Carles
Miró Sabaté
*a,
Henri
Delalu
a,
Valérian
Forquet
a and
Erwann
Jeanneau
b
aLaboratoire Hydrazines et Composés Ènergétiques Polyazotés, Université Claude Bernard Lyon 1, Bâtiment Berthollet, 3è étage, 22, avenue Gaston Berger, 69622, Villeurbanne, France. E-mail: carlos.miro-sabate@univ-lyon1.fr; Fax: +33-472-431-291
bCentre de Diffractométrie Henri Longchambon, Université Claude Bernard Lyon, 1, 43 Bd. du 11 novembre 1918, 69622, Villeurbanne, France. E-mail: erwann.jeanneau@univ-lyon1.fr; Fax: +33-472-431-160
First published on 6th March 2012
The reaction of 1,1-dimethylhydrazine with excess dichloromethane led to the formation of the chloride salt of the 1-(chloromethyl)-1,1-dimethylhydrazinium cation ([(CH3)2N(CH2Cl)NH2]Cl, 1). The reaction of 1 with a suitable silver salt provided the nitrate ([(CH3)2N(CH2Cl)NH2][NO3], 2), perchlorate ([(CH3)2N(CH2Cl)NH2][ClO4], 3), azide ([(CH3)2N(CH2Cl)NH2][N3], 4), dicyanamide ([(CH3)2N(CH2Cl)NH2][N(CN)2], 5) and sulphate ([(CH3)2N(CH2Cl)NH2]2[SO4], 6) salts. Compound 6 reacted with barium 5,5′-azobistetrazolate pentahydrate (Ba[N4C–N
N–CN4]·5H2O), barium dipicrate tetrahydrate (Ba[(NO2)3Ph–O]2·4H2O) and barium 5-amino-1H-tetrazolate tetrahydrate (Ba[H2N–CN4]2·4H2O) to form the corresponding metathesis products: [(CH3)2N(CH2Cl)NH2]2[N4C–N
N–CN4] (7), [(CH3)2N(CH2Cl)NH2][(NO2)3Ph–O] (8) and [(CH3)2N(CH2Cl)NH2][H2N–CN4] (9). Compounds 1–9 were characterized by elemental analysis, mass spectrometry, NMR (1H and 13C) and vibrational spectroscopy (infrared and Raman). Additionally, we measured the 15N NMR spectrum of the nitrate salt 2 and identified the solid state structure of compounds 3, 6, 7 and 8 by low temperature X-ray crystallography (3: Triclinic P
, a = 5.983(1) Å, b = 7.502(1) Å, c = 9.335(1) Å; α = 93.86(1)°, β = 101.21(1)°; γ = 91.13(1)°; V = 409.8(1) Å3, 6: Monoclinic C2/c, a = 11.674(2) Å, b = 17.503(3) Å, c = 6.616(1) Å; β = 90.27(1)°; V = 1351.8(4) Å3, 7: Triclinic P
, a = 8.851(1) Å, b = 8.872(1) Å, c = 11.529(1) Å; α = 80.98(1)°, β = 83.47(1)°; γ = 71.37(1)°; V = 845.4(1) Å3 and 8: Monoclinic C2/c, a = 24.168(3) Å, b = 7.375(1) Å, c = 17.062(3) Å; β = 116.19(2)°; V = 1351.8(3) Å3). The solid state structure of barium dipicrate hexahydrate (Ba[(NO2)3Ph–O]2·6H2O) was also elucidated: Triclinic P
, a = 6.641(1) Å, b = 11.588(1) Å, c = 15.033(1) Å; α = 84.64(1)°, β = 80.07(1)°; γ = 86.80(1)°; V = 1133.8(1) Å3. Furthermore, we studied the thermal properties of compounds 1–9 by differential scanning calorimetry (DSC). Salts 2–4, 8 and 9 fall within the category of ionic liquids. Lastly, the energetic salts were subjected to standard sensitivity tests and a software code was used to predict the detonation parameters and specific impulses of the compounds and their mixtures with an oxidizer.
N–CN4]2−).
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| Scheme 1 A general method for the synthesis of a) alkyltriazanium salts8,9 and b) alkylhydrazinium salts.10,11 | ||
Later on, the authors of ref. 8 also reported the synthesis of a new family of salts based on the [(CH3)2N(R)NH2]+ cation (R = Me, Et, n-Bu, allyl, propargyl, –CH2CH2OH and –CH2CN) and dicyanamide ([N(CN)2]−) and nitrocyanamide ([N(CN)(NO2)]−) anions.10 From these two studies it could be concluded that both [(CH3)2N(NH2)2]+ and [(CH3)2N(R)NH2]+ cations can be used for the formation of ionic liquids with hypergolic properties.
In 2001, the Sharp group11 reported on the unexpected easy reaction between 1,1-dimethylhydrazine (UDMH) and dichloromethane or 1,2-dichloroethane to form [(CH3)2N(CH2Cl)NH2]Cl (1) and [(CH3)2N(CH2CH2Cl)NH2]Cl, respectively. Our research in the field of hydrazines12 drew our attention to the easy synthesis of 111,13 and we hypothesised whether the [(CH3)2N(CH2Cl)NH2]+ cation might form salts with interesting energetic properties. In this report we present our results on the synthesis, characterization and energetic testing of several energetic salts based on the previously relatively neglected [(CH3)2N(CH2Cl)NH2]+ cation.
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| Scheme 2 The synthesis of salts of the [(CH3)2N(CH2Cl)NH2]+ cation. | ||
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| Scheme 3 A general reaction equation leading to the formation of [MeNH–NH3]Cl. B = monomethylhydrazine (MMH). | ||
Compound 1 was weighed in a nitrogen-filled glove box and reacted with a suitable silver salt in either water or alcohol, leading to the precipitation of silver chloride and the formation of the nitrate ([(CH3)2N(CH2Cl)NH2][NO3], 2), perchlorate ([(CH3)2N(CH2Cl)NH2][ClO4], 3), azide ([(CH3)2N(CH2Cl)NH2][N3], 4), dicyanamide ([(CH3)2N(CH2Cl)NH2][N(CN)2], 5) and sulphate ([(CH3)2N(CH2Cl)NH2]2[SO4], 6) salts (Scheme 1). Subsequently, the sulphate salt (6) was reacted in either water or alcohol with a suitable barium compound to form insoluble barium sulphate and the corresponding 5,5′-azobistetrazolate ([(CH3)2N(CH2Cl)NH2]2[N4C–N
N–CN4], 7), picrate ([(CH3)2N(CH2Cl)NH2][(NO2)3Ph–O], 8) and 5-amino-1H-tetrazolate ([(CH3)2N(CH2Cl)NH2][H2N–CN4], 9) salts. Alternatively, the corresponding silver salts can be used to synthesise compounds 7, 8 and 9. However, due to the high sensitivity of silver 5,5′-azobistetrazolate and silver picrate towards impact and friction, the barium salts are preferred from the standpoint of safety. Compounds 1–6 are colourless materials, whereas 7 and 8 are bright yellow solids. Salts 1–9 are readily soluble in alcohol, acetone (except for 1), water, DMSO or DMF and insoluble in apolar solvents, such as dichloromethane and ether. Lastly, all the materials in this work are stable to hydrolysis.
The harmonic vibrational frequencies computed for the [(CH3)2N(CH2Cl)NH2]+ cation are summarized in the supporting information (SI Table 1†) with the average experimental data. The B3LYP computed values show an overestimation in comparison to the experimental frequencies since anharmonicity was neglected in the real system.18 The frequencies of the [(CH3)2N(CH2Cl)NH2]+ cation observed experimentally in the different compounds were found at fairly consistent values. The Raman spectra were characterized by two bands of strong activity at ca. 2980 cm−1 (C–H symmetrical stretching) and at ca. 740 cm−1 (N–N and C–Cl stretching modes). The IR spectra, however, were dominated by asymmetric and symmetric N–H stretching modes at 3275 and 3180 cm−1, respectively. Additionally, other bands of lower intensity could be assigned as follows (ν = stretching, δ = in-plane bending, γ = out-of-plane bending, ω = in-plane rocking, τ = torsion and s = symmetric): 2880–3050 cm−1 [νs(C–H)], 1430–1620 cm−1 [δ(N–H) + δ(N–H)], 1290–1390 cm−1 [γ(C–H) + γ(N–H)], 970–1250 cm−1 [τ(C–H) + τ(N–H)], 740–970 cm−1 [ω(N–H) + ω(C–H)], ca. 565 cm−1 [νs(N–C)] and <500 cm−1 [ω(C–H) + ω(N–H)].19,20
The structure of the [(CH3)2N(CH2Cl)NH2]+ cation in compounds 1–9 was also characterized by multinuclear (1H, 13C and 15N) NMR spectroscopy in DMSO-d6 (SI Table 2†). The 1H NMR spectra showed the three expected resonances. The methyl group resonated at ca. 3.3 ppm, whereas the –CH2Cl group resonance is shifted to a lower field at ca. 5.4 ppm and the –NH2 group protons were found between ca. 6.2 and 6.7 ppm. In the 13C NMR spectra the methyl groups resonated at ca. 53 ppm and the –CH2Cl carbon atoms at ca. 72 ppm. Lastly, we measured the 15N NMR spectrum (natural abundance) of the [(CH3)2N(CH2Cl)NH2]+ cation for the nitrate salt 2 (Fig. 1). The –N(CH3)2) group resonated at ca. 85 ppm and no coupling was observed whereas the –NH2 group coupled at one bond with its protons (1JN–H = 66.7 Hz) and appeared as a triplet at ca. 116 ppm.
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| Fig. 1 The 15N NMR spectrum of [(CH3)2N(CH2Cl)NH2][NO3] (2) in DMSO-d6. | ||
To obtain a better understanding of the structure of the [(CH3)2N(CH2Cl)NH2]+ cation, the optimized structure of the [(CH3)2N(CH2Cl)NH2]+ cation in the gas phase was obtained using B3LYP functional analyses with a B3LYP/6-311+G(d,p) basis set.21 A natural bond orbital (NBO) analysis22 was performed on the optimized structure of the [(CH3)2N(CH2Cl)NH2]+ cation (Fig. 2). The optimized gas phase geometry of the [Me2N(CH2Cl)NH2]+ cation is identical to that found in the solid state structure of [(CH3)2N(CH2Cl)NH2]2Cl (1, Fig. 3) but not to that found for [(CH3)2N(CH2Cl)NH2][ClO4] (3, Fig. 4), which forms an intramolecular hydrogen bond (see the discussion further on). According to the NBO analysis, N6 carries a relatively large negative charge (−0.604 e), whereas Cl1 carries a small positive charge (+0.047 e). This charge distribution suggests that N6 can form hydrogen bonds, whereas Cl1 should not. These results are in agreement with the X-ray crystallography studies that show, in contrast to Cl1, that N6 participates in the formation of medium-to-strong hydrogen bonds (SI Table 5†).
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| Fig. 2 Optimized geometry and charge distribution in the [Me2N(CH2Cl)NH2]+ cation as found with NBO analysis (B3LYP/6-31+G(d,p)). | ||
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| Fig. 3 Diamond plot (at 50% probability) of the asymmetric unit of [Me2N(CH2Cl)NH2]Cl (1) with the labelling scheme. The dashed line represents the hydrogen bond between the [(CH3)2N(CH2Cl)NH2]+ cation and the Cl− anion. | ||
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| Fig. 4 Diamond plot (at 50% probability) of the asymmetric unit of [Me2N(CH2Cl)NH2](ClO4) (3) with the labelling scheme and the formation of an intramolecular hydrogen bond (dashed line). | ||
Contrary to the structure of the previously reported chloride salt 1 (Fig. 3),13 the N3–C2 bond in [Me2N(CH2Cl)NH2][ClO4] (3) is twisted so that the chlorine atom forms an intramolecular hydrogen bond (N6⋯Cl1 = 3.117(5) Å) with the graph-set descriptor S(5) (Fig. 4).23,24 This intramolecular hydrogen bond is also found for one of the two crystallographically independent [(CH3)2N(CH2Cl)NH2]+ cations in the crystal structure of [(CH3)2N(CH2Cl)NH2]2[N4C–N
N–CN4] (6) (see X-ray discussion in the supporting information†).
The cation in [Me2N(CH2Cl)NH2][ClO4] (3) forms two classical hydrogen bonds to the anion, which result in the formation of infinite zig-zag chains running parallel to the a-axis (Fig. 5). These chains take the graph-set descriptor C2,2(6) and are analogous to the C2,2(4) motifs found in the crystal structure of [Me2N(CH2Cl)NH2]Cl (1).13
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| Fig. 5 The formation of zig-zag chains along the a-axis via hydrogen-bonding (dashed lines) in the crystal structure of [Me2N(CH2Cl)NH2](ClO4) (3, view along the c-axis). | ||
The sensitivities towards impact, friction and electrostatic discharge of the salts of the [(CH3)2N(CH2Cl)NH2]+ cation in this study were tested using BAM procedures (Table 1).29–32 None of the compounds tested positive towards impact (BAM drop-hammer sensitivity: >40 J) and friction (BAM friction tester sensitivity: >360 N) nor when spraying sparks across a small sample of the materials using a Tesla coil (ESD testing). Also, no decomposition reaction was observed when grinding the compounds vigorously in a ceramic mortar. Therefore, the salts of the [(CH3)2N(CH2Cl)NH2]+ cation in this study are safe for transport according to international standards.32 In comparison to commonly used energetic materials, e.g. TNT or RDX = 1,3,5-trinitroperhydro-1,3,5-triazine,33 the compounds described in this report are less sensitive towards classical stimuli and they are also less sensitive than other salts based on the same anions.34,35
| T ex (K)a | V 0 (L kg−1)b | P det (kbar)c | D (m s−1)d | I sp (s)e | Impact (J) f | Friction (N) f | ESD (±)g | Thermal Shock h | |
|---|---|---|---|---|---|---|---|---|---|
| a Temperature of the explosion gases. b Volume of the explosion gases. c Detonation pressure (detonation run with 1% TFNA = trifluoro-trinitro-azahexane). d Detonation velocity (detonation run with 1% TFNA = trifluoro-trinitro-azahexane). e Specific impulse (isobaric combustion for the pure compound at a chamber pressure = 60.0 bar). f Impact and friction sensitivity values according to BAM methods (see ref. 29–32). g Rough sensitivity to electrostatic discharge using a Tesla coil (∼20 kV), + sensitive, − insensitive. h Response of fast heating in the “flame test”. | |||||||||
| 2 | 3672 | 794 | 190 | 7395 | 193 | >40 | >360 | — | Burns |
| 3 | 5190 | 749 | 279 | 8160 | 225 | >40 | >360 | — | Deflagrates |
| 4 | 2524 | 757 | 187 | 7120 | 196 | >40 | >360 | — | Burns |
| 5 | 3005 | 675 | 145 | 6518 | 189 | >40 | >360 | — | Burns |
| 7 | 3632 | 725 | 240 | 7926 | 223 | >40 | >360 | — | Burns |
| 8 | 3671 | 654 | 203 | 7278 | 181 | >40 | >360 | — | Burns |
| 9 | 2415 | 746 | 189 | 7250 | 201 | >40 | >360 | — | Burns |
The electronic energies of the [(CH3)2N(CH2Cl)NH2]+ cation and the anions of salts 2, 3, 4, 5, 7, 8 and 9 were obtained from quantum chemical calculations (MP2). These values were used to predict the formation energies of salts 2, 3, 4, 5, 7, 8 and 9 (Table 2). The predicted formation energies of compounds 2, 3, 4, 5, 7, 8 and 9 have positive values and are lowest for the carbon-richer picrate salt (8, ΔU°f = 195 kJ kg−1) and highest for the nitrogen-richer 5,5′-azotetrazolate salt (7, ΔUf = 2866 kJ kg−1). These values are between those of TNT33 and of the highly endothermic bis(hydrazinium) 5,5′-azotetrazolate (ΔU°f = +3700 kJ kg−1).36
| 2 | 3 | 4 | 5 | 7 | 8 | 9 | |
|---|---|---|---|---|---|---|---|
| Formula | C3H10N3ClO3 | C3H10N2Cl2O4 | C3H10N5Cl | C5H10N5Cl | C8H20N14Cl2 | C9H12N5ClO7 | C4H12ClN7 |
| a Phase transition temperature. b Decomposition point (DSC onsets) from measurement with β = 5°C min−1. c Oxygen balance according to ref. 46. d Density from pycnometer (2, 4 and 5) or X-ray (3, 7 and 8) measurements. e Lattice enthalpy. f Computed (MP2)35 energy of formation. g Computed (MP2) enthalpy of formation. | |||||||
| MW (g mol−1) | 171.58 | 209.03 | 151.60 | 175.62 | 383.24 | 337.67 | 193.64 |
| T m/Tg (°C)a | −9.7 | 52.0 | 17.2 | — | — | 77 | 64 |
| T d (°C)b | 161 | 180 | 147 | 188 | 172 | 208 | 165 |
| Ω (%)c | −70 | −46 | −111 | −132 | −104 | −78 | −111 |
ρ/g cm−3 d |
1.474 | 1.694 | 1.418 | 1.308 | 1.521 | 1.644 | 1.521 |
ΔHL/kJ mol−1 e |
514 | 507 | 525 | 496 | 771 | 444 | 502 |
ΔU°f/kJ kg−1 f |
566 | 1557 | 2376 | 2041 | 2866 | 195 | 2317 |
ΔH°f/kJ kg−1 g |
507 | 1512 | 2261 | 1985 | 2809 | 170 | 2202 |
The performance of new materials has been the centre of attention of recent investigations.37,38 Using the EXPLO539 computer software, it might be possible to calculate certain performance and detonation parameters of interest for compounds based on C, H, N, O, Al, Cl, Si and F. The program is based on Becker–Kistiakowsky–Wilson (BKWN) rules40 and uses the following values for the BKWN equation of state: α = 0.5, β = 0.176, κ = 14.71 and θ = 6620. The formation energies (ΔU°f) of the salts of the [(CH3)2N(CH2Cl)NH2]+ cation were back-calculated on the basis of the combustion equations of the compounds (see below), Hess's Law, the known standard heats of formation for dioxygen, carbon dioxide, water, dinitrogen and hydrogen chloride.41 Using the EXPLO5 computer code.39 these values were subsequently used in conjunction with the molecular formula and density of the compounds (either from the X-ray or from the pycnometer measurements) to predict the detonation performance parameters (pressure and velocity) and the specific impulse for each compound. The densities of the salts of the [(CH3)2N(CH2Cl)NH2]+ cation in this study varied from 1.308 (compound 5) to 1.694 (compound 3) g cm−3 and were higher than those of salts of the [(CH3)3NNH2]+ cation. For example, dicyanamide salt 3 (ρ = 1.308 g cm−3) was significantly denser than the analogous salt of the [(CH3)3NNH2]+ cation (ρ = 1.10 g cm−3).10
2: [(CH3)2N(CH2Cl)NH2][NO3] (l) + 3.75 O2 → 3 CO2 (g) + 4.5 H2O (l) + HCl (g) + 1.5 N2 (g)
3: [(CH3)2N(CH2Cl)NH2][ClO4] (s) + 3 O2 → 3 CO2 (g) + 4 H2O (l) + 2 HCl (g) + N2 (g)
4: [(CH3)2N(CH2Cl)NH2][N3] (s) + 5.25 O2 → 3 CO2 (g) + 4.5 H2O (l) + HCl (g) + 2.5 N2 (g)
5: [(CH3)2N(CH2Cl)NH2][N(CN)2] (l) + 7.25 O2 → 5 CO2 (g) + 4.5 H2O (l) + HCl (g) + 2.5 N2 (g)
7: [(CH3)2N(CH2Cl)NH2]2[N4C–N
N–CN4] (s) + 12.5 O2 → 8 CO2 (g) + 9 H2O (l) + 2 HCl (g) + 7 N2 (g)
8: [(CH3)2N(CH2Cl)NH2][(NO2)3Ph–O] (s) + 8.25 O2 → 9 CO2 (g) + 5.5 H2O (l) + HCl (g) + 2.5 N2 (g)
9: [(CH3)2N(CH2Cl)NH2][H2N–CN4] (s) + 6.75 O2 → 4 CO2 (g) + 5.5 H2O (l) + HCl (g) + 3.5 N2 (g)
The detonation parameters (i.e. detonation pressure and velocity) of compounds 2, 3, 4, 5, 7, 8 and 9 varied from P = 145 to 279 kbar and from D = 6518 to 8160 m s−1. Note that the formation energies were predicted using MP2-calculated electronic energies thus the calculated detonation parameters tended to be an overestimation.42 Whatever the case, the detonation velocities of compounds 2, 3, 6 and 7 were higher than that of TNT (D = 7171 m s−1) and the detonation velocities of the perchlorate (3, D = 8160 m s−1) and the 5,5′-azotetrazolate (7, D = 7926 m s−1) salts were expected to be comparable to that of nitroglycerine (D = 7714 m s−1).33 In comparison to analogous salts of the [(CH3)3NNH2]+ cation, the salts of the [(CH3)2N(CH2Cl)NH2]+ cation in this work had higher detonation parameters. For example, the dicyanamide salt 5 (Pdet = 145 kbar and D = 6518 m s−1) was expected to be more energetic than the dicyanamide salt of the [(CH3)3NNH2]+ cation (Pdet = 108 kbar and D = 6317 m s−1).10 On the other hand, the predicted specific impulses (Isp) varied between 181 s (8) and 225 s (3), higher than for recently reported salts based on the guanylurea cation43 and comparable to those of 1,1-dimethylhydrazine energetic salts.10
It is known that the performance of an energetic material is dependent on the compound's density, heat of formation and oxygen balance and that it reaches a maximum value when the oxygen balance is neutral.44 The densities of all the compounds in this work were calculated using the X-ray data of experimental measurements using a pycnometer. The compounds had moderate density values ranging from 1.308 (5) to 1.694 (3) g cm−3, which were, however, higher than those of recently reported polycyano-anion-based45 and 1,1-dimethylhydrazine energetic salts.10 The oxygen balances (Ω) of all the salts in this work were negative and varied between −46% (3) and −132% (5), in the range between commonly used RDX (Ω = −22%) and recently reported hypergolic ionic liquids, such as trimethylhydrazinium dicyanamide (Ω = −176%).10 Due to the negative oxygen balance (Ω) of compounds 2, 3, 4, 5, 7, 8 and 9, the performance parameters of mixtures of the compounds with an oxidizer, namely AN = ammonium nitrate (Ω = +20%) and ADN = ammonium dinitramide (Ω = +26%) were also calculated in order to increase the performance of the mixture in comparison to the stand-alone materials (SI Tables 7 and 8†). Formulations of compounds 2, 3, 4, 5, 7, 8 and 9 with AN or ADN are predicted to have higher detonation pressures and detonation velocities than isolated compounds. Mixtures with ADN are predicted to perform particularly well with detonation velocities comparable to pure RDX (D = 8750 m s−1).33 Also, formulations with AN and in particular with ADN are expected to have higher specific impulses than stand-alone compounds 2, 3, 4, 5, 7, 8 and 9, and those calculated for AN (Isp = 159 s) and ADN (Isp = 199 s).
Additionally, the melting points/glass transition temperatures and thermal stability of all the salts in this work were assessed by differential scanning calorimetry (DSC) measurements. The DSC measurements were carried out on small samples of the salts of the [(CH3)2N(CH2Cl)NH2]+ cation at a heating rate of β = 5°C min−1. Salts 2–4, 8 and 9 are ionic liquids (m.p. < 100 °C). Salts 2, 4 and 5 are room temperature ionic liquids. On the other side, the thermal stabilities of the compounds vary from moderate (4: 147 °C) to high (8: 208 °C). We are currently investigating the hypergolic properties of mixtures of the compounds in this study with WFNA in view to developing a possible energetic application. These results will be the subject of a future publication.
In addition to the DSC analysis, the response to fast heating under non-confinement conditions was tested by placing a small sample of the materials under a Bunsen burner flame. This resulted in normal burning for all the compounds except for the better oxygen-balance perchlorate salt (3), which presented a burning-to-deflagration transition. Under similar test conditions, commonly used energetic materials, such as TNT and RDX burn and deflagrate, respectively.
N–CN4] (7).
Method 1 (using silver 5,5′-azotetrazolate): Sodium 5,5′-azotetrazolate pentahydrate (0.337 g, 1.12 mmol) was dissolved in distilled water (5 mL) in a plastic beaker and reacted with two equivalents of silver nitrate (0.381 g, 2.24 mmol) producing the precipitation of the highly sensitive orange powder of silver 5,5′-azotetrazolate. The reaction mixture was stirred for ca. 15 min. in darkness and the solvent was then decanted, the silver salt was washed with a small amount of distilled water (2 times) and the water was eliminated by washing with methanol (2 times). Then, the orange solid was redissolved in fresh methanol (5 mL) and added to a solution of 1 (0.325 g, 2.24 mmol) in the same solvent (5 mL). Immediate precipitation of silver chloride took place and the reaction mixture was stirred in darkness. After 1.5 h, the insoluble materials were filtered, washed with fresh methanol and the solvent was rotavaporated, leaving behind the title compound as a yellow powder, which was purified by ether diffusion into a methanolic solution of the compound (0.401 g, 93%).
Method 2 (using barium 5,5′-azotetrazolate): This is a safer procedure, which avoids the use of highly sensitive silver 5,5′-azotetrazolate that can be used as an alternative: Barium 5,5′-azotetrazolate pentahydrate (0.627 g, 1.19 mmol) was suspended in distilled water (10 mL) and reacted with an equivalent amount of bis[1-(chloromethyl)-1,1-dimethylhydrazinium] sulphate (0.373 g, 1.19 mmol). The reaction mixture was stirred for 1.5 h at room temperature and the insoluble materials were filtered through a plug of Celite (previously washed with distilled water), washed with water and the filtrate was rotavaporated to dryness providing the crude material (0.442 g, 97%). Purification proceeded by ether diffusion into a methanolic solution of the compound. This procedure afforded X-ray quality single crystals. ρ (X-ray) = 1.521 g cm−3; C8H20N14Cl2 (MW = 383.24 g mol−1, calc./found): C 25.07/25.38, H 5.26/5.02, N 51.17/50.84; DSC (5 °C min−1): >172 °C (dec.); m/z (+c ESI, H2O): 109.0 (52, [Cat]), 492.9 (100, [Cat3A]), 876.2 (32, [Cat5A2]), 1259.5 (14, [Cat7A3]); m/z (–c ESI): 164.8 (18, [A2− + H+]−), 272.8 (11, [CatA]−), 655.2 (54, [Cat3A2]−), 1039.3 (100, [Cat5A3]−); 1H NMR (DMSO-d6, 400.18 MHz, TMS) δ (ppm): 3.41 (6 H, s, –CH3), 5.57 (2 H, s, –CH2Cl), 6.59 (2 H, s(br), –NH2); 13C 1H NMR (DMSO-d6, 100.52 MHz, TMS) δ (ppm): 173.19 (2 C, [C2N10]2−), 72.08 (1 C, –CH2Cl), 53.51 (2 C, N–CH3); Raman v˜/cm−1 (rel. int.): 3036(3), 2971(2), 2882(1), 2421(1), 1476(52), 1402(14), 1371(100), 1342(3), 1296(1), 1183(3), 1152(1), 1072(12), 1050(17), 918(8), 887(2), 811(2), 741(3), 371(1), 320(1); IR v˜/cm−1 (golden gate, rel. int.): 3276(m) 3197(m) 3075(m) 3029(m) 2322(w) 2194(w) 2037(w) 1958(w) 1656(w) 1466(m) 1435(w) 1419(w) 1406(w) 1378(m) 1347(w) 1336(w) 1303(w) 1244(w) 1180(w) 1165(w) 1149(w) 1123(w) 1095(w) 1067(w) 1050(w) 1034(w) 1025(w) 1006(w) 981(w) 947(w) 922(w) 890(s) 803(s) 772(m) 742(w) 720(s) 666(w) 596(w) 583(w) 554(m) 531(m) 509(m) 494(w) 487(w) 471(w).
Footnote |
| † Electronic supplementary information (ESI) available: complete cyrstal structure discussion, table of computed IR and Raman frequencies, NMR resonances table, X-ray tables, tables for formulations of compounds 2, 3, 4, 5, 7, 8 and 9 with AN and ADN, general method and synthesis of the starting materials. Additionally, the cif files of 3, 6, 7, 8 and Ba[(NO2)3Ph–O]2·6H2O have been deposited with the Cambridge Crystallographic Data Centre (CCDC). CCDC reference numbers 808540–808544. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c2ra00968d |
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