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Basicities of primary arylamines and calculated amine nitrogen electronic charges

Basicidades de arilaminas primárias e cargas eletrônicas calculadas do nitrogênio amínico

Abstracts

Mülliken charges on nitrogen atoms were calculated for several arylamines, utilizing the AM1 Quantum Chemistry method, relating their values to experimental amine pKa . Direct relation between pKa and nitrogen charges was found. The amines energies of protonation, calculated by the same method, also correlate directly with these charges.

Arylamines; basicity; N Mülliken charge; AM1


Foram calculadas as cargas de Mülliken sobre os átomos de nitrogênio para diversas arilaminas, empregando-se para tal o método AM1 da Química Quântica. Tais cargas foram relacionadas com os valores experimentais dos pKa das aminas. Foi obtida uma relação direta entre pKa e carga dos átomos de nitrogênio. As energias de protonação das aminas, calculadas pelo mesmo método, também se correlacionam diretamente com aquelas cargas.

Arilaminas; basicidade; cargas de Mülliken; AM1


Basicities of primary arylamines and calculated amine nitrogen electronic charges

Sérgio Roberto de Andrade LEITE* * Instituto de Química - Universidade Estadual Paulista - 14801-970 - Araraquara - SP - Brazil.

ABSTRACT: Mülliken charges on nitrogen atoms were calculated for several arylamines, utilizing the AM1 Quantum Chemistry method, relating their values to experimental amine pKa . Direct relation between pKa and nitrogen charges was found. The amines energies of protonation, calculated by the same method, also correlate directly with these charges.

KEYWORDS: Arylamines; basicity ; N Mülliken charge; AM1.

Introduction

The primary amines are organic bases with general formula RNH2 , that react with the proton according to the equation:

RNH2 + H+ RNH+3

If R is an aryl group, then the amine is an aromatic amine or arylamine, represented by ArNH2.

The logarithm of the dissociation constant of the protonated arylamine, pKa , is defined as

It increases with the amine basicity as the acidity of the protonated amine decreases. On the other hand, it is reasonable to suppose that the greater the electronic charge on the amine nitrogen the stronger will be its basicity.

Quantum Chemistry methods offer the possibility of calculating atomic charges. There are several ways to define them, and the Mlliken atomic charges are the most commonly used in molecular orbital theory. These quantities are not "observables" in the Quantum Mechanics sense, and have only an approximate relation to experiment. Their values are sensitive to the semi-empirical calculation method or to the basis set of an ab initio procedure. But, values obtained by the same method for similar chemical groups in related molecules, can be of significance for comparative purposes.

Calculations have been performed for atomic charges on nitrogen for several arylamines, utilizing the AM1 semi-empirical Quantum Chemistry method. These results are compared with the trend of experimental pKa values and of calculated protonation energies.

We have chosen an ensemble of arylamines chemically very similar in order to test the sensitivity of the method . All of them, except aniline, have fused benzene rings. Different quantum model chemistry methods have also been tested for the same purpose. The method which resulted in the best correlation between nitrogen charge and pKa, was utilized for further investigation on this matter.

Methods

The amine structures were initially optimized by Molecular Mechanics calculation with a modified MM2 force field.1,2,4 A trial of the electronic calculation method more suitable to our purpose was carried out by single point calculation for the resulting structures using the following Quantum Chemistry methods: a) Semi-empirical: Extended Hückel, EH,10 and the SCF techniques CNDO/2,12,13 INDO,13 MINDO/3,3 MNDO6 and AM1,7 ; b) Ab initio procedure with a minimal STO-3G basis set.5,9,14

After this initial search, the structures were reoptimized by the AM1 Quantum Chemistry method and the Mülliken charges of the amine nitrogens and the protonation energies were calculated by the same method. These charges and energies were correlated one with other and both with the experimental pKa values. The protonation energy was expressed as:

DE = EAH+ – ( EA + EH+)

Where AH+ protonated amine A amine in the base form H+ proton Since EH+ = 0 , DE = EAH+ – EA = f ( pKa ) (Figure 2)

The amines pKa were obtained from the literature.8

Results and discussion

Table 1 shows the net charges on amine nitrogens, as obtained by various calculation methods, and the amines pKa. First, we observe that the charges vary according to the method, confirming the lack of significance of their absolute values. On the other hand, the results obtained by a given method may be compared among themselves and vary slightly from one compound to another. The sensibility to differentiate the nitrogen charge among compounds of different amine pKa varies according to the method, and this was one important criterion to the method choice.

The difference expressed in percentages between the extreme N charge values calculated by each method are as follows: EH 3.8% , CNDO/2 1.6% , INDO 3.1% , MINDO/3 10.0% , MNDO 5.0% , AM1 4.8% and ab initio (minimal basis set) 1.4% . The ab initio and CNDO/2 methods show little sensibility to detect amine nitrogen charge variation in function of aryl group. By this point of view, the ab initio calculation with the minimal basis set STO-3G gave the poorest result, showing very little charge variation and several identical N charge values for different arylamines. Even the semi-empirical single-electron potential Extended Hückel method shows a better result. This points for the necessity of more sofisticated basis sets utilization for having more reliable ab initio calculations results. More sensible methods are MINDO/3, AM1 and MNDO. On the other hand, the AM1 method gave a better correlation coefficient (R) for the individual data points in relation to the line fitted to this plot, under linear regression calculation of pKa= f ( N charge ) (Table 2). This result, summed to the fact that the AM1 method is the more precise semi-empirical Quantum Chemical method available, have suggested its choice for the present work.

Figure 1 shows the amines pKa in function of their AM1 calculated N Mülliken charges. The points were fitted to a linear function (top) , with R = 0.9515, and to a second order polynomial function (bottom ), with R = 0.9770 , which is better. The pKa increases with N charge, as was expected. So, the Mülliken negative charge value on every atom of the molecule can be related with electron density distribution, and a high electron density site or an intense local negative charge is a protonic affinity place. In other words, it is a high basicity center, manifested by a high pKa value.


The calculated in vacuum energies of protonation absolute values grow with the amine pKa or, which has the same meaning, with the amine basicities. Figure 2 shows the linearity between both, and Figure 3 the analogous (like the pKa) behavior of calculated protonation energies against the amines nitrogen charges. This coherent result confirms the utility of the AM1 method for the comparison among electronic amine properties calculated in vacuum and their experimental pKa values in solution.



A doubt may arise as to the correctness of the comparison between the pKa value, measured in solution, and a figure calculated for the molecule in vacuum. The protonation equilibrium constant in vacuum and in solution may vary depending on the difference between the solvatation energy of the protonated and non-protonated species. We have performed an AM1 calculation of the arylamines for a simulated water medium , in which each amine would be surrounded by 43 TIP3P water molecules models.11 Hydration energy was calculated as the difference between the total energy of the amine and water together and separately for each other. The hydration energy has changed 43% in average with protonation. Otherwise, the energy of protonation, calculated also by AM1 method, and directly related with the basicity, has grown only 7.1% in average with hydration, showing that in this case it is less sensible to the medium parameters. Protonation energy relates directly to the equilibrium constant of the protonation reaction, namely, to its basicity constant. The analogous behavior of the protonation energy calculated in vacuum and the experimental pKa value in solution, when compared mutually and both with N charges, indicates the validity of predictions made.

In conclusion, it is possible to correlate the calculated electronic charge on amine nitrogen with the amine basicity. For the studied arylamines, whose pKa varie little from one to the other, the nitrogen charges also do not show major changes. Hence, although sensibility of the method is not very good, it may be considered as useful for semi-quantitative predictions.

Acknowledgments

We are grateful to Fapesp (Brazilian Agency) for the financial support.

LEITE, S. R. A. Basicidades de arilaminas primárias e cargas eletrônicas calculadas do nitrogênio amínico. Ecl. Quím. (São Paulo), v.23, p.71-80, 1998.

RESUMO: Foram calculadas as cargas de Mülliken sobre os átomos de nitrogênio para diversas arilaminas, empregando-se para tal o método AM1 da Química Quântica. Tais cargas foram relacionadas com os valores experimentais dos pKa das aminas. Foi obtida uma relação direta entre pKa e carga dos átomos de nitrogênio. As energias de protonação das aminas, calculadas pelo mesmo método, também se correlacionam diretamente com aquelas cargas.

PALAVRAS-CHAVE: Arilaminas; basicidade; cargas de Mülliken; AM1.

References

1. ALLINGER, N. L. Conformational analysis. 130. MM2. A hydrocarbon force field utilizing V1 and V2 torsional terms. J. Am. Chem. Soc., v.99, p.8127, 1977.

2. ALLINGER, N. L., YUH, Y. H. Quantum Chemistry Program Exchange; Bloomington, IN ; Program # 395 .

3. BAIRD, N. C., DEWAR, M. J. S. Ground states of s-bonded molecules. IV. The MINDO method and its application to hydrocarbons. J. Chem. Phys., v.50, p.1262, 1969.

4. BURKERT, U., ALLINGER, N. L. Molecular Mechanics, ACS Monograph 177, 1982

5. COLLINS, J. B., SCHLEYER, P. V., BINKLEY, J. S., POPLE, J. A. Self-consistent molecular orbital methods. XVII. Geometries and binding energies of second-row molecules. A comparison of three basis sets. J. Chem. Phys., v.64, p.5142, 1976.

6. DEWAR, M. J. S., McKEE, M. L., Ground states of molecules. 41. MNDO results for molecules containing boron. J. Am. Chem. Soc., v.99, p. 5231, 1977.

7. DEWAR, M. J. S., ZOEBISCH, E. G. ; HEALY, E. F., STEWART, J. J. P. AM1: a new general purpose quantum mechanical molecular model. J. Am. Chem. Soc., v.107, p. 3902, 1985.

8. ELLIOTT, J. J., MASON, S. F. The heats and entropies of ionisation of some aromatic and N-heteroaromatic amines. J. Chem. Soc., p. 2352 , 1959.

9. HEHRE, W. J., STEWART, R. F., POPLE, J. A. Self-consistent molecular-orbital methods. I. Use of gaussian expansions of Slater-type atomic orbitals. J. Chem. Phys., v.51, p.2657, 1969.

10. HOFFMANN, R. An extended Hückel theory. I. Hydrocarbons. J. Chem. Phys., v. 39, p.1397, 1963.

11. JORGENSEN, W.L., CHANDRASEKHAR, J., MADURA, J.D. Comparison of simple potential functions for simulating liquid water. J. Chem. Phys., v. 79, p. 926, 1983.

12. POPLE,J. A., SANTRY, D. P., SEGAL, G. A. Aproximate self-consistent molecular orbital theory. I. Invariant procedures. J. Chem. Phys., v. 43, p. S129, 1965.

13. POPLE, J. A., BEVERIDGE, D. L. Approximate Molecular Orbital Theory; McGraw- Hill ; New York, 1970.

14. STEWART, R. F. Small gaussian expansions of Slater-type orbitals. J. Chem. Phys., v. 52, p. 431, 1970.

Recebido em 21.11.1997.

Aceito em 24.11.1997.

  • *
    Instituto de Química - Universidade Estadual Paulista - 14801-970 - Araraquara - SP - Brazil.
  • Publication Dates

    • Publication in this collection
      05 May 2000
    • Date of issue
      1998

    History

    • Accepted
      24 Nov 1997
    • Received
      21 Nov 1997
    Fundação Editora da Universidade Estadual Paulista Júlio de Mesquita Filho - UNESP Instituto de Química / UNESP, 14801-970 Araraquara SP Brazil, Tel.: +55 16 3301-9636/3301-9631 - São Paulo - SP - Brazil
    E-mail: ecletica@iq.unesp.br