Advanced
Preparation and Characterization of Tin(II) Complexes with Isomeric Series of Schiff Bases as Ligands
Preparation and Characterization of Tin(II) Complexes with Isomeric Series of Schiff Bases as Ligands
Journal of the Korean Chemical Society. 2006. Apr, 50(2): 107-115
Copyright © 2006, The Korean Chemical Society
  • Received : December 12, 2005
  • Published : April 20, 2006
Download
PDF
e-PUB
PubReader
PPT
Export by style
Article
Author
Metrics
Cited by
TagCloud
About the Authors
Sadeek S. A.
Chemistry Department, Faculty of Science, Zagazig University, Zagazig, Egypt
Refat M. S.

Abstract
Complexes of Sn(II) with L 1 = acac- o -phdnH 2 [N,N’- o -phenylene bis(acetylacetoneimine)], L 2 = acac- m -phdnH 2 [N,N’- m -phenylene bis(acetylacetoneimine)] and L 3 = acac- p -phdnH 2 [N,N’- p -phenylene bis(acetylacetoneimine)] have been prepared and characterized by elemental analyses, vibrational, electronic spectra and thermal studies(TGA and DTA). Vibrational spectra indicated the coordination mode of imine and carbonyl oxygen for ligands giving(ONNO) that belong to C 2V point group symmetry. The [Sn( L 3 )] complex has a maximum activation energy and [Sn( L 2 )] complex has a minimum activation energy.
Keywords
INTRODUCTION
Schiff base are capable of forming coordinate bonds with many of metal ions through both azomethine group and phenolic group or via its azomethine or phenolic groups. 1 - 3 Infrared spectroscopy has been widely used as a powerful means of distinguishing between the three possible donation sites of Schiff bases. A large number of Schiff bases and their complexes are significant interest and attention because of their biological activity including anti-tumor, antibacterial, fungicidal and anti-carcinogenic properties. 4 , 5 Tetradentate Schiff bases are well known to coordinate with various metal ions forming stable compounds, and some of these complexes are recognized as oxygen carriers. 6
To continue our investigation in the field of Schiff base complexes, 7 - 11 we reported here preparation and characterization of the new complexes [Sn(acac- o -phdnH 2 )]Cl 2 , [Sn(acac- m -phdnH 2 )]Cl 2 and [Sn(acac- p -phdnH 2 )]Cl 2 ; (acac- o -phdnH 2 ( L 1 ), acac- m -phdnH 2 ( L 2 ) and acac- p -phdnH 2 ( L 3 ) are N,N’- o -phenylenebis (acetylacetoneimine), N,N’- m -phenylenebis(acetylacetoneimine) and N,N’-p-phenylenebis(acetylacetoneimine, respectively). The solid products are well characterized through its elemental analysis, electronic spectra and thermal analysis, along with the assignment of their infrared spectra for most of the fundamental vibrations.
PPT Slide
Lager Image
EXPERIMENTAL
All chemical used throughout this work were analytical reagent grade. The Schiff bases L 1 =acac- o -phdnH 2 [N,N’- o -phenylene bis(acetylacetoneimine)], L 2 =acac- m -phdnH 2 [N,N’- m -phenylene bis(acetylacetoneimine)] and L 3 =acac- p -phdnH 2 [N,N’- p -phenylene bis(acetylacetoneimine)] were prepared according to published method 12 from the condensation of o -phenylenediamine, m -phenylenediamine or p -phenylenediamine with acetylacetone in ethyl alcohol as a solvent. The separated precipitate was filtered, washed several times with minimum amount of ethyl alcohol and dried under vacuum at room temperature. The isolated three Schiff bases were characterized through its infrared and elemental analysis. The deep pink solid complex [Sn(acac- o -phdnH 2 )]Cl 2 was prepared from the addition of tin(II) chloride (4 mmol) in acetone to a stoichiometric amounts of the acac- o -phdnH 2 , (1.088 g, 4 mmol) in acetone. The mixture was then stirred at room temperature for about 6-8 hrs. The separated solid product was filtered off, washed several times with acetone and dried under vacuum. The other two complexes [Sn(acac- m -phdnH 2 )]Cl 2 (yellowish orange crystalline) and [Sn-(acac- p -phdnH 2 )]Cl 2 (brownish black) were prepared in a similar way to that described above by the reaction of tin(II) chloride with acac- m -phdnH 2 and acacp-phdnH 2 , respectively. The complexes formed were characterized through their elemental analysis, infrared spectra as well as thermogravimetric (TG) and differential thermal analysis (DTA). Analysis of the products obtained is summarized in 1 . The percentage of tin was determined using atomic absorption method. An atomic absorption spectrometer PYE-UNICAM SP 1900 fitted with a tin lamp was used for this purpose. The infrared spectra of the Schiff bases and tin(II) Schiff base complexes were recorded from KBr discs using a Perkin-Elmer 1430 ratio recording infrared spectrophotometer. Thermogravimetric (TG) and differential thermal analysis (DTA) of the Schiff base complexes [Sn(acac- o -phdnH 2 )]Cl 2 , [Sn(acac- m -phdnH 2 )]Cl 2 and [Sn(acac- p -phdnH 2 )]Cl 2 were carried out using a Shimadzu computerized thermal analysis system DT-40. The system includes programs that process data from the analyzer with the chromotpac C-R 3A. The rate of heating of the samples was kept at 5℃ min –1 . Accurate samples were analyzed under a N 2 flow at 40 ml min –1 α-alumina powder was used as the DTA standard materials. Electronic spectra of the reactants and products were recorded at room temperature using Jenway 6405 Spectrophotometer with quartz cell of 1 cm path length.
The elemental analysis data
PPT Slide
Lager Image
The elemental analysis data
RESULTS AND DISCUSSION
The three new complexes [Sn(acac- o -phdnH 2 )]Cl 2 , [Sn(acac- m -phdnH 2 )]Cl 2 and [Sn(acac- p -phdnH 2 )]Cl 2 formed in the reaction of SnCl 2 with the Schiff bases acac- o -phdnH 2 , acac- m -phdnH 2 and acac- p -phdnH 2 are characterized through their elemental analysis, infrared spectra and through their thermogravimetric investigation. The results enable us to characterize the complexes and make an assessment of the bonding and structures inherent in them.
The structural formula of these three complexes was obtained according to the following facts. Elemental analysis of the three complexes under investigation shows the presence of chloride ions in the three complexes. Solutions of these complexes react with silver nitrate giving a white precipitate of silver chloride indicating the existence of chloride in the ionic form i.e. outside the coordination sphere of the tin ion.
However, the Schiff bases under study may be present in tautomeric equilibrium (forms I-III), which resemble the forms given by Dudek and Holm 13 for similar Schiff bases.
PPT Slide
Lager Image
Distinction between the forms II and III is not large as a slight displacement of the hydrogen nucleus. It has been concluded from infrared evidences that similar Schiff bases are largely tautomerized into II and III with appreciable amount of each existing in the solid state and in solution. 13 , 14
- Vibrational spectra
Infrared spectra of the Schiff bases under studies give a broad absorption band at about 3170 cm −1 , which may be due to the stretching vibration of either an O-H group in accordance with formula II or an N-H group of the type indicated by the formula III. Evidence of that 14 is found in the broadening of this band and shift from normal positions (3700-3400 cm −1 for free O-H and 3400-3300 cm −1 for free N-H). Also the free Schiff bases do not absorb in the region of carbonyl group, thus the formula I is eliminated and the ligand is believed to be a tautomeric equilibrium mixture of structures II and III.
The characteristic IR bands of [Sn(acac- o -phdnH 2 )]Cl 2 , [Sn(acac- m -phdnH 2 )]Cl 2 and [Sn(acac- p -phdnH 2 )]Cl 2 are shown in 2 . Before explaining such assignments, the structures of these complexes must first be discussed. Bottcher et al . 16 reported the crystal structure of some related Schiff base complexes of Co(III) and indicated that the tetradentate Schiff base ligand (ONNO) coordinates the cobalt atom in a planar fashion with a slightly irregular tetragon with Co(III). The values of the Co-O and Co-N bond lengths in the equatorial ligand plane are 1.881 and 1.892 A°, respectively.
The complexes under investigations indicate that the tin(II) is only four coordinated and may take the structures shown in IV . With such structures the complexes may belong to C 2V symmetry and are expected to display 117 vibrational fundamental which are all monodegenerate. These are distributed between A 1 , A 2 , B 1 and B 2 motions; all are IR and Raman active, except for the A 2 modes, which are only Raman active.
In the spectra of the complexes, medium strong bands in the region 3340-3217 cm −1 do exist, . 1 . These bands occur at lower frequency values known for O-H groups, therefore, the two bands found at 3279 and 3217 cm −1 for the complex [Sn(acac- o -phdnH 2 )]Cl 2 , and at 3320, 3200 cm −1 for [Sn(acac- m -phdnH 2 )]Cl 2 and 3340 cm −1 for [Sn(acac- p -phdnH 2 )]Cl 2 complexes, respectively, are assigned to coordinated N-H groups. 15 Accordingly, the three complexes under study have coordinated N-H groups which indicated that, the Schiff bases under study coordinates with Sn(II) as a tetradentate through the two nitrogen and oxygen atoms as shown in IV and in the ketoamine form (III).
Infrared frequencies(a)(cm−1) and tentative assignments for (A): [Sn(acac-o-phdnH2)]Cl2, (B): [Sn(acac-m-phdnH2)]Cl2and (C): [Sn(acac-p-phdnH2)] Cl2complexes. complexes.
PPT Slide
Lager Image
(a): s=strong, w=weak, m=medium, sh=shoulder, v=very, br = broad. (b): ν, stretching; δ, bending.
The ν (C-H) for the phenyl group are assigned in the region 3150-3020 cm −1 , 2 , while those for the CH 3 and =CH- groups are shown as expected at 2970, 2960, 2915, 2880 and 2860 cm −1 . The carbonyl bands ν (C=O) of our complexes are shown at 1630 and 1605 cm −1 as a strong and medium strong band. The ν (C=C) stretching vibrations and phenyl breathing modes of the three complexes are observed in the range 1590-1490 cm −1 . The bending vibrations, δ (-CH 3 ) and (=CH) are observed in the region 1476-1310 cm −1 . The description of their assignments follow the expression developed and used by others. 17 , 18
The stretching vibrations of ν (C-O), ν (C-C) and ν (C-N) occur in the region 1285-1110 cm −1 , 2 . The tin-oxygen (O of Schiff base) stretching vibration, ν as (Sn-O) are assigned for the three complexes at 514, 555 and 550 cm −1 , while the corresponding ν s (Sn-O) are assigned at 475, 490 and 505, 480 cm −1 for o-, m- and p- Schiff base complexes, respectively. The ν as (Sn-N) are assigned at 345, 320 cm −1 and 325, 315 cm −1 and 350, 330 cm −1 , for our study complexes, while ν s (Sn-N) are assigned to the strong and weak infrared bands around 295 cm −1 . The assignments of these metal-ligand stretches are made on the basis of their activities as well as the relative bond strengths shown from the crystal structure data known 16 for some related Schiff base complexes, and also that the assigned bonds do not exist in the free ligand spectra. However, the ν(Sn-N) stretches were assigned at relatively low frequency values compared to ν(Sn-O). This is in agreement with the bond length values, which indicate that the Sn-N bond is the weakest with a large value of bond length.
PPT Slide
Lager Image
PPT Slide
Lager Image
Infrared spectra of (a): acac-o-phdnH2 Schiff base, (b): [Sn(acac-o-phdnH2)]Cl2, (c): [Sn(acac-m-phdnH2)]Cl2 and (d): [Sn(acac-p-phdnH2)]Cl2 complexes.
- Thermal studies
Differential thermal analysis (DTA) and thermogravimetric (TG) were measured for the three complexes to investigate the mode of decomposition of these types of complexes, . 2 . The maximum temperature values T max /℃ together with the corresponding weight loss for each step of the decomposition are recorded in 3 . The decomposition of the complex [Sn(acac- o -phdnH 2 )]Cl 2 falls in one degradation stage. This stage of decomposition appears at two maxima 120 and 165 ℃ is associated with a weight loss of 54.96% corresponding to the loss of 5C 2 H 2 +2HCl+2NH 3 +H 2 O. The weight loss in this stage 54.96% is in full agreement with the calculated value of 55.23%. The thermal degradation for the other two complexes, [Sn(acac- m -phdnH 2 )]Cl 2 and [Sn(acac- p -phdnH 2 )]Cl 2 , exhibit approximately one main decomposition step, . 2 , this stage of decomposition occurs at maximum temperatures 141, 259 and 109, 153 ℃, respectively, and accompanied by a weight loss of 47.11 and 66.16% correspond to the loss of 3C 2 H 4 +2HCl+2NH 3 +CO and 7C 2 H 2 +2HCl+N 2 +H 2 O+H 2 in agreement with our predicted weight loss of 47.44 and 65.63% for [Sn(acac- m -phdnH 2 )]Cl 2 and [Sn(acac- p -phdnH 2 )]Cl 2 complexes, respectively. The above going conclu-sion was also supported by the fact that the infrared spectra of the final decomposition products for the complexes under investigation shows the absence of all bands associated with the Schiff base ligands and instead the characteristic spectrum of SnO is appeared. Accordingly, the following mechanisms are proposed for the thermal decomposition of the Schiff base complexes as follows:
PPT Slide
Lager Image
TGA and DTA curves of (A): [Sn(acac-o-phdnH2)]Cl2, (B): [Sn(acac-m-phdnH2)]Cl2 and (C): [Sn(acac-p-phdnH2)]Cl2 complexes.
The maximum temperature, Tmax/℃, and weight loss values of the decomposition stages for the [Sn(acac-o-phdnH2)]Cl2, [Sn(acac-m-phdnH2)]Cl2and [Sn(acac-p-phdnH2)]Cl2complexes.
PPT Slide
Lager Image
The maximum temperature, Tmax /℃, and weight loss values of the decomposition stages for the [Sn(acac-o-phdnH2)]Cl2, [Sn(acac-m-phdnH2)]Cl2 and [Sn(acac-p-phdnH2)]Cl2 complexes.
  • 1-[Sn(acac-o-phdnH2)]Cl2
  • →SnO+6C+5C2H2+2HCl+2NH3+H2O
  • 2-[Sn(acac-m-phdnH2)]Cl2
  • →SnO+9C+3C2H4+2HCl+2NH3+CO
  • 3-[Sn(acac-p-phdnH2)]Cl2
  • → SnO+2C+7C2H2+2HCl+N2+H2O+ H2
- Electronic spectra
The electronic spectra of the SnCl 2 , acetylacetonate, schiff base (e.g, acac- o -phdnH 2 ) and the complex, [Sn(acac- o -phdnH 2 )]Cl 2 have been measured in methanol as a solvent, . 3 . The spectra of the uncomplexed ligand (acac- o -phdnH 2 ) show a characteristic band at 275 nm which is assigned to n→π* transition to the chromophoric C=O group. This band shows a bathochromic shift in the tin(II) complexes of all the ligands. This is attributed to the involvement of carbonyl group in metal complexation as indicated by IR studies. The Schiff bases, acac- o -phdnH 2 , acac- m -phdnH 2 and acac- p -phdnH 2 were prepared in this study play a role of donor type (n-donor). The n-donor is neutral, even systems containing relatively an easily ionized atomic lone pair of electrons. 19 The donated electrons come from a non-bonding molecular orbital occupied in the original donor by a lone pair of electrons as follows:
  • n + A → n.A ↔ n+− A−
On the other side tin(II) chloride reacted as a vacant orbital acceptor 19 which is neutral even system or even ions in which an orbital or orbitals of relatively high electron affinity are vacant. This type of acceptors combine especially with n-donors to form fairly stable compounds by partial dative acceptance of electron into vacant orbital as follows:
  • D: +V → D: V
To make a comparison between reactants and products ( . 3 ), there are three electron spectra bands observed around 260 and 310 nm due to π→π* of acetylacetonate ring (C=O) and at around 379 nm as shoulder broad peak due to the metal-toligand charge transfer transition, 20 between Schiff bases and SnCl 2 (the color of schiff base widely change as soon as tin(II) chloride added from brownish yellow to pink color).
PPT Slide
Lager Image
Electronic spectra of (a): SnCl2, (b): Acetylacetonate, (c): acac-o-phdnH2, (d): acac+o-phenylenediamine, (e): Acetylacetonate+o- phenylenediamine / SnCl2 complex.
- Kinetic calculation
From TGA curves, the order ( n ), activation energy ( E * /kJ mol −1 ), and the pre-exponential factor, Z, for thermal reactions of the complexes have been elucidated by linearisation method of Horowitz-Metzger(HM) approximation method and Coats-Redfern integral method. 21 , 22 The entropy of activation ΔS * in (JK −1 mol −1 ) was calculated by using the equation: Δ S * = R ln( Ah/kB Ts ), where kB is the Boltzmann constant, h is the Plank’s constant and Ts is the DTA peak temperature. 23
PPT Slide
Lager Image
Kinetic parameter of (A): [Sn(acac-o-phdnH2)]Cl2, (B): [Sn(acac-m-phdnH2)]Cl2 and (C): [Sn(acac-p-phdnH2)]Cl2 complexes using Horowitz-Metzger (HM) approximation method and Coats-Redfern (CR) integral method.
Kinetic parameters determined using the Coats-Redfern (CR) and Horowitz-Metzger (HM).
PPT Slide
Lager Image
Kinetic parameters determined using the Coats-Redfern (CR) and Horowitz-Metzger (HM).
The enthalpy activation, Δ H * , and Gibbs free energy, Δ G * , were calculated from; Δ H * = E * RT and Δ G * H * T Δ S * , respectively. The data is presented in . 4 and 4 . The complexes with all the ligands start decomposing in the range 382-583 K. This shows that the complexes are anhydrous. All complexes decomposed via first order kinetics and energy of activation is 16-25 kJmol −1 . The order of activation energy is: L 3 > L 1 > L 2 for tin(II) complexes. The literatures contain various explanations of the relative order of thermal stability of complexes. 24 - 26 The final product of the decomposition in all the complexes is SnO as confirmed by experimental and calculated weight losses.
References
Sheat S. V. , Waters T. V. 1964 J. Inorg. Nucl. Chem. 26 1221 -    DOI : 10.1016/0022-1902(64)80203-7
Cozens R. J. , Murray K. S. , West B. O. 1971 Organomet. Chem. 27 399 -    DOI : 10.1016/S0022-328X(00)82173-7
Bigotto A. , Galasso V. , Dealti G. 1972 Spectrochim. Acta 28A 1581 -    DOI : 10.1016/0584-8539(72)80129-6
Ren S. , Wang R. , Komatsu K. , Bonaz-Krause P. , Zyrianov Y. , McKenna C. E. , Csipke C. , Tokes Z. A. , Lien E. J. 2002 J. Med. Chem. 45 410 -    DOI : 10.1021/jm010252q
Raman N. , Thangaraja A. , Kulandaisamy C. 2003 Trans. Met. Chem. 28 29 -    DOI : 10.1023/A:1022544126607
Floriani C. , Calderazzo F. 1969 J. Chem. Soc.(A) 949 -
Sadeek S. A. , Teleb S. M. 1993 J. Phys. Chem. Solids 54 489 -    DOI : 10.1016/0022-3697(93)90332-L
Teleb S. M. , Sadeek S. A. , Nour E. M. 1993 Spectroscopic Lett. 26 (1) 169 -    DOI : 10.1080/00387019308011523
Sadeek S. A. , Refat M. S. , Teleb S. M. 2004 Bull. Chem. Soc. Ethiop. 18 (2) 149 -    DOI : 10.4314/bcse.v18i2.61433
Sadeek S. A. , Teleb S. M. , Refat M. S. , Elmosallamy M. A. F. 2005 J. Coord. Chem. 58 (12) 1077 -    DOI : 10.1080/0095897050012279
Sadeek S. A. , Teleb S. M. , Al-Kority A. M. 1993 J. Indian Soc. 70 63 -
McCarthy P. J. , Havey R. J. , Ueno K. , Martell A. E. 1955 J. Am. Chem. Soc. 77 5820 -    DOI : 10.1021/ja01627a011
Dudek G. O. , Holm R. H. 1961 J. Am. Chem. Soc. 5
Ueno K. , Martell A. E. 1955 J. Phys. Chem. 59 998 -    DOI : 10.1021/j150532a002
Martell A. E. , Belford R. L. , Calvin M. 1958 J. Inorg. Nucl. Chem. 5 170 -    DOI : 10.1016/0022-1902(58)80127-X
Bottcher A. , Takeuchi T. , Hardcastle K. I. , Meacle T. J. , Gray H. B. 1997 Inorg. Chem. 36 2498 -    DOI : 10.1021/ic961146v
Colthup N. B. , Daly L. H. , Wiberly S. E. 1975 Introduction of Infrared and Raman spectroscopy Academic New York
Datta M. , Brown D. H. , Smith W. E. 1983 Spectrochim. Acta 39 37 -    DOI : 10.1016/0584-8539(83)80052-X
Foster R. 1969 Organic Charge-Transfer Complexes Academic Press London and New York
Khalil M. M. H. , Aboaly M. M. , Ramadan R. M. 2005 Spectrochim. Acta 61A 157 -
Horowitz H. W. , Metzger G. 1963 Anal. Chem. 35 1464 -    DOI : 10.1021/ac60203a013
Coats A.W. , Redfern J. P. 1964 Nature 68 201 -
Flynn J. H. F. , Wall L. A. 1996 J. Res. Natl. Bur. Stand. 70A 487 -    DOI : 10.6028/jres.070A.043
Botti S. R. , Quana D. 1964 J. Inorg. Nucl. Chem. 26 1919 -    DOI : 10.1016/0022-1902(64)80017-8
Shashagiri V. , Rao S. B. 1972 Z. Anal. Chem. 262 175 -
Naidu R.S. , Naidu R.R. 1977 Indian J. Chem. 15A 652 -