Abstract
The ketoenamine-enolimine tautometic equilibrium has been studied by the analysis of aromaticity and electron-topological parameters. The influence of substituents on the energy of the transition state and of the tautomeric forms has been investigated for different positions of chelate chain. The quantum theory of atoms in molecules method (QTAIM) has been applied to study changes in the electron-topological parameters of the molecule with respect to the tautomeric equilibrium in intramolecular hydrogen bond. Dependencies of the HOMA aromaticity index and electron density at the critical points defining aromaticity and electronic state of the chelate chain on the transition state (TS), OH and HN tautomeric forms have been obtained.
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Introduction
The carbonylamines presented in the paper (Scheme 1) are prototypes of malonaldehydes investigated in a number of experimental and computational studies [1–3]. The given compounds can be referred to so-called resonance assisted hydrogen bond (RAHB) system being elaborated by Gilli et al. [4]. Recently the interest in RAHB has much grown due to the critics presented in refs [5, 6]. It is noteworthy that the aryl Schiff bases were properly studied [7–9]. However, theoretical studies of the carbonylamine (alkyl derivatives of Schiff bases) are not as numerous [10–14]. Both the alkyl Schiff bases and the aryl Schiff bases (Scheme 1) contain a quasi-aromatic formation as a common feature. But, the experimental data [15–23] expose the principle difference between these two types of compounds. What makes them different is that the HN (ketoenamine) tautomeric form prevails for the alkyl derivatives [10–26], meanwhile OH (enolimine) tautomeric form (Scheme 2) prevails for the aryl derivatives [7–9]. The transition from one form to another (the proton transfer) requires energetic expenditure (∆EPT). The change of tautomeric equilibrium is evoked by an acid-base balance and polarity of the environment. A series of papers [27–40] deals with the ways the tautomeric equilibrium affects the aromatic state of a molecule with intramolecular hydrogen bonding.
To trace a change of a tautomeric equilibrium in carbonylamines experimentally is really challenging. It is also difficult to estimate the substituent influence in the chelate chain (O = C-C = C-N) on the hydrogen bonding strength. This task is hampered by complementary phenomena (trans-cis isomerization [11] and HO-CH = CH-C = NR⇄O = C-CH2-CH = NR equilibrium [15–17]) observed experimentally for carbonylamines. However, quantum-mechanical calculations make it possible to describe a complicated nature of hydrogen bond. This paper is concerned with the ketoenamine-enolimine tautomeric equilibrium (Scheme 2) and the calculations of the carbonylamines with various substituents (CH3, H, NH2, Cl and F) in the chelate chain. The calculations were performed for the OH and HN tautomeric forms and transition state (Scheme 2) describing two main stages of the proton transfer process [41]. For description of these stages we calculated the difference of energies between them (∆EPT = EOH - ENH, ∆ETS = ETS – EHN; the energy of HN tautomer is taken as the ground energetic level) and the HOMA aromaticity index [42] and electron-topological parameters [43, 44]. HOMA index is a widely accepted parameter applied in the description of the aromaticity [45, 46]. The merit of HOMA index is in its ability to be used for the experimental [47] and computational [48] results. The difference of energies is one of the most reliable parameters in the description of the hydrogen bonding [49].
As for the HOMA aromaticity index, it has been repeatedly verified by the researchers of intramolecular hydrogen bonding during last decade [26, 27, 30–40]. There are papers dwelling on the influence of tautomeric equilibrium on the aromaticity of phenol, aniline and naphthol complexes [50]. This paper develops these studies with aim to unify the HOMA aromaticity index in the area of hydrogen bonding and electron-topological analysis.
Computational details
The calculations were performed with Gaussian 03 [51] sets of code using the 6-311 + G(d,p) basis set [52–55] at the Møller–Plesset second-order perturbation level (MP2) [56]. QTAIM analysis was performed using the AIM2000 program [57] with all the default options.
The HOMA aromaticity index was calculated by the following formula:
where n is a number of bonds, α is an empirical constant, Ropt and Ri are the optimal and individual bond lengths taken from ref. 42. A higher HOMA aromaticity index corresponds to a more delocalized π-electronic system, hence a more aromatic formation [58].
Results and discussion
The influence of substituents on the intramolecular hydrogen bonding in the carbonylamines
The influence of substituents (R1 – R3) in the α, β and γ positions on the ketoenamine-enolimine equilibrium can be described by the inductive constants [59] (σF = 0, ∼0, 0.14, 0.44 and 0.45 for H, CH3, NH2, Cl and F, respectively). It is noteworthy, that the π-electron donation of NH2 group is small due to perpendicular orientation of its lone electron pair with respect to quasi-aromatic formation. This phenomenon was properly described by Sola et al. [60]. The increase of the electron acceptor ability of the R1 and R2 substituents (the increase of σF constant) in the α and β positions results in the growth of both the energetic barrier of transition state (ΔETS) and the OH form (ΔEPT), (Fig. 1a and b). This trend is traced for the CH3 (Fig. 1a) and H (Fig. 1b) substituents at the nitrogen atom, which serve as the basic ones for the predominant HN tautomeric form. An opposite picture is observed for the substituent (R3) in the γ position (Fig. 1a and b) which reveals the decrease of the ΔETS and ΔEOH values under the σF constants increase. These trends originate in the following phenomena: 1) the substitution (R1) in the α position greatly affects the C = O group by weakening its basicity, consequently, it attenuates the hydrogen bond strength and enhances the ΔETS and ΔEHN-OH barriers according to the CH3, H, NH2, Cl and F sequence; 2) the substitution (R3) in the γ position mostly influences the amine group by increasing its acidity according to the Cl, F, NH2 and H ≅ CH3 sequence. Some exception from the expected CH3, H, NH2, Cl and F sequence is observed for the fluoro-substituent (R3) in the γ position. The reason for this disagreement is a marked polarizability effect of the fluorine atom (σα = −0.25 [59]) which causes some attenuation of the acidity of the HN group and the intramolecular hydrogen bonding. Remarkably, the substituent (R2) in the β-position influences but to a lesser extent the ΔETS and ΔEOH values due to its remote position from the acidic (NR4) and basic (O = C) moieties.
The picture changes for the N-F derivatives (R4). The majority of these derivatives is characterized by the OH tautomeric form prevailing over the HN tautomeric form (Fig. 1c). The development of the electron acceptor ability of the R1 substituent (under weak basicity of the nitrogen atom, at N-F substituent) brings about both the decrease of the ΔETS values and the strengthening of the OH tautomeric form prevailing. However, the increase of the electron acceptor properties of the substituent (R2) in the β-position is accompanied by the growth of the ΔETS values and the weakening of the OH tautomeric form prevailing.
With respect to the substituent impact on the nitrogen atom (R4), the ΔETS and ΔEOH values are getting smaller according to the H, CH3, NH2, Cl and F sequence (Fig. 1d). Some discrepancy as to the expected CH3, H, NH2, Cl and F sequence is observed for the H substituent which slightly influences the acidity of the amine group. A similar deviation was discovered for ortho-hydroxy aryl Schiff bases and explained by a significant polarization effect of the NH group [41, 60, 61].
In terms of the structural data of the hydrogen bridge (d(OH), d(HN) and d(OH)), they are characterized by the following tendencies: 1) the elongation of the HN bond results in the reduction of the hydrogen bond and the OH bond lengths; 2) the elongation of the OH bond also triggers the reduction of the hydrogen bond and the HN bond lengths; 3) the shortest hydrogen bridge is found for the transition state; 4) the position of the TS is more shifted toward the reagents (d(O-H)TS < d(N-H)TS for prevailing of the NH…O form) according to Leffler-Hammond rule [62, 63].
Analysis of aromatic and AIM parameters vs. tautomeric equilibrium
To verify the calculations obtained by the QTAIM method the ρBCP(XH) = f(d(XH)) (X = N or O atom) dependence was developed (Fig. 2; ρBCP(OH) = 0.3489 × (OH)-3,522, R2 = 0.9991; ρBCP(NH) = 0.3071 × (NH)-3,5938, R2 = 0.9987). The dependence taken by means of full optimization for different substituents in α - γ positions appears to be an exponential curve which is in accordance with the results obtained by non-adiabatic approach [41, 64]. Remarkably, the results for different substituents under full optimization are in agreement with those found under non-adiabatic approach for ortho-hydroxy aryl Schiff bases [65].
The next stage of the study was to verify the ρRCP(ch) = f(d(OH)) and ρRCP(ch) = f(ρBCP(OH)) dependencies (Fig. 3) calculated for the OH, TS and HN states of the compounds. These dependencies look like Morse or bell-shaped curves. A similar shape of the curve is traced for HOMA(ch) = f(d(OH)) scatter plot (Fig. 4). The calculated scatter plot conditioned by some scattering of points supports the trends which are not observed under non-adiabatic approach [66]. The correlations reveal that the maximum of the electronic density at quasi-aromatic critical point (ρRCP(ch)) and maximum aromaticity reaches its top in the transition state. This result comes in agreement with the results obtained in paper 66, where the comparison of the aromaticity of hydrogen-bonded and Li bonded aryl Schiff bases derivatives was carried out.
The d(ON) = f(ρRCP(ch)) correlation (Fig. 5; d(ON)) = −35.482 × (ρRCP(ch)) + 3.2575, R2 = 0.9849) appears to be one of the most interesting dependencies which states that the shortening of the hydrogen bridge results from the growth of the electron density at the critical point of quasi-aromatic formation. But comparatively, the parabolic dependence d(ON) = f(ρBCP(XH)) is more informative with respect to tautomeric equilibrium (Fig. 6) in terms of the basic parameter (d(ON)) describing the hydrogen bond strength.
The ρRCP(ch) = f(d(OH)), ρRCP(ch) = f(ρBCP(OH)), HOMA(ch) = f(d(XH)) and d(ON) = f(ρRCP(OH)) dependencies (Figs. 3, 4 and 5) show that strengthening of the hydrogen bond brings about the increase of both electron density at the critical point of quasi-aromatic formation and the chelate chain aromaticity (Scheme 3).
Bearing in mind the fact of mutual increase of aromaticity and π-component in the aromatic formation one can confirm that the increase of ρRCP(ch) provokes the active participation of π-component.
Conclusions
It has been shown that for the HN tautomeric form the increase of the electron-acceptor ability of the substituents (R1 and R2) in α and β positions evokes a larger prevailing this form. In case of the OH tautomeric form the growth of the electron-acceptor ability of the substituents (R1) in β position contributes into the OH tautomeric form prevailing, whereas for the substituent (R2) in β position it reveals a reverse trend. With respect to the influence of substituent (R3) in the γ-position for carbonylamines, the growth of the electron-acceptor ability hinders the prevailing of the HN tautomeric form. However, for the HN tautomeric form the impact of the substituent (R3) in γ-position seems quite complicated due to mutual compensating action of the steric, inductive, resonance and polarizability effects, as well as local N-H…F hydrogen bond influence.
The HOMA(ch) = f(d(OH), ρBCP(ch) = f(d(OH)), d(ON) = f(ρBCP(ch)) dependencies have been obtained. The HOMA(ch) = f(d(OH)) and ρBCP(ch) = f(d(OH)) dependencies are bell-shaped and indicate that the transfer process from one tautomeric form to another goes via a transition state. According to these dependencies in the transition state one can observe the maximum delocalization of π-component of the chelate chain and the maximum electron density of quasi-aromatic formation. The d(ON) = f(ρBCP(ch)) dependence states that the electron density at the critical points of quasi-aromatic formation is a measure of the intramolecular hydrogen bond strength. According to the presented dependencies the enhancement of the hydrogen bond strength leads to the growth of ρBCP(ch) and HOMA(ch) and reaches its maximum in the transition state. Krygowski et al. [58] stated earlier that the increase of aromaticity strengthens π-component participation. Therefore, the strengthening of the hydrogen bond in the studied compounds is conditioned by the π-electron delocalisation in the chelate chain.
References
Buemi G, Grabowski SJ (Eds) (2006) The hydrogen bonding–new insights. Springer, Berlin, pp 51–107
Raczyńska ED, Kosińska W, Ośmiałowski B, Gawinecki (2005) Chem Rev 105:3561–3612
Grabowski SJ, Leszczynski J (eds) (2006) The hydrogen bonding – new insights, Springer, Berlin, pp 487–512
Gilli G, Gilli P (2009) The Nature of the Hydrogen Bond. Oxford University Press
Sanz P, Mó O, Yanez M, Elguero J (2008) Chem Eur J 14:4225–4232
Sanz P, Mó O, Yanez M, Elguero J (2009) Phys Chem Chem Phys 11:762–769
Filarowski A, Koll A, Sobczyk L (2009) Curr Org Chem 13:172–193, and references cited herein
Nedeltcheva D, Antonov L, Lycka A, Damyanova B, Popov S (2009) Curr Org Chem 13:217–239, and references cited herein
Sheikhshoaie I, Fabian WMF (2009) Curr Org Chem 13:149–171, and references cited herein
Buemi G, Zuccarello F, Venuvanalingam P, Ramalingam M (2000) Theor Chem Acc 104:226–234
Musin RN, Mariam YH (2006) J Phys Org Chem 19:425–444
Bouchy A, Rinaldi D, Rivail J-L (2004) Int J Quantum Chem 96:237–281
Lenain P, Mandado M, Mosquera RA, Bultinck P (2008) J Phys Chem A 112:10689–10696
Raissi H, Moshfeghi E, Jalbout AF, Hosseini MS, Fazli M (2007) Int J Quantum Chem 107:1835–1845
Kania L, Kamieńska-Trela K, Witkowski M (1983) J Mol Struct 102:1–17
Dąbrowski J, Kamieńska-Trela K (1976) J Am Chem Soc 98:2826–2834
Dąbrowski J, Kamieńska-Trela K, Kania L (1976) Tetrahedron 32:1025–1029
Dudek GO, Holm RH (1962) J Am Chem Soc 84:2691–2696
Dudek GO, Dudek EP (1966) J Am Chem Soc 88:2407–2412
Tayyari SF, Raissi H, Tayyari F (2002) Spectrochim Acta A 58:1681–1695
Dudek GO, Holm RH (1961) J Am Chem Soc 83:2099–2104
Brown NMD, Nouhebal DC (1968) Tetrahedron 24:5655–5664
Martin R-F, Jamsosis GA, Martin BB (1961) J Am Chem Soc 83:73–75
Rybarczyk-Pirek AJ, Grabowski SJ, Malecka M, Nawrot-Modranka J (2002) J Phys Chem A 106:11956–11962
Nowroozi AR, Raissi H, Farzad F (2005) J Mol Struct THEOCHEM 730:161–169
Raczyńska ED (2005) Pol J Chem 79:1003–1006
Krygowski TM, Wozniak K, Anulewicz R, Pawlak D, Kolodziejski W, Grech E, Szady A (1997) J Phys Chem 101:9399–9404
Filarowski A, Koll A, Głowiak T, Majewski E, Dziembowska T (1998) Ber Bunsenges Phys Chem 102:393–402
Filarowski A, Koll A, Głowiak T (2002) J Mol Struct 615:97–108
Filarowski A, Kochel A, Cieślik K, Koll A (2005) J Phys Org Chem 18:986–993
Raczynska ED, Krygowski TM, Zachara JE, Osmialowski B, Gawinecki R (2005) J Phys Org Chem 18:892–897
Grabowski SJ, Sokalski WA, Leszczynski J (2006) J Phys Chem A 110:4772–4779
Grabowski SJ, Sokalski WA, Dyguta E, Leszczynski J (2006) J Phys Chem B 110:6444–6446
Palusiak M, Simon S, Sola M (2006) J Org Chem 110:5875–5822
Palusiak M, Krygowski TM (2007) Chem Eur Chem 13:7996–8006
Zubatyuk RI, Volovenko YM, Shishkin OV, Gorb L, Leszczynski J (2007) J Org Chem 72:725–735
Filarowski A, Kochel A, Kluba M, Kamounah F (2008) J Phys Org Chem 21:939–944
Kluba M, Lipkowski P, Filarowski A (2008) Chem Phys Lett 463:426–430
Karabiyik H, Petek H, Iskeleli NO, Albayrak C (2009) Struct Chem 20:903–910
Karabiyik H, Petek H, Iskeleli NO, Albayrak C (2009) Struct Chem 20:1055–1065
Filarowski A, Majerz I (2008) J Phys Chem 112:3119–3126
Krygowski TM (1993) J Chem Inf Comput Sci 33:70–78
Bader RF (1990) Atoms in molecules: a quantum theory. Oxford University Press, New York
Koch U, Popelier PL (1995) J Phys Chem 99:9747–9754
Krygowski TM, Cyrański MK (2001) Chem Rev 101:1385–1420
Sobczyk L, Grabowski SJ, Krygowski TM (2005) Chem Rev 105:3513–3560
Filarowski A, Kochel A, Cieslik K, Koll A (2005) J Phys Org Chem 18:986–993
Raczyńska ED, Krygowski TM, Zachara JE, Ośmiałowski B (2005) J Phys Org Chem 18:892–897
Korth H-G, de Heer MI, Mulder R (2002) J Phys Chem A 106:8776–8789
Krygowski TM, Zachara JE, Szatylowicz H (2005) J Phys Org Chem 18:110–114, and references cited herein
Frisch MJ, Trucks GW, Schlegel HB, Scuseria GE, Robb MA, Cheeseman JR, Montgomery JA, Vreven T, Kudin KN, Burant JC, Millam JM, Iyengar SS, Tomasi J, Barone V, Mennucci B, Cossi M, Scalmani G, Rega N, Petersson GA, Nakatsuji H, Hada M, Ehara M, Toyota K, Fukuda R, Hasegawa J, Ishida M, Nakajima T, Honda Y, Kitao O, Nakai H, Klene M, Li X, Knox JE, Hratchian HP, Cross JB, Bakken V, Adamo C, Jaramillo J, Gomperts R, Stratmann RE, Yazyev O, Austin AJ, Cammi R, Pomelli C, Ochterski JW, Ayala PY, Morokuma K, Voth GA, Salvador P, Dannenberg JJ, Zakrzewski VG, Dapprich S, Daniels AD, Strain MC, Farkas O, Malick DK, Rabuck AD, Raghavachari K, Foresman JB, Ortiz JV, Cui Q, Baboul AG, Clifford S, Cioslowski J, Stefanov BB, Lui G, Liashenko A, Piskosz P, Komaromi I, Martin RL, Fox DJ, Keith T, Al-Laham MA, Peng CY, Nanayakkara A, Challacombe M, Gill PMW, Johnson B, Chen W, Wong MW, Gonzalez C, Pople JA (2004) Gaussian 03, Revision B.03. Gaussian Inc, Wallingford, CT
McLean AD, Chandler GS (1980) J Chem Phys 72:5639–5648
Krishnan R, Binkley JS, Seeger R, Pople JA (1980) J Chem Phys 72:650–654
Clark T, Chandrasekhar J, Spitznagel GW, Schleyer PvR (1983) J Comput Chem 4:294–301
Frisch MJ, Pople JA, Binkley JS (1984) J Chem Phys 80:3265–3269
Møller C, Plesset MS (1934) Phys Rev 46:618–622
Biegler-König J, Schönbohm D, Bayles D (2001) J Comput Chem 22:545–559
Krygowski TM, Cyranski M, Czarnoski Z, Hafelinger G, Katritzky A (2000) Tetrahedron 56:1783–1796
Hansch C, Leo A, Taft RW (1991) Chem Rev 91:165–195
Fores M, Duran M, Sola M (2000) Chem Phys 260:53–64
Palomar J, De Paz JLG, Catalan J (2000) J Phys Chem A 104:6453–6463
Leffler JE (1953) Science 117:340–341
Hammond GS (1955) J Am Chem Soc 77:334–338
Espinosa E, Alkorta I, Elguero J, Molins E (2002) J Chem Phys 117:5529–5542
Filarowski A, Majerz I, Martyniak A (2010) J Phys Chem A in preparation
Krygowski TM, Zachara-Horeglad JE, Palusiak M (2010) J Org Chem 75:4944–4949
Acknowledgments
The authors acknowledge the Wrocław Center for Networking and Supercomputing for generous computer time. P.L. acknowledges the Wrocław University of Technology for financial support.
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Open Access This is an open access article distributed under the terms of the Creative Commons Attribution Noncommercial License (https://creativecommons.org/licenses/by-nc/2.0), which permits any noncommercial use, distribution, and reproduction in any medium, provided the original author(s) and source are credited.
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Martyniak, A., Lipkowski, P., Boens, N. et al. Electron-topological, energetic and π-electron delocalization analysis of ketoenamine-enolimine tautomeric equilibrium. J Mol Model 18, 257–263 (2012). https://doi.org/10.1007/s00894-011-1075-7
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DOI: https://doi.org/10.1007/s00894-011-1075-7