Theoretical Investigation on the Stability and Reactivity of Imidazo [1,2-a] Pyridine N-Acylhydrazone Derivatives Using Density Functional Theory ()
1. Introduction
In recent years, research interest in N-acylhydrazones containing the heterocyclic imidazo [1,2-a] pyridine scafflold has seen remarkable growth [1]-[3]. N-acylhydrazones represent a conjugated system with 6π electrons, provided that the azomethine group adopts the most stable E configuration. This conjugated system can undergo two additional isomerizations, resulting from slow rotation around the N-N and N-CO bonds (Figure 1), potentially yielding four distinct conformers. This conformational diversity underscores the importance of understanding the structure and reactivity of these compounds. N-acylhydrazone molecules hold significant interest due to their diverse potential applications, including as ligands in asymmetric catalysis, antibacterial agents [4]-[6], antifungals [7], antitumor agents [8]-[10], among others [11]-[13]. In previous study, our team synthesized a series of molecules belonging to this family [14]. The current study aims to theoretically examine the reactivity, stability, and identify nucleophilic/electrophilic attack sites using various quantum chemistry methods to optimize their properties. All simulations were conducted in the gas phase, employing the B3LYP/6-31+G (d, p) level of theory. Reactivity and stability were assessed through the calculation of descriptors such as energy gap (
), chemical hardness (η), and softness (S). Nucleophilic/electrophilic attack sites were determined via analysis of the molecular electrostatic potential (MEP) map as well as the dual descriptor. This systematic approach will illuminate our understanding of molecular interactions and pave the way for the design and modelling of more effective and targeted compounds for a diverse range of applications.
![]()
Figure 1. Four possible rotamers of the N-acylhydrazone moiety
2. Materials and methods
2.1. Materials
The molecules studied were listed in Table 1.
Table 1. Variations in aromatic (Ar) substituents among studied N-Acylhydrazone derivatives: set of the molecular structures.
Compounds |
Ar |
9a |
Phenyl |
9b |
2-hydroxyphenyl |
9c |
4-fluorophenyl |
9d |
4-toluyl |
9e |
4-nitrophenyl |
9f |
4-methoxyphenyl |
9g |
4-hydroxy-3-methyloxyphenyl |
9h |
4-hydroxyphenyl |
9i |
4-cyanophenyl |
9j |
4-N,N-dimethylaminophenyl |
9k |
4-chlorophenyl |
9m |
3,5-dichlorophenyl |
9n |
4-methylbenzyloxyphenyl |
9o |
4-methoxybenzyloxyphenyl |
9p |
benzylthiophenyl |
9q |
thiophen-2-yl |
9r |
furan-2-yl |
2.2. Computational Details
The computational analysis was conducted utilizing Gaussian 09 software [15], leveraging the density functional theory (DFT) method [16]. The results have been visualized using the GaussView 6 program [17]. DFT was chosen due to its established capability in accurately predicting molecular properties. Specifically, hybrid functional methods like B3LYP, known for their robustness and wide applicability, were employed [18]. The selected level of theory for this investigation was B3LYP/6-31+G(d,p). Each N-acylhydrazone molecule underwent rigorous molecular geometry optimization, followed by frequency calculations to verify the stability of the optimized structure. Furthermore, a comprehensive suite of stability and reactivity parameters were computed for in-depth analysis of the molecular properties, providing nuanced insights into the structure and behavior of these compounds.
Reactivity descriptors
1) Electrostatic Potential Surface (EPS) Area
Electrostatic Potential Surfaces (EPS) and its cartography serve as indispensable tools for analyzing and predicting the reactive behavior of molecules. By scrutinizing the EPS surface, one can identify potentially reactive regions through an intuitive colorimetric representation. The color gradient typically progresses as follows: red < orange < yellow < green < cyan < blue [19] [20]. In the electrostatic potential surface, areas with zero potential are depicted in green, negative regions (red and yellow) denote electrophilic attack sites, while positive areas (cyan and blue) signify nucleophilic attack sites. This visual representation facilitates rapid and accurate identification of reactive sites, thereby enhancing our comprehension and predictive capabilities regarding molecular reactions.
This method hinges on Equation (1), defining the EPS as the interaction energy of a proton with the nucleus and electrons of a molecule.
(1)
In this equation, ZA represents the charge of the nucleus A,
,
signify the proton-nucleus and proton-electron distances respectively, while p(r') represents the electron density.
2) Global molecular descriptors
Global descriptors plays are indispensable tools in characterizing molecular properties, offering a comprehensive view of a system’s stability and reactivity. Unlike local descriptors, which vary across chemical space, global descriptors maintain a uniform value throughout the system under examination. Their uniformity enables an assessment of the system’s response to global perturbations, providing insights into macroscopic properties [21]. Among these descriptors, hardness (η) and softness (S) hold particularly significance. Hardness the first derivative of the chemical potential with respect to the electron number N, and its inverse, softness, provide crucial information about the system’s response to external perturbations [22]-[24].
Incorporating these descriptors into our analysis allows for a deeper understanding and prediction of the physicochemical properties of the studied N-acylhydrazones, thereby offering avenues for the design and optimization of more efficient compounds.
Drawing on Pearson’s theory of acids and bases, [25] hardness (η) and softness (S) can be expressed in terms of ionization potentials (PI) and electron affinity (AE) as follows:
Ionization potential (PI) and electron affinity (AE) can be readily determined using the Koopmans approximation [26].
and
Here,
and
represent respectively the energies of the highest occupied orbital (HOMO) and the lowest unoccupied orbital (LUMO), respectively, in accordance with the theory of frontier molecular orbitals [27]. Furthermore, the energy gap (
) serves as a crucial stability index, measuring a molecule’s excitability. A reduced energy gap signifies heightened interaction with the environment, implying greater reactivity. Conversely, a larger gap between HOMO and LUMO energies indicates higher stability, thereby reducing the molecule’s reactivity in chemical reactions.
3) Local and dual descriptors
In 2004, Morell et al. [28] introduced a groundbreaking reactivity descriptor, known as the “dual descriptor”, offering a novel approach on characterizing reactive sites within a molecule. This descriptor, defined as the difference between the Fukui functions (
and
) for nucleophilic and electrophilic attacks, respectively, provides valuable insights into the reactivity of molecular sites. The value of the dual descriptor is calculated as follows:
for nucleophilic attack;
for electrophilic attack;
Electronic population of atom k in the neutral molecule;
Electronic population of atom k in the anionic molecule;
Electronic population of atom k in the cationic molecule.
When
, the region is identified as electrophilic, indicating a propensity for nucleophilic attack. Conversely, when
, the region is deemed nucleophilic, suggesting a predilection for electrophilic attack.
This method offers a robust approach to pinpointing and characterizing reactive sites in a molecule, thereby enhancing our ability to comprehend and predict chemical interactions. By integrating the dual descriptor into our analysis, we can delve deeper into molecular reactivity mechanisms, thereby unlocking novel avenues for the design and optimization of compounds with desired chemical properties. The introduction of the “dual descriptor” index presents a significant advancement, allowing for the simultaneous detection of both electrophilic and nucleophilic regions within a molecule. By examining a given region’s dual descriptor, we can discern its preference for either nucleophilic or electrophilic attack.
4) The Hirshfeld populations
Incorporating Hirshfeld population analysis into our research promises a comprehensive characterization of molecular reactivity properties, thereby advancing our understanding of chemical mechanisms and facilitating the rational design of novel compounds with optimized chemical attributes. Hirshfeld charges provide a qualitative perspective align with fundamental chemical principles, affording a means to quantify the electrophilicity and nucleophilicity of molecular surfaces [29] [30]. This method relies on an intuitive approach wherein the charge density at each point of the molecule is distributed among its constituent atoms, proportionally to their respective free atomic densities at the corresponding distances from the nucleus [31]. In this study, atomic charge values were determined via Hirshfeld population analysis, renowned for its robustness and capacity to furnish intricate insights into charge distribution within molecules. Through the quantification of atomic charges, we gain the ability to pinpoint electrophilic and nucleophilic regions within the molecule, offering invaluable insights into potential reactive sites. This analytical framework could promise for advancing our understanding of molecular reactivity and guiding the strategic design of compounds with tailored chemical properties.
3. Results and Discussion
As shown in Figure 2, we adopted this general numbering of imidazo [1,2-a] pyridine N-acylhydrazones derivatives to facilitate interpretation of the results.
Figure 2. Numbered basic structure of imidazo [1,2-a] pyridine N-acylhydrazones.
3.1. Global Reactivity
For each compound, the energies of the Highest Occupied Molecular Orbital (HOMO) and Lowest Unoccupied Molecular Orbital (LUMO) orbitals provide vital insights into its stability and reactivity. A high HOMO energy signifies an enhanced ability to accept electrons, whereas a low LUMO energy indicates a predisposition to donate electrons. The evaluation of hardness (η) and softness (S) allows for the assessment of global reactivity, with higher hardness associated with lower reactivity and vice versa. These reactivity parameters offer a comprehensive overview of the physicochemical properties of the compounds under investigation, furnishing valuable insights into their behavior in reaction contexts and their potential applications across various domains of chemistry and pharmacology. The reactivity parameters examined in this series of compounds encompass HOMO energies (
), LUMO energies (
), hardness (η), softness (S), and the energy gap between the boundary orbitals (
). The calculated values of these parameters are presented in Table 2.
The energy gap between the frontier orbitals (
) serves as a pivotal indicator of molecular stability and reactivity: a larger
signifies lower reactivity and heightened stability, whereas a diminished
suggests increased reactivity. Analysis of the data presented in Table 2 reveals a range of
values spanning from 2.49 eV to 3.91 eV among the studied compounds. Notably, a smaller energy gap indicates a greater likelihood of electron transfer from the Highest Occupied Molecular Orbital (HOMO) to the Lowest Unoccupied Molecular Orbital (LUMO), indicative of heightened reactivity. Among the examined molecules, 9e exhibits the largest energy gap (3.91 eV), signifying its superior stability and reduced reactivity. Conversely, 9j displays the smallest energy gap (2.49 eV), rendering it the least stable yet most reactive compound in the series. By ranking the compounds based on stability, we obtain the following order:
Table 2. Energies of HOMO and LUMO frontier orbitals, hardness, softness (eV) −1, and energy gap. The other parameters are expressed in eV.
Compounds |
|
|
|
η |
S |
9a |
−6.36 |
−2.89 |
3.47 |
1.74 |
0.58 |
9b |
−6.10 |
−2.84 |
3.26 |
1.63 |
0.61 |
9c |
−6.41 |
−2.93 |
3.48 |
1.74 |
0.57 |
9d |
−6.19 |
−2.87 |
3.32 |
1.66 |
0.60 |
9e |
−7.00 |
−3.09 |
3.91 |
1.96 |
0.51 |
9f |
−6.20 |
−2.86 |
3.34 |
1.67 |
0.60 |
9g |
−5.87 |
−2.85 |
3.02 |
1.51 |
0.66 |
9h |
−6.00 |
−2.87 |
3.13 |
1.56 |
0.64 |
9i |
−6.81 |
−3.03 |
3.78 |
1.89 |
0.53 |
9j |
−5.28 |
−2.78 |
2.49 |
1.25 |
0.80 |
9k |
−6.43 |
−2.94 |
3.49 |
1.74 |
0.57 |
9m |
−6.58 |
−2.98 |
3.60 |
1.80 |
0.56 |
9n |
−5.92 |
−2.76 |
3.16 |
1.58 |
0.63 |
9o |
−6.00 |
−2.88 |
3.12 |
1.56 |
0.64 |
9p |
−5.83 |
−2.88 |
2.95 |
1.47 |
0.68 |
9q |
−6.10 |
−2.89 |
3.21 |
1.61 |
0.62 |
9r |
−6.01 |
−2.89 |
3.12 |
1.56 |
0.64 |
9j < 9p < 9g < 9o; 9r < 9h < 9n < 9q < 9b < 9d < 9f < 9a < 9c < 9k < 9m < 9i < 9e.
This correlation underscores the significance of the energy gap in predicting the chemical properties and stability of the studied compounds, thereby offering valuable insights for the design of molecules with tailored characteristics, particularly in drug design and catalysis.
Examining the hardness values (η) provided in Table 2, we observe variations ranging from 1.25 eV to 1.96 eV among the molecules studied. Notably, lower hardness values correspond to higher reactivity. For instance, molecule 9j exhibits the lowest hardness value (1.25 eV), rendering it the most reactive compound in the series. Ranking the molecules based on hardness yields the following order:
9j > 9p > 9g > 9o; 9r > 9h > 9n > 9q > 9b > 9d > 9f > 9a > 9c > 9k > 9m > 9i > 9e.
This order aligns with the ranking derived from the energy gap (
), corroborating the coherence of our findings.
Softness values (S), as reported in Table 2, range from 0.51 eV−1 to 0.80 eV−1. Higher softness values indicate less stability and greater reactivity. Once again, classifying the molecules according to softness reaffirms their reactivity order:
9j > 9p > 9g > 9o; 9r > 9h > 9n > 9q > 9b > 9d > 9f > 9a > 9c > 9k > 9m > 9i > 9e.
These results underscore the coherence of the three descriptors (
, hardness, and softness) in providing insights into the stability and reactivity of the studied molecules.
3.2. Local Reactivity
3.2.1. Electrostatic Surface Potential Map
To gain insight into the electrophilic and nucleophilic sites within the compounds, an analysis of the electrostatic potential map was conducted, as depicted in Figure 3. In this analysis, negative regions (colored red or yellow) denote nucleophilic sites, whereas positive regions (colored cyan or blue) are indicative of electrophilic sites. This examination allows for a comprehensive understanding of the distribution of electrophilic and nucleophilic character within the compounds.
(9a)
(9b)
(9c)
(9d)
(9e)
(9f)
(9g)
(9h)
(9i)
(9j)
(9k)
(9m)
(9n)
(9o)
(9p)
(9q)
(9r)
Figure 3. Map of the electrostatic potential of N-acylhydrazones.
Analysis of the electrostatic potential maps reveals distinct nucleophilic and electrophilic sites within the N-acylhydrazones under study. Specifically, the N9 and N14 nitrogen atoms, along with the O10 oxygen atom, exhibit nucleophilic character, making them favorable targets for electrophilic attack. In contrast, the N8 and N11 nitrogen atoms emerge as electrophilic sites, poised for nucleophilic interaction. Additionally, the S1 sulfur atom displays a discernible electrophilic tendency, due certainly to the lone pair electrons in its orbital. This meticulous examination of the electrostatic potential maps yields a comprehensive understanding of the reactive sites within each N-acylhydrazone. Such insights are instrumental for predicting and elucidating chemical reactions involving these compounds, thereby advancing our comprehension of their reactivity profiles.
3.2.2. Dual Descriptors
The values of the various dual descriptors are given in the following tables:
The comprehensive analysis of the dual descriptor values, outlined in Table 3 and Table s1-s16 (Tables s1-s16 in Supplemental material), unveils pivotal insights into the reactivity profiles of various reactive sites within the N-acylhydrazone molecules. In the case of the reference molecule 9a, barring the nitro group, all heteroatoms exhibit nucleophilic character, rendering them susceptible to electrophilic attack. For molecules 9b, 9c, 9d, 9f, 9h, 9i, 9k, 9q, and 9r, modification on the aryl ring at positions 2 or 4 imparts an electrophilic nature to nitrogens N8 and N11, thus facilitating nucleophilic attack. Conversely, nitrogens N9 and N14, oxygen O10, and sulfur S1 manifest nucleophilic behavior, promoting electrophilic attack.
Table 3. Local reactivity descriptors for 9a using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
|
|
|
|
|
|
1 |
7.973 |
7.922 |
7.948 |
−0.051 |
0.026 |
−0.077 |
2 |
3.029 |
3.022 |
3.026 |
−0.007 |
0.004 |
−0.011 |
3 |
2.980 |
2.978 |
2.979 |
−0.002 |
0.001 |
−0.003 |
4 |
2.907 |
2.893 |
2.900 |
−0.014 |
0.007 |
−0.021 |
7 |
2.973 |
2.959 |
2.966 |
−0.014 |
0.007 |
−0.021 |
8 |
3.608 |
3.605 |
3.607 |
−0.004 |
0.002 |
−0.005 |
9 |
3.529 |
3.503 |
3.516 |
−0.026 |
0.013 |
−0.039 |
10 |
4.154 |
4.106 |
4.130 |
−0.047 |
0.024 |
−0.071 |
11 |
3.502 |
3.497 |
3.499 |
−0.005 |
0.003 |
−0.008 |
13 |
2.941 |
2.935 |
2.938 |
−0.006 |
0.003 |
−0.009 |
14 |
3.557 |
3.534 |
3.545 |
−0.024 |
0.012 |
−0.035 |
20 |
2.985 |
2.957 |
2.971 |
−0.028 |
0.014 |
−0,042 |
In molecule 9e, the introduction of a nitro group on the aryl ring at position 4 confers nucleophilic character to nitrogen N11, fostering electrophilic attack. Meanwhile, nitrogen N14 exhibits a preference for nucleophilic attack, with negligible changes observed in the remaining heteroatoms. For molecules 9g, 9j, 9n, 9o, and 9p, modification of the aryl ring at positions 3 and 4 or solely at position 4 induces an electrophilic character in nitrogens N8 and N11, as well as oxygen O10, promoting nucleophilic attack. Nitrogens N9 and N14, conversely, become more prone to electrophilic attack. Furthermore, the sulfur atom demonstrates electrophilic tendencies, further facilitating nucleophilic attack. In the case of molecule 9m, chlorination of the aryl ring at positions 3 and 5 imparts nucleophilic character to all heteroatoms, except nitrogen N11, thereby promoting electrophilic attack. These detailed observations underscore the intricacies of molecular reactivity and emphasize the significance of analyzing the dual descriptor to characterize reactive sites within the studied compounds.
4. Conclusion
This theoretical investigation delves into seventeen N-acylhydrazones, shedding light on their reactivity and stability. Among these, molecule 9e emerges as a standout, exhibiting distinct stability characteristics indicative of heightened resistance to electron transfer, as discerned through comprehensive analysis of global reactivity descriptors. By scrutinizing the electrostatic potential (ESP) maps and employing the dual descriptor, we pinpoint potential attack sites within the molecules. Notably, nitrogen atoms N9 and N14, along with oxygen O10, emerge as nucleophilic sites, while N8 and N11 nitrogen atoms generally exhibit electrophilic tendencies. Additionally, the sulfur atom displays a predisposition towards electrophilic attack. This study furnishes fundamental insights into the molecular reactivity of imidazo [1,2-a] pyridine N-acylhydrazones, with broad implications across diverse realms of chemistry, including drug design and catalysis. The acquired knowledge could serve as a springboard for future investigations aimed at the strategic design of compounds with tailored properties, geared towards pharmacomodulation.
Supplemental Material
Supplementary information for this article is provided in the online supplement.
Supplemental Material
Procedure for the synthesis of N-acylhydrazones (9a-r)
1.23 mmol of 2-(1.8a-dihydro-3-nitroimidazo [1.2-a] pyridin-2-ylthio) acetohydrazide and 1.23 mmol (1 eq) of benzaldehyde derivative were dissolved in methanol. The reaction mixture was refluxed for 1 h. After cooling to room temperature, the precipitate formed was filtered, dried and then purified by recrystallization in a water/ethanol mixture (1/1) to give 2-(1.8a-dihydro-3-nitroimidazo [1.2-a] pyridin-2-ylthio)-N’-benzylideneacetohydrazide with yields between 56% and 86%.
(E)-2-(3-nitro-H-imidazo[1.2-a]pyridin-2-ylthio)-N’-benzylideneacetohydrazide (9a)
Orange powder. M.p = 232 - 234˚C; Yield = 79 %, 1H NMR (300 MHz, DMSO -d6) δ (ppm) 11.77ap, 11.67sp (s, 1H; NH), 9.34(sp+ap) (dt.J = 6.9, 1.1 Hz, 1H; HAr), 8.22ap, 8.05sp (s, 1H; N=CH), 7.90 – 7.77(sp+ap) (m, 2H; HAr), 7.71(sp+ap) (td, J = 3.8; 2.2 Hz, 2H; HAr), 7.51 – 7.34(sp+ap) (m, 4H; HAr), 4.63sp, 4.22ap (s, 2H, S-CH2). 13C NMR (75 MHz, DMSO-d6) δ (ppm) 169.39sp, 164.18ap (C=O), 153.54sp, 153.15ap (N=CH), 147.44, 146.23, 144.16, 134.53, 134.48, 133.52sp, 133.46ap (CAr), 130.60sp, 130.44ap (CAr), 129.29, 128.65sp, 128.40ap (CAr), 127.58, 127.34, 11697sp, 116.87ap (CAr), 116.79, 33.95ap, 33.08sp (S-CH2), HRMS (ESI):Calc for [M+Na+] C16H13N5NaO3S = 378.0521. Found = 378.0525.
1H and 13C NMR spectra of 2-(3-nitro-H-imidazo [1.2-a] pyridin-2-ylthio)-N’-benzylideneacetohydrazide (9a)
Figure S1. 1H NMR spectra.
Figure S2. 13C NMR spectra.
Table S1. Local reactivity descriptors for 9b using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.974 |
7.931 |
8.002 |
−0.043 |
−0.028 |
−0.015 |
2 |
3.029 |
3.023 |
3.036 |
−0.006 |
−0.007 |
0.001 |
3 |
2.980 |
2.978 |
2.998 |
−0.001 |
−0.019 |
0.018 |
4 |
2.908 |
2.895 |
2.910 |
−0.013 |
−0.002 |
−0.011 |
7 |
2.973 |
2.961 |
2.979 |
−0.012 |
−0.006 |
−0.006 |
8 |
3.608 |
3.605 |
3.623 |
−0.002 |
−0.016 |
0.013 |
9 |
3.530 |
3.507 |
3.529 |
−0.023 |
0.001 |
−0.024 |
10 |
4.154 |
4.112 |
4.168 |
−0.043 |
−0.014 |
−0.029 |
11 |
3.502 |
3.498 |
3.512 |
−0.004 |
−0.010 |
0.006 |
13 |
2.941 |
2.936 |
2.961 |
−0.005 |
−0.020 |
0.015 |
14 |
3.557 |
3.533 |
3.564 |
−0.024 |
−0.007 |
−0.017 |
20 |
2.984 |
2962 |
2.994 |
−0.022 |
−0.010 |
−0.013 |
Table S2. Local reactivity descriptors for 9C using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.974 |
7.923 |
8.001 |
−0.050 |
−0.027 |
−0.023 |
2 |
3.029 |
3.022 |
3.036 |
−0.007 |
−0.007 |
0.000 |
3 |
2.980 |
2.978 |
2.999 |
−0.002 |
−0.019 |
0,017 |
4 |
2.907 |
2.893 |
2.909 |
−0.014 |
−0.003 |
−0.011 |
7 |
2.973 |
2.959 |
2.979 |
−0.015 |
−0.006 |
−0.009 |
8 |
3.609 |
3.605 |
3.624 |
−0.003 |
−0.016 |
0.012 |
9 |
3.529 |
3.504 |
3.529 |
−0.025 |
0.001 |
−0.026 |
10 |
4.153 |
4.107 |
4.168 |
−0.046 |
−0.015 |
−0.031 |
11 |
3.502 |
3.497 |
3.512 |
−0.005 |
−0.010 |
0.005 |
13 |
2.941 |
2.935 |
2.961 |
−0.006 |
−0.020 |
0.014 |
14 |
3.557 |
3.534 |
3.566 |
−0.023 |
−0,009 |
−0.015 |
20 |
2.985 |
2.959 |
2.996 |
−0.026 |
−0.011 |
−0.016 |
Table S3. Local reactivity descriptors for 9d using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.973 |
7.930 |
8.002 |
−0.043 |
−0.029 |
−0.013 |
2 |
3.029 |
3.023 |
3.036 |
−0.006 |
−0.007 |
0.001 |
3 |
2.980 |
2.979 |
3.000 |
−0.001 |
−0.020 |
0.020 |
4 |
2.907 |
2.893 |
2.909 |
−0.014 |
−0.002 |
−0.012 |
7 |
2.973 |
2.964 |
2.979 |
−0.010 |
−0.006 |
−0.004 |
8 |
3.608 |
3.605 |
3.625 |
−0.003 |
−0.017 |
0.014 |
9 |
3.530 |
3.503 |
3.528 |
−0.027 |
0.001 |
−0.028 |
10 |
4.154 |
4.109 |
4.168 |
−0.046 |
−0.014 |
−0.032 |
11 |
3.502 |
3.498 |
3.513 |
−0.004 |
−0.011 |
0.007 |
13 |
2.941 |
2.936 |
2.962 |
−0.005 |
−0.021 |
0.017 |
14 |
3.558 |
3.532 |
3.564 |
−0.026 |
−0.006 |
−0.021 |
20 |
2.985 |
2.958 |
2.993 |
−0.027 |
−0.008 |
−0.018 |
Table S4. Local reactivity descriptors for 9e using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.974 |
7.911 |
7.987 |
−0.062 |
−0.014 |
−0.048 |
2 |
3.029 |
3.020 |
3.034 |
−0.009 |
−0.005 |
−0.004 |
3 |
2.981 |
2.976 |
2.989 |
−0.005 |
−0.008 |
0.003 |
4 |
2.905 |
2.893 |
2.910 |
−0.012 |
−0.005 |
−0.007 |
7 |
2.973 |
2.950 |
2.976 |
−0.024 |
−0.002 |
−0.022 |
8 |
3.609 |
3.603 |
3.616 |
−0.006 |
−0.007 |
0.002 |
9 |
3.528 |
3.508 |
3.530 |
−0.021 |
−0.002 |
−0.019 |
10 |
4.148 |
4.104 |
4.165 |
−0.045 |
−0.017 |
−0.028 |
11 |
3.502 |
3.496 |
3.507 |
−0.006 |
−0.005 |
−0.001 |
13 |
2.941 |
2.932 |
2.951 |
−0.009 |
−0.010 |
0.002 |
14 |
3.552 |
3.535 |
3.571 |
−0.016 |
−0.019 |
0.003 |
20 |
2.985 |
2.960 |
2.995 |
−0.026 |
−0.009 |
−0.016 |
Table S5. Local reactivity descriptors for 9f using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.970 |
7.914 |
8.000 |
−0.057 |
−0.030 |
−0.027 |
2 |
3.029 |
3.022 |
3.036 |
−0.007 |
−0.008 |
0.001 |
3 |
2.980 |
2.980 |
2.998 |
0.000 |
−0.018 |
0.018 |
4 |
2.909 |
2.895 |
2.913 |
−0.014 |
−0.004 |
−0.010 |
7 |
2.973 |
2.961 |
2.978 |
−0.012 |
−0.006 |
−0.006 |
8 |
3.607 |
3.607 |
3.621 |
0.000 |
−0.014 |
0.014 |
9 |
3.530 |
3.498 |
3.529 |
−0.033 |
0.001 |
−0.033 |
10 |
4.153 |
4.108 |
4.169 |
−0.045 |
−0.017 |
−0.028 |
11 |
3.500 |
3.496 |
3.510 |
−0.004 |
−0.011 |
0.007 |
13 |
2.941 |
2.938 |
2.960 |
−0.003 |
−0.019 |
0.016 |
14 |
3.558 |
3.532 |
3.568 |
−0.026 |
−0.009 |
−0.017 |
20 |
2.985 |
2.954 |
2.995 |
−0.031 |
−0.010 |
−0.021 |
Table S6. Local reactivity descriptors for 9g using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.974 |
7.952 |
8.002 |
−0.022 |
−0.028 |
0.007 |
2 |
3.029 |
3.025 |
3.036 |
−0.004 |
−0.007 |
0.003 |
3 |
2.980 |
2.980 |
2.999 |
0.001 |
−0.020 |
0.020 |
4 |
2.908 |
2.896 |
2.909 |
−0.012 |
−0.001 |
−0.010 |
7 |
2.973 |
2.962 |
2.979 |
−0.011 |
−0.006 |
−0.005 |
8 |
3.607 |
3.606 |
3.624 |
−0.001 |
−0.017 |
0.015 |
9 |
3.530 |
3.506 |
3.529 |
−0.025 |
0.001 |
−0.026 |
10 |
4.154 |
4.119 |
4.167 |
−0.035 |
−0.013 |
−0.022 |
11 |
3.502 |
3.500 |
3.513 |
−0.002 |
−0.011 |
0.009 |
13 |
2.941 |
2.938 |
2.962 |
−0.003 |
−0.021 |
0.018 |
14 |
3.560 |
3.530 |
3.565 |
−0.030 |
−0.005 |
−0.026 |
20 |
2.986 |
2.963 |
2.995 |
−0.023 |
−0.009 |
−0.014 |
Table S7. Local reactivity descriptors for 9h using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.974 |
8.002 |
7942 |
0.028 |
0.032 |
−0.004 |
2 |
3.029 |
3.036 |
3.024 |
0.007 |
0.005 |
0.002 |
3 |
2.980 |
2.999 |
2.979 |
0.019 |
0.000 |
0.019 |
4 |
2.908 |
2.909 |
2.895 |
0.002 |
0.013 |
−0.011 |
7 |
2.973 |
2.979 |
2.964 |
0.006 |
0.010 |
−0.004 |
8 |
3.608 |
3.624 |
3.607 |
0.016 |
0.001 |
0.015 |
9 |
3.530 |
3.529 |
3.505 |
−0.001 |
0.025 |
−0.026 |
10 |
4.154 |
4.167 |
4.113 |
0.014 |
0.041 |
−0.028 |
11 |
3.502 |
3.513 |
3.498 |
0.011 |
0.004 |
0.007 |
13 |
2.941 |
2.962 |
2.937 |
0.021 |
0.004 |
0.017 |
14 |
3.560 |
3.565 |
3.531 |
0.006 |
0.029 |
−0.023 |
20 |
2.986 |
2.995 |
2.963 |
0.009 |
0.023 |
−0.014 |
Table S8. Local reactivity descriptors for 9i using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.973 |
7.916 |
7.993 |
−0.057 |
−0.020 |
−0.037 |
2 |
3.029 |
3.021 |
3.035 |
−0.008 |
−0.006 |
−0.002 |
3 |
2.981 |
2.977 |
2.993 |
−0.003 |
−0.012 |
0.009 |
4 |
2.905 |
2.892 |
2.911 |
−0.013 |
−0.006 |
−0.007 |
7 |
2.973 |
2.955 |
2.977 |
−0.018 |
−0.004 |
−0.014 |
8 |
3.609 |
3.604 |
3.620 |
−0.005 |
−0.011 |
0.006 |
9 |
3.528 |
3.505 |
3.529 |
−0.023 |
−0.001 |
−0.021 |
10 |
4.150 |
4.105 |
4.168 |
−0.044 |
−0.018 |
−0.027 |
11 |
3.502 |
3.496 |
3.509 |
−0.006 |
−0.007 |
0.002 |
13 |
2.941 |
2.934 |
2.956 |
−0.007 |
−0.014 |
0.007 |
14 |
3.553 |
3.534 |
3.571 |
−0.019 |
−0.018 |
−0.001 |
20 |
2.985 |
2.959 |
2.999 |
−0.026 |
−0.014 |
−0.012 |
Table S9. Local reactivity descriptors for 9j using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.972 |
7.966 |
8.003 |
−0.006 |
−0.031 |
0.025 |
2 |
3.029 |
3.026 |
3.037 |
−0.003 |
−0.007 |
0.004 |
3 |
2.979 |
2.981 |
3.000 |
0.002 |
−0.021 |
0.023 |
4 |
2.909 |
2.898 |
2.910 |
−0,011 |
−0.001 |
−0.009 |
7 |
2.973 |
2.974 |
2.978 |
0.001 |
−0.006 |
0.007 |
8 |
3.608 |
3.608 |
3.625 |
0.000 |
−0.017 |
0.017 |
9 |
3.530 |
3.512 |
3.528 |
−0.018 |
0.002 |
−0.019 |
10 |
4.157 |
4.127 |
4.171 |
−0.030 |
−0.014 |
−0.015 |
11 |
3.502 |
3.502 |
3.513 |
0.001 |
−0.011 |
0.012 |
13 |
2.940 |
2.940 |
2.962 |
−0.001 |
−0.022 |
0.021 |
14 |
3.564 |
3.530 |
3.568 |
−0.034 |
−0.004 |
−0.029 |
20 |
2.987 |
2.973 |
2.993 |
−0.014 |
−0.006 |
−0.008 |
Table S10. Local reactivity descriptors for 9k using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.973 |
7.925 |
7.999 |
−0.048 |
−0.026 |
−0.022 |
2 |
3.029 |
3.022 |
3.036 |
−0.007 |
−0.007 |
0.000 |
3 |
2.980 |
2.979 |
2.998 |
−0.002 |
−0.018 |
0.016 |
4 |
2.906 |
2.893 |
2.910 |
−0.013 |
−0.004 |
−0.010 |
7 |
2.973 |
2.961 |
2.979 |
−0.012 |
−0.005 |
−0.007 |
8 |
3.609 |
3.606 |
3.624 |
−0.004 |
−0.015 |
0.011 |
9 |
3.529 |
3.504 |
3.528 |
−0.025 |
0.000 |
−0.025 |
10 |
4.152 |
4.108 |
4.168 |
−0.044 |
−0.016 |
−0.028 |
11 |
3.502 |
3.497 |
3.511 |
−0.005 |
−0.010 |
0.005 |
13 |
2.941 |
2.935 |
2.960 |
−0.006 |
−0.019 |
0.013 |
14 |
3.556 |
3.533 |
3.567 |
−0.023 |
−0.011 |
−0.012 |
20 |
2.985 |
2.960 |
2.997 |
−0.026 |
−0.012 |
−0.014 |
Table S11. Local reactivity descriptors for 9m using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.968 |
7.896 |
7.995 |
−0.072 |
−0.027 |
−0.045 |
2 |
3.028 |
3.020 |
3.035 |
−0.008 |
−0.007 |
−0.001 |
3 |
2.980 |
2.978 |
2.995 |
−0.002 |
−0.015 |
0.013 |
4 |
2.907 |
2.895 |
2.918 |
−0.013 |
−0.011 |
−0.002 |
7 |
2.973 |
2.955 |
2.978 |
−0.018 |
−0.005 |
−0.013 |
8 |
3.608 |
3.605 |
3.300 |
−0.002 |
0.308 |
−0.310 |
9 |
3.530 |
3.502 |
3.530 |
−0.028 |
0.000 |
−0.027 |
10 |
4.149 |
4.105 |
4.167 |
−0.043 |
−0.018 |
−0.025 |
11 |
3.500 |
3.496 |
3.510 |
−0.005 |
−0.009 |
0.004 |
13 |
2.942 |
2.936 |
2.958 |
−0.006 |
−0.016 |
0.010 |
14 |
3.554 |
3.534 |
3.568 |
−0.019 |
−0.014 |
−0.005 |
20 |
2.985 |
2.955 |
2.998 |
−0.030 |
−0.013 |
−0.017 |
Table S12. Local reactivity descriptors for 9n using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.974 |
7.957 |
8.002 |
−0.017 |
−0.029 |
0.011 |
2 |
3.029 |
3.025 |
3.036 |
−0.004 |
−0.007 |
0.003 |
3 |
2.980 |
2.981 |
2.999 |
0.001 |
−0.020 |
0.021 |
4 |
2.908 |
2.897 |
2.909 |
−0.011 |
−0.001 |
−0.010 |
7 |
2.973 |
2.970 |
2.979 |
−0.004 |
−0.006 |
0.002 |
8 |
3.607 |
3.608 |
3.624 |
0.000 |
−0.017 |
0.017 |
9 |
3.530 |
3.508 |
3.529 |
−0.023 |
0.001 |
−0.024 |
10 |
4.155 |
4.120 |
4.167 |
−0.035 |
−0.013 |
−0.022 |
11 |
3.502 |
3.500 |
3.513 |
−0.002 |
−0.011 |
0.009 |
13 |
2.941 |
2.939 |
2.962 |
−0.002 |
−0.021 |
0.019 |
14 |
3.561 |
3.532 |
3.565 |
−0.028 |
−0.004 |
−0.024 |
20 |
2.986 |
2.966 |
2.994 |
−0.020 |
−0.009 |
−0.011 |
Table S13. Local reactivity descriptors for 9o using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.974 |
8.002 |
7.961 |
0.028 |
0.012 |
0.016 |
2 |
3.029 |
3.036 |
3.026 |
0.007 |
0.003 |
0.004 |
3 |
2.980 |
2.999 |
2.981 |
0.020 |
−0.001 |
0.021 |
4 |
2.908 |
2.909 |
2.898 |
0.001 |
0.010 |
−0.009 |
7 |
2.973 |
2.979 |
2.971 |
0.006 |
0.002 |
0.004 |
8 |
3.607 |
3.624 |
3.608 |
0.017 |
0.000 |
0.017 |
9 |
3.530 |
3.529 |
3.510 |
−0.001 |
0.020 |
−0.021 |
10 |
4.155 |
4.168 |
4.124 |
0.013 |
0.031 |
−0.018 |
11 |
3.502 |
3.513 |
3.501 |
0.011 |
0.001 |
0.009 |
13 |
2.941 |
2.962 |
2.939 |
0.021 |
0.002 |
0.020 |
14 |
3.561 |
3.565 |
3.536 |
0.004 |
0.025 |
−0.021 |
20 |
2.986 |
2.995 |
2.969 |
0.009 |
0.017 |
−0.009 |
Table S14. Local reactivity descriptors for 9p using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.972 |
8.002 |
7.962 |
0.031 |
0.010 |
0.020 |
2 |
3.029 |
3.036 |
3.025 |
0.007 |
0.003 |
0.004 |
3 |
2.979 |
3.000 |
2.980 |
0.021 |
−0.001 |
0.023 |
4 |
2.907 |
2.909 |
2.898 |
0.001 |
0.010 |
−0.009 |
7 |
2.972 |
2.978 |
2.972 |
0.006 |
0.000 |
0.006 |
8 |
3.608 |
3.625 |
3.607 |
0.017 |
0.001 |
0.016 |
9 |
3.530 |
3.528 |
3.512 |
−0.002 |
0.017 |
−0.019 |
10 |
4.155 |
4.169 |
4.125 |
0.014 |
0.030 |
−0.016 |
11 |
3.501 |
3.512 |
3.502 |
0.011 |
0.000 |
0.011 |
13 |
2.940 |
2.962 |
2.939 |
0.021 |
0.001 |
0.020 |
14 |
3.559 |
3.563 |
3.532 |
0.005 |
0.026 |
−0.022 |
20 |
2.985 |
2.992 |
2.970 |
0.007 |
0.015 |
−0.008 |
Table S15. Local reactivity descriptors for 9q using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.974 |
7.999 |
7.947 |
0.025 |
0.026 |
−0.001 |
2 |
3.029 |
3.036 |
3.024 |
0.007 |
0.005 |
0.002 |
3 |
2.980 |
2.996 |
2.980 |
0.016 |
0.000 |
0.016 |
4 |
2.906 |
2.910 |
2.894 |
0.004 |
0.012 |
−0.009 |
7 |
2.973 |
2.978 |
2.958 |
0.005 |
0.015 |
−0.010 |
8 |
3.608 |
3.622 |
3.605 |
0.014 |
0.003 |
0.011 |
9 |
3.529 |
3.529 |
3.502 |
0.000 |
0.027 |
−0.028 |
10 |
4.151 |
4.167 |
4.113 |
0.015 |
0.038 |
−0.022 |
11 |
3.502 |
3.511 |
3.499 |
0.009 |
0.003 |
0.007 |
13 |
2.941 |
2.959 |
2.937 |
0.018 |
0.004 |
0.014 |
14 |
3.560 |
3.571 |
3.528 |
0.011 |
0.032 |
−0.020 |
20 |
3.023 |
3.042 |
3.012 |
0.019 |
0.011 |
0.009 |
Table S16. Local reactivity descriptors for 9r using Hirschfeld charges at the theory 6-31+G(d,p) level.
ATOMS |
(N) |
(N + 1) |
(N − 1) |
|
|
|
1 |
7.972 |
8.002 |
7.938 |
0.030 |
0.033 |
−0.004 |
2 |
3.029 |
3.036 |
3.023 |
0.007 |
0.006 |
0.002 |
3 |
2.979 |
2.998 |
2.979 |
0.020 |
0.000 |
0.020 |
4 |
2.908 |
2.910 |
2.893 |
0.002 |
0.014 |
−0.012 |
7 |
2.973 |
2.978 |
2.966 |
0.005 |
0.007 |
−0.001 |
8 |
3.607 |
3.623 |
3.604 |
0.016 |
0.003 |
0.013 |
9 |
3.530 |
3.528 |
3.500 |
−0.001 |
0.030 |
−0.031 |
10 |
4.154 |
4.169 |
4.110 |
0.015 |
0.044 |
−0.029 |
11 |
3.502 |
3.512 |
3.499 |
0.010 |
0.003 |
0.007 |
13 |
2.940 |
2.961 |
2.936 |
0.021 |
0.004 |
0.016 |
14 |
3.559 |
3.567 |
3.526 |
0.008 |
0.034 |
−0.026 |
20 |
3.023 |
3.044 |
3.009 |
0.021 |
0.013 |
0.008 |