Scientific paper The Binding Sites of Cadmium to a Reduced Form of Glutathione Martina Glusic,1 Polona Ropret,2 Katarina Vogel-Mikus3 and Jože Grdadolnik1'4* 1 National Institute of Chemistry, Hajdrihova 19, SI-1000 Ljubljana, Slovenia 2 Institute for the Protection of Cultural Heritage of Slovenia, Restoration Center, Poljanska 40 SI-1000 Ljubljana, Slovenia 3 Biotechnical Faculty, University of Ljubljana, Ve~na pot 111, SI-1000 Ljubljana, Slovenia 4 EN-FIST Centre of Excellence, Dunajska 156, SI-1000 Ljubljana, Slovenia * Corresponding author: E-mail: joze.grdadolnik@ki.si Received: 01-06-2012 Abstract Glutathione is the most abundant low molecular weight thiol-containing molecule in biological cells with a strong tendency to interact with metal ions. Among the eight possible glutathione binding sites, only two are determined as groups that interact with the Cd2+ ion. Analysis of vibrational spectra and 13C and NMR spectra revealed that thiol and glu-tamyl's carboxylic groups are groups that cooperate in interaction with Cd2+ ions. The coordination of Cd2+ with those groups was supported by the application of auxiliary molecules (D-penicillamine, glycine, cysteine and glutamic acid dipeptides, mercaptosuccinic acid and N-acetyl-L-cysteine). These molecules provide a reliable assignment of the fundamental vibrations in the glutathione vibrational spectra. Concentration-dependent measurements of Cd2+ ions showed that the optimal stoichiometry of coordination with the glutathione molecule is 1:1. The analysis of 3J(Ha, HN) coupling constants and conformational sensitive bands in the glutathione vibrational spectra suggest that interaction with Cd2+ ions significantly alters glutathione backbone conformation. The binding of ions induced the conformational change of the cysteine backbone from a predominantly ¡5 structure to Pn. Keywords: Glutathione, cadmium complex, vibrational spectroscopy, NMR spectroscopy 1. Introduction Glutathione (y- glutamylcysteinylglycine; GSH) is an essential metabolite and the principal low-molecular weight thiol usually present at millimolar concentrations in most living cells. The fundamental and earliest recognized functions of GSH are thiol-disulphide interactions in which reduced glutathione (GSH) is continuously oxidized to a disulphide form (GSSG) that is recycled back to GSH by NADPH-dependent glutathione reductase. Because of this unique redox and nucleophilic properties, GSH serves in bio-reductive reactions as an important line of defence against reactive oxygen species, xenobiotics and heavy metals, preventing excessive oxidation of sensitive cellular storage and transport of nonprotein reduced sulfur, regulation of sulphur metabolism, synthesis of proteins and nucleic acids, regulation of gene expression, development of embryos and meristems, signaling in plant pathogen interactions, binding of toxic metals and others.2-4 Heavy metal ions are highly reactive and consequently toxic to living cells, although like all living organisms, plants have evolved a suite of mechanisms that control and respond to the uptake and accumulation of heavy metals in tissues. Biosynthesis of glutathione is markedly induced by heavy metals. Plants overexpress y-EC syn-thetase, the key enzyme responsible for GSH synthesis. Other mechanisms include the chelation and sequestration of heavy metals by particular ligands5 and compartmenta-tion of metal ions in less metabolically active cell parts, components.1'2 GSH plays an indispensable role also in such as vacuoles.6'7 Cadmium for example can be trans-many other physiological processes in plant cells such as ported into the vacuole as a free ion or associated with thi- ol compounds, GSH or phytochelatins.1 Phytochelatins (y-Glu-Cys)211-Gly are one of the best-characterized heavy metal-binding ligands in plant cells.810 They are short peptides that are synthesized from GSH by phy-tochelatin synthase, a specific enzyme activated by heavy metals, especially cadmium.11,12 Although the role of phytochelatins in heavy metal detoxification is well documented,13 studies of metal accumulation and detoxification mechanisms in metal hyperaccumulating plants have shown that increased tolerance is not explained solely by the accumulation of phytochelatin-heavy metal complex-es,14-17 but rather GSH, cysteine and other low molecular weight thiols might be involved in Cd detoxification in the Since GSH has been considered to be the first cells. line of defence against cadmium toxicity in many cell types knowledge of the coordination chemistry of GSH is essential for understanding the molecular mechanism of the accumulation and tolerance to cadmium in plants. In principle, the glutathione molecule has eight possible binding sites. The determination of privileged binding sites of GSH with Cd2+ was the object of a wide range of studies. 1H NMR spectroscopy indicates that metal ions bind to the potential coordination sites of GSH with a high degree of specificity, which depends on the type of metal ion and the pH value of the solution.19 Dorcak and Kre-zel20 assumed that in phytochelatins besides thiol groups, the amino groups, glutamic acid and glycine deprotonated carboxyls also participate in cadmium coordination. Li et al.21 observed that in yeast, a Cd(GSH)2 complex is formed, rather than the 1:1 complex, while Leverrier et al.22 concluded that at the physiological pH value, Cd2+ ions form 1:1 complexes with GSH at micromolar concentration. The authors showed that 1:2 Cd(GSH)2 complexes become dominant at higher concentrations of GSH. Delalande et al.23 demonstrated that Cd2+ is linked by two thiol groups from distinct GSH and that Cd2+ ligation by nitrogen (the amino group of glutamic acid or the amide of cysteine) does not seem to occur. They also asserted that no carboxylate groups are involved in the interaction. The present study is focused on structural studies of the GSH Cd2+ complex and identification of the favored coordination sites by applying vibrational (Raman and FTIR) and NMR (1H and 13C) spectroscopy. Mercaptosuccinic acid, D-penicillamine and N-acetyl-L-cysteine are thiol-containing components and were used as model compounds to assure the proper assignment of GSH vibrational spectra. Glutamic acid, glycine and cysteine dipeptides were applied for determining the effects of complex formation on the backbone conformation of the GSH molecule. 2. Materials and Methods Glycine, glutamic acid and cysteine in the form of dipeptides, blocked by CH3-CO- and -NH-CH3 groups, were purchased from Bachem. The reduced form of L-glutathione, mercaptosuccinic acid and N-acetyl-L-cys-teine were purchased from Sigma-Aldrich, and O-penicil-lamine from Fluka. The samples were prepared in a concentration range between 0.125 M and 1.0 M in mQ H2O and D2O, where the equimolar concentrations of CdSO4 were added. The infrared spectra were measured using Bruker FTS-66 and Bruker Vertex 80 infrared spectrometers. Spectra were recorded in the range between 7000 and 370 cm1. Typically, 256 scans were averaged and apodi-zed using a Gapp-Henzel function. The infrared spectra were recorded using a diamond ATR cell equipped with a heated top plate and KRS-5 lenses. The frequency differences between the bands recorded in absorption and ATR mode are large, particularly for the strong bands.24,25 In order to eliminate anomal dispersion effects, pure absorption spectra were calculated from the ATR ones using a method proposed by Bertie and Lan26 and Bertie and Eysel.27 The procedure25 is written in the Matlab environment. The regions between 1750 cm1 and 1150 cm1 were analyzed using the Grams band fitting procedures (GRAMS program, Thermo Electron, San Jose, CA). The shape of individual components was fitted by the sum of bands with Lorentzian and Gaussian shapes. The critical point of applying band fitting algorithm is determination of the number of model bands. We applied two mathematical tools i.e. Fourier avtodeconvolution and second derivative spectroscopy. Both methods are sensitive on the shape of the experimental bands and give the number and approximate position of overlapped component bands. These data are used as starting parameters in the band fitting procedure. The optimization procedure varies peak shape, position, intensity and band halfwidth of individual model bands to minimize the difference between the experimental spectrum and calculated one. The optimized calculated model bands are appropriate for explaining the overlapped region if the resulting difference between the experimental and calculated spectrum contains only recorded noise. Raman spectra were recorded using the HORIBA Jobin Yvon LabRAM HR800, with a nominal resolution of 0.83 cm-1/pixel, equipped with an NIR Raman source with the excitation line at 785 nm and Bruker Ram II FT Raman spectrometer with a nominal resolution of 2 cm1. The excitation laser line in the FT Raman experiments was 1064 nm. Typically, up to 5000 scans were averaged. The laser power varies from 100 mW to 300 mW. The 1H experiments were recorded at 30 °C on a Varian INOVA 600 MHz spectrometer and the 13C experiments on a Varian Unity INOVA 300 MHz spectrometer equipped with automated triple broadband (ATB) probes. The concentration of GSH was 20 mM and different equivalents of concentrated CdSO4 solutions were added as required. The pH values at 4.5 and 7 were adjusted by adding NaOH and HCl. All the samples were prepared in a mixed solvent of 90% H2O and 10% D2O. The concentration-dependent measurement of GSH was performed in the range between 0.5 mM and 20 mM. The chemical shift data for were referenced to 2,2-dimethyl-2-silapentane-5-sul-fonate (DSS). The stoichiometry of interactions between ligand and metal was determined using the Jobs method. Series of 2D NMR experiments (COSY, gHSQC and gHMBC) were recorded on a Varian Unity INOVA 300 MHz spectrometer applying standard sequences. Peak assignments for :H resonances were carried out using COSY and gHSQC and for 13C resonances using gHMBC. 3J(Ha HN) coupling constants were measured from HN resonances. A band fitting procedure (GRAMS program, Thermo Electron, San Jose, CA) was used to calculate the peak frequency of the broad overlapped HN doublet. During the fitting procedure, a Lorentzian lineshape was used. Band frequencies, bandwidths and intensities were allowed to vary simultaneously with no restrictions. 3. Results and Discussion Figure 2. The infrared spectra of GSH in D2O (a) and H2O (b) and the Raman spectrum in D2O (c) and H2O (d). The spectra of bulk D2O and H2O are subtracted. The pH (pD) value is adjusted to 7. 3. 1. Assignment of Vibrational Bands The GSH molecule consists of four groups with a structure that strongly depends on the pH value (Fig. 1). The state of protonation has severe consequences on the number and position of vibrational bands in the infrared and Raman spectra. Therefore, the prerequisite condition of successfully applying vibrational spectroscopy to study a cadmium complex with a GSH molecule is the consistent assignment of infrared and Raman spectra (Fig. 2). MK nh; O y-Glu Cys Gly Figure 1. The structure of the GSH molecule in ionized form at pH 7. The common characteristic of these spectra is extensive band overlapping. We separated the overlapped bands by applying the band-fitting algorithm. The basis for the assignment of the component bands presented the spectra of auxiliary molecules (glutamic acid, glycine and cys-teine dipeptides, N-acetyl-L-cysteine, D-penicillamine and mercaptosuccinic acid), which possess only particular functional groups of interest. The detailed frequency tables and deconvolved spectra of the auxiliary molecules are added in the Supplementary file. The infrared vibrational bands in the spectra of GSH, N-acetyl-L-cysteine and D-penicillamine are associated with the carboxylic acid, amide, thiol and amino functional groups that were examined in acidic, neutral and alkaline pH values. We used the pKa values of the car- boxylic acid, thiol and amino functional groups determined by the NMR study of the aqueous solution of GSH28 and potentiometric measurement of penicillamine.29 The results of the curve-fitting procedure of IR and Raman GSH spectra at neutral pH in H2O and in D2O are presented in Figs. 3 and 4 and Table 1. The common spectral characteristic of the GSH molecule and model compounds containing the thiol gro- Table 1. The assignment and peak frequencies in cm-1 of GSH dissolved in H2O and D2O. The assignment of the bands in D2O is written in parentheses. t - vibration is weak or not active, * - vibration not assigned. Intensities: s-strong, m-medium and w-weak Assignation H2O (D2O) Infrared Raman vSH (vSD) t 2580s (1875s) Amide I (Amide I') 1646s (1638s) 1660s (1652s) SaSNH3+ (¿aND + ) 1630m (t) 1636w (t) VasCOO- 1616m 1621w 1595s 1590w Amide II (Amide II') 1555s (1474s) 1560w (1472s) SsNH3+ (8ND3+m) 1530m (t) t 8CH and CH2 1450m 1450m 1426m 1426s 1411m 1412s 1361m 1360s 1345m 1345s 1275w 1275m 1266w 1266m vsCOO- 1393s(Gly) 1393s(Gly) 1316m (Glu) 1316s(Glu) Amide III (Amide III') Pii 1305 (*) 1305 (*) «R 1298 (*) 1298 (*) P 1288 (*) 1288 (*) a) 1700 1600 1500 1400 1300 1200 wavenumber (cm1) b) Amide 1' >CtJO Amide ir SCH awj CH, .,000 (Glu) celculeied spectra fitted cu(v& XI (0 1700 1600 1500 1400 1300 1200 waven umber (cm1) Figure 3. Model bands in the infrared fingerprint region of the GSH spectra in H2O (a) and D2O (b), after subtraction of the spectrum of bulk water. The pH (pD) value is adjusted to 7. up is a band at 2580 cm-1 due to SH stretching vibration (Fig. 4a), which appears in acidic and neutral solutions. In the Raman spectrum, this band is always strong while the intensity in the infrared is variable and usually weak. Deuteration moves the v SD vibration to 1875 cm1. In acidic conditions, a carboxylic group vibration v C=O is identified as an intense band around 1730 cm-1 (Fig. 3). A feature that arises together with the C=O stretching band is the C-OH deformation near 1400 cm-1. The coupled C-O stretching mode absorbs predominantly in the 1250-1300 cm-1 region.30 This mode is located in the spectrum of N-acetyl-L-cysteine at 1286 cm-1 and moves to higher wavenumbers in the spectrum of D-peni-cillamine (1293 cm-1) and finally reaches 1311 cm-1 in the spectrum of GSH. A C=O stretching band is due to the de-protonation of a carboxylic group absent in neutral and basic solutions. The deprotonated state of the carboxylic acid groups in general gives rise to antisymmetric and symmetric stretching vibrations in the regions between 1550 cm-1 and 1620 cm-1 (vasCOO) and 1300 cm-1 and 1420 cm-1 (vsCOO-), respectively. The decomposed spectra revealed that antisymmetric vibrations of both car- boxylate ions in the GSH molecule are located in the infrared spectrum at 1616 cm-1 and 1595 cm-1 and in the Raman spectrum at 1621 cm-1 and 1590 cm-1, respectively.31'32 The assignment of both symmetric counterpart vibrations is not so evident.33 The assignment of corresponding vibration in the spectra of glutamic acid dipeptide and mercaptosuccinic acid was used to clarify the position of both stretchings. A significant change of band intensity in the region between 1400 cm-1 and 1315 cm-1 is observed in the spectra of mercaptosuccinic acid by changing the pH value from 2 to 7. Moreover, at pH 4.9, the glu-tamic acid dipeptide has an indicative band at 1317 cm-1 in the amide III region, which significantly loses intensity by reducing the pH value to 2.9.34 The same intensity changes were detected in GSH spectra upon changing the pH values. Therefore, we ascribe a band at 1316 cm-1 in the spectra of GSH with a neutral pH to symmetrical stretching of the COO- group from the glutamic acid side chain and a band at 1393 cm-1 to the same type of vibration of the C-terminal end of the GSH molecule. The a) 0.004 0 003 m (D c 0.002- ~ ra E ra ÙL 0.001 0000 2600 1700 1600 1500 1400 1300 1200 wavenumber (cm1) b) 0.000 1900 1800 1700 1600 1500 1400 1300 wavenumber (cm1) Figure 4. Model band components in the Raman fingerprint region of the GSH spectra in H2O (a) and D2O (b), after subtracting the spectra of bulk water. The pH (pD) value is adjusted to 7. bands are observed in same positions in the Raman spectra of GSH as well. A weak deformation band due to the NH3+ group vibration is expected at around 1600 cm-1 (¿asNH3+), with a more intense symmetrical counterpart in the region between 1500-1550 cm-1 (¿sNH3+).30 The assignment of these bands is hampered by their low intensity and overlap with stronger amide I and II bands. A relatively weak band found at 1530 cm-1 is assigned to the symmetric NH3+ deformation. The antisymmetric deformation is located at 1630 cm-1. This band is deprotonated in the basic solution, resulting in NH2. The latter group exhibits a scissoring mode around 1590-1650 cm-1.35 We found a broad band at 1560 cm-1 in GSH, which gains in intensity upon the deprotonation of the NH3+ group. Intense bands in the region between 1410 cm-1 and 1450 cm-1 and at around 1350 cm-1 were assigned to CH2 scissoring modes. The latter can also be assigned to CH or CH2 wagging modes.36 In accordance with the literature, we assign the band at 1270 cm-1 to CH and CH2 twisting.36 The most prominent bands in the spectra of GSH are the so-called amide I and amide II vibrations at 1646 cm-1 (Raman 1660 cm-1) and 1555 cm-1 (Raman 1560 cm-1), respectively. The amide III vibrations fall in region between 1308 and 1288 cm-1. The shape of the amide III band suggests a complex intrinsic structure, similar to one found in dipeptides.37 The important characteristic of these bands is connected to their sensitivity to backbone conformation. In general, the amide bonds in peptides and proteins have several vibrational modes, commonly referred as amide A, I, II and III.38,39 All amide bands are sensitive to the conformation of the backbone. However, the amide III bands are the most applicable for structural studies of the smallest peptides.34,37 The conformational sensitivity of the amide III band components has been proven by numerous experimental and theoretical studies.40-44 These studies show that the frequency of the amide III band depends on both dihedral angles. The band intensities of the amide III components in infrared and Raman spectra are thus indicators of the peptide backbone conformation. It has been shown that the most populated conformations of dipeptides in water are PII, p, and aR 34,37 Bands in similar positions to the spectra of dipeptides were also found in GSH spectra. With an analogy to dipeptides, we assign the band at 1305 cm-1 to the PII conformation, the band at 1298 cm-1 to the aR conformation and the band at 1288 cm-1 to the p conformation. Comparison of the area of particular band components re- vealed that the main population of the GSH backbone represents the p conformation. The results of conformational analysis of the GSH backbone are summarized in Fig. 5 and Table 2. To confirm the band positions of the amide vibrations, we dissolve GSH in deuterium oxide. The shifts of the amide I, II and III bands for the solution in D2O compared to the solution in H2O are in the accordance with the predictions. By dissolving GSH in D2O, an intense and sharp band appears at 1638 cm-1 (Raman 1652 cm-1) corresponding to the amide I' band. The small frequency change of amide I is due to the weak coupling between amide C=O stretching and NH deformation modes. A more significant shift is observed for the amide II band. It redshifts to 1474 cm-1. The shifted amide III' band was not identified. 3. 2. Binding Sites in the GSH Molecule Vibrational spectroscopy provides direct monitoring of the interaction between a metal and a GSH functional group.33 The most prominent change upon the addition of cadmium ions is the decreasing intensity of the v SH band presented in Fig. 6. The decrease in intensity indicates de-protonation due to the coordination of the thiol group with cadmium ions.35 A similar approach was used to confirm the interaction of Cu2+ and Co2+ ions with a reduced form of GSH molecules.45,46 Additional evidence of the interaction of cadmium ions with sulfur is the appearance of a band at 389 cm-1 in all complexes indicating a stretching vibration of the Cd-S group (v Cd-S). Other spectral changes due to interaction with cadmium ions are not so evident. The decomposition of amide III regions reveals changes in the intensity of the amide III band components and band location at 1316 cm-1 and assigned to the vsym COO- of the glutamic acid side chain (Fig. 5). From band intensity changes, it is evident that only a fraction of these COO- groups are involved in this type of interaction with cadmium ions. The level increases with the increase in the concentration of cadmium ions (Fig. 6). With a comparison of the band area of vas COO- at the beginning and at the molar ratio metal-ligand of 1, it can be roughly estimated that approximately two thirds of the glutamyl side chains interact with cadmium ions. The analysis of the amide III region reveals a distribution of conformations of the GSH backbone (Fig. 5). A GSH molecule has three amino acids where only glycine Table 2. Calculated distribution of conformations (%) of the GSH (0.5 M in H2O, pH 7) backbone with and without Cd2+ ions. For calculation, the amide III region from Raman spectra was applied. 0.5M GSH 0.0625M Cd2+ 0.125M Cd2+ 0.25M Cd2+ 0.5M Cd2+ P„ 15 13 25 27 55 «R 25 27 26 27 27 ß 60 60 49 46 18 Figure 5. Raman spectra of 0.5M GSM in water with added Cd2+. (a) no Cd2+, (b) 0.0625 M Cd2+, (c) 0.125 M Cd2+, (d) 0.25 M Cd2+ and (e) 0.5 M Cd2+ added. The meshed band is assigned to the vasCOO- vibration of glutamic acid side chain and the grey, blue and red bands to amide III components that belong to the Pn, aR and 5 conformation of the peptide backbone. and cysteine are linked by peptide bonds. Since two peptide bonds are present in the GSH molecule, we are not able to determine which amide III band component belongs to the vibration of a particular amino acid residue. Therefore, we can only attribute the observed changes in the calculated distribution of the conformations presented in Table 1 to the whole GSH molecule and not to a specific y map of a particular amino acid residue. However, the presented distribution of conformations for the GSH backbone reveals that interaction between the GSH molecule and Cd2+ ions has a severe influence on the GSH backbone conformations. The addition of metal ions substantially decreases the population of the 5 structure and gives rise to the Pn conformation. The portion of the aR conformation remains unaffected by cadmium ions (Table 2). 3. 3. The Interaction Between Cadmium Ions and the GSH Molecule Monitored by 1H and 13C NMR Spectroscopy The assignment of the 1H and 13C was checked by the 1H-13C correlations in the 2D gHSQC and gHMBC spectra. Spectra with corresponding assignment are presented in the supplementary file; in Fig. 7, only changes in the 1H and 13C chemical shifts induced by the presence of cadmium ions are presented. The most significant change in proton chemical shift after the addition of Cd2+ ions was observed for the GluHa, GluH5 and CysH5 protons Figure 6. The intensity change of the vSH stretching and vsymCOO- (Glu) as a function of the molar ration of GSH and Cd2+ ions at pH 7. (Fig. 7). The addition of Cd2+ ions also substantially alters the GluCOO- and CysCp resonance in the 13C spectra. Smaller shifts were observed for the 13C resonances of the GluCa and GluCp groups. The addition of one quarter of the equivalent of metal ions induced only minor changes in the 1H resonance. More significant are the changes to the 13C chemical shifts of the GluCOO-, GluCp and CysCp carbons. Upon further increasing the Cd2+ ratio, considerable deshielding of CysHp protons was observed. The addition of cadmium ions separates the two cysteine P protons, which are strongly overlapped in the spectrum of GSH alone. Deshielding is also observed for CysCp carbons. The pronounced deshielding of the CysHp proton upon the addition of a molar equivalent of cadmium ions indicates a strong interaction with Cd2+. This interaction is also reflected in the upfield shifts of GluHa protons and downfield shift of the GluHp protons. In the 1H spectrum, two well-separated glutamyl P protons were observed, while the GluHy and GlyHa protons show only negligible shifts. The 1H chemical shift of CysHp and 13C chemical shift of CysCp move linearly up to the equivalent molar concentration of cadmium ions and GSH. The large 13C GluCOO- chemical shift indicates the second binding side of cadmium ions in the GSH molecules. The variations in the chemical shifts in both the 13C and 1H spectra as a function of the molar ration between the cadmium ions and the GSH indicate that the optimal complex is formed between one cadmium ion and one GSH molecule. This prediction is confirmed by a Jobs plot47 presented in Fig. 8. From this plot, it is evident that the metal-ligand stoichiometry is 1. Figure 7. 13C (left) and 'H (right) chemical shift changes monitored from the 'H and 13C GSH spectra induced by the addition of different equivalents of Cd2+. The concentrations of GSH were 20 mM. Figure 8. Jobs-plots for the interaction of GlyHa with Cd2+. The total molarity of the metal and ligand was 20 mM. 3. 4. Conformation of the GSH Backbone Determined by 3J(Ha, NH) Coupling Constant The 3J(Ha, Nh) coupling constant was efficiently used for determining the distribution of backbone conformations.48 The vicinal coupling constants of glycine and cysteine residues are presented in Fig. 9. As expected, the interaction between GSH with cadmium ions mainly perturbed the cysteine vicinal coupling constant. The initial value of the 3J(Ha, NH) coupling constant of the cysteine residue (7.64 Hz) monotonically decreased to 7.16 Hz after the addition of Cd2+ ions. The trend of the vicinal coupling constant to lower values indicates the decrease in the population of the P structure of the glutamine backbone. It has to be emphasized that the initial value cysteine coupling constant found in the GSH spectrum is larger for 0.34 Hz than the same coupling constant found in cysteine dipeptide48 or GGCysGG blocked peptides.49 The value of the measured coupling constant is comparable with the value of the coupling constant of the histi-dine dipeptide (7.76 Hz), which is known to possess a backbone conformation predominantly in the P structure.48 The application of glycine vicinal constants for conformational studies is more complicated since the glycine y map is complex. Moreover, the value of the glycine vicinal constants alternate with respect to the addition of cadmium ions. Figure 9. The 3/(Ha, NH) coupling constant of GSH at pH 4.5. The concentrations of GSH were 20 mM. All the spectra were recorded in 90% H2O/ 10% D2O at 30 °C. 4. Conclusions We have demonstrated by the application of infrared, Raman, and 13C experiments that cadmium ions interact predominantly with the thiol group of cysteine residue and the ionized carboxylic group from the side chain of the glutamyl residue. The binding analysis between GSH and Cd2+ demonstrates that the chelating abilities of the GSH molecule is intimately associated with the SH group. The broadening of the cysteine P proton after cadmium addition suggests the existence of an exchange process involving the metal ion and the cysteine residue. The decreasing intensity of the SH stretching band with the addition of Cd2+ ions supports the thesis that this group is the primary binding site. Another important functional group that contributes to the formation of Cd-GSH complexes, are glutamyl car-boxyl group. The analyses of 1H and 13C resonance showed a broadening of glutamyl a and P protons and GluCOO- carbon after cadmium addition. The interaction of cadmium is also reflected in the changing of the chemical shifts of particular protons and carbon atoms. Additional confirmations of the presence of the second interaction site are decomposed Raman spectra. These spectra are indicative that addition of the Cd2+ ions substantially decreases the band area of the glutamyl COO- side chain group. The functional groups in the GSH molecule involved in the coordination of metal ions have been established from changes in the chemical shifts of groups close to the binding site and changes in intensities in the vibra-tional spectra. Following the concentration measurements and corresponding spectral changes indicates that at physiological pH values, the 1:1 complex is the dominant form. Our results indicate that both thiol and glutamyl car-boxyl groups are essential for the formation of a tight cad-mium-peptide complex. This conclusion is in agreement with the result presented by Satofuka and coworkers.50 Negatively charged carboxyl groups in the peptide stabilize the cadmium-peptide complexes by interacting with positively charged Cd2+.50 The formation of metal complexes has a strong influence on the GSH structure. Interaction with cadmium ions induced a conformational change in the cysteine side in the GSH molecule, where the population of the P structure is reduced upon the addition of the cadmium ions. The decrease of the P structure upon interaction was observed in the diminishing of the cysteine vicinal constant and the reduction of the area of the amide III band component assigned to this structure. Concomitant to this reduction, the area of the band characteristic for the PII structure increases. Conformational changes of GSH induced by binding of cadmium ions may result in malfunction of the GSH molecule which results in impairment of its biochemical and signaling functions in the plant cell and consecutive development of toxicity symptoms. Conformati- onal changes of GSH after the binding of cadmium may also partly explain the lack of phytochelatin synthesis in hyperaccumulating plants. When cadmium ions enter the symplast in concentrations typical for hyperaccumulating plants, the pool of functional GSH molecules decreased resulting in deficiency of precursors required for phy-tochelatin synthesis. 5. Acknowledgment This work was supported by the grant from the Ministry of Education, Science, Culture and Sport of Republic of Slovenia 6. References 1. D. Mendoza-Cozatl, H. Loza-Tavera, A. Hernandez-Navarro, R. Moreno-Sanchez, Fems Microbiol. Rev. 2005, 29, 653-671. 2. G. Noctor, A. Mhamdi, S. Chaouch, Y. Han, J. Neukermans, B. Marquez-Garcia, G. Queval, C. H. Foyer, Plant Cell Environ. 2012, 35, 454-484. 3. W. Bae, R. K. Mehra, J. Inorg. Biochem. 1997, 68, 201-210. 4. M. J. May, T. Vernoux, C. Leaver, M. Van Montagu, D. Inze, J. Exp. Bot. 1998, 49, 649-667. 5. S. Clemens, Planta 2001, 212, 475-486. 6. J. L. Freeman, D. Garcia, D. G. Kim, A. Hopf, D. E. Salt, Plant Physiol. 2005, 137, 1082-1091. 7. B. Leitenmaier, H. Kupper, Plant Cell Environ. 2011, 34, 208-219. 8. W. E. Rauser, Plant Physiol. 1995, 109, 1141-1149. 9. C. Cobbett, P. Goldsbrough, Annu. Rev. Plant Biol. 2002, 53, 159-182. 10. M. Mejare, L. Bulow, Trends Biotechnol. 2001, 19, 67-73. 11. T. Maitani, H. Kubota, K. Sato, T. Yamada, Plant Physiol. 1996, 110, 1145-1150. 12. J. J. Chen, J. M. Zhou, P. B. Goldsbrough, Physiol. Plantarum 1997, 101, 165-172. 13. J. L. Hall, J. Exp. Bot. 2002, 53, 1-11. 14. J. A. Deknecht, M. Vandillen, P. L. M. Koevoets, H. Schat, J. A. C. Verkleij, W. H. O. Ernst, Plant Physiol. 1994, 104, 255-261. 15. S. Ebbs, I. Lau, B. Ahner, L. Kochian, Planta 2002, 214, 635-640. 16. H. Harmens, P. R. Denhartog, W. M. Tenbookum, J. A. C. Verkleij, Plant Physiol. 1993, 103, 1305-1309. 17. J. Hernandez-Allica, C. Garbisu, J. M. Becerril, O. Barrutia, J. I. Garcia-Plazaola, F. J. Zhao, S. P. Mcgrath, Plant Cell Environ. 2006, 29, 1422-1429. 18. Q. Sun, Z. H. Ye, X. R. Wang, M. H. Wong, J. Plant Physiol. 2007, 164, 1489-1498. 19. B. J. Fuhr, D. L. Rabenstein, J. Am. Chem. Soc. 1973, 95, 6944-6950. 20. V. Dorcak, A. Krezel, Dalton Transactions 2003, 2253-2259. 21. Z. S. Li, Y. P. Lu, R. G. Zhen, M. Szczypka, D. J. Thiele, P. A. Rea, P. Natl Acad. Sci. USA 1997, 94, 42-47. 22. P. Leverrier, C. Montigny, M. Garrigos, P. Champeil, Anal. Biochem. 2007, 371, 215-228. 23. O. Delalande, H. Desvaux, E. Godat, A. Valleix, C. Junot, J. Labarre, Y. Boulard, Febs J. 2010, 277, 5086-5096. 24. U. Opara-Krasovec, R. Jese, B. Orel, J. Grdadolnik, G. Drazic, Monatshefte Fur Chemie 2002, 133, 1115-1133. 25. B. Grobelnik, J. Grdadolnik, Acta Chim. Slov. 2008, 55, 978-984. 26. J. E. Bertie, Z. D. Lan, J. Chem. Phys. 1996, 105, 85028514. 27. J. E. Bertie, H. H. Eysel, Appl. Spectrosc. 1985, 39, 392401. 28. D. L. Rabenstein, J. Am. Chem. Soc. 1973, 95, 2797-2803. 29. T. Zucconi, G. Janauer, S. Donahe, Abstr. Pap. Am. Chem. Soc. 1977, 174, 36-36. 30. J. F. Pearson, M. A. Slifkin, Spectrochim. Acta A 1972, A 28, 2403-&. 31. S. Y. Venyaminov, N. N. Kalnin, Biopolymers 1990, 30, 1243-1257. 32. W. W. Wright, J. M. Vanderkooi, Biospectroscopy 1997, 3, 457-467. 33. L. L. Schevchenko, Russian Chemical Reviews 1963, 32, 201-207. 34. J. Grdadolnik, V. Mohacek-Grosev, R. L. Baldwin, F. Avbelj, P. Natl Acad. Sci. USA 2011, 108, 1794-1798. 35. L. J. Bellamy, The Infrared Spectra of Complex Molecules, Chapman and Hall, London, 1975. 36. N. B. Colthup, L. H. Daly, S. E. Wiberley, Introduction to Infrared and Raman Spectroscopy, Third Edition, Academic Press, 1990. 37. J. Grdadolnik, S. G. Grdadolnik, F. Avbelj, J. Phys. Chem. B 2008, 112, 2712-2718. 38. S. Krimm, J. Bandekar, Adv. Protein Chem. 1986, 38, 181364. 39. A. Barth, C. Zscherp, Q. Rev. Biophys. 2002, 35, 369-430. 40. J. Bandekar, Biochim. Et Biophys. Acta 1992, 1120, 123143. 41. T. M. Watson, J. D. Hirst, J. Phys. Chem. A 2002, 106, 78587867. 42. F. N. Fu, D. B. Deoliveira, W. R. Trumble, H. K. Sarkar, B. R. Singh, Appl. Spectrosc. 1994, 48, 1432-1441. 43. R. C. Lord, Appl. Spectrosc. 1977, 31, 187-194. 44. T. M. Watson, J. D. Hirst, Phys. Chem. Chem. Phys. 2004, 6, 998-1005. 45. B. K. Singh, R. K. Sharma, B. S. Garg, Spectrochim. Acta A 2006, 63, 96-102. 46. D. N. Kumar, B. K. Singh, B. S. Garg, P. K. Singh, Spectrochim. Acta A 2003, 59, 1487-1496. 47. C. S. Wilcox, in: H. J. Schneider, H. Durr (Ed.): Frontiers in Supramolecular Chemistry and Photochemistry, VCH, Weinheim, Germany, 1991. 48. F. Avbelj, S. G. Grdadolnik, J. Grdadolnik, R. L. Baldwin, P Natl. Acad. Sci. USA 2006, 103, 1272-1277. 49. K. W. Plaxco, C. J. Morton, S. B. Grimshaw, J. A. Jones, M. Pitkeathly, I. D. Campbell, C. M. Dobson, J. Biomol. Nmr 1997, 10, 221-230. 50. H. Satofuka, T. Fukui, M. Takagi, H. Atomi, T. Imanaka, J. Inorg. Biochem. 2001, 86, 595-602. Povzetek Glutation je najbolj razširjenamajhna molekula v bioloških celicah z veliko afiniteto vezave s kovinskimi ioni. Teoretično ima molekula glutationa osem funkcionalnih skupin, ki lahko sodelujejo pri vezavi s kovinskimi ioni. Z analizo infrardečih in ramanskih spektrov ter 13C in NMR spektrov smo pokazali, da sta v kompleksacijo s Cd ioni udeleženi le dve skupini; tiolna in glutamilna karboksilna skupina. Za natančno asignacijo vibracijskih spektrov glutationa in koordinacije s kovinskimi ioni smo uporabili serijo modelnih spojin (D-penicilamin, dipeptide glicina, cisteina in glutaminske kisline ter merkaptosukcinsko kislino in N-acetil-L-cistein). Koncentracijsko odvisne meritve s Cd ioni pokažejo, da je optimalno stehiometrijsko razmerje z glutationom 1:1. Analiza 3J(Ha, HN) sklopitvenih konstant in kon-formacijsko odvisnih trakov v amidnem III območju v vibracijskih spektrih pokaže, da se z vezavo Cd ionov spremeni tudi konformacija glutationskega skeleta. Kompleksacija inducira prehod iz pretežno ¡5 strukture v Pn konformacijo.