Sohan Lala,
Haixiang Gao
b and
Jean'ne M. Shreeve
*a
aDepartment of Chemistry, University of Idaho, Moscow, Idaho 83844-2343, USA. E-mail: jshreeve@uidaho.edu; Fax: +1-208-885-6173
bDepartment of Applied Chemistry, China Agricultural University, 100193, Beijing, China
First published on 30th January 2025
Cage compounds are potential kinetic rocks and thermodynamic powerhouses. Their strain energy plays a crucial role. Hence, adamantane, cubane, homocubanes, and bishomocubane skeletons have become prominent recently. However, research on the design and development of azahomocubane-based energetic materials has yet to be explored. The aim of the present work is to illustrate the potential of azahomocubanes as next-generation propellants, explosives and oxidizers. The energetic potential of any new materials was determined using B3LYP/6-31+G**, G2, and MP2/6-311++G** levels at the Gaussian 03 suite of programs. The new azahomocubanes possess a density range of 1.33 g cm−3 to 2.14 g cm−3. Most of the azahomocubanes have significantly elevated high-positive heats of formation ( to 728.41 kJ mol−1). Compounds AHC-12–19 have superior potentials as solid propellants in rocket propulsion. Additionally, this study reveals that compounds AHC-20 and AHC-21 could be highly effective primary explosives (AHC-20, P = 44.46 GPa, D = 9706 m s−1; AHC-21, P = 45.64 GPa, D = 9708 m s−1) exceeding the performance of RDX, HMX and comparable to that of ONC and CL-20. Our finding suggests that azahomocubanes have great potential in the field of energetic materials.
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Scheme 2 Highly dense top-performance energetic cage compounds.7,8 |
A homocubane was synthesized by Dunn et al.9 and Paquette et al.10 Subsequently, various research groups reported notable homocubanes derivatives.1,2,10,11 In contrast, an azahomocubane (AHC) is a relatively new compound synthesized by Eaton et al. by acid-catalyzed rearrangement of cubyl azides, giving 1-substituted 9-azahomocubanes.12 This transformation inspired Williams and co-workers to synthesize and characterize novel azahomocubane derivatives using dimethyl 1,4-cubanedicarboxylate 10.13 Subsequently, a new derivative of AHC, 1-azahomocubane, was reported.14 These recent reports demonstrate the feasibility of introducing nitrogen atoms into the homocubane skeleton. Based on the position of nitrogen, nine theoretical isomers are possible (Fig. 1).
Recent studies suggest that a secondary amine (9i, 9-azahomocubane) bearing isomer was the most stable skeleton compared to the other isomers with a tertiary amine.15 In contrast, 9-azahomocubane (9i, 9-AHC), rarely explored in the field of energetic materials, is a promising scaffold from the stereochemical perspective because it is effectively functionalized through the secondary amine moiety and the most stable skeleton over the other isomers, which allows the design of various novel energetic materials identified as an optimal cage skeleton for the present work (Scheme 3).
The densities of the title compounds were calculated using a newly developed modified Pulitzer method.18 Subsequently, based on their solid phase enthalpies of formation and calculated densities (Table 1), the corresponding propulsive (Isp and C*) and detonation performances (P and D) were evaluated using EXPLO5 V7.01 software.19
Compound | Formulaa | FWb [g mol−1] | N + Oc [%] | OBCO2![]() |
ΔHfse [kJ mol−1] | ρf [g cm−3] | Pg [GPa] | Dh [m s−1] | h50i [cm] |
---|---|---|---|---|---|---|---|---|---|
a Molecular formula.b Formula weight.c N + O contents in %.d CO2 based oxygen balance.e Calculated solid-phase standard enthalpy of formation.f Density calculated using the correlation of ρ = 1.0330 (M/V) + 0.001836 (σtot2ν) − (ν/6).18g Detonation pressure calculated using EXPLO5 V 7.01.h Detonation velocity calculated using EXPLO5 V 7.01.i h50 [cm] is the height from where 50% probability of the dropped materials resulted in an explosion calculated using equation S13. Then their corresponding impact energies h50[J] were calculated using a correlation h50[J] = mgh, where, m = 2.5 kg hammer weight, g = 9.81 m/s, and h = h50 [cm] values. | |||||||||
AHC-12 | C8H9N | 119.16 | 11.76 | −275.25 | 390.22 | 1.33 | 12.52 | 5670.94 | 27.07 |
AHC-13 | C8H8N2O2 | 164.16 | 36.55 | −175.44 | 402.36 | 1.53 | 15.88 | 6297.39 | 21.96 |
AHC-14 | C8H9N3O2 | 179.18 | 41.31 | −165.20 | 454.36 | 1.53 | 15.66 | 6593.09 | 44.66 |
AHC-15 | C9H10N2O2 | 178.19 | 33.68 | −188.57 | 356.02 | 1.47 | 14.67 | 6155.14 | 42.50 |
AHC-16 | C9H10N2O3 | 194.19 | 39.15 | −164.79 | 289.82 | 1.51 | 15.57 | 6278.67 | 45.26 |
AHC-17 | C9H10N4 | 174.21 | 32.16 | −211.25 | 728.41 | 1.40 | 14.41 | 6259.27 | 41.02 |
AHC-18 | C9H8N4O6 | 268.19 | 56.68 | −95.46 | 345.45 | 1.71 | 21.40 | 7254.70 | 56.70 |
AHC-19 | C10H10N4O6 | 282.21 | 53.86 | −107.72 | 322.45 | 1.66 | 19.20 | 7009.23 | 51.22 |
AHC-20 | C8HN9O16 | 479.14 | 79.74 | 25.04 | 309.04 | 2.08 | 44.46 | 9706.85 | 6.96 |
AHC-21 | C8N10O18 | 524.14 | 81.66 | 30.53 | 304.94 | 2.14 | 45.64 | 9708.21 | 6.98 |
Cubane | C8H8 | 104.15 | 0.0 | −307.69 | 602.64 | 1.29 | 12.70 | 5990.00 | 24.14 |
TNT | C7H5N3O6 | 227.13 | 60.76 | −73.96 | −59.30 | 1.65 | 18.56 | 6839.96 | 46.79 |
RDX | C3H6N6O6 | 222.12 | 81.06 | −21.61 | 70.30 | 1.80 | 34.01 | 8858.00 | 26.14 |
HMX | C4H8N8O8 | 296.16 | 81.06 | −21.61 | 74.80 | 1.91 | 38.44 | 9285.00 | 27.58 |
CL-20 | C6H6N12O12 | 438.18 | 82.17 | −10.95 | 397.80 | 2.04 | 46.70 | 9455.00 | 9.25 |
ONC | C8N8O16 | 464.13 | 79.29 | 0.0 | 604.20 | 2.06 | 46.60 | 9864.00 | 2.86 |
Additionally, the stability parameters of the new compounds, such as impact sensitivity (h50) (eqn (S13)‡), kinetic energy (ΔEHOMO–LUMO), and electrostatic potential (ESP) were predicted at the B3LYP/6-311++G (d,p) level of theory with the help of Multiwfn20 and VMD software21
Interestingly, derivatives AHC-14 and AHC-20 have vast potentials to generate energetic salts AHC-22–23, and that could be the future generation green solid propellants, explosives, and oxidizers (Scheme 4).
The computationally based design and studies of new high energy density materials (HEDMs) reveals the potential of new materials as an explosive and propellent in military and space industry applications. Thus, the efficiency of potential explosives can be measured in terms of their detonation performance (P and D), an oxidizer can be identified based on the combination of available oxygen for combustion, which is typically quantified in terms of oxygen balance (OB%) and specific impulse (Isp). High specific impulse (Isp) and density specific impulse (Isp) of a material, suggest their potential use as a propellant. In the present study, we evaluated all materials as solid materials, and their explosive and propulsive performances were calculated with different propellant formulations with hydroxylterminated polybutadiene (HTPB, a novel energetic binder), ammonium perchlorate (AP, oxidizer), and aluminium (Al, fuel supplement). Subsequently, their performance was compared with well-known energetic materials as listed in Tables 1 and 2.
Compound | ΔEa,i [HOMO–LUMO] | Ispb,i [s] | ρIspc,i [s] | C*![]() |
Ispe,i [s] | Ispf,i [s] | Ispg,i [s] | Isph,i [s] |
---|---|---|---|---|---|---|---|---|
a Energy difference between HOMO and LUMO orbitals in eV.b Isp = specific impulse of neat compound (monopropellant).c ρIsp = density specific impulse of neat compound (monopropellant).d Characteristic velocity.e Isp = specific impulse at 88% compound and 12% Al.f Isp = specific impulse at 78% compound, 12% Al (fuel additive) and 10% binder (HTPB).g Isp = specific impulse at 20% compound and 80% AP.h Isp = specific impulse at 80% compound and 20% HTPB.i Specific impulse calculated at an isobaric pressure of 70 bar and initial temperature of 3300 K using EXPLO5 V 7.01. | ||||||||
AHC-12 | 6.080 | 167.55 | 223.52 | 990.40 | 178.30 | 173.79 | 246.08 | 158.48 |
AHC-13 | 5.825 | 202.64 | 311.66 | 1226.70 | 267.98 | 248.30 | 258.38 | 185.10 |
AHC-14 | 5.446 | 207.17 | 318.63 | 1257.60 | 270.04 | 253.04 | 258.98 | 188.72 |
AHC-15 | 4.733 | 191.82 | 283.52 | 1155.60 | 242.20 | 226.34 | 256.28 | 177.16 |
AHC-16 | 4.869 | 199.36 | 301.63 | 1208.50 | 223.30 | 227.87 | 257.79 | 182.92 |
AHC-17 | 5.372 | 194.68 | 273.53 | 1166.10 | 203.03 | 195.66 | 255.71 | 179.49 |
AHC-18 | 4.326 | 227.86 | 390.78 | 1415.80 | 240.91 | 232.06 | 243.45 | 201.99 |
AHC-19 | 3.432 | 219.73 | 365.41 | 1358.50 | 236.95 | 229.91 | 247.79 | 196.94 |
AHC-20 | 5.183 | 263.02 | 548.40 | 1563.40 | 266.40 | 267.44 | 194.66 | 232.91 |
AHC-21 | 5.331 | 256.49 | 549.40 | 1525.40 | 261.51 | 273.27 | 189.49 | 237.40 |
Cubane | 7.046 | 114.30 | 147.45 | 667.40 | 105.44 | 106.87 | 231.53 | 108.99 |
TNT | 4.926 | 206.49 | 341.54 | 1283.5 | 232.00 | 225.11 | 186.98 | 200.55 |
RDX | 5.991 | 266.91 | 480.45 | 1648.00 | 276.68 | 274.08 | 254.06 | 234.12 |
AP | — | 156.63 | 306.15 | 977.00 | 232.00 | 262.11 | 156.63 | 227.37 |
Newly designed azahomocubanes AHC-12–21 possess high calculated densities (ρ = 1.33 g cm−3 to 2.14 g cm−3), associated with significantly positive solid-phase enthalpy of formation ( to 728.41 kJ mol−1), those are comparable to top performing energetic materials as listed in Table 1, which establish them as viable candidatesin the field of energetic materials. Compounds AHC-20–21 have high positive oxygen balances (AHC-20, OB% = 25.04 and AHC-21, OB% = 30.53) comparable to well-known oxidizers such as ammonium dinitramide (ADN, OB% = 25.80), ammonium perchlorate (AP, OB% = 27.23), 2,2,2-tetranitroacetimidic acid (TNAA, OB% = 30.12).
The detonation performance of azahomocubane was calculated using EXPLO5 V7.01 software as listed in Table 1. Compounds AHC-12–19 have an average detonation performance (P = 12.52 GPa to 21.40 GPa; D = 5670 m s−1 to 7254 m s−1) and which are comparable to cubane (P = 12.70 GPa; D = 5990 m s−1), and TNT (P = 18.56 GPa; D = 6839 m s−1). On the other hand, compound AHC-20–21 have detonation properties (AHC-20, P = 44.46 GPa, D = 9706 m s−1; AHC-21, P = 45.64 GPa, D = 9708 m s−1) which are better than those of top performing primary explosives RDX and HMX and comparable to ONC and CL-20.
The propulsive performance of azahomocubanes were predicted using EXPLO5 V7.01 software at five different propellent formulations and was examined (i) as a neat compound; (ii) at the ratio of 88:
12 (azahomocubanes
:
Al); (iii) at the ratio of 78
:
12
:
10 (azahomocubanes
:
Al
:
HTPB); (iv) at the ratio of 20
:
80 (azahomocubanes
:
AP); and (v) at the ratio of 80
:
20 (azahomocubanes
:
HTPB) listed in Table 2 and Fig. 3. This indicates that the specific impulse (Isp, s) and density specific impulse (ρIsp, g cm−3 s) of compounds AHC-20 and AHC-21 are significantly higher than TNT, RDX and AP. On the other hand, most of the compounds possess high characteristic velocity, making them promising candidates for solid rocket propulsion. Interestingly, compounds AHC-13 and AHC-14 at the ratio of 88
:
12 (azahomocubanes
:
Al) exhibit optimal specific impulse (AHC-13, Isp = 268 s; AHC-14, Isp = 270 s), revealing the best combination of strain (azahomocubanes core) and energy (–N–NO2 and –N–NH–NO2).
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Fig. 3 Comparison of physicochemical properties. (a) Densities (b) Detonation properties. (c) Propulsive properties. |
As for the kinetic stability, the energy gaps between HOMO and LUMO were estimated and are in the order of CB > AHC-12 > RDX > AHC-13 > AHC-14 > AHC-17 > AHC-21 > AHC-20 > TNT > AHC-16 > AHC-15 > AHC-18 > AHC-19, as listed in Table 2. Interestingly, the impact sensitivity of 20 and 21 is significantly higher (h50 (cm) = 6.96 and 6.98 respectively) compared to the impact sensitivity of RDX (26.14), HMX (27.58) and lower than that of ONC (2.86), making them promising primary explosive.
Additional analysis of stabilities of title compounds were evaluated with the help of electrostatic potential (ESP) measurements as shown in Fig. 4 and Fig. S14–S23.‡ Compounds 20 and 21 have comparable ESP maxima (+67.48 kcal mol−1 and +65.57 kcal mol−1, respectively) and global ESP minima (−12.03 kcal mol−1 and −10.13 kcal mol−1, respectively) to CL-20 (+66.61 kcal mol−1 and −15.74 kcal mol−1). For RDX (+50.01 kcal mol−1 and −20.81 kcal mol−1), and HMX (+53.74 kcal mol−1 and −24.80 kcal mol−1) see Fig. S3.‡ Furthermore, using scatter diagram and reduced density gradient (RDG), the high strain in the core structure and weak interaction between the substituents can be explained as shown in the Fig. 4b, 4c, 4d, 4e and Fig. S14–S23.‡
Footnotes |
† Dedicated to Professor Eaton for his pioneer work in cubane chemistry. |
‡ Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4dt03457k |
This journal is © The Royal Society of Chemistry 2025 |