planar conformation (Fig. 4). Furthermore, the N1–N2 bond, expected to be longer due to the protonated nitrogen atom, was refined to be elongated as anticipated. However, the refined length of 1.378 Å is slightly longer than in both the dimethyl analogue 7d (1.3608(15) Å, see below) and PBE0-D3/POB-TZVP optimized structure (1.359 Å). In turn, as expected, the N2–N3 bond appears to be shortened with the length of 1.320 Å but to a greater extend as compared to the 7d analogue (1.3299(14) Å).
The packing pattern of TT 1 is primarily defined by H-bonds of average strength (N1⋯N2 2.848(3), H1⋯N2 1.952 Å, N1–H1⋯N2 145° with N–H 1.020 Å), which connect molecules into nearly flat layers. As discussed previously, the molecule resides at the inversion center, which in the space group P21/n necessarily belongs to the (1 0 −1) diagonal plane. Furthermore, the molecule adopts a nearly coplanar arrangement with respect to this plane. This geometric configuration allows for the straightforward calculation of the interlayer distance based on the distance between equivalent planes, which is equal to 3.206 Å. The molecules in the layers are in turn connected by π⋯π contacts. As molecules in the adjacent layers are shifted relative to each other, the shortest interlayer contacts are characterized by slightly higher distances (C3A⋯C3A 3.312(3) and N2⋯N2 3.382 Å).
Density (d) is an important characteristic of energetic materials as their detonation performance is directly proportional to this one.42 Among triazolo–triazoles obtained in this study only TT 1 is an energetic compound itself. The density of TT 1 calculated from the PXRD data is equal to 1.842 g cm−1 (298 K) and virtually coincides with the value from the pycnometer measurement. Such a high value is supported by the presence of strong intermolecular interactions in the crystal lattice, which usually lead to an increase in the density. This value of density is comparable to that of 3,3′-azo-bis(6-amino-1,2,4,5-tetrazine) (DAAT) which is considered the most dense C,H,N molecule known to date43,44 (for details see the ESI†).
The 1,4-dimethyl substituted TT 7d also crystallizes in non-centrosymmetric space group P, with half of the molecule in the independent part of the unit cell (Fig. 5). Bond lengths and angles are comparable with those obtained for TT 1via a restrained refinement, and with the values characteristic of similar heterocyclic compounds containing an annulated triazole cycle, as proven by Mogul geometry check.45 The N1–N2 bond with the substituted nitrogen atom (1.3608(15) Å) is expectedly longer than the N2–N3 bond (1.3299(14)), while C3A–N1 and C3A–N3 bond lengths are nearly equal (1.3561(15) and 1.3590(16) Å).
Despite the absence of the classical H-bonds as in TT 1, the crystal packing of the molecules in 7d is also layered. The layers are co-planar to the (1 0 1) and equivalent crystallographic planes, with the calculated interlayer distance of 3.169 Å. The molecule itself is tilted with respect to this plane by 9.4°, thus forming a step-like arrangement. The molecules within the layers are connected by non-classical C–H⋯N bonds (C⋯N 3.5798(18), H⋯N 2.497 Å, C–H⋯N 171° with C–H 1.092 Å), forming a pattern quite similar to that observed in TT 1, despite the apparent weakness of the intermolecular bonds. The layers are connected by π⋯π stacking interactions, with the shortest interatomic distance C⋯N of 3.3338(15) Å. In addition, due to the presence of methyl groups, there are also C–H⋯N contacts between the layers (C⋯N 3.4768(16), H⋯N 2.742 Å), which are not possible in the case of TT 1.
Compd | N-1 | N-2 | N-3 | N-4 | N-5 | N-6 |
---|---|---|---|---|---|---|
TT 1 | −105.9 | −36.0 | −105.9 | −105.9 | −36.0 | −105.9 |
TT 1 (solid state) | −168.3 | −7.8 | −77.6 | −168.3 | −7.8 | −77.6 |
7a | −178.1 | 14.2 | −57.7 | −91.3 | −116.4 | −74.1 |
7b | −79.9 | −107.8 | −79.9 | −79.9 | −107.8 | −79.9 |
7c | −179.0 | 3.3 | −54.6 | −54.6 | 3.3 | −179.0 |
7d | −172.2 | 7.4 | −71.9 | −172.2 | 7.4 | −71.9 |
![]() | ||
Fig. 7 15N NMR spectra for (a) TT 1 (solid-state, 9.5 kHz MAS, 18 msec CP) and (b) its 1,4-dimethyl derivative 7d (solution). |
The combination of data on the thermal stability obtained from our work and literature allows us to conclude that 2,5-substituted derivatives exhibit the highest thermal stability among triazolo–triazoles.
The thermal stability of TT 1 was investigated under both non-isothermal (DSC analysis for solid TT 1 and its solution in 2,4,6-trinitrotoluene) and isothermal conditions (decomposition study using Bourdon manometers for solid TT 1). The decomposition of TT 1 in the solid state can be described by the Arrhenius equation: k1 = 6.18 × 1020·e(−25215/T) which characterizes the decomposition in a defect-free crystal lattice, while k2 = 1.20 × 1020·e(−23890/T) characterizes the decomposition at crystal defects. The activation energies Ea of these two processes are 210 and 199 kJ mol−1, respectively (see the ESI†). Additional experiments investigating the decomposition of TT 1 in a 2,4,6-trinitrotoluene solution have showed that the decomposition rate was significantly higher than that in the solid state. The decomposition of TT 1 in solution is described by the following equation: kliq = 9.14 × 1014·e(−16930/T) (Ea = 141 kJ mol−1). Based on the kinetic data, we proposed a mechanism for the thermal decomposition of TT 1 (Scheme 5). Apparently, the rate-limiting stage of decomposition is the opening of the TT ring.
Besides the thermal stability another important property of energetic materials is the standard enthalpy of formation .42 The standard enthalpy of combustion
of TT 1 was experimentally determined by the combustion calorimetry (bomb calorimetry) method. The standard enthalpy of formation
was calculated from
(for details see the ESI†). TT 1 has
, which is much higher than those of the most common energetic materials such as 1,3,5-trinitro-1,3,5-triazinane (RDX) and N-methyl-N-(2,4,6-trinitrophenyl)nitramide (tetryl) (Table 3). Preliminary safety testing and detonation performance evaluation of TT 1 were carried out. As can be seen in Table 3, TT 1 has a calculated detonation velocity of 8.5 km s−1 and detonation pressure of 34 GPa. Compared to DAAT and common energetic materials (RDX, N-methyl-N-(2,4,6-trinitrophenyl)-nitramide (tetryl)), the studied compound demonstrated superior detonation performance to DAAT (8.4 km s−1 and 33.0 GPa), and tetryl (7.6 km s−1 and 26.0 GPa). However, the performance of TT 1 was somewhat lower than that of RDX (8.9 km s−1 and 36.0 GPa).46 The impact sensitivity of TT 1 (8 J) was slightly higher than that of RDX (10 J). TT 1 has a friction sensitivity value close to the primary explosives (FS = 15 N).
Compounds | TT 1 | DAATo | RDXr | Tetrylu |
---|---|---|---|---|
a Molecular weight. b Nitrogen content. c Oxygen balance toward CO2. d Oxygen coefficient for a compound with the molecular formula of CxHyNwOz, α = z/(2x + y/2). e Density. f Melting point. g Decomposition temperature measured at a heating rate of 5 °C min−1. h Experimentally measured standard enthalpy of formation. i Calculated detonation velocity. j Calculated detonation pressure. k Impact sensitivity. l Friction sensitivity. m Density measured by powder diffraction at 298 K. n Calculated from empirical equations implemented in the PILEM application. o 3,3′-Azo-bis(6-amino-1,2,4,5-tetrazine). p Ref. 43. q Ref. 44. r 1,3,5-Trinitro-1,3,5-triazinane. s Ref. 47. t Ref. 48. u N-Methyl-N-(2,4,6-trinitrophenyl)-nitramide. | ||||
Formula | C2H2N6 | C4H4N12 | C3H6N6O6 | C7H5N5O8 |
M w | 110.03 | 220.07 | 222.03 | 287.01 |
Nb (%) | 76.35 | 76.35 | 37.84 | 24.39 |
Ω CO2 (%) | −72.7 | −72.7 | −21.6 | −47.4 |
α | 0 | 0 | 0.67 | 0.49 |
d (g cm−3) | 1.84m | 1.84p | 1.82s | 1.73s |
1.76q | ||||
T m (°C) | — | — | 204s | 129s |
T onset (°C) | 193 | 252p | 204s | 188t |
301q | ||||
ΔHf°![]() |
+1005 | +940p | +72s | +17s |
+1123q | ||||
D (km s−1) | 8.5n | 8.4n | 8.9n | 7.60n |
8.1n | 8.75s | 7.57s | ||
P C–J (GPa) | 34.0n | 33.0n | 36.0n | 26.0n |
30.0n | 35.0s | |||
ISk (J) | 8 | — | 10t | 14t |
IFl (N) | 15 | 324q | 130t | 204t |
Footnote |
† Electronic supplementary information (ESI) available: Experimental procedures and characterization of new compounds including NMR spectra and X-ray. CCDC 2382714 and 2382722–2382729. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d4nj04427d |
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