Abstract
Solid-state MBz compounds, where M stands for bivalent Mn, Fe, Co, Ni, Cu and Zn and Bz is benzoate, have been synthesized. Simultaneous thermogravimetry and differential thermal analysis (TG-DTA), differential scanning calorimetry (DSC), infrared spectroscopy and complexometry were used to characterize and to study the thermal behaviour of these compounds. The procedure used in the preparation of the compounds via reaction of basic carbonates with benzoic acid is not efficient in eliminating excess acid. However the TG-DTA curves permitted to verify that the binary compounds can be obtained by thermosynthesis, because the benzoic acid can be eliminated before the thermal decomposition of these compounds. The results led to information about the composition, dehydration, thermal stability, thermal decomposition and structure of the isolated compounds. On heating, these compounds decompose in two (Mn, Co, Ni, Zn) or three (Fe, Cu) steps with formation of the respective oxide (Mn3O4, Fe2O3, Co3O4, NiO, CuO and ZnO) as final residue. The theoretical and experimental spectroscopic studies suggest a covalent bidentate bond between ligand and metallic center.
bivalent transition metals; benzoate; thermal behaviour
ARTIGO
Synthesis, characterization and thermal behaviour of solid-state compounds of benzoates with some bivalent transition metal ions
Adriano B. Siqueira; Elias Y. Ionashiro; Cláudio T. de Carvalho; Gilbert Bannach; Emanuel C. Rodrigues; Massao Ionashiro* * e-mail: massaoi@iq.unesp.br
Instituto de Química, Universidade Estadual Paulista, CP 355, 14801-970 Araraquara - SP, Brazil
ABSTRACT
Solid-state MBz compounds, where M stands for bivalent Mn, Fe, Co, Ni, Cu and Zn and Bz is benzoate, have been synthesized. Simultaneous thermogravimetry and differential thermal analysis (TG-DTA), differential scanning calorimetry (DSC), infrared spectroscopy and complexometry were used to characterize and to study the thermal behaviour of these compounds. The procedure used in the preparation of the compounds via reaction of basic carbonates with benzoic acid is not efficient in eliminating excess acid. However the TG-DTA curves permitted to verify that the binary compounds can be obtained by thermosynthesis, because the benzoic acid can be eliminated before the thermal decomposition of these compounds. The results led to information about the composition, dehydration, thermal stability, thermal decomposition and structure of the isolated compounds. On heating, these compounds decompose in two (Mn, Co, Ni, Zn) or three (Fe, Cu) steps with formation of the respective oxide (Mn3O4, Fe2O3, Co3O4, NiO, CuO and ZnO) as final residue. The theoretical and experimental spectroscopic studies suggest a covalent bidentate bond between ligand and metallic center.
Keywords: bivalent transition metals; benzoate; thermal behaviour.
INTRODUCTION
Benzoic acid and some of their derivatives have been used as conservant, catalyst precursors polymers, in pharmaceutical industries, beyond other applications. A survey of literature shows that the complexes of rare earth and d-block elements with benzoic acid and some of its derivatives have been investigated in aqueous solutions and in the solid state.
In aqueous solutions, the publications reported the thermodynamics of complexation of lanthanides by some benzoic acid derivatives1, the spectroscopic study of trivalent lanthanides with several carboxylic acids including benzoic acid2, the influence of pH, surfactant and synergic agent on the luminescent properties of terbium chelates with benzoic acid derivatives3, the thermodynamic of complexation of lanthanides by benzoic and isophthalic acids4 and the synthesis, crystal structure and photophysical and magnetic properties of dimeric and polymeric lanthanide complexes with benzoic acid and their derivatives5.
In the solid state the publications reported the vibrational and electronic spectroscopic study of lanthanides and effect of sodium on the aromatic system of benzoic acid6; the thermal and spectral behaviour on solid compounds of m-methoxybenzoate with rare earth elements7; the reaction of bivalent copper, cobalt and nickel with 3-hidroxy-4-methoxy and 3-methoxy-4-hidroxybenzoic acids and a structure for these compounds has been proposed on the basis of spectroscopic and thermogravimetric data8; the thermal decomposition of thorium salts of benzoic and 4-methoxybenzoic acids in air atmosphere9; the thermal and spectral behaviour on solid compounds of 5-chloro-2-methoxybenzoate with rare earth and d-block elements10-13; the synthesis and characterization of 2,3-dimethoxybenzoates of heavy lanthanides and yttrium14; the thermal studies on solid compounds of phenyl substituted derivates of benzylidenepyruvates with several metal ions15,16; the spectral and magnetic studies of 2-chloro-5-nitrobenzoates of rare earth elements17 and thermal behaviour of solid state 4-methoxybenzoates of some bivalent transition metal ions18.
In an endeavour to extend the literature works, the present publication deals with the synthesis of Mn (II), Fe (II), Co (II), Ni (II), Cu (II) and Zn (II) benzoates, studied by means of infrared spectroscopy, simultaneous thermogravimetry and differential thermal analysis (TG-DTA), differencial scanning calorimetry (DSC) and other methods of analysis. The results permitted to obtain information concerning the structure, thermal stability and thermal decomposition of these compounds.
EXPERIMENTAL
The benzoic acid, C6H5COOH (HBz) 99.9% was obtained from MERCK. Hydrated basic carbonates of Mn (II), Co (II), Ni (II), Cu (II) and Zn (II) were prepared by adding slowly with continuous stirring satured sodium carbonate solution to the corresponding metal chloride or sulphate for copper solutions until total precipitation of the metal ions. The precipitates were washed with distilled water until elimination of chloride or sulphate ions (qualitative test with AgNO3/HNO3 solution for chloride ions or BaCl2 solution for sulphate ions) and maintained in aqueous suspension.
Solid state Mn (II), Co (II), Ni (II), Cu (II) and Zn (II) compounds were prepared by mixing the corresponding metal basic carbonates with benzoic acid, in slight excess. The aqueous suspension was heated slowly up to near ebullition, until total neutralization of the respective basic carbonates. The resulting solutions after cooled were maintained in an ice bath to recrystallize the acid in excess and filtered through a Whatman nº 40 filter paper. Thus, the aqueous solutions of the respective metal benzoates were evaporated to near dryness in a water bath and kept in a desiccator over phosphorous pentoxide. The same procedure to synthesize the iron (II) compound was unsucessful, due to oxidation reaction of Fe (II) to Fe (III) during the washing of the precipitate of basic carbonate of Fe (II), even by using solutions and washing water purged with nitrogen gas.
The iron (II) benzoate was synthesized by adding solution of sodium benzoate (pH=9.5) to iron (II) sulphate solution, both purged with nitrogen gas. No precipitate was observed during the addition of sodium benzoate; however the precipitation occurred after five day when the solution satured with N2 was maintained in a freezer at about 6 ºC.
In the solid-state compounds, metal ions, hydration water and benzoate contents were determined from TG curves. The metal ions were also determined by complexometry with standard EDTA solution19,20 after igniting the compounds to the respective oxides and their dissolution in hydrochloric acid solution.
Infrared spectra for sodium benzoate as well as for its metal-ion compounds were run on a Nicolet model Impact 400 FT-IR instrument, within the 4000-400 cm-1 range. The solid samples were pressed into KBr pellets.
Simultaneous TG-DTA curves were obtained with thermal analysis system model SDT 2960 from TA Instruments. The purge gas was a dry air flow of 100 mL min-1. A heating rate of 20 ºC min-1 was adopted with samples weighing about 7 mg. Platinum crucibles were used for TG-DTA.
DSC curves were obtained with thermal analysis systems model DSC 25 from Mettler Toledo. The purge gas was a dry air flow of 100 mL min-1. A heating rate of 20 ºC min-1 was adopted with samples weighing about 5 mg. Aluminium crucibles, with perforated cover, were used for DSC.
Computational strategy
Calculation of theoretical infrared spectrum of nickel benzoate has been necessary to evaluate the structure and wave function computed by the ab initio SCF Hartree-Fock-Roothan method21 using a split valence (3-21g) basis set22,23. The performed molecular calculations in this work were done by using the Gaussian 98 routine23 and the hardware IBM power 3. The geometry optimization was carried out without any constraints. The molecule of benzoate contains rings with conformational flexibility, and all variables optimized. The optimization proceeded more uniformly when all variables were optimized.
RESULTS AND DISCUSSION
Preliminary studies based on TG-DTA curves and infrared spectra, permitted to verify that the synthesized compounds, except iron, were obtained contaminated. The TG-DTA curves also show that the contamination is evolved before the thermal decomposition of the binary compounds. Thus, sample of these compounds were heated in a long test glass tube, and dehydration for manganese and nickel compounds and sublimation for all the compounds were observed. The sublimated material was identified as benzoic acid, m.p. 121 ºC (found); 122 ºC (literature)24.
The presence of benzoic acid in the compounds must be due to the aggregation phenomenon provoked by the increase of the solubility of benzoic acid in benzoate solution, and it is not recrystallized even an ice bath. Therefore, the procedure used to eliminate the acid in excess is not efficient. This behaviour had already been observed in the 3-methoxybenzoate of the same metal ions, except copper compound25.
Therefore these compounds were heated up to 260 (Mn), 140 (Co), 230 (Ni), 210 (Cu) and 140 ºC (Zn), as indicated by the TG-DTA curves and so to obtain binary compounds free from benzoic acid.
Infrared spectroscopic data on benzoate and their compounds with bivalent ions considered in this work are shown in Table 1. The investigation was focused mainly within 1700-1400 cm-1 range because this region is potentially most informative to assign coordination sites. In sodium benzoate, strong band at 1551 cm-1 and a medium intensity band located 1414 cm-1 are attributed to the anti-symmetrical and symmetrical frequencies of the carboxylate groups, respectively6. In all the compounds considered in this work the symmetrical and anti-symmetrical vibrations of the COO- groups when compared with the sodium salt, suggesting that the compounds have a covalent bidentate bond.
The theoretical infrared spectrum of the Ni(Bz)2 was calculated by the using an harmonic field27 and the obtained frequencies were not scaled. The geometry optimization was computed by the optimized algorithm of Berny27. The obtained geometry from calculations is presented in Table 2.
The theoretical infrared spectrum of the Ni(Bz)2 (electronic state 1A) was obtained with frequency values (cm-1), relative intensities, assignments and description of vibrational modes. The theorical frequency, assignments and description was visualized by using graphic software Molden 4.2 for Linux28. It was compared with the experimental infrared spectrum of the NiBz2.
A comparative analysis between the experimental and theoretical spectrum permitted to verify that: (a) the first assignment shows a strong contribution at 1552 cm-1 suggesting a nasym(COO-) assignment, while the theoretical results show the corresponding peak at 1562 cm-1 with discrepancies of 0.64%; (b) the second assignment shows a strong contribution at 1435 cm-1 suggesting a nsym(COO-) assignment, while the theoretical results show the corresponding peak at 1487 cm-1 with discrepancies of 3.6%. The theoretical and experimental data suggesting that compounds considered in this work have a covalent bidentate bond.
Thus, Table 3 presents the analytical and thermoanalytical (TG) results for the prepared compounds by thermosynthesis exception the iron compound, Fe(Bz)2.0.5H2O, from which the general formula M(Bz)2 can be established, where M=Mn, Ni, Co, Cu, Zn and Bz = benzoate.
The thermal behaviour of the compounds is heavily dependent on the nature of the metal ion and so the features of each of these compounds are discussed individually.
Manganese compound. The TG-DTA and DSC curves are shown in Figure 1(a). The TG curve shows mass losses in two overlapping steps and thermal events corresponding to these losses or physical phenomenon. The small endothermic peak at 260 (DTA) or 265 ºC (DSC) is attributed to the fusion. The mass loss, between 260 and 500 ºC, corresponding to the exothermic peak at 470 (DTA) or 440 and > 500 ºC (DSC) is attributed to the oxidation of organic matter. The total mass loss up to 500 ºC is in agreement with the formation of Mn3O4, as final residue (Calcd = 74.34%; TG = 74.31%).
Iron compound. The TG-DTA and DSC curves are shown in Figure 1(b). These curves show mass losses in three steps between 60 and 470 ºC and thermal events corresponding to these losses. The first mass loss observed between 60-172 ºC is due to dehydration with loss of 1H2O (Calcd = 2.93%; TG = 2.75%); as the dehydration occurs through a slow process, the absorbed heat in this step is probably not enough to produce the endothermic peak. The thermal decomposition of the anhydrous compound occurs in two steps between 172275ºC, and 275-470ºC, with losses of 9.66 and 61.39%, respectively, corresponding to the exothermic peaks at 423.5 and 448 ºC. The profiles of the TG and DTA curves, in the last step show that the oxidation of organic matter is accompanied by combustion. The total mass loss up to 470 ºC is in agreement with the formation of Fe2O3, as final residue (Calcd. = 73.99%; TG. = 73.81%).
Cobalt compound. The TG-DTA and DSC curves are shown in Figure 1(c). The TG curve also shows that the thermal decomposition occurs in two overlapping steps, and thermal events due to these losses or physical phenomenon. The endothermic peaks at 275 and 295 ºC (DSC) are attributed to fusion and evaporation of the compound, respectively. The mass loss between 300 and 480 ºC, corresponding to the exothermic peak at 480 ºC (DTA) or the exotherm with three peaks at 430, 480, and 590 ºC (DSC) is ascribed to the oxidation of organic matter. The profile of the TG-DTA curves in this step show that the oxidation of the organic matter occurs with combustion. The total mass loss up to 480 ºC is in agreement with the formation of Co3O4, as final residue (Calcd = 73.35%; TG = 73.26%).
Nickel compound. The TG-DTA and DSC curves are shown in Figure 1(d). These curves show mass losses in two overlapping steps and thermal events corresponding to these losses. The mass loss, between 230 and 440 ºC, corresponding to the exothermic peak at 440 ºC (DTA) and several thermal events between 300 and 550 ºC (DSC) are attributed to the oxidation of the organic matter. The profiles of the TG-DTA curves in this step also show that the oxidation of the organic matter occurs with combustion. The total mass loss up to 440 ºC is in agreement with the formation of NiO, as final residue (Calcd = 75.18%; TG = 75.15%).
Copper compound. The TG-DTA and DSC curves are shown in Figure 1(e). These curves show that the cooper compound is stable up to 280 ºC and above this temperature up to 400 ºC, the TG curve shows that the mass loss occurs in three overlapping steps, being the first one corresponding to the sharp endothermic peak at around 295 ºC (DTA, DSC) attributed to the presence of both unreacted copper benzoate and degradation products and this temperature represents the melting point of the compound when assessed in an oxidative atmosphere. The last two steps corresponding to the exotherm with the peaks at 385 and 400 ºC (DTA) or the exotherm between 370 and 550 ºC (DSC) is ascribed to the oxidation of the organic matter. In the last step the TG-DTA also show that the oxidation occurs with combustion. The total mass loss up to 400 ºC is in agreement with the formation of CuO as final residue (Calcd. = 73.99%); TG = 74.01%).
Zinc compound. The TG-DTA and DSC curves are shown in Figure 1(f). The mass loss that occurs between 280 and 550 ºC, corresponding to the exothermic peak at 520 ºC (DTA) or 525 ºC (DSC) is attributed to the oxidation of organic matter. The endothermic peak at 325 ºC (DTA) is due to the fusion accompanied by thermal decomposition and the endothermic peak at 340 ºC (DSC) is due to the fusion without thermal decomposition. This disagreement is because the DSC and the TG-DTA curves were not obtained in the same conditions. The total mass loss up to 550 ºC is in agreement with the formation of ZnO as final residue (Calcd.=73.55%; TG = 73.77%).
CONCLUSION
The TG-DTA curves, infrared spectra and chemical analysis, permitted to verify the presence of benzoic acid in all the synthesized compounds, showing that the procedure used to eliminate the benzoic acid in excess is not efficient.
The TG-DTA, also permitted to verify that the binary compounds can be obtained by thermosynthesis, because the benzoic acid is eliminated before the thermal decomposition of these compounds.
The theoretical and experimental infrared spectroscopic data suggest that the benzoate acts as a bidentate ligand towards the metal ions considered in this work.
The TG-DTA and DSC provided previously unreported information about the thermal stability and thermal decomposition of these compounds.
ACKNOWLEDGEMENTS
The authors thank FAPESP, CNPq and CAPES Foundations (Brazil) for financial support and computational facilities of IQ-UNESP and CENAPAD-UNICAMP.
Recebido em 10/11/05; aceito em 25/5/06; publicado na web em 24/10/06
- 1. Yun, S. J.; Kang, S. K.; Yun, S. S.; Thermochim. Acta 1999, 331, 13.
- 2. Wang, Z. M.; van de Burgt, L. J.; Choppin, G. R.; Inorg. Chim. Acta 1999, 293, 167.
- 3. Arnaud, N.; Georges J.; Analyst 2000, 125, 1487.
- 4. Choppin, G. R.; Bertrand P. A.; Hasegawa, Y.; Rizalla, N.; Inorg. Chem 1982, 21, 3722.
- 5. Lam, A. W. H.; Wang, W. T.; Gao, S.; Wen, G.; Zhang, X. X.; Eur. J. Inorg. Chem. 2003, 1, 149.
- 6. Lewandowski, W.; Baranska, H.; J. Raman Spectrosc. 1986, 17, 17.
- 7. Makushova, G. N.; Pirkes, S. B.; Russ. J. Inorg. Chem. 1987, 32, 876.
- 8. Glowiak, T.; Kozlowski, H.; Erre, L. S.; Gulinati, B.; Micera, G.; Pozzi A.; Brunni, S.; J. Coord. Chem 1992, 25, 75 .
- 9. Brzyska, W.; Karasinski, S.; J. Therm. Anal. 1993, 39, 429.
- 10. Ferenc, W.; Bocian, B.; J. Therm. Anal. Cal 2000, 831, 62.
- 11. Bocian , B.; Czajka, B.; Ferenc, W.; J. Therm. Anal. Calorim. 2001, 66, 729.
- 12. Czajka, B.; Bocian, B.; Ferenc, W.; J. Therm. Anal. Calorim. 2002, 67, 631.
- 13. Ferenc, W.; Bocian, B.; J. Therm. Anal. Calorim. 2003, 74, 521.
- 14. Ferenc, W.; Walkow-Dziewulska, A.; J. Therm. Anal. Calorim. 2003, 71, 375.
- 15. Fernandes, N. S.; Carvalho Filho, M. A. S.; Melios, C. B.; Ionashiro, M.; J. Therm. Anal. Calorim. 2003, 73, 307.
- 16. Fernandes, N. S.; Carvalho Filho, M. A. S.; Mendes, R. A.; Melios, C. B.; Ionashiro, M.; J. Therm. Anal. Calorim. 2004, 76, 193.
- 17. Ferenc, W.; Bocian B.; Walków-Dziewulska, A.; J. Therm. Anal. Cal. 2004, 76, 179.
- 18. Rodrigues, E. C.; Siqueira, A. B.; Ionashiro, E. Y.; Bannach, G.; Ionashiro, M.; J Therm. Anal. Calorim. 2005, 79, 323.
- 19. Flaschka, H. A.; EDTA Titrations, Pergamon Press: Oxford, 1964.
- 20. De Oliveira, C. N.; Ionashiro, M.; Graner, C. A. F.; Ecl. Quim 1985, 10, 7.
- 21. Roothan, C. C. J.; Rev. Mod. Phys 1951, 23, 69.
- 22. Dobbs, K. D.; Hehre, W. J.; J. Comput. Chem. 1987, 8, 861.
- 23. Dobbs, K. D.; Hehre, W. J.; J. Comput. Chem. 1987, 8, 880.
- 24. Wendlant, W. W.; Chemical Analysis: Thermal Analysis, 3rd ed., John Wiley & Sons: New York, Chichester, Brisbane, Toronto, Singapore, 1985, vol. 19, 409.
- 25. Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M. A.; Cheeseman, J. R.; Zakrzewski, V. G.; Montgomery, J. A.; Stratmann, R. E.; Burant, J. C.; Dapprich, S.; Millam, J. M.; Daniels, A. D.; Kudin, K. N.; Strain, M. C.; Farkas, O.; Tomasi, J.; Barone, V.; Cossi, M.; Cammi, R;. Mennucci, B.; Pomelli, C.; Adamo, C.; Clifford, S.; Ochterski, J.; Petersson, G. A.; Ayala, P. Y.; Cui, Q.; Morokuma, K.; Rega, N.; Salvador, P.; Dannenberg, J. J.; Malick, D. K.; Rabuck, A. D.; Raghavachari, K.; Foresman, J. B.; Cioslowski, J.; Ortiz, J. V.; Baboul, A. G.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz, P.; Komaromi, I.; Gomperts, R.; Martin, R. L.; Fox, D. J.; Keith, T.; Al-Laham, M. A.; Peng, C. Y.; Nanayakkara, A.; Challacombe, M.; Gill, P. M. W.; Johnson, B.; Chen, W.; Wong, M. W.; Andres, J. L.; Gonzalez, C.; Head-Gordon, M.; Replogle, E. S.; Gaussian 98, Revision A.11.2, Gaussian, Inc., Pittsburgh PA, 2001.
- 26. Vallejo, A. C.; Siqueira, A. B.; Rodrigues, E. C.; Ionashiro, E. Y.; Bannach, G.; Ionashiro M.; Ecl. Quim. 2005, 30, 7.
- 27. Goodson, D. Z.; J. Phys. Chem 1998, 86, 659.
- 28. Schelegel, H. B. In New theoretical concepts for understanding organic reaction; Berdron J., ed., Academic: Holanda, 1989, p. 33-53.
- 29. Schaftenaar, G.; Molden 4.2, CAOS/CAMM Center Nijmegen Toernooiveld: Holanda, 1991.
Publication Dates
-
Publication in this collection
13 Mar 2007 -
Date of issue
Apr 2007
History
-
Received
10 Nov 2005 -
Accepted
25 May 2006