C O M M U N I C A T I O N S
Table 1. Properties of Dianionic Energetic Salts
a
b
3
c
d
OB
e
f
g
h
h
i
j
k
compd
T
m
(°C)
T
d
(°C)
d
meas (g/cm )
IS (J)
∆
f
Hcation (kJ/mol)
∆
f
Hlat (kJ/mol)
∆
f
Hsalt (kJ/mol)
∆
f
Hsalt (kJ/g)
P (GPa)
v
D
(m/s)
Isp (s)
l
3
dec
217
218
220
265
248
235
244
198
281
222
290
295
1.83 (1.89) -49.6
-
-
626.4
669.5
770.0
575.9
667.4
769
1392.8
1309.3
1269.4
1234.5
1183.1
1143.4
1104.1
1121.1
1019.4
1963.2
1829.6
-
105.8
275.5
516.4
163.1
397.5
640.4
884.7
808.7
837.0
47.2
319.8
-67.0
-154.2
92.6
0.36
0.86
1.61
0.44
0.98
1.47
1.91
1.67
1.34
0.14
0.71
34.9
32.4
26.2
26.6
26.3
27.0
27.0
28.3
27.3
36.0
24.3
19.5
31.2
35.2
39.6
9407
8856
8455
8634
8603
8701
8705
8792
8474
9399
8267
6881
8114
8977
9320
200.8
240.0
227.1
191.3
202.3
212.6
221.9
207.8
212.3
194.7
182.8
-
4
5
6
7
8
9
1
1
1
1
dec
dec
dec
242
dec
237
178
dec
162
dec
81
1.78
1.63
-34.8
-50.0
11
l
1.70 (1.77) -64.1 >40
1.71
1.68
1.64
-63.3 >40
-62.6
-62.0
31
23
871.5
842
l
0
1
2
3
1.75 (1.78) -66.1 >40
1.80
1.95
1.80
1.65
1.93
1.82
1.91
-63.9 >40
805.3
1764.6
1903.6
-
-46.2
-63.7
-74.0
-55.8
-21.6
-21.6
38
32
15
50
7.4
7.4
TNT
-0.30
-0.54
0.42
TATB
RDX
HMX
350
dec
dec
∼360
-
-
-
230
-
-
-
-
-
287
-
104.8
0.35
a
b
c
Melting point. Thermal degradation temperature. Measured density. Values in parentheses were corrected by subtracting the volume of a water
3
d
e
f
g
molecule [V(H O) ) 25 Å ]. Oxygen balance. Impact sensitivity. Calculated molar heat of formation of the cation. Calculated molar lattice energy.
Calculated heat of formation of the salt. Calculated detonation pressure. Calculated detonation velocity. Calculated specific impulse in seconds.
Calculations were performed using the corrected density.
2
h
i
j
k
l
of 6, 7, 10, and 11 are greater than 40 J, so they can be classified as
salts fall in the range for new high-performance energetic materials
11
3
insensitive materials.
(1.8-2.0 g/cm ). One dicationic salt possesses the highest density of
The calculated heat of formation of BNT2- (245.8 kJ/mol) is much
more positive than that of monoanionic 3-nitroimino-1,2,4-triazolate
the reported energetic salts (1.95 g/cm ). The calculated detonation
3
velocities and detonation pressures of the salts are higher than those
of conventionally used TNT and TATB. Interestingly, the properties
of ammonium, hydroxyammonium, and carbonic dihydrazidinium salts
are similar and even superior to that of RDX, which suggests that
they may serve as a series of promising alternatives to RDX.
5c
(
-13.5 kJ/mol). Thus, it is not surprising that 6 and 7 exhibit much
higher heats of formation than their monoanionic guanidinium (0.27
5c
kJ/g) and aminoguanidinium (0.78 kJ/g) analogues. All of the salts
possess positive heats of formation that fall in the range 0.14-1.91
kJ/g. As anticipated, the calculated heats of formation increase with
increasing nitrogen content in the guanidinium-derivatized salts 6-9.
The calculated detonation pressures of 3-13, which lie in the range
Acknowledgment. The authors gratefully acknowledge the
support of DTRA (HDTRA1-07-1-0024), NSF (CHE-0315275),
ONR (N00014-10-1-0097), and NSFC (20971122), “One Hundred
Talent Project” in Chinese Academy of Sciences.
2
4.3-36.0 GPa, are higher than that of TNT (19.53 GPa) and
comparable to those of TATB (31.15 GPa) and RDX (35.2 GPa).
Detonation velocities (V ) were found in to be the range 8267-9407
D
Supporting Information Available: Experimental details for the
syntheses and characterization of all compounds; descriptions, figures, and
a CIF file of the crystal structure; details of the calculations; and description
m/s; they are higher than those of TNT (6881 m/s) and TATB (8114
m/s) and comparable to those of RDX (8977 m/s) and HMX (9320
m/s). All of the salts have specific impulse values ranging between
2
of and figure showing the charge distributions of H BNT. This material is
1
82.8 and 240.0 s. The promising performance suggests potential
available free of charge via the Internet at http://pubs.acs.org.
2-
applications of BNT salts as ingredients in explosives and propellants.
This is especially the case for 3, 4, and 12, as their energetic
performance values are very similar and even superior to those of RDX.
Single-crystal X-ray diffraction analysis confirmed the structure
References
(
(
1) Agrawal, J. P. Prog. Energy Combust. Sci. 1998, 24, 1.
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of H
Information). The strong intramolecular and intermolecular hydro-
gen bonds link the discrete H BNT molecules into a 2D layer
Figures S2 and S3). Structure optimization calculations on H BNT
2
BNT to be a nitroimine (Figure S1 in the Supporting
(
3) (a) Smiglak, M.; Metlen, A.; Rogers, R. D. Acc. Chem. Res. 2007, 40,
2
1
182. (b) Schmidt, M. W.; Gordon, M. S.; Boatz, J. A. J. Phys. Chem. A
(
2
2005, 109, 7285. (c) Talawar, M. B.; Sivabalan, R.; Senthilkumar, N.;
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further suggested that the nitroimine is the more stable form, as it
has a lower total energy (the threshold value between the two stable
isomers is 12.55 kcal/mol; Figure S4).
(
4) (a) Singh, R. P.; Verma, R. D.; Meshri, D. T.; Shreeve, J. M. Angew. Chem.,
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(
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Piotrowski, H.; Polborn, K.; Willer, R. L.; Weigand, J. J. J. Org. Chem.
2-
2-
To define the structure of BNT , four possible models of BNT
are provided (Figure S5). The differences in binding energy and binding
enthalpy between the models and H BNT were calculated. The
-positioned protons of 1,2,4-triazole in H BNT form intramolecular
2
(
1
2
hydrogen bonds with the nearest nitroimine oxygen atoms. The
hydrogen bonds were kept in model 1, and the binding energy of model
1
triazole in H BNT are easily lost during the reaction.
In summary, a simple and straightforward approach for the synthesis
of bis[3-(5-nitroimino-1,2,4-triazole)] has been developed. The structure
2
006, 71, 1295. (c) Drake, G. W.; Hawkins, T. W.; Hall, L. A.; Boatz,
J. A.; Brand, A. J. Propellants, Explos., Pyrotech. 2005, 30, 329.
7) Astakhov, A. M.; Vasil’ev, A. D.; Molokeev, M. S.; Revenko, V. A.;
Stepanov, R. S. Russ. J. Org. Chem. 2005, 41, 910.
(
was the lowest (Table S1). Thus, the 4-positioned protons of 1,2,4-
2
(8) (a) Metelkina, E. L.; Novikova, T. A. Russ. J. Org. Chem. 2004, 40, 1737.
(
b) Metelkina, E. L.; Novikova, T. A.; Berdonosova, S. N.; Berdonosov,
D. Y. Russ. J. Org. Chem. 2005, 41, 440.
(
9) Astachov, A. M.; Revenko, V. A.; Kruglyakova, L. A.; Buka, E. S. New
Trends Res. Energ. Mater., Proc. Semin., 10th 2007, 505.
2
of H BNT was confirmed as an N-nitroimine rather than a primary
(
(
10) Shreve, R. N.; Charlesworth, R. K. U.S. Patent 2,744,116, 1956.
11) According to the U.N. Recommendations on the Transport of Dangerous
Goods, impact sensitivity is defined as follows: insensitive, >40 J; less
sensitive, g35 J; sensitive, g4 J; very sensitive, g3 J.
N-nitroamine. Its salts, which can be easily synthesized and safely
handled, exhibit promising physical properties, such as low solubility
in common solvents, excellent thermal stability, high density, positive
heats of formation, and low shock sensitivity. The densities of some
JA1055033
J. AM. CHEM. SOC. 9 VOL. 132, NO. 34, 2010 11905