Xueli Zhang,
Junqing Yang,
Ming Lu and
Xuedong Gong*
School of Chemical Engineering, Nanjing University of Science and Technology, Nanjing 210094, China. E-mail: gongxd325@mail.njust.edu.cn
First published on 12th March 2015
Pyridylpentazole (PyN5) and its derivatives with 1–2 electron withdrawing groups (–NO2, –CN, –CF3 and –NF2) were studied using density functional theory to assess their potentials as the source of pentazole anion N5− for replacement of phenylpentazole (PhN5). N5− can be produced more easily from PyN5s because the activation energies (Ea,1 = 364.7–387.1 kJ mol−1) for the cleavage of the central C–N bonds of PyN5s are lower than that of PhN5 (395.3 kJ mol−1) and the C–N bond decomposition reactions of the former are faster than that of the latter. The energies (Ea,2) required for dissociation of the N5 ring of PyN5s (67.6–84.1 kJ mol−1) are smaller than that of PhN5 (88.7 kJ mol−1), and the rates of the former are faster than that of the latter. Comparing the stabilities of the C–N bond and the N5 ring of PyN5s and PhN5, the decrement in the C–N bond stability (2.1–7.8%) caused by the pyridine ring and substituents is less obvious than that of the N5 ring (12.7–23.7%). Although N5− can be obtained more easily and faster from PyN5s than PhN5, the smaller Ea,2 makes PyN5s less stable than PhN5, so pyridylpentazoles may not be a better source of N5− than phenylpentazole.
Previous study5 proposed that phenylpentazole (PhN5) can be used as the N5− source. This suggestion is supported by the experiments of Ostmark et al.12 and Vij et al.11 who detected that the central C–N bond linking the phenyl and pentazole rings could break and N5− exists in gas phase from high-energy mass spectrometric degradation of phenylpentazole. In addition, our recent study has shown that HN5 can be produced by breaking of the C–N bond of PhN5 and its derivatives with electron donating group.22 And the acidity of HN5 was estimated to be stronger than that of HNO3.23 Hence, once HN5 is generated by dissociation of the C–N bond of phenylpentazoles in the aqueous solution of nitrate, N5− will be easily produced and its metallic complexes can be formed.24 These experimental and theoretical researches show that N5− can be produced by PhN5.
However, the N5 ring decomposes easily.12,24,25 And our investigation22 showed that the C–N bond is much more stable than the N5 ring for PhN5, which is not good for generating N5−. If one wants to find a good source of N5− from the analogues of PhN5, improving the stability of the N5 ring and lowering the strength of the central C–N bond should be the crucial keys. Our study22 revealed that introducing electron donating groups into PhN5 slightly improves the stability of the N5 ring, while strengthens the C–N bond, too. This implies that introduction of electron donating groups is not a good strategy for producing the excellent source of N5−. Peter et al. found that electron withdrawing groups slightly weaken the N5 ring of PhN5.5 This discovery inspires us to think that the electron withdrawing groups may bring hope for finding the good source of N5− when the strength of the C–N bond is significantly lowered while the stability of the N5 ring is little affected by the electron withdrawing substituents. In addition, the pyridine ring has similar planar conjugated structure and the same number of electrons to the benzene ring, while the pyridylpentazole (PyN5) has been rarely researched. According to our exploratory computations on pentazole derivatives, we found that the central C–N bond of PyN5 is less stable than that of PhN5, which implies that PyN5 more easily provides N5− than PhN5 does. In this paper, PyN5 and its derivatives (IA–IVD, cf. Fig. 1) with the electron withdrawing groups –NO2, –CN, –CF3 and –NF2 were studied for searching the potential N5− source. A–D represent the groups –NO2, –CN, –CF3 and –NF2, respectively. Series I and II are pyridine substituted with one group on the ortho-position and meta-position, III and IV are pyridine substituted with two groups on the ortho-position and meta-position. IA–ID are the isomers of the corresponding ones of IIA–IID, and the same is true for series III and IV.
The relaxed potential energy surface scans along the stretching of the central C–N bond and the N–N bonds of the N5 ring were carried out at the RB3LYP/6-31G* level for searching transition states (TSs). The TSs were then optimized at the RM06-2X/6-311++G** level which is reliable for computation of transition state.26–29 The optimized TSs were confirmed by the presence of only one imaginary frequency.
Geometry optimizations of the radicals produced by the central C–N bond breaking were carried out at the UM06-2X/6-311++G** level. All geometry optimizations and the relaxed potential energy surface scans were finished with the Gaussian program package.30
The bond dissociation energy (BDE), the energy difference between the parent molecule and the corresponding radical products in the unimolecular bond dissociation,31–34 was calculated using the following equation:
BDE = ER1˙ + ER2˙ − E | (1) |
The activation energy (Ea) was obtained by eqn (2):
Ea = ETS − ER | (2) |
ETS and ER respectively represent the total energies of TS and reactant obtained at the CSC-MP2/cc-pvtz//RM06-2X/6-311++G** level.
The density of electron at the bond critical point of the central C–N bond (ρBCP) was analyzed using the Multiwfn35 program. The wavefunction files (.wfn) obtained from the Gaussian package were used as inputs for Multiwfn to perform these quantum theory of atoms in molecules (QTAIM)36 analyses.
Compound | LC1–N1 (Å) | LN1–N2 (Å) | LN1–N3 (Å) | Lmax (Å) | LN4–N5 (Å) | D (°) |
---|---|---|---|---|---|---|
PhN5 | 1.430 | 1.317 | 1.317 | 1.317 | 1.337 | 0 |
PyN5 | 1.424 | 1.319 | 1.319 | 1.319 | 1.342 | 0 |
IA | 1.416 | 1.321 | 1.321 | 1.321 | 1.346 | 42 |
IB | 1.419 | 1.321 | 1.325 | 1.325 | 1.347 | 0 |
IC | 1.423 | 1.322 | 1.320 | 1.322 | 1.345 | 44 |
ID | 1.417 | 1.322 | 1.323 | 1.323 | 1.346 | 38 |
IIA | 1.420 | 1.321 | 1.321 | 1.321 | 1.345 | 0 |
IIB | 1.420 | 1.320 | 1.320 | 1.320 | 1.345 | 0 |
IIC | 1.421 | 1.320 | 1.320 | 1.320 | 1.344 | 0 |
IID | 1.420 | 1.320 | 1.320 | 1.320 | 1.345 | 0 |
IIIA | 1.411 | 1.320 | 1.320 | 1.320 | 1.347 | 58 |
IIIB | 1.415 | 1.325 | 1.325 | 1.325 | 1.349 | 50 |
IIIC | 1.424 | 1.321 | 1.321 | 1.321 | 1.345 | 67 |
IIID | 1.413 | 1.324 | 1.324 | 1.324 | 1.349 | 52 |
IVA | 1.415 | 1.323 | 1.323 | 1.323 | 1.349 | 0 |
IVB | 1.417 | 1.322 | 1.322 | 1.322 | 1.347 | 0 |
IVC | 1.418 | 1.321 | 1.321 | 1.321 | 1.346 | 0 |
IVD | 1.416 | 1.321 | 1.322 | 1.322 | 1.348 | 0 |
Data in Table 1 show that LC1–N1 of PyN5 is smaller than that of PhN5, that is, the pyridine ring shortens the C–N bond in comparison with the benzene ring. LC1–N1s of derivatives are generally smaller than that of PyN5, i.e., these electron withdrawing groups reduce the C–N bond of PyN5. Increasing number of substituents shortens the C–N bond, which is reflected by the smaller LC1–N1s of series III–IV in comparison with that of series I–II. The ortho-substituted derivative with the –NO2, –CN or –NF2 group has smaller LC1–N1s than the meta-substituted isomer. LC1–N1s of series I–IV increase in the order of A ≤ D ≤ B < C, –CF3 is the most effective in reducing the C–N bond, –NO2 is the least effective one. Generally, the smaller bond length corresponds to the higher bond stability. Are the C–N bonds of the PyN5 derivatives with smaller bond length more stable than that of PhN5? This question will be answered in the following studies.
Lmax and LN4–N5 have the same order of derivatives > PyN5 > PhN5, this shows that the pyridine ring and electron withdrawing groups elongate the N–N bonds of the N5 ring. For series II and IV, increasing number of the substituted groups elongates the N–N bonds of the N5 ring which can be reflected by the larger Lmax and LN4–N5 of series IV. For N4–N5 bonds of series I and III, introducing more substituents also elongates this bond. However, the opposite situation is found in Lmaxs of series I and III. Lmaxs of IA–ID are comparable to or even larger than the corresponding ones of IIIA–IIID. This diverse case can be explained by the remarkably different dihedral angles between the pyridine ring and the pentazole ring of series I and III. Unlike series II and IV, the pyridine ring and the pentazole ring of series I and III but IB are not coplanar. The obvious tortuosities may be caused by the strong electronic and steric repulsion between the substituted pyridine ring and the N5 ring. The dihedral angles of series III are larger than the corresponding ones of series I because of the stronger repulsion of the formers caused by more substituents, the larger dihedral angles make the effects of substituents on the N5 ring be weaker. Generally speaking, the N–N bonds of the meta-substituted series II and IV are shorter than that of series I and III. For Lmax and LN4–N5 of the derivatives with the same substituted position and number, the maximum differences caused by different groups are only 0.004 Å, that is, the different substituents do not significantly affect the N–N bond lengths.
Fig. 3 shows that H rearrangement happens and one transition state appears during decomposition of the C–N bond of IIB, the final products are HN5 and cyanopyridyne (C5H3N(CN)). For IIIB, breaking of the C–N bond produces two radicals (N5 radical and cyanopyridine radical), and no TS presents in this process. Since there is one H atom adjoining the N5 ring of series I, H rearrangement may occur, i.e., TS may exist too when their C–N bonds dissociate. In addition, decompositions of the C–N bonds of series II and IV may proceed without TS and finally produce two radicals, too. It can be concluded that there are two possible C–N breaking patterns for series I, II and IV: (1) no TS appears and products are two radicals, the required energy for this process is the difference between total energies of two radicals and parent molecule, i.e., BDE; (2) C–N bond breaks through a TS and two ground state molecules are final products (HN5 and pyridyne (C5H3N) derivatives), the needed energy for this process is activation energy (Ea,1). Two decomposition paths of IB are shown in Fig. 4 for more intuitively comparing these decomposition paths. BDEs and Ea,1s of series I, II and IV were calculated and are listed in Table 2 to figure out the most possible pyrolysis mechanism.
Compound | BDE (kJ mol−1) | Ea,1a (kJ mol−1) | Ea,1b (kJ mol−1) | k (s−1) | ρ (kJ mol−1) |
---|---|---|---|---|---|
a Results obtained at the M06-2X/6-311++G** level.b Results obtained at the CSC-MP2/cc-pvtz level. | |||||
PhN5 | 535.8 | 376.3 | 395.5 | 3.53 × 10−53 | 683.2 |
PyN5 | 525.6 | 368.7 | 387.1 | 9.02 × 10−52 | 695.0 |
IA | 493.7 | 356.2 | 368.1 | 2.45 × 10−49 | 721.1 |
IB | 504.6 | 355.7 | 367.3 | 1.42 × 10−49 | 711.0 |
IC | 502.9 | 352.3 | 364.7 | 1.00 × 10−48 | 707.0 |
ID | 506.1 | 356.0 | 367.7 | 2.68 × 10−49 | 715.5 |
IIA | 516.7 | 368.7 | 384.7 | 3.03 × 10−52 | 707.8 |
IIB | 517.8 | 359.1 | 376.3 | 7.31 × 10−50 | 705.3 |
IIC | 523.5 | 361.1 | 379.4 | 1.72 × 10−50 | 703.2 |
IID | 519.2 | 368.5 | 384.3 | 2.56 × 10−51 | 705.9 |
IIIA | 473.6 | 741.6 | |||
IIIB | 494.5 | 727.9 | |||
IIIC | 488.9 | 714.8 | |||
IIID | 496.4 | 731.5 | |||
IVA | 508.6 | 358.1 | 367.5 | 1.20 × 10−48 | 720.0 |
IVB | 510.8 | 357.5 | 371.0 | 2.48 × 10−49 | 714.6 |
IVC | 514.9 | 359.7 | 374.3 | 4.29 × 10−50 | 711.0 |
IVD | 513.5 | 350.7 | 367.3 | 4.12 × 10−49 | 715.7 |
BDEs of series III are quite large, which implies that breaking of the C–N bond of this series is very hard. As is evident from Table 2, Ea,1s of PhN5, PyN5, series I, II and IV are considerably smaller than the corresponding BDEs by 137.5–162.8 kJ mol−1, which reveals that breaking of their central C–N bonds is more likely to follow the path 2 rather than path 1. Therefore, PyN5, series I, II and IV can provide HN5 and N5−. Ea,1 of PyN5 is smaller than that of PhN5, so HN5 is more easily produced from PyN5. Compared with PyN5, derivatives have smaller Ea,1s. Ea,1s have the order of derivatives < PyN5 < PhN5. According to these results, the strategies of introducing pyridine and the electron withdrawing groups are effective in weakening the C–N bond and improving the easiness of producing HN5. Ea,1s of derivatives with the same substituent generally have the order of I < IV < II. Obtaining N5− from series I is the easiest, followed by series IV. N5− is more easily produced by the ortho-substituted derivatives than the para-substituted derivatives.
To comprehensively assess the potentials of these molecules as the source of N5−, the reaction rate constants (ks) of path 2 were calculated at 300–1500 K with the KiSThelP program37 according to the transition state theory (TST). In this paper, only ks at 300 K are shown in Table 2, results at other temperatures are supplied in Table S1.† As we expected, ks sharply increase with the improving temperature, this reveals that high temperature is good for producing HN5. ks have the order of I > IV (IV > I) > II > PyN5 > PhN5, decomposition reactions of pyridylpentazoles are about 9–33994 times (kPyN5s/kPhN5) faster than that of PhN5. Based on the lower Ea,1 (ΔEa,1 = Ea,1(PhN5) − Ea,1(PyN5s) = 8.4–30.8 kJ mol−1, ΔEa,1/Ea,1(PhN5) = 2.1–7.8%) and larger ks of PyN5 and its derivatives, especially series I and IV, N5− can be more easily derived from pyridylpentazoles in comparison with PhN5.
The above mentioned LC1–N1s have the order of PhN5 > PyN5 > II > IV > I which is in agreement with the C–N bond stability. This result is not consistent with the common viewpoint that the longer bond links with the lower bond stability. In addition, electron density at the C–N bond critical point (ρ, Table 2) related to bond strength was evaluated, too. The variation trend of ρs is contrary to that of LC1–N1, i.e., the larger ρ generally corresponds to the shorter C–N bond. The relationship between ρ and LC1–N1 is in line with chemical intuition. However, the smaller ρ corresponds to the larger Ea,1 and higher bond stability, which is contrary to the common situation. How do these “abnormal phenomena” happen? Since the bond length and electron density at the bond critical point are all the properties of the static molecule, if the decomposition of bond directly proceeds by breaking the bond (path 1), they can be the indexes reflecting the bond stability. But when the deformation presents in the bond breaking process (path 2), they are no longer directly related with the bond stability, as was observed in series I, II, and IV.
The decomposition path of the N5 ring of PyN5 (path 3) is presented in Fig. 6 for clearly describing the pyrolysis process. When SC1 and SC2 respectively elongate to about 1.695–1.712 Å and 1.712–1.743 Å, TS2s of title molecules emerge. The final products are N2 and azido pyridine or its derivatives. The activation energy (Ea,2) needed for path 3 and reaction rate constant, the essential factors determining the decomposition reaction, are tabulated in Table 3.
Compound | Ea,2 (kJ mol−1) | k (s−1) |
---|---|---|
a Ea,2 and k of PyN5 (PhN5) are 84.1 (88.7) kJ mol−1 and 4.90 × 10−4 (2.23 × 10−5) s−1, respectively. | ||
IA | 77.1 | 3.47 × 10−2 |
IB | 72.1 | 1.10 × 10−1 |
IC | 77.4 | 2.51 × 10−2 |
ID | 76.0 | 5.16 × 10−2 |
IIIA | 74.4 | 3.04 × 10−1 |
IIIB | 67.6 | 1.47 |
IIIC | 73.4 | 1.69 × 10−1 |
IIID | 70.6 | 6.99 × 10−1 |
IIA | 78.9 | 8.92 × 10−4 |
IIB | 79.7 | 2.57 × 10−3 |
IIC | 81.1 | 9.62 × 10−4 |
IID | 80.3 | 2.73 × 10−3 |
IVA | 73.8 | 7.59 × 10−2 |
IVB | 75.4 | 2.36 × 10−2 |
IVC | 78.1 | 9.16 × 10−3 |
IVD | 76.5 | 4.01 × 10−3 |
We can see that Ea,2s are far smaller than the corresponding Ea,1s and BDEs, so decomposition of the N5 ring should be the first step on dissociation of title molecules. Ea,2 of PyN5 is 4.6 kJ mol−1 smaller than that of PhN5. Electron withdrawing groups obviously lower the stability of the N5 ring due to the smaller Ea,2s of derivatives. The differences (ΔEa,2s) between Ea,2s of PhN5 and pyridylpentazoles are 11.3–21.0 kJ mol−1 (ΔEa,2/Ea,2(PhN5) = 12.7–23.7%). The pyridine ring and these electron withdrawing groups both weaken the N5 ring.
For the derivatives with the same functional groups, Ea,2 generally decreases in the order of II > IV > I > III. Ortho-substituted groups more obviously affect the stability of the N5 ring than the meta-substituted groups, and the stability of the N5 ring decreases with the increasing number of substituents. Compared with other groups, –NF2 causes the tiniest decrements in Ea,2s. The maximum differences of Ea,2s caused by different groups are 5.2, 2.1, 6.7 and 4.4 kJ mol−1 for series I–IV respectively. These results agree with the conclusions obtained from the N–N bond lengths, i.e., the larger N–N bond distance corresponds to the lower N5 ring stability, because N5 ring directly decomposes by breaking of N–N bonds.
The reaction rate constants of path 3 were assessed at 300–1500 K. Only results at 300 K are shown in this paper, the other data are listed in Table S2.† k values of all molecules but IIIB are smaller than 1, this implies that decomposition of the N5 ring of title molecules is not very fast under the normal condition. k increases drastically with the improving temperature, i.e., elevating temperature speeds up breaking of the N5 ring, so high temperature is not good for molecules with the N5 ring. While high temperature is beneficial to dissociation of the C–N bond, so the appropriate temperature is important for molecules analogous to title molecules as the source of N5−. Reaction rate constant decreases in the order of III > I > IV (IV > I) > II > PyN5 > PhN5, decompositions of the N5 ring of pyridylpentazoles are 44–11437 times (kPyN5s/kPhN5) faster than that of PhN5. Dissociation of the N5 ring of series III are the fastest, decomposition speeds of series I and IV are comparable. The smaller Ea,2s and the larger ks of these derivatives with the electron withdrawing groups show that the stability of the N5 rings of PyN5 is obviously lowered by the electron withdrawing groups, which is beyond our expectation that the stability of the N5 ring is slightly affected.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra00813a |
This journal is © The Royal Society of Chemistry 2015 |