Open Access Article
Parastoo
Vahdatiyekta
a,
Mohammed
Zniber
a,
Kostiantyn
Nikiforow
b and
Tan-Phat
Huynh
*a
aLaboratory of Molecular Science and Engineering, Åbo Akademi University, 20500 Turku, Finland. E-mail: tan.huynh@abo.fi
bInstitute of Physical Chemistry, Polish Academy of Sciences, 01-224 Warsaw, Poland
First published on 23rd April 2024
The synthesis of N,N′-bis(2-thienylmethylene)-1,2-diaminobenzene, N,N′-bis(2-thienylmethylene)-1,3-diaminobenzene, and N,N′-bis(2-thienylmethylene)-1,4-diaminobenzene, three isomers with the molecular formula of (C16H12N2S2) and their metal complexation with Co(II), Fe(III), and Ni(II) is reported in this study. The formation of the ligands and their metal complexes, along with their physicochemical behaviors, are confirmed and characterized using electrochemical and spectroscopic techniques. The coordination chemistry and stoichiometry of the ligand–metal complexes are investigated using UV-vis absorption spectral titration, which reveals that the ligand-to-metal ratio varies from 3
:
1 to 4
:
1 in different cases. The calculated binding constants based on these spectroscopic data, ranging between 103 M−1 and 108 M−1, indicate the isomers' high affinity for the metal ions. Experimental data show that the nitrogen atoms from the azomethine linkage play an important role in coordinating with the metal ions. This observation supports findings reported in the literature for some studied Schiff base ligands.
O group of the carbonyl compound is typically replaced by a C
N–R group through a nucleophilic addition reaction, where R can be aryl or alkyl groups. In this mechanism, the elimination of water during the acid-catalyzed reversible reaction determines the reaction rate, and Schiff bases typically form under neutral conditions,2 but the process is often accelerated by heating or adding an acid catalyst.3 The reaction yields an imine (azomethine) and water as a by-product. In comparison, Schiff bases with aryl substituents exhibit significantly greater stability and ease of synthesis than those with alkyl substituents. Furthermore, Schiff base compounds from aliphatic aldehydes are usually less stable and can easily polymerize, while aromatic aldehydes lead to more stable compounds because of conjugation.3 Functionally substituted Schiff bases, containing additional donor groups, are among the most important heteropolydentate ligands, capable of forming complexes ranging from mononuclear to polynuclear with metal ions.4 Most resulting imines use nitrogen lone pair electrons to bind to metal ions.5 These ligands interact with almost all metal ions to form stable complexes, where ligands are Lewis bases and donate electrons to metal ions, which are Lewis acids. These complexes play a significant role in various fields, including organic and inorganic chemistry, biochemistry,6 and supramolecular chemistry.7 At high temperatures and in the presence of moisture, many Schiff base complexes exhibit catalytic activity which is entirely dependent on metal ions, the type of ligands, and the coordination sites. For example, Schiff base complexes of Co(II)8 showed a profound catalytic effect in the ring-opening of large cycloalkanes, which is a usually complicated process. Cobalt Schiff base complexes have drug properties like antiviral drugs, and chloro(pyridine)cobaloxime is also a well-known model of coenzyme vitamin B12.9 The Ni(II) and Cu(II) complexes in the alkylation reaction of enolates exhibited high activity and stereoselectivity.10–12 For cyclic ester polymerization, aluminum complexes have a high catalytic conversion.13,14 Also, as an example, the Fe(III) of pyridine bis(imine) ligands had significant activity and a high yield in the polymerization of ethylene.15 Schiff bases ligands and their metal complexes have been discovered to possess biological activities,16 such as anticonvulsant, antibacterial,17,18 antimicrobial,19 anti-inflammatory,20 antimalarial,16 anti-tumor,21 anti-HIV,22 anticancer,23 antifungal properties,24 and enzyme immobilization ability.25 The presence of donor atoms, azomethine linkages, and conjugated double bonds in the structure of these organic compounds contributes to their biological functions and industrial applications. Additionally, these compounds are well-known for their role as metal corrosion inhibitors.26 π-conjugated Schiff bases are interesting materials because of their straightforward synthesis, environmental stability, and electrical and optical properties, which have made them useful in electrochemical and non-linear optical devices,27 actuators,28 supercapacitors,29 solar cells,30 anti-corrosion coatings,31 sensors,32 electrochromic devices,33 and batteries.34 They can even be used in Dielse–Alder reactions.35 Last but not least are applications of Schiff base complexes with transition metals as sensing material for selective or non-selective (e-tongue) chemical or electrochemical sensors.36–41 In this study, we have reported Schiff base condensation of o-pheneylediamne, m-pheneylediamne, and p-phenylenediamne with 2-thiophenecarboxaldehyde. These reactions have been characterized using electrochemical techniques such as cyclic voltammetry and spectroscopic techniques like, Fourier-transform infrared spectroscopy (FT-IR), Raman spectroscopy, proton nuclear magnetic resonance (1H-NMR) spectroscopy, gas chromatography–mass spectrometry (GC-MS), and UV-visible (UV-vis) spectrophotometry. Afterward, we studied the complexation of each isomer with transition metals, including Co2+, Fe3+, and Ni2+, and calculated the binding constants.
:
1. 2-Thiophenecarboxaldehyde (0.02 mol, 1.869 ml) was added to a stirred ethanol solution of phenylenediamine isomers (0.01 mol, 1.0814 g). The reaction mixture was stirred vigorously (∼700 rpm) with a magnetic stirrer for about 3 h at room temperature (RT∼25 °C).42 Two or three drops of acetic acid may serve as a catalyst to enhance the reaction rate and precipitate formation. The completion of the reaction was determined using thin-layer chromatography (TLC). The resulting light-yellow colored precipitate was collected by filtration through a Buchner funnel, washed with cold ethanol, and dried in a vacuum desiccator. Then, the o-BTMD and m-BTMD products were recrystallized from ethanol and dried at room temperature, resulting in yields of 65% and 50%, respectively. Unlike the other isomers, p-BTMD was obtained without recrystallization process with a yield of 70%. The chemical structures of BTMDs (Fig. S1, ESI†), with a molecular mass of approximately 296 g mol−1, were confirmed by mass spectrometry and NMR and further characterized by XPS, Raman, FT-IR, and UV-vis spectroscopy, and CV. The information related to the characterization of BTMD isomers is summarized here, with figures provided in the ESI.†
Then, the metal salt solution (0.25 × 10−2 M) was used as a titrant. In the molar ratio method,43 the BTMD concentration was maintained constant while the concentration of the metal ion (with Co(II), Fe(III), and Ni(II)) was varied to cover the range of molar ratios [M]
:
[ligand] from 0.16 to 0.52. The spectra of all prepared solutions of BTMDs and complexes were recorded within the wavelength range of 200–700 nm. The UV-vis spectrum was recorded after each addition to monitor the progress of the complexation reaction during the titration.
N–) protons, downfield doublets, triplets or multiplets attributed to the resonance of aromatic (HAr) and heterocyclic protons in the range of 7–7.8 ppm.42,44–46 According to mass spectra of isomers, ESI-MS (m/z) was calc.: 296.41: found: ∼296 with different retention times of 18.9, 19.9, and 20.1 minutes for o-, m- and p-BTMD, respectively (Fig. S2–S4, ESI†). Further characterizations of BTMDs using FT-IR and Raman spectroscopy (Fig. 2) show a good agreement with proposed chemical structures. Details of bonding analysis are shown in Table S1 (ESI†). In NMR spectra of metal complexes (Fig. S5, ESI†), the azomethine proton peaks of BTMDs with Co(II), Ni(II) slightly shifted, but in complexes with Fe(III), especially in the case of o-BTMD, where changes are more pronounced, proton peaks of azomethine noticeably shifted downfield. In the literature, peak shifting is often attributed to several phenomena, including the formation of metal complexes, configurational changes within complexes that differ from the free ligands, the deshielding of protons due to coordination with metal ions, and the deprotonation of ligands. These interactions can significantly alter the electronic environment around the absorbing species, leading to observable shifts in NMR peaks.47 Significant variations are observed in the behavior of Fe(III) in the ortho- and meta-positions compared to other metal ion complexes. The NMR peaks of heterocyclic protons stayed partially unchanged. This can be attributed to their distance from the metal–ligand binding sites. A trend of line broadening is also seen from the spectrum of the free ligands to the metal complexes. In NMR spectroscopy, when comparing the spectra of a ligand to its metal complexes, line broadening in the metal complexes can often be attributed to the presence of unpaired electrons associated with a paramagnetic metal ion.
![]() | ||
| Fig. 1 (a)–(c) 1H-NMR of (A) o-BTMD, (B) m-BTMD, and (C) p-BTMD in DMSO-d6 and (D) UV-vis spectra of these isomers with the concentration of 10−5 M in acetonitrile. | ||
UV-vis absorption spectroscopy was used to study optical properties of BTMDs and their complexes (Fig. 1D and Table 1). According to UV-vis spectra of ligands, o-BTMD showed absorption at 265, 293(λmax), 339 nm,44m-BTMD absorptions happened at 233, 270, 309(λmax), 323 nm and p-BTMD had absorption at 249, 272, 300, and 365 nm (λmax), where λmax is the maximum absorption wavelength.48 In the structure of BTMDs, the presence of aromatic rings and imine groups primarily results in π → π* electronic transitions, which are typically observed in the UV region, around 260–290 nm. Additionally, the ligand possesses lone pairs on nitrogen and sulfur atoms, introducing n → π* transitions that appear at longer wavelengths, approximately in the range of 300–470 nm. When comparing isomers, it is notable that variations in λmax can be observed, which can be attributed to changes in the conjugation length of the isomers. This trend can also be seen in other molecules with ortho, meta, and para substituents.49,50 Regarding the metal complexes of BTMDs, most displayed new peaks with lower absorbance in their UV-vis spectra at wavelengths greater than 360 nm. These peaks can be associated with ligand-to-metal charge transfer (LMCT) transitions51,52 and d–d transition.53,54 Almost all the metal complexes displayed shifts in their UV-vis spectra upon complexation, with some peaks showing a redshift (bathochromic shift) and others a blueshift (hypsochromic shift). An increase in peak intensity, especially for these shifted peaks, can be linked to ligand–metal coordination.55–57
| Compounds | Absorption bands(nm) | |
|---|---|---|
| Blue/red shift | New bands | |
| o-BTMD (free ligand) | 265, 293(λmax), 339 | — |
| [Co(o-BTMD)3]2+ | 261(λmax), 293, 344 | 570, 610, 680 |
| [Fe(o-BTMD)3]3+ | 242(λmax), 315, 360 | 420 |
| [Ni(o-BTMD)3]2+ | 260(λmax), 292, 363 | — |
| m-BTMD (free ligand) | 232, 270, 309(λmax), 323 | — |
| [Fe(m-BTMD)3]3+ | 241(λmax), 310 | 460 |
| [Ni(m-BTMD)4]2+ | 262, 309, 323(λmax) | — |
| p-BTMD (free ligand) | 249, 272, 300, 365(λmax) | — |
| [Co(p-BTMD)3]2+ | 230, 260, 300, 365(λmax) | 570, 616, 680 |
| [Fe(p-BTMD)3]3+ | 241(λmax), 295, 306, 364 | 422 |
| [Ni(p-BTMD)3]2+ | 249, 267, 297, 366(λmax) | — |
The energy gap between the HOMO and LUMO indicates the molecular chemical stability of compounds, reflecting their chemical hardness or softness.58 The HOMO and LUMO levels, often referred to as the bandgap, can be determined using the Tauc plot method.59 Tauc plot method (eqn (S1) and (S2), ESI†) is frequently employed to calculate both direct and indirect energy gaps of molecules based on their UV-vis spectra. The determination of bandgap values is essential in understanding a compound's intrinsic properties, including the optical absorption characteristics and the electrical conductivity inherent to organic semiconductors, such as Schiff base compounds.56 The bandgap value (Eg) was determined by identifying the point of intersection between the extended linear portion of the (αhυ)n plot and the hυ (photon energy) axis on the abscissa. Fig. S6 and S7 (ESI†) illustrate the plots of (αhυ)2 and (αhυ)0.5versus hυ, respectively, demonstrating the determination of bandgap for all isomers. The (αhυ)2vs. hυ plot reveals that BTMDs possess a direct optical bandgap, with values of 3.14 eV, 3.35 eV, and 3.05 eV for o-BTMD, m-BTMD, and p-BTMD, respectively, as seen in Fig. S6 (ESI†). Additionally, the (αhυ)0.5vs. hυ plot displays a more pronounced linear section for BTMDs, verifying the presence of an indirect optical transition in the isomers. Linear extrapolation to the x-axis yields indirect bandgaps of 2.85 eV, 3.06 eV, and 2.78 eV for o-BTMD, m-BTMD, and p-BTMD, respectively, as shown in Fig. S7 (ESI†). Based on the calculated bandgap values, BTMDs can be classified as organic semiconductors.60,61 The bandgap values of Schiff base complexes, as determined by the Tauc plot method (Fig. S8–S13, ESI†), are presented in Table 2. The data suggests that metal complexation reduces the bandgap in several complexes.62 This reduction in bandgap might be associated with changes in the stability of the Schiff base ligands.
| Compounds | Bandgap values | |
|---|---|---|
| Direct (eV) | Indirect (eV) | |
| o-BTMD (free ligand) | 3.14 | 2.85 |
| [Co(o-BTMD)3]2+ | 3.81 | 2.92 |
| [Fe(o-BTMD)3]3+ | 3.50 | 2.49 |
| [Ni(o-BTMD)3]2+ | 3.81 | 2.64 |
| m-BTMD (free ligand) | 3.35 | 3.06 |
| [Co(m-BTMD)3]2+ | 3.29 | 3.02 |
| [Fe(m-BTMD)3]3+ | 3.13 | 2.75 |
| [Ni(m-BTMD)4]2+ | 3.34 | 3.05 |
| p-BTMD (free ligand) | 3.05 | 2.78 |
| [Co(p-BTMD)3]2+ | 2.91 | 2.38 |
| [Fe(p-BTMD)3]3+ | 2.70 | 2.34 |
| [Ni(p-BTMD)3]2+ | 3.01 | 2.80 |
XPS deconvoluted spectra of the BTMD isomers are presented in Fig. 3. Presence of the carbon, nitrogen, and sulfur is discovered. Analysis of the high-resolution C 1s core level spectra shows three component peaks, for instance, at around 284.7, 285.4, and 286.4 eV for m-BTMD molecule. Those could be attributed to C
C, C–C/C–H, C–N\C–S carbon bounds in BTMDs;48,63,64 particularly, the peak at 286.8 eV is prominent for o-BTMD. The N 1s core level spectra of the isomers can be deconvoluted into three environments: imine N (399 and 400 eV) and protonated imine N+ (402.4 eW).48,65,66 Protonated imine peak could have been formed in the polymers due to surface oxidation products.67 Due to spin–orbit splitting, the S 2p spectrum appears as a doublet. High-resolution spectra were fitted with 2 S 2p doublets with the S 2p3/2 positions of 164.4 and 165.1 eV with a ratio of 2
:
1 (S 2p3/2 to S 2p1/2), spin–orbit splitting of 1.2 eV and the same full width at half maximum. Bigger intensity doublet at lower binding energy is ascribed to thiophene-type sulfur.48,68 Second doublet at higher energy could be attributed to an oxidized sulfur species, which means that some sulfur atoms carry a partial positive charge.63
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| Fig. 3 High-resolution XPS scan spectra over (A) C 1s, (B) N 1s, and (C) S 2p peaks of the o-, m- and p-BTMD samples. | ||
The Beer–Lambert plots for BTMD isomers are presented in Fig. S14 (ESI†). Subsequently, the concentration of the complex and its binding constant were calculated using the provided formulas (eqn (2) and (3)), respectively.
| A = εbc | (1) |
![]() | (2) |
![]() | (3) |
The binding constant values were calculated for ligands, Co(II), Fe(III) and Ni(II) complexes using the equations above. The results revealed that the binding constants of the metal complexes with Schiff base ligands have the following order Co(II) < Ni(II) < Fe(III) in o-BTMD complexes, Fe(III) < Ni(II) for m-BTMD complexes and Fe(III) < Co(II) < Ni(II) in p-BTMD complexes.57 Greater K values indicate stronger binding of a complex.70
| Compounds | E pa (V) | E pc (V) |
|---|---|---|
| o-BTMD | 0.9, 1.27, 1.46 | 1.3 |
| [Co(o-BTMD)3]2+ | 1.29 | — |
| [Fe(o-BTMD)3]3+ | 1.31 | — |
| [Ni(o-BTMD)3]2+ | 1.27, 1.47 | — |
| m-BTMD | 0.96, 1.48, 1.67 | — |
| [Co(m-BTMD)3]2+ | 0.91, 1.43 | — |
| [Fe(m-BTMD)3]3+ | 0.68, 0.9, 1.2 | 1.1 |
| [Ni(m-BTMD)4]2+ | 0.9, 1.45 | — |
| p-BTMD | 0.78, 1.28, 1.4 | — |
| [Co(p-BTMD)3]2+ | 0.68, 1.22 | — |
| [Fe(p-BTMD)3]3+ | 0.73, 1.3 | 1.2, 0.32 |
| [Ni(p-BTMD)3]2+ | 0.66, 1.18 | 1.1, 0.32 |
Several factors influence the electrochemical properties of metal complexes, including substitution pattern,72 degree and distribution, degree and unsaturation,73,74 axial ligation,75 chelate ring size,76 coordination number, and charge type.77 Most BTMD metal complexes exhibit electroactivity in both the ligands and the central metal ion. All relevant electrochemical data of BTMDs and their metal complexes are provided in Table 3. No significant changes were observed for complexes of all BTMDs with Co(II) and Ni(II), this is likely due to their low binding constants, especially in the complexes involving o- and p-BTMDs. Additionally, the electrochemical oxidation of Co2+ to Co3+ occurs at a much higher potential (>2.0 V) than what was used in our study. Meanwhile, Ni2+ is electrochemically stable and is rarely oxidized to a higher oxidation state. In Fe(III) complexes, the oxidation peaks shifting to more positive potentials indicate that the free ligands undergo oxidation more readily than their corresponding complexes. In the [Fe(p-BTMD)3]3+ complex, the quasi-reversible redox couple characterized by an anodic peak at Ea = 0.73 V, and a cathodic peak at Ec = 0.32 V can be attributed to the redox process. Conversely, this redox process exhibits irreversible behavior in the [Fe(m-BTMD)3]3+ complex with an anodic peak at Ea = 0.68 V, and no corresponding peaks are observed for the [Fe(o-BTMD)3]3+ complex. The variations in redox potentials for Fe(III) when complexed with o-, m-, and p-BTMD align well with their respective binding constants. Notably, the [Fe(o-BTMD)3]3+ complex exhibits the highest binding constant.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ma01179h |
| This journal is © The Royal Society of Chemistry 2024 |