Paweł A.
Wieczorkiewicz
*a,
Tadeusz M.
Krygowski
b and
Halina
Szatylowicz
*a
aFaculty of Chemistry, Warsaw University of Technology, Noakowskiego 3, 00-664 Warsaw, Poland. E-mail: pawel.wieczorkiewicz.dokt@pw.edu.pl; halina.szatylowicz@pw.edu.pl
bDepartment of Chemistry, University of Warsaw, Pasteura 1, 02-093 Warsaw, Poland
First published on 1st July 2024
Five-membered N-heterocycles are principal constituents of many compounds of vital importance in various fields of chemistry, biochemistry or pharmaceutical chemistry. For this reason, unequivocal identification of structural factors determining electron donating/withdrawing properties of specific groups attached to the heterocyclic moiety becomes an utmost need together with elucidation of the substitution-induced changes in cyclic and noncyclic electron delocalization. Thus, quantum-chemical calculations were performed for pyrrole, imidazole, pyrazole, 1,2,3- and 1,2,4-triazole, and their C-substituted mono-derivatives (X = NO2, CN, Br, Cl, F, SH, OH, NH2). The obtained dataset contains information on substituent properties (cSAR – charge of the substituent active region method), delocalization (EDDB – electron density of delocalized bonds) and geometry. It follows that the positions of endocyclic N atoms relative to the substituent influence in the most profound manner its properties. N atoms in ortho positions significantly boost the electron-donation and weaken the electron-withdrawal by induction. Another factor is the resonance charge transfer from the substituents to N atoms, and then inductive interactions with further (non-ortho) N atoms. While substituent constants correctly describe the changes of their properties (including those attached to the heterocycles), a testimony to Hammett's genius, quantum chemical models must be used to quantify the exact properties. In most heterocycles, electron-donating substituents hinder the cyclic delocalization, except 4-pyrazole. The applied recent EDDB method allows to study this phenomenon in detail. It follows that changes in aromaticity originate from the π-electronic effects of substituents on the ring bonds, changing the localization and delocalization of particular bonds in a correlated manner.
However, the use of biological activities of pyrazole, pyrrole, imidazole and triazole derivatives should not be overestimated.18 In recent years, many publications have appeared summarizing their biological significance.19–27 Pyrrole does not occur naturally, but many of its derivatives can be found in various cofactors and natural products, for example, vitamin B12 or bile pigments such as bilirubin and biliverdin. The first natural pyrazole, pyrazole-1-alanine, was isolated from watermelon seeds.28 Pyrazole moieties are listed by the US FDA among frequently used ring systems in small molecule drugs. The imidazole moiety, which has two nonadjacent nitrogen atoms, is incorporated into many important biological compounds (nucleobases, histidine, histamine). Triazole, containing three nitrogen atoms, exists as two isomers 1,2,3-triazole and 1,2,4-triazole, each of which has two tautomers, as shown in Fig. 1. The latest (2024) review focuses on current progress in the biological use and preparation of triazole derivatives, highlighting their role in pharmaceutical chemistry.29 Tetrazole, in addition to its biological activity,30,31 due to its unique properties and practical importance, is considered an important precursor for the development of a wide range of energetic compounds.32
All of the above-mentioned five-membered heterocycles, shown in Fig. 1, are aromatic, as documented below (Table 1). The systems whose properties and applications are outlined above contain these units. Therefore, they can be regarded as substituted systems in which one or more functional groups (substituents) are attached to the heterocyclic ring. Undoubtedly, this is a great simplification, but it can be very helpful in understanding and planning subsequent compounds with the desired properties. In this case, it is very helpful to use studies on the substituent effect, one of the most important concepts in chemistry, biochemistry and related fields.33 Many such studies have been performed, computationally and experimentally, for example for pyrroles,34,35 pyrazoles,36 imidazoles37,38 and triazoles39–41 and references therein. However, they mainly concern the influence of the substituent on the tautomeric stability, the geometric and electronic structure of the ring and their aromaticity, while the substituents are characterized by the σ Hammett constants.42,43 The use of σ constants implies the assumption that the properties of the substituent attached to the benzene and the five-membered heterocyclic ring are similar. However, it has been shown that the properties of the substituent depend both on the place of its attachment and on the substituted system,35 the so-called reverse substituent effect. For this purpose, quantum-chemical descriptors calculated specifically for each molecule, such as cSAR (charge of the substituent active region),44 should be used. One of the goals of this work is to determine the properties (and their changes) of substituents attached to pyrrole, pyrazole, triazoles and their tautomers (Fig. 1). For this purpose, a wide set of substituents was selected (X = NO2, CN, Br, Cl, F, SH, OH, NH2) with properties ranging from electron withdrawing to electron donating. By analyzing all possible five-membered N-heterocycles with many substituents, our aim is to unravel the general principles determining the properties of substituents, geometry of individual systems and the electron delocalization – cyclic associated with aromaticity, and non-cyclic. HOMA (Harmonic Oscillator Model of Aromaticity) is undoubtedly the most popular geometric aromaticity index.45 HOMA compares the bond lengths with those of the reference aromatic system, whilst taking into account the lengths of the reference single and double bonds encoded in the normalization constant. For fully aromatic reference systems, HOMA = 1, while lower values indicate lower aromatic character of a ring. Originally, it was formulated in 1972 and included parametrization only for CC bonds.45 In 1993 Krygowski extended HOMA by adding parameters for CC, CN, CO, CP, CS, NN, and NO bonds, thus expanding its applicability to heterocycles.46 However, it has been noticed that this parametrization suffers from inconsistent choice of reference systems. For example, the parameters for the CC and C
O bonds are based on (Z)-1,3-butadiene and formic acid, respectively, two systems in which resonance of the double bond is present, whereas the C
N bond was parametrized from methylimine, where only marginal resonance is present by hyperconjugation. This sometimes causes strange results, for example, furan is classified as non-aromatic (HOMA = 0.298). Another consequence is that HOMA has different scales depending on the bonds found in the molecule. For example, for systems with CC bonds it can vary from highly negative values to 1, while for CN, only from 0 to 1. This problem of different scales of HOMA is discussed in detail by Raczyńska.47 The shortcomings of HOMA were addressed in its new parametrization, called HOMED (Harmonic Oscillator Model of Electron Delocalization).48 HOMED attempts to describe various resonance effects (conjugation, hyperconjugation, aromaticity) and has a fixed scale from 0 to 1. It greatly improves the description of electron delocalization in small heteroaromatic systems. However, the parametrization procedure, which requires a choice of a single Lewis structure, is unclear for macrocycles (e.g. porphyrins), where the ground state electronic structure is described as superposition of many Lewis structures. It should also be remembered that the values of HOMA and HOMED are influenced by noncyclic delocalization. On the one hand, it allows to assess delocalization also in non-aromatic systems, but on the other, contributions of cyclic and non-cyclic delocalization (e.g. resonance between atoms in considered delocalization pathway and other atoms) cannot be separated as with the novel EDDB (electron density of delocalized bonds) method, which is the main tool used in this study.49–52
a Isosurfaces of EDDBP(π) (0.02 electron) superimposed onto Lewis structures and below the number of cyclically delocalized π-electrons. b Normalized multicenter index in NAO basis. c Aromatic stabilization energies in kcal mol−1, taken from ref. 53. d Low absolute value results from the ring size extensivity of NICS. e Bottleneck for cyclic delocalization – the bond at which connection between EDDBP(π) isosurfaces first breaks when increasing isovalue. |
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As shown in Table 1, HOMED, unlike HOMA, correctly describes the sequence of increasing aromaticity of five-membered N-heterocycles with one or two N atoms: imidazole > pyrrole > pyrazole. The sequence agrees with ASE (aromatic stabilization energy) and EDDBP(π) results. Tautomeric forms also differ in aromaticity. Furthermore, more aromatic tautomers are also more stable (in the gas phase), in agreement with B3LYP/6-311+G(d,p) calculations by Raczyńska.47 However, it should be remembered that in solution, tautomeric equilibria may shift, for example, in polar solvents like DMSO, tetrazole exists mostly in N1H form, as evidenced by NMR studies.54,55 Among the aromaticity indices shown, ASE, MCI and EDDBP(π) allow to directly compare the aromaticity of heterocycles with benzene, since they do not depend on parametrization (HOMA/HOMED), nor on the ring size (NICS). Generally, heterocycles with fewer C–N(H) bonds are more aromatic. There is a decent correlation (R2 = 0.733) between EDDBP(π) and the number of C–N(H) bonds in the ring (Fig. S1, ESI†). No correlation is observed between EDDBP(π) and the total number of N atoms or the number of other C–N bonds. The bond at which the connection between the isosurfaces first breaks when increasing EDDBP(π) value, is the bottleneck for cyclic delocalization.
The slope values of EDDBP(π) vs. cSAR(X) relations (collected in Table S1, ESI†) indicate that the cyclic delocalization in imiC2 is the most sensitive to the change in substituent properties. In this system, the number of cyclically delocalized π-electrons increases 2.3 times when changing from the strongly electron donating to the withdrawing group. Other systems with slopes lower than −3.7 and high R2 values are all 1,2,4-triazoles and two pyrazoles: pyraC3 and pyraC5. Systems with moderate changes (slope between −1.8 and −2.6) and lower R2 values (0.290 to 0.781) are pyrrC2, 1,2,3-triC5, 1,2,3-triC4(N2H), imiC5 and imiC4. It should be noted that for the imiC4 and imiC5 systems the slope is approximately −2 (R2 > 0.72), so their aromaticity is 3.4 times less sensitive to the substituent effect than in the imiC2 derivatives. Fig. 3 presents electron delocalization in derivatives with electron-withdrawing X = NO2, slightly π-donating but withdrawing by induction X = Cl, and strongly π-donating X = OH groups. As for Cl, its π-donating properties are more important, since we consider the π-electron structure. Similar visualizations for all substituents are shown in ESI† (Table S2). It should be mentioned that the conclusions drawn from NO2, Cl and OH extend to other π-electron withdrawing and donating groups, as confirmed by the data for all substituents (Table S2, ESI†). The OH group gives better assessment of how π-electron donation changes aromaticity because the other strongly donating group, X = NH2, rotates in some derivatives due to interaction between its hydrogens and endocyclic N atoms. Rotation weakens π-donating effect of NH2, as it decreases overlap between the π orbitals of substituted system and the lone electron pair orbital of NH2. Such effects in aminopyrazoles (pyraC5 and N-substituted) have already been reported in the literature.36,56 Therefore, the OH group is simpler and adds no additional effects to consider. In pyrrC2, the NO2 group enhances the total cyclic delocalization by increasing delocalization through two single bonds (C3–C4 and N1–C5), which in unsubstituted pyrrole have a larger localized character. Bond lengths follow changes in the electronic structure – these single bonds are shorter for X = NO2 than for Cl and OH. In pyrrC2–OH derivative, the C4–C5 double bond is more localized and shorter, which is pictured by separated EDDBP(π) isosurfaces (Fig. 3). In pyrrC3, both the donating and withdrawing substituents disrupt the cyclic delocalization, but weaker electron donors, such as Cl, disrupt it to a much smaller extent (the points in Fig. 2 form an inverse ‘v’ shape). Adding another N atom to the ring in the C2 position (pyrazole), enhances cyclic delocalization. PyraC3 and pyraC5 derivatives are characterized by similar changes in aromaticity due to the substituent effect, although the C5 derivatives have slightly better cyclic delocalization. PyraC5–NO2 is the most aromatic of the systems studied with two endocyclic N atoms. On the contrary, pyraC4 is the only system in which electron-donating substituents increase aromaticity, and electron-withdrawing groups reduce it. Comparing the shapes of EDDBP(π) isosurfaces (Fig. 3), the NO2 group increases the localization of N2–C3 and adjacent bonds. The N2–C3 double bond is the shortest for the least aromatic X = CN and NO2 and the longest for the most aromatic X = OH; the correlation between EDDBP(π) and its length is remarkable (R2 = 0.96) (Fig. 4). The increase in localization of this bond along with the electron-withdrawing properties of X may be responsible for the inverse correlation between aromaticity and substituent properties in pyraC4. In no other system does the electron-withdrawal by substituent cause such a large shortening of the N2–C3 double bond, for X = CN down to 1.3265 Å which is below the optimal value of the CN aromatic bond, 1.3337 Å (Fig. 4). In the pyraC4–CN derivative, this bond, rather than N1–N2 as in unsubstituted pyrazole (Table 1), is the bottleneck for cyclic delocalization. This is further confirmed by the high R2 of the N2–C3 bond length vs. EDDBP(π) relation (Fig. 4).
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Fig. 3 Isosurfaces of the EDDBP(π) function (0.02 electrons) and the number of cyclically delocalized π-electrons in the ring for selected systems (X = H, NO2, Cl, OH). |
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Fig. 4 (a) Schematic representation of changes in bond lengths due to the substituent effect and relations between ring bond lengths and resonance constants, R, of X substituents (example: pyraC4). (b) Relations between ring bond lengths and number of cyclically delocalized π-electrons; calculated reference aromatic bond lengths are marked. Isosurfaces of EDDBP(π) for X = CN and OH derivatives. Data for all systems in Fig. S3 (ESI†). |
Imidazole, with the second endocyclic N atom in the 3-position is less aromatic than pyrrole. However, this is the most labile system when it comes to aromaticity, as already shown by the slope of EDDBP(π) vs. cSAR(X) plot (Fig. 2). Changing the substituents in the C2 position may increase (X = NO2) or decrease (X = OH) the effectiveness of cyclic delocalization by ∼40% relative to the unsubstituted system. The shapes of isosurfaces change uniformly around the ring, so that disruption of aromaticity by electron-donating groups cannot be attributed to changes in one or two bonds. The aromaticity of imiC4 and C5 derivatives is less prone to change due to the substituent effect than imiC2 ones.
The results of previous studies on imidazole derivatives indicate that the ranges of variability of HOMA due to the substituent effect are larger for imiC2 than for imiC4 and imiC5, which agrees with the above conclusion; similarly, electron-withdrawing groups boost aromaticity.38 Interestingly, if the N position of imidazole and pyrazole is substituted, the aromaticity decreases with increasing electron-withdrawing properties of the substituent, as shown by Curutchet et al.57 Thus, the N-substitution effect on aromaticity of pyrazoles and imidazoles is similar to that in the pyraC4 systems. In addition, linear regressions between aromaticity indices HOMA, NICS, FLU, MCI, and the resonance constants (R), had similar slope values for pyrazole and imidazole N-derivatives, indicating similar sensitivity to the substituent effect in both cases. This cannot be said for the C-derivatives, since the slopes for the “imi” and “pyra” systems in relations EDDBP(π) vs. cSAR(X) (Fig. 2) and R (Fig. S2, ESI†) vary.
Among the systems with three endocyclic N atoms, 1,2,4-triazoles are less aromatic than 1,2,3-triazoles, while the N4H tautomer of 1,2,4- is the least aromatic of all the N-heterocycles studied (Table 1). The aromaticity of 1,2,4-triC3(N4H) shows a similar sensitivity to the substituent effect as 1,2,4-triC3(N1H) (a = −3.8 and −3.7, respectively, Fig. 2). These systems behave similarly to imiC4 and imiC5, but the changes in aromaticity are higher. 1,2,4-triC5 and imiC2 are the two systems with the greatest sensitivity of the cyclic delocalization to the substituent effect (a = −5.0 and −6.8, respectively, Fig. 2), but in this case, imidazole is characterized by larger changes in aromaticity.
In highly aromatic 1,2,3-triazole derivatives (EDDBP(π) = 3.2 and 3.3 for N1H and N2H tautomers, respectively), all substituents but one (X = F in 1,2,3-triC4(N1H)) disrupt the cyclic delocalization. The F-substituted molecule is characterized by the most extensive cyclic delocalization among all studied. In 1,2,3-triC4(N1H) derivatives, the smallest changes in the cyclic delocalization occur compared to the other substituted systems. Moreover, the points for this system in Fig. 2 form an inverse ‘v’ shape, similar to the pyrrC3 systems. However, in 1,2,3-triC5(N1H) and 1,2,3-triC4(N2H), the NO2 group disrupts cyclic delocalization only slightly, while the OH group significantly. It can be noticed that the N1(H)–N2 or N2(H)–N3 bonds in these two systems are more localized for X = OH (and also longer, Fig. S3, ESI†), than for X = NO2. Since our study did not include tetrazole derivatives, it is worth mentioning Sadlej-Sosnowska's study on C-substituted tetrazoles (X = BH2, NO2, CN, Br, Cl, F, H, CH3, OCH3, NH2).58 The obtained results showed that for derivatives of the N2H tautomer the variation in aromaticity is small, while for the N1H tautomer the aromaticity is the highest for π-electron withdrawing substituents (BH2, NO2, CN).
The structure of a molecule is a valuable source of information about its properties. Considering the series of substituted X-derivatives for each heterocycle, the bond lengths in the ring correlate well with the number of cyclically delocalized π-electrons (Fig. 4 and Fig. S3, ESI†). In systems with more efficient delocalization, bonds approach the reference lengths for aromatic systems. In general, no correlation is observed in systems with small changes in aromaticity and for two bonds with a substituted ring atom. However, it is important to mention here that the substituents influence the three other bonds in a consistent manner. As the π-withdrawing properties of substituent increase, the bond opposite to the substituent (e.g., N1–N2 in pyraC4) is elongated, while the two bonds ‘parallel’ to the C–X bond (N1–C5 and N3–C4 in pyraC4) are shortened. The regularity of these changes is reflected in the good correlations between the bond lengths and the resonance substituent constants, R (Fig. 4a). Interestingly, the lengthening and shortening of these bonds are observed regardless of their double or single character in the primary Lewis structure. This trend is also observed in the crystallographic data found for monosubstituted compounds (Table S3, ESI†). Moreover, the trend also applies to N-substituted pyrazoles, which is evident from the MP2/6-31G(d,p) results presented by Mó et al.,56 thus, it appears to be a universal characteristic of N- and C-substituted five-membered N-heterocycles. However, the effect is discussed by Mó et al. only qualitatively, in terms of hybridization changes and resonance effects by substituents. Our NBO results do not reveal any correlations between hybridization of natural hybrid orbitals forming particular bonds and their lengths (Fig. S4, ESI†), as suggested in the article, so the interpretation in terms of π-electronic effects is more valid (which is further supported by good correlations between bond lengths and R constants). Regularity in ring bond length changes are due to the fact that the shapes of the π orbitals are similar in all monoderivatives of five-membered N-heterocycles (Fig. S5, ESI†), regardless of the substituent, the number of N atoms, and the positions of both. Therefore, it appears that the changes in aromaticity come from the interplay between how the substituent resonance properties influence the ring bond lengths and the bond lengths in the unsubstituted system. In most cases, π-electron withdrawing groups enhance cyclic delocalization by affecting particular bonds, while π-electron donating groups create bottlenecks for cyclic delocalization by shortening double bonds or elongating single. This can be noticed by comparing the slopes of the linear equations correlating the bond length and R or EDDBP(π) (Fig. 4 and Fig. S3, ESI†) – both have the same sign. As mentioned above, the only systems in which electron-donating substituents increase and electron-withdrawing groups decrease aromaticity in a correlated manner are pyraC4 derivatives (slopes have opposite signs, Fig. 4), and N-substituted imidazoles and pyrazoles.57
The relationships between the number of cyclically delocalized electrons (EDDBP(π)) and HOMA or HOMED (Fig. S6, ESI†) are curvilinear due to the harmonic oscillator model used in the HOMA definition. The points in HOMED relation are more condensed than in HOMA due to the fixed 0 to 1 scale of HOMED, and the position of three deviating points is improved. The system with almost zero cyclically delocalized electrons is the imino (NH) form of pyraC3–NH2. However, the HOMED value indicates some electron delocalization (HOMED = 0.59). This is because EDDBP(π) only accounts for cyclic delocalization, while HOMED also accounts for non-cyclic delocalization. A variant of EDDB that takes into account all delocalization (cyclic and non-cyclic, EDDBF) gives a value of 1.16 delocalized π-electrons for atoms in the ring.
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Fig. 5 Isosurfaces of EDDBG–P function (0.02 electrons) for selected systems – a visual representation of non-cyclic electron delocalization. Data for all systems in Table S4 (ESI†). |
a indN – the number of endocyclic N atoms in ortho positions relative to substituent, 2o – grey shading of compound name, 1o – light grey shading, 0 – no shading. b resN – the number of endocyclic N atoms interacting via resonance (singly excited structures) with substituent and their position relative to substituent: o – ortho, p – para-like. |
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On the graph between cSAR(X) and σp substituent constants, it can be noticed that these two parameters correlate well and series for different heterocycles are almost parallel – they differ mostly by the intercept (b) of cSAR(X) = a·σp + b linear equations (Fig. 6). This indicates that the nature of the substituent effect is similar for different heterocycles; in other words, none of the heterocycles interacts with the substituents in a specific way, for example by much stronger resonance effect like a charged substituent would.43 The source of differences in the intercepts is mainly the inductive electron withdrawal by ortho-N atoms as discussed earlier (Table 2). Interestingly, heterocycles with 0 indN are better electron donors to the substituents compared to benzene, while all the others are better electron acceptors (Fig. 6).
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Fig. 6 Relationships between cSAR(X) and the substituent constants σp. Parameters of fitted functions cSAR(X) = a·σp + b in table. |
Points for the SH group regularly lie above the fitted lines in systems where the SH conformation is coplanar relative to the ring plane. It indicates that in this conformation SH is more electron donating relative to other substituents than according to its σp substituent constant. Indeed, the coplanar conformation of SH allows for stronger electron donation by resonance due to the larger 3p-π orbital overlap. The resonance between the substituent and the heterocycle is associated with shortening of the C–X bond connecting them. For this reason, in the dCXvs. cSAR(X) plot (Fig. 7) we can see a correlated series for each substituent – π-electron donating groups (Br, Cl, F, SH, OH, NH2) have negative slope values, while π-electron withdrawing (NO2, CN) have positive slope values. This is another example of how changes in the electronic structure shift the positions of atomic centers and change molecular geometry. The worst R2 values are observed for X = CN and SH, since the C–X bond in these derivatives is the least susceptible to changes in length (both have range of variation ∼0.014 Å). For the bulky NO2 substituent, systems with ortho NH group form a series with slightly shorter C–X bonds due to the lack of repulsive steric interaction (with CH or N) as in the case of other systems. It should be mentioned that the analysis of non-covalent interactions with NCI method61 does not detect through space interactions between substituent atoms and endocyclic N/NH groups in ortho positions (for example NO⋯HN for X = NO2 and NH⋯N for X = NH2). Some very weak interactions are detected only in NO2 derivatives (Fig. S7, ESI†). This indicates the weakness of such interactions, mainly due to the sharp angles between the atoms involved, imposed by the five-membered ring geometry.
Therefore, there must be a substantially stabilizing (by approximately 20 kcal mol−1) effect associated with the interaction between NH/
O/
S and ortho N(H) groups. A possible explanation is the strong resonance interactions between the substituent and two ortho N(H) groups, exemplified by two zwitterionic resonance forms with O− and N(H)+. Endocyclic N(H) groups have a 2pz electron pair that can be delocalized onto nearby electron withdrawing
NH/
O/
S groups. This resonance is clearly visible on the EDDBG–P plots (Fig. 5). Such interaction is stronger than that between the substituent and the endocyclic N atom with only one 2pz electron.
Generally, the NH/
O/
S forms have poor cyclic delocalization (EDDBP(π) < 1.0), due to the possible π-electron excess in the ring – from the Lewis structure there are formally seven 2pz electrons, each N(H) group provides two, each C and N one. However, some of these forms have good cyclic delocalization; five systems have EDDBP(π) between 1.0 and 2.0, and four systems between 2.05 and 2.23 (Table S7, ESI†). Interestingly, the anisotropy of the induced current density (AICD)62 plot of pyraC4
O, the most aromatic keto form (EDDBP(π) = 2.05), reveals diatropic ring current, whereas in imiC2
O the lack of diatropic ring current suggests its nonaromatic character in agreement with low EDDBP(π) value, 0.605 (Fig. S8, ESI†). Among the
NH/
O/
S forms,
S are always the most aromatic, followed by
O and the least aromatic
NH. From Fig. 8 and Table S7 (ESI†) it can be noticed that HOMED values do not correlate well with EDDBP(π) in the
NH/
O/
S forms; unlike EDDBP(π), HOMED also accounts for non-cyclic delocalization effects, which are significant in these forms, as visualized by voluminous EDDBG–P isosurfaces (Fig. 5 and Table S4, ESI†). The highly negative cSAR(X) values (Fig. 8 and Table S7, ESI†) indicate a strong electron-withdrawal via resonance by
NH/
O/
S groups.
This particularly strong resonance between the substituent and heterocycle can be noticed in EDDBG–P plots (Table S4, ESI†). Furthermore, the EDDBG–P plots of four heterocycles with the lowest cSAR(X) values of O,
S and
NH (pyraC4, 1,2,3-triC4(N1H,N2H), 1,2,3-triC4(N1H,N3H), imiC4) clearly show more extensive resonance than in the other six. It should be remembered here that, depending on the N/N(H) positions, the rings themselves have different inductive electron withdrawing strength, and that
O/
S/
NH withdraw electrons both by induction and resonance. Moreover, the four most aromatic systems among the
O,
S and
NH forms have the lowest cSAR(X) values and longer CX bonds (Fig. 8 and Table S7, ESI†). This indicates a large contribution of zwitterionic forms with O− and N(H)+ to their ground state. Such resonance forms formally have six delocalizable 2pz electrons in the ring, which contribute to their higher aromaticity.
Furthermore, the CX bond lengths (CO, C
S and C
NH) are well correlated with electronic properties of X (Fig. 7); elongating the bond increases the electron-withdrawing ability of X. This indicates that with an increase in the electron-withdrawal by X, also increases the contribution of X− and N(H)+ zwitterionic resonance forms with a single bond between C and X−. Nonetheless, despite relatively high aromaticity,
NH/
O/
S forms of pyraC4, 1,2,3-triC4(N1H,N2H), 1,2,3-triC4(N1H,N3H) and imiC4 are not stable, as shown by large ΔE values (Fig. 8 and Table S7, ESI†). Interestingly, there is a decent correlation (R2 = 0.738) between EDDBP(π) and cSAR(X) of
NH,
O and
S (Fig. S9, ESI†). This indicates that the systems in which these substituents withdraw more electrons from the rings (with π-electron excess relative to aromatic sextet) have better cyclic delocalization. It resembles the situation in heptafulvenes, which are non-aromatic conjugated molecules with exocyclic double bond and π-electron excess in the ring; similarly, strongly electron-withdrawing exocyclic substituent can enhance the cyclic delocalization.63 The HOMO and LUMO orbital energies of all studied heterocycles correlate with the properties of substituents evaluated by cSAR(X) (Fig. S10, ESI†). In all cases, the energies increase with electron-donating ability of X. However, the HOMO–LUMO gaps do not correlate with cSAR(X).
Substituents influence the π-electron structure and geometry of heterocycles in an orderly manner due to the fact that the π orbitals in all derivatives have a similar shape and node location. The length of the bond opposite the substituent increases with π-electron withdrawing strength of the substituent (R constant), while the two bonds adjacent to the opposite one are shortened.
Interplay between ring bond lengths and substituent resonance properties determines the aromaticity of heterocycle. For example, when short, highly localized double bonds are further shortened by substituents, bottlenecks for cyclic delocalization are created. In most cases, this effect causes that π-electron withdrawing groups enhance, while π-donating groups disrupt the cyclic delocalization in a correlated manner. The exceptions are 4-substituted pyrazoles, in which opposite correlation is observed; the same was found for N-substituted pyrazoles and imidazoles. In the case of 3-substituted pyrrole and 4-substituted 1,2,3-triazole derivatives, no correlation is observed. However, the 4-F-1,2,3-triazole(N1H) molecule is characterized by the most intense cyclic delocalization among all studied systems, while pyrrole is the most aromatic of the pyrrC3 series. Moreover, changing the substituent to a more electron-donating or electron-withdrawing one disrupts cyclic delocalization.
The properties of the substituents depend on the number and positions of the endocyclic N-atoms. For example, cSAR values for NO2 vary from 0.00 to −0.216, while for NH2 from 0.230 to 0.012. The most important is the number of N atoms in ortho positions, which withdraw electrons from the substituents by induction, increasing their electron-donation or weakening their electron-withdrawal. The second, less important factor, is the number of ring N-atoms which interact with the substituent via resonance. Every such N-atom increases the electron-donating or weakens the electron-withdrawing properties of substituent. This is because the ring N-atoms more readily accept the negative charge delocalized by electron-donating groups than less electronegative C-atoms, and less readily the positive charge delocalized by electron-withdrawing groups.
Each series of heterocyclic derivatives forms a linear relationship between the quantum-chemical descriptor of substituent properties, cSAR(X), and the Hammett constants σp. Relationships for different heterocycles are parallel and differ only in their intercept, according to the structural features discussed in the previous point. This indicates that the nature of the substituent effect and the variability of substituent properties are similar for different heterocycles. The unique utility of substituent constants should also be emphasized. Hammett's choice of the acid–base equilibrium constants of benzoic acids to determine the substituent constants was a clever idea. These constants describe well the changes in the properties of substituents also in heterocycles, but to quantify the exact properties, quantum-chemical models should be used, or the structural features should be considered in e.g. multivariate model.
The tautomeric keto and thioketo forms are more stable than their OH and SH counterparts only in systems with two endocyclic ortho-NH groups (3-substituted 1,2,4-triazole(N2H,N4H) and 2-imidazole derivatives). This is explained by the strong resonance interaction between O/
S and NH, which stabilizes these keto and thioketo forms by ∼20 kcal mol−1.
Footnote |
† Electronic supplementary information (ESI) available: Computational details, data and additional figures. See DOI: https://doi.org/10.1039/d4cp01709a |
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