The FT-IR, FT-Raman, 1 Hand 13 CNMR study on molecular structure of sodium(i), calcium(ii), lanthanum(iii) and thorium(iv) cinnamates

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Spectroscopy 24 (2010) 277 281 277 DOI 10.3233/SPE-2010-0442 IOS Press The FT-IR, FT-Raman, 1 Hand 13 CNMR study on molecular structure of sodium(i), calcium(ii), lanthanum(iii) and thorium(iv) cinnamates M. Kalinowska, W. Lewandowski,R.Świsłocka and E. Regulska Department of Chemistry, Białystok Technical University, Białystok, Poland Abstract. In this work the effect of sodium(i), calcium(ii), lanthanum(iii) and thorium(iv) ions on the electronic structure of cinnamic acid (phenylacrylic acid) was studied. In this research: infrared (FT-IR), Raman (FT-Raman), nuclear magnetic resonance ( 1 H, 13 C NMR) were used. In the series of Na(I) Ca(II) La(III) Th(IV) cinnamates: (1) systematic shifts of several bands in the FT-IR and FT-Raman spectra, and (2) regular chemical shifts of protons 1 Hand 13 C nuclei were observed. Keywords: Sodium, calcium, lanthanum and thorium cinnamates, FT-IR, FT-Raman, NMR 1. Introduction In this work we studied the effect of Na(I) Ca(II) La(III) Th(IV) cations on the electronic system of cinnamic acid by means of many complementary methods: infrared (FT-IR), Raman (FT-Raman), nuclear magnetic resonance ( 1 H, 13 C NMR). In the chosen series of metals the oxidation state changes whereas the ionic radius remains almost the same. Previously we studied the effect of Li Na K Rb Cs on the molecular structure of cinnamic acid (in this series of metals the oxidation state is the same, but the ionic radius increases) [4]. Application different and specially selected metal ions allows to study the spectroscopic properties of complexes depending on the metal parameters. The participation of double bond in cinnamic acid molecule on the influence of metals on the electronic system of ligand was discussed as well. 2. Experimental The preparation of metal complexes was described previously [4 6]. The elementary and thermogravimetric analyses showed that obtained complexes were anhydrous, the metal:ligand ratio was 1:1 in case of Na cinnamate, 1:2 in case of Ca cinnamate, 1:3 La complex and 1:4 Th complex. The IR spectra * Corresponding author: W. Lewandowski, Department of Chemistry, Białystok Technical University, Zamenhofa 29, 15-435 Białystok, Poland. Tel.: +48 85 469790; Fax: +48 85 7469782; E-mail: w-lewando@wp.pl. 0712-4813/10/$27.50 2010 IOS Press and the authors. All rights reserved

278 M. Kalinowska et al. / The FT-IR, FT-Raman, 1 H and 13 C NMR study on molecular structure were recorded with the EQUINOX 55, BRUKER FT-IR spectrometer within the range 4000 400 cm 1. Samples in the solid state were measured: (1) in KBr matrix and (2) by the use of ATR technique. Pellets were obtained with a hydraulic press under 739 MPa pressure. Raman spectra of solid samples in capillary tubes were recorded in the range of 4000 400 cm 1 with a FT-Raman accessory of the Perkin Elmer System 2000. The resolution of spectrometer was 1 cm 1. The NMR spectra of DMSO solution were recorded with the Bruker Avance II 400 MHz unit at room temperature. TMS was used as an internal reference 3. Results and discussion In Table 1 wavenumbers of selected bands from the FT-IR, FT-Raman spectra of Na(I), Ca(II), La(III) and Th(IV) cinnamates were collected. The spectral assignments were done on the basis of the literature data [3,4,8]. The change of metal cation in the carboxylic group of cinnamic acid did not evoke serious changes in the wavenumbers of bands from the IR and Raman spectra of cinnamates. Only bands: γ(cch) C=C ( 980 cm 1 ), α(c=c C) C=C ( 540 cm 1 ), band no. 4 and bands assigned to carboxylate anion vibrations undergo distinct displacements along the metal series of Na Ca La Th. The regular displacement of bands suggests that the influence of metal ions on the electronic charge distribution in the ligand depends on selected metal parameters. In this study the analysis for linear correlation between selected metal ions parameters (ionic potential, ionic radius, reverse of atomic mass) and wavenumbers of bands from FT-IR and FT-Raman spectra was done. Among studied parameters the highest correlation coefficients were in most cases obtained for ionic radii of metal ions. The difference between wavenumbers of bands from FT-IR spectra assigned to asymmetric and symmetric stretching vibrations of carboxylate anion [Δν(COO )] reveals the type of metal coordination [1,2]. The values of Δν(COO ) were following: 136 cm 1 for sodium cinnamate, 125 and 104 cm 1 for calcium complex, 125 and 106 cm 1 for lanthanum complex, 133 and 102 cm 1 for thorium cinnamate. Comparing the values of Δν(COO ) and the location of ν as (COO )andν s (COO ) in the FT-IR of complexes the following type of coordination was suggested: bidentate chelating, bidentate bridging or tridentate bridging chelating. The metal complex formation caused the biggest changes in the FT-IR and FT-Raman spectra in the region of carboxylic anion and double bond vibrations. The location of selected bands from the FT-IR and FT-Raman spectra of cinnamic and benzoic acids [7] as well as Na, Ca, La, Th cinnamates and benzoates [5,6] were compared. More significant changes in the displacement of appropriate bands from the spectra of acid and complexes were visible after the substitution of metal in the carboxylic group of benzoic acid than cinnamic acid. In the spectra of Na(I) Ca(II) La(III) Th(IV) complexes bigger differences were observed in the spectra of benzoates than cinnamates. In the 1 H NMR spectra of cinnamates all signals were shifted downfield compared with signals from the spectra of acid (Table 2). The biggest differences in the location of appropriate signals were noticeable between the spectra of sodium cinnamate and the rest of studied cinnamates. This may be caused by different type of bonding, i.e. ionic in the case of sodium salt and covalent in the structure of calcium, lanthanum and thorium cinnamates. The 13 C NMR spectra of studied compounds showed an increased in the electronic charge density around the carbon atom no. 9 and a decrease around the carbon atoms nos 7 and 8 in the structure of cinnamates compared with the structure of acid (Fig. 1). In the series of Ca(II) La(III) Th(IV) complexes an increase in the values of chemical shifts assigned to carbon atoms nos 2, 4, 6, 9 and a decrease in the values of chemical shifts derived from the carbon atoms nos 1, 3, 5 and 8 were observed.

Table 1 Wavenumbers, intensities and assignments of bands occurring in the FT-IR Sodium(I) Calcium(II) cinnamate Lanthanum(III) cinnamate Thorium(IV) cinnamate Assignments Aromatic cinnamate ring vibrations IR KBr IR KBr IR ATR solid Raman IR KBr IR ATR solid Raman IR KBr IR ATR solid Raman 1640 m * 1641 s 1641 m 1645 vs 1640 s 1640 m 1642 vs 1638 s 1638 w 1640 vs ν(c=c) C=C 1599 vw 1602 s 1602 s 1602 s ** ν(cc) ar 8a 1577 m 1579 s 1580 vw 1578 s 1578 w 1580 vw 1578 m 1579 w ν(cc) ar 8b 1548 vs 1545 s 1531 s 1532 m 1545 sh 1506 m ν as(coo ) 1524 sh 1520 s 1516 s 1516 m 1514 s 1495 m 1496 m 1497 s 1495 m 1497 s ν(cc) ar 19a 1451 m 1452 s 1450 m 1458 w 1450 s 1450 m 1456 vw 1450 s 1450 w 1461 w ν(cc) ar 19b 1412 s 1420 vs 1410 vs 1419 vw 1410 vs 1408 vs 1412 vs 1406 vs ν s(coo ) 1392 m 1398 vw 1401 w β(ch) ar 3 1244 w 1252 m 1250 w 1255 m 1250 m 1250 w 1253 m 1250 m 1253 m β(ch) C=C 970 m 977 m 978 m 980 m 978 w 980 w 984 w γ(cch) C=C 852 vw 852 vw 850 vw 852 vw 851 w 851 vw 853 w 841 vw 852 vw β s(coo ) 728 m 737 w 737 m 739 w 745 w 741 vw ϕ(ccc) 4 713 w 717 w 718 m 718 m 714 w 716 w 716 w 717 vw γ s(coo ) 586 w 590 w 590 m 588 m 590 m 590 m 590 m β as(coo ) 530 w 539 w 540 w 567 vw 548 w α(c=c C) C=C 486 w 485 w 484 w 484 w ϕ(ccc) 16b Notes: KBr sample registered in KBr matrix, ATR solid sample registered in solid state by the use of ATR technique) and the FT-Raman spectra of sodium, calcium, lanthanum and thorium cinnamates ( C=C double bond vibrations, ar aromatic ring vibrations. * s strong; m medium; w weak; v very; sh shoulder, ** ν stretching vibrations, β in-plane bending modes, γ out-of-plane bending modes; ϕ(ccc) the aromatic ring out-of-plane bending modes; α(ccc) aromatic ring in-plane bending modes. M. Kalinowska et al. / The FT-IR, FT-Raman, 1 H and 13 C NMR study on molecular structure 279

280 M. Kalinowska et al. / The FT-IR, FT-Raman, 1 H and 13 C NMR study on molecular structure Table 2 The experimental chemical shifts of protons in the 1 H NMR and carbons in the 13 C NMR spectra of DMSO solution of cinnamic acid and sodium, calcium, lanthanum and thorium cinnamates (atom numbering in Fig. 1) Cinnamic acid Cinnamates Na(I) Ca(II) La(III) Th(IV) Proton position A 12.40 C 7.68 7.44 7.49 7.49 7.58 D, H 7.67 7.32 7.44 7.44 7.53 F 7.60 7.24 7.26 7.30 7.31 E, G 7.41 7.06 7.26 7.30 7.31 B 6.53 6.36 6.51 6.49 6.45 Carbon position 7 167.61 169.84 173.16 176.62 173.30 9 143.95 136.93 139.61 139.95 141.69 1 134.27 134.76 135.75 135.32 134.91 4 130.23 130.93 128.75 129.01 129.56 3, 5 128.92 128.59 128.66 128.65 128.56 2, 6 128.22 127.72 127.34 127.47 127.83 8 119.27 126.81 126.41 125.59 124.92 Fig. 1. Atom numbering for cinnamic acid molecule and cinnamates. 4. Conclusions Na(I), Ca(II), La(III) and Th(IV) metal ions affect the molecular structure of cinnamic acid. The metal ions mostly influence the electronic charge distribution in carboxylate anion and double bond between aromatic ring and carboxylate group of ligand. The effect of metals depends mainly on the ionic radii of metals and the type of metal coordination.

Acknowledgement M. Kalinowska et al. / The FT-IR, FT-Raman, 1 H and 13 C NMR study on molecular structure 281 This work was supported by Białystok Technical University (theme No. G/WBIIŚ/21/08). References [1] C.R. Choudhury, A. Datta, V. Gramlich, G.M.G. Hossain, K.M.A. Malik and S. Mitra, Inorg. Chem. Commun. 6 (2003), 790 793. [2] G.B. Deacon and R.J. Philips, Coordin. Chem. Rev. 33 (1980), 227 250. [3] K. Hanai, A. Kuwae, T. Takai, H. Senda and K.-K. Kunimoto, Spectrochim. Acta A 57 (2001), 513 519. [4] M. Kalinowska, R. Świsłocka and W. Lewandowski, J. Mol. Struct. 834 836 (2007), 572 580. [5] W. Lewandowski, J. Inorg. Chem. 4 (1988), 79 80. [6] W. Lewandowski and H. Barańska, J. Mol. Struct. 174 (1988), 417 421. [7] W. Lewandowski, B. Dasiewicz, P. Koczoń, J. Skierski, K. Dobrosz-Teperek, R. Świsłocka, L. Fuks, W. Priebe and A.P. Mazurek, J. Mol. Struct. 604 (2002), 189 193. [8] G. Varsanyi, Assignments for Vibrational Spectra of 700 Benzene Derivatives, Akademiai Kiado, Budapest, 1973.

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