Mouhieddinne Guergueba,
Soumaya Nasri*b,
Jihed Brahmia,
Frédérique Loiseauc,
Florian Moltonc,
Thierry Roisneld,
Vincent Guerineaue,
Ilona Turowska-Tyrkf,
Kaïss Aouadig and
Habib Nasria
aUniversity of Monastir, Laboratoire de Physico-chimie des Matériaux, Faculté des Sciences de Monastir, Avenue de l'environnement, 5019 Monastir, Tunisia
bDepartment of Chemistry, College of Science Al-Zulfi, Majmaah University, Saudi Arabia. E-mail: soumaya.n@mu.edu.sa; Fax: + 966 0164044044
cDépartement de Chimie Moléculaire, Université Grenoble Alpes, 301 rue de la Chimie, CS 40700, 38058 Grenoble Cedex 9, France
dInstitute of Chemical Sciences of Rennes, UMR 6226, University of Rennes 1, Beaulieu Campus, 35042 Rennes, France
eInstitut de Chimie des Substances Naturelles CNRS, Avenue de la Terrasse, F-91198 Gif-sur-Yvette, France
fFaculty of Chemistry, Wrocław University of Technology, Wybrzeże Wyspiańskiego 27, 50-370 Wrocław, Poland
gDepartment of Chemistry, College of Science, Qassim University, Buraidah 51452, Saudi Arabia
First published on 14th February 2020
To examine the influence of both the important π-acceptor character of the 4-cyanopyridine ligand and the nature of the para-substituted phenyls of meso-porphyrins on the electronic, electrochemical and structural properties of cobaltous metalloporphyrins, we prepared and fully characterized two coordination compounds: the (4-cyanopyridine)[meso-tetra(para-methoxyphenyl)porphyrinato]cobalt(II) and the (4-cyanopyridine)[meso-tetra(para-chlorophenyl)porphyrinato]cobalt(II) with the [CoII(TMPP)(4-CNpy)] and [CoII(TClPP)(4-CNpy)] formulas (complexes 1–2). The solution structures of compounds 1–2 were confirmed by 1H NMR spectroscopy and mass spectrometry methods. They were further characterized by cyclic voltammetry and photoluminescence studies. The X-ray molecular structure data show that the Co-TClPP-4-NCpy derivative (2) exhibits high ruffling deformation compared to that of the Co-TMPP-4-CNpy species (1). Notably, the crystal packing of complex 1 shows the formation of Co⋯Co supramolecular dimers with a distance of 5.663 Å. As an application of our two cobaltous compounds, an investigation involving complexes 1–2 in the degradation of the methylene blue dye in the presence and absence of H2O2 in aqueous solutions was carried out. These promising results show that 1–2 can be used as catalysts in the degradation processes of dyes.
It is noteworthy that the interaction of metalloporphyrins with neutral or anionic species via axial coordination plays an important role in the structural, electronic, magnetic and physical properties of these coordination compounds. The most studied of these species are the ones with iron and zinc as center metals. Cobalt metalloporphyrins have been less studied so far, but interest in them is growing and so are their reports in literature. Cobalt(II) porphyrin complexes are paramagnetic and have the 3d7 electron configuration in the ground state. These cobaltous species are much more stable than the iron(II) metalloporphyrins17 and are very easy to prepare compared to the ferrous metalloporphyrins. Early EPR investigations16,18,19 indicated that these Co(II) species are low-spin (S = 1/2) in that the unpaired electron is located in the axial dz2 orbital (2A1 state). These electronic properties of cobaltous complexes is the principal reason why Co(II) porphyrin complexes are increasingly investigated and their application fields are becoming wider.7,20
In continuation of our investigations on metalloporphyrins, we report herein the preparation and the characterization of two cobaltous porphyrin complexes involving the 4-cyanopyridine (4-CNpy) N-donor axial ligand and the two meso-porphyrins with either the phenyl para-substituted methoxy group or chlorine atom, namely the meso-tetra(para-methoxyphenyl)porphyrin (H2TMPP) and the meso-tetra(para-chlorophenyl)porphyrin (H2TClPP). The principal goal of this work is to study the electronic and the structural effects when the 4-cyanopyridine axial ligand, known to have a very important π-acceptor character, reacts with the two starting material tetracoordinated cobaltous complexes with a meso-porphyrinato para-substituted with a good donor OMe group (TMPP porphyrinato) and with a meso-porphyrinato para-substituted with the acceptor chlorine atom (TClPP moiety).
Many studies on the 4-cyanopyridine ion iron(III) ion complex types [FeIII(Porph)(4-CNpy)2]+, using the following four meso-porphyrins: (1) the unsubstituted meso-tetraphenylporphyrin (H2TPP), (2) the methyl para-substituted meso-porphyrin (the meso-tertratolylphenylporphyrin H2TTP), (3) the 2,3,4-methyl para-substituted meso-porphyrin (the meso-tetramesitylporphyrin H2TMP) and (4) the OMe para-substituted meso-porphyrin (H2TMPP) have been carried out.21,23 For these ferric low-spin metalloporphyrins, the very high ruffling of the porphyrin is related to the important π-acceptor character of the 4-CNpy axial ligand. Thus, it has been shown that for three of the porphyrinato, i.e. TTP, TMP and TMPP, the ruffling deformation of the porphyrin core of these complexes are affected by the type of the phenyl-substitution of these three meso-porphyrins, unlike in the unsubstituted porphyrin derivative [FeIII(TPP)(4-CNpy)2]+. The second important goal of the present study is to test the efficiency of our two cobaltous species 1–2 in the adsorption and the catalytic oxidative degradation of the methylene blue dye in aqueous solutions.
1H NMR spectroscopic characterization were performed with a Bruker DPX 400 spectrometer and chemical shifts (δ) are reported in ppm downfield from internal tetramethylsilane (TMS).
The UV-visible spectra were recorded with a WinASPECT PLUS (validation for SPECORD PLUS version 4.2) scanning spectrophotometer. Fourier-transform infrared spectroscopy (FT-IR) spectra were recorded on a PerkinElmer Spectrum Two FT-IR spectrometer.
Emission spectra were recorded in dichloromethane for complex 1 and in THF for complex 2 at room temperature on a Horiba Scientific Fluoromax-4 spectrofluorometer. Samples were placed in 1 cm path length quartz cuvettes. Luminescence lifetime measurements were performed after irradiation at wavelength values between 412 and 550 nm obtained by the second harmonic of a titanium:Sapphire laser (picosecond Tsunami laser spectra physics 3950-M1BB + 39868-03 pulse picker doubler) at an 800 kHz rate of repetition. For the decay acquisition, Fluotime 200 (AMS technologies) was utilized consisting of a GaAsmicro channel plate photomultiplier tube (Hamamatsu model R3809U-50) followed by a time-correlated single photon counting system from Picoquant (PicoHarp300). The ultimate time resolution of the system is close to 30 ps. Luminescence decays were analyzed with FLUOFIT software available from Picoquant. Emission quantum yields were determined at room temperature in dichloromethane solutions using the optically dilute method.26 [Zn(TPP)] in air-equilibrated dichloromethane solution was used as quantum yield standard (ϕf = 0.031). The instrumental uncertainties are as follows: absorption maxima 2 nm; molar absorption, 20%; emission maxima, 5 nm; emission lifetimes, 10%; emission quantum yields, 20%. The fluorescence quantum yield (ϕf) was measured using the following equation (eqn (1)):27
(1) |
Electrospray (ESI) spectra were obtained using an amaZon speed instrument. The samples were made by a 5 × 10−3 M in dichloromethane and the ESI-HSMS spectra were recorded in an LTQ Orbitrap XL (Thermo Scientific). The samples were made by 3 × 10−3 M in tetrahydrofuran (THF) then diluted to 5 × 10−5 M in methanol.
Electrochemistry: cyclic voltammetry (CV) experiments were performed with a CH-660B potentiostat (CH Instruments). All analytical experiments were conducted at room temperature under an argon atmosphere (argon stream) in a standard one-compartment, three-electrode electrochemical cell. Tetra-n-butylammonium perchlorate (TBAP) was used as the supporting electrolyte (0.2 M) in dichloromethane previously distilled over calcium hydride under argon. An automatic ohmic drop compensation procedure was systematically implemented before the CV data were recorded with electrolytic solutions containing the studied compounds at concentrations of ca. 10−3 M. CH Instruments vitreous carbon (ϕ = 3 mm) working electrodes were polished with 1 μm diamond paste before each recording. The Ag/AgNO3 0.01 M (TBAP 0.2 in CH2Cl2) redox couple was used as the reference electrode. The potential of the ferrocene/ferrocenium redox couple was used as an internal reference (86 mV vs. Ag/AgNO3 under our experimental conditions). For comparison with previously published data, all potentials given in the text and in Table 5 have been converted to values relative to the saturated calomel electrode (SCE) by using the following relationship: E(SCE) = E(Ag/AgNO3) + 298 mV.
Adsorption and oxidation degradation of the methylene blue dye: the experiments were carried out at room temperature using 10 mg of complexes 1–2 and 5 ml of an aqueous solution of the methylene blue (MB) dye (at pH = 6). The agitation was kept at 150 rpm. The resultant mixture was filtrated and then the concentration was determined by measuring the absorption at 665 nm. The adsorbed amount qt (mg g−1) was calculated according to the following formula (eqn (2)):
Q (mg g−1) = (Co − Ct) (V m−1) | (2) |
Elemental analysis (%) calcd for C51H30N6Cl6Co (998.49). C, 61.35, H, 3.03, N, 8.42; found: C, 61.87, H, 3.21, N, 8.50. 1H NMR (400 MHz, CDCl3) δ (ppm): 14.61 (s, 8H β-pyrrole), 11.53 (s, 8H ArH), 9.42 (s, 2H HL2,6), 9.01 (s, 8H, ArH), 8.81 (s, 2H HL3,5). UV-visible (CH2Cl2), [λmax (nm) in CH2Cl2 (ε × 10−3, mol−1 l cm−1)]: 436(420), 556(49), 598(44) FTR-IR ( in cm−1): 2970–2830 ν[(CH) porphyrin], 993 [δ(CCH) porphyrin], 2234 [ν(CN) 4-CNpy]. MS (ESI+, THF): m/z = 808.45 [CoII(TClPP)]+ found 808.98, m/z = 913.55 [CoII(TMPP)(4-CNpy)] found 913.04.
(3) |
The dnorm values are displayed using a red-white-blue color scheme corresponding to negative values (red regions) for shorter contacts, zero (white regions) for contacts around the van der Waals separation and positive (blue regions) for longer contacts. On the other hand, the Hirshfeld surface dnorm appears with a red concave region around the acceptor atom and a corresponding blue region around the donor atom. The fingerprint plots appear where one molecule acts as a donor (de > di) and the other as an acceptor (de < di). The proportions of the intermolecular interactions are presented in a 2D fingerprint which is obtained by a combination of de and di.32
Fig. 1 ESI-HRMS full spectrum of complex 1 showing the isotopic ratio. The solvent used is the dichloromethane with a concentration of 5 × 10−5 M. |
Fig. 2 ESI-HRMS full spectrum of complex 2. The insets show enlarged views. The solvent used is the THF with a concentration of 5 × 10−3 M and diluted in methanol with a concentration of 5 × 10−5 M. |
The proton NMR spectroscopy is a very convenient technique to determine if a cobalt metalloporphyrin is a diamagnetic cobalt(III) complex or a paramagnetic cobalt(II) coordination compound with the 3d6 and 3d7 ground state electronic configurations of the Co(III) and the Co(II) cations, respectively.20 For cobalt(III) meso-porphyrin derivatives, the β-pyrrolic and the phenyl ring protons are slightly shifted compared to those of the corresponding free base porphyrins with a chemical shift values in the range [8.5; 9] ppm and between 8.5 and 7.5 ppm for the phenyl protons (Table 1). However, the cobalt(II) meso-arylporphyrins present 1H NMR spectra more downfield shifted, with chemical shift values of the β-pyrrole protons between 12 and 16.5 ppm and δ values of the phenyl protons in the range [13; 8.5] ppm (Table 1). Shirazi et al.,33 reported that the δ values of the meso-arylporphyrin protons are much higher for tetracoordinated Co(II) porphyrin complexes than those for five and six-coordinated cobaltous metalloporphyrins (Table 1).
Compound | Hβ-pyrrolic protons | H-phenyl protons | H–OCH3a | Ref. |
---|---|---|---|---|
a H–OCH3 = protons of the OCH3 group in the para-phenyl positions of the H2TMPP porphyrin.b TPP = meso-tetraphenylporphyrinato.c TpivPP = meso-(α,α,α,α-tetrakis(o-pivalamidophenyl)porphyrinato).d DMI = N,N′-dimethylimidazolylidene.e HIm = imidazole. | ||||
Meso-porphyrins | ||||
H2TMPP | 8.86 | 8.08; 7.27 | 4.10 | This work |
H2ClTPP | 8.89 | 8.18; 7.74 | — | This work |
H2TpivPPc | 8.82 | 8.70; 7.88; 7.50 | — | 34 |
H2TPPb | 8.84 | 8.23; 7.91; 7.67; 7.26 | — | 34 |
Cobalt(III)-meso-porphyrin complexes | ||||
[CoIII(TPP)Cl(DMI)]b,d | 8.83 | 7.87; 7.65 | — | 35 |
[CoIII(TPP)(DMI)]+b,d | 8.95 | 7.86; 7.71 | — | 35 |
[CoIII(TPP)(N3)(py)]b | 9.22 | 8.38; 7.80 | — | 36 |
[CoIII(TPP)Cl(py)]b | 9.00 | 8.80; 7.70 | — | 36 |
Cobalt(II)-meso-porphyrin complexes | ||||
[CoII(TPP)]b | 15.75 | 13.10; 9.80; 7.95 | — | 2 |
[CoII(TpivPP)]c | 15.30 | 11.50; 10.90; 7.80 | — | 35 |
[CoII(TMPP)] | 15.90 | 13.10; 9.43 | 5.25 | This work |
[CoII(TClPP)] | 15.75 | 12.93; 9.9 | — | This work |
[CoII(TPP)(py)]b | 12.50 | 8.5; 8.33; 7.82 | — | 37 |
[CoII(TPP)(HIm)]b,e | 12.8 | 8.8; 8.40; 7.69 | — | 37 |
[CoII(TMPP)(4-CNpy)] CHCl3 (1) | 14.64 | 11.42; 8.87; 9.01 | 5.01 | This work |
[CoII(TClPP)(4-CNpy)] (2) | 14.61 | 11.53; 9.01; 9.42 | This work |
The proton NMR spectra of our synthetic complexes 1–2 are reported in Fig. SI-2 and SI-3† while the chemical shift values of the β-pyrrole and phenyl protons of these species and other related compounds are given in Table 1.
The β-pyrrole protons of 1–2 resonate at ∼14.60 ppm while the aryl protons of these two cobaltous complexes are in range [11.53; 7.98] ppm which confirm that both derivatives are cobaltous metalloporphyrins. The chemical shift values of the OCH3 protons at the para-phenyl positions of the TMPP are 4.10, 5.25 and 5.01 ppm for the H2TMPP, [CoII(TMPP)] and [CoII(TMPP)(4-CNpy)] species, respectively. The protons of the 4-CNpy axial ligand at the 2,6 and 3,5 positions resonate at 9.01 and 7.98 ppm, respectively, for the TMPP derivative (1) and 9.42 and 8.81 ppm, respectively, for the TClPP-Co(II) species (2). These values are quite different from those of the free 4-cyanopyridine molecule with chemical shifts of 7.96 ppm and 8.75 ppm indicating the coordination of the 4-CNpy in complexes 1–2.
Compound | λmax (nm) (ε × 10−3) | Egap-opt (eV) | Ref. | ||||
---|---|---|---|---|---|---|---|
Soret band | Q bands | ||||||
a H2TTP = meso-tetratolylporphyrin.b TPP = meso-tetraphenylporphyrinato.c TpivPP = α,α,α,α-tetrakis(o-pivalamidophenyl)porphyrinato.d TPBP = meso-{tetrakis-[4-(benzoyloxy)phenyl]porphyrinato}.e pip = piperidine.f Spectrum recorded in toluene.g Hon = 2-aminophenol. | |||||||
Free base meso-porphyrins | |||||||
H2TClPP | 417(320) | 515(85) | 548(36) | 590(29) | 646(26) | 1.68 | This work |
H2TMPP | 423(344) | 521(24) | 558(20) | 597(16) | 650(15) | 1.76 | This work |
H2TTPa | 420 | 616 | 552 | 594 | 640 | 1.86 | 38 |
H2TPBP | 420(513) | 516(17) | 552(7) | 591(5) | 646(4) | 1.82 | 5 |
Cobaltous meso-porphyrin complexes | |||||||
[CoII(TClPP)] | 412(380) | 529(64) | — | — | 2.01 | This work | |
[CoII(TMPP)] | 414(450) | 535(23) | — | — | — | 2.11 | This work |
[CoII(TPP)]b | 412 | 528 | — | — | — | 34 | |
[CoII(TpivPP)]c | 412 | 524 | — | — | — | 34 | |
[CoII(TPBP)]d | 412 | 528 | — | — | 7 | ||
[CoII(TMPP)(pip)]e | — | 532 | — | — | — | 39 | |
[CoII(TMPP)(py)]f | — | 535 | — | — | — | 40 | |
[CoII(TPBP)(4,4′-bpy)2]d,e | 435(562) | 552(30) | — | — | — | 7 | |
[CoII(TPP)(Hon)2]b,g | 434 | 555 | — | — | 41 | ||
[CoII(TMPP)(4-CNpy)] (1) | 437(420) | 558(40) | 600(35) | — | — | 2.003 | This work |
[CoII(TClPP)(4-CNpy)] (2) | 436(453) | 556(49) | 598(44) | — | — | 1.971 | This work |
In solution and in absence of any ligand (or coordinating solvent), cobalt(II) metalloporphyrins are tetracoordinated species type [CoII(Porph)]. The addition of axial ligands lead to pentacoordinated or hexacoordinated derivatives type [CoII(Porph)(L)x]−m (m = 0 and −1 for neutral and anionic L ligand respectively, x = 1 or 2). Staring material [CoII(Porph)] complexes present Soret band values at ∼412 nm. The addition of a N-donor neutral axial ligands leads to the redshift of the Soret band to ∼436 nm. In solid state, our two cobaltous-4-CNpy derivatives 1–2 are pentacoordinated as shown by X-ray molecular structures (see X-ray crystallographic section). In dichloromethane solution, 1–2 present very close UV-visible Soret and Q band values with Soret λmax values of 437 and 436, respectively and Q(0,0) bands λmax values of 558 nm and 556 nm, respectively. These values are very close to those of the reported hexacoordinated cobalt(II) porphyrin complexes (Table 2) such as [CoII(TPP)(Hon)2] (Hon = 2-aminophenol).41 Unfortunately, for the known pentacoordinated Co(II) porphyrin derivatives, only the Q(0,0) values are reported; i.e., the λmax of [CoII(TMPP)(pip)] (pip = piperidine) is 532 nm which is quite different from those of hexacoordinated cobaltous metalloporphyrins with a λmax value ∼550 nm.39 Thus, the UV-visible investigation indicates that in solution, complexes 1–2 are pentacoordinated cobaltous metalloporphyrins. Since the UV-visible data of 1–2 are very close, the donor–acceptor character of the MeO and chlorine groups in the para-position of the phenyls of the TMPP and TClPP moieties have no effect on the electronic spectra of these two Co(II) metalloporphyrins.
The porphyrins and the metalloporphyrins are known to present optical gap energy values (Eg-opt) close to 2.00 eV.5 This is also the case for our synthetic free base porphyrins, the starting material [CoII(Porph)] complexes (Porph = TMPP or TClPP) and 1–2 (Table 2).
Guo et al.,42 reported that the insertion of Co(II) in the porphyrin macrocycle has practically no effect on the positions of the Q(0,0) and Q(0,1) bands but the intensities of the bands of cobaltous metalloporphyrins are much weaker than those of the correspondent free base porphyrin. This is explained by the fact that cobaltous metalloporphyrins are paramagnetic low-spin (S = 1/2) complexes with the 3d7 ground state electronic configuration which enhance the intersystem crossing to the triplet state, thereby lowering the intensity of the fluorescence.
The S1 → S0 fluorescence spectra of H2TMPP, [CoII(TMPP)] and [CoII(TMPP)(4-CNpy)] (1) are shown in Fig. 4a, while those of H2TClPP, [CoII(TClPP)] and [CoII(TClPP)(4-CNpy)] (2) are shown in Fig. 4b. Representative fluorescence decays for 1–2 are shown in Fig. SI-4† and the fluorescence data of these species and those of several meso-porphyrins and cobalt(II) metalloporphyrins are given in Table 3.
Fig. 4 The emission spectra of (a) H2TMPP, [CoII(TMPP)] and [CoII(TMPP)(4-CNpy)] (1). (b) The emission spectra of H2TClPP, [CoII(TClPP)] and [CoII(TClPP)(4-CNpy)] (2). The spectra were recorded in dichloromethane solvent with a concentration ∼10−6 M. The excitation wavelength values are given in Table 3. |
Compound | λexcia | Q(0,0) | Q(0,1) | ϕf b | τfc (in ns) | Solvent | Ref. |
---|---|---|---|---|---|---|---|
a λexci = wavelength value of excitation.b ϕf = fluorescence quantum yields.c τf = fluorescent lifetime.d TPP = meso-tetraphenylporphyrinato.e TPBP = meso-{tetrakis-[4-(benzoyloxy)phenyl]porphyrinato}.f 4,4′-bipy = 4,4′-bipyridine. | |||||||
Free base meso-porphyrins | |||||||
H2TMPP | 424 | 656 | 719 | 0.082 | 7.16 | CH2Cl2 | This work |
H2TClPP | 418 | 651 | 714 | 0.089 | 7.42 | CH2Cl2 | This work |
H2TPPd | — | 654 | 712 | 0.11 | — | CH2Cl2 | 43 and 44 |
H2TPPd | — | 656 | 717 | 0.09 | — | CH2Cl2 | 45 |
H2TPPd | — | 653 | 722 | 0.12 | 9.6 | DMF | 46 |
Tetracoordinated cobalt(II) meso-metalloporhyrins | |||||||
[CoII(TPBP)]e | 552 | 653 | 719 | 0.032 | — | CH2Cl2 | 7 |
[CoII(TMPP)] | 414 | 655 | 719 | 0.035 | 6.02 | CH2Cl2 | This work |
[CoII(TClPP)] | 412 | 652 | 713 | 0.04 | 6.10 | CH2Cl2 | This work |
Pentacoordinated and hexacoordinated cobalt(II) meso-porphyrins | |||||||
[CoII(TPBP)(4,4′-bipy)2]e,f | 550 | 652 | 718 | 0.036 | — | CH2Cl2 | 7 |
[CoII(TMPP)(4-CNpy)]·CHCl3 (1) | 437 | 652 | 717 | 0.054 | 1.97 | CH2Cl2 | This work |
[CoII(TClPP)(4-CNpy)] (2) | 439 | 653 | 714 | 0.06 | 1.997 | CH2Cl2 | This work |
These two figures and Table 3 show that the λmax values of the Q(0,0) and Q(0,1) bands of H2TMPP, H2TClPP, the corresponding cobaltous porphyrin species and the coordinated 4-CNpy [CoII(Porph)(4-CNpy)] (Porph = TMPP and TClPP) species are very close (∼652 nm and ∼715 nm, respectively). Our previous studies have shown that following the insertion of the cobalt in the porphyrin core, the positions of the Q bands are practically the same while the intensities of the cobaltous metalloporphyrins are much weaker than those of the H2TMPP and H2TClPP free bases.42 For the two meso-porphyrins free bases, the fluorescence quantum yields (ϕf) values are 0.082 and 0.089, respectively, while those of the corresponding [CoII(TMPP)] and [CoII(TClPP)] starting materials are 0.035 and 0.04, respectively. The coordination of the 4-CNpy leads to a slight increase of the quantum yield compared to those of the tetracoordinated complexes [CoII(Porph)] (Porph = TMPP and TClPP) with ϕf values of 0.054 and 0.06 for 1–2, respectively. The λmax values of the Q(0,0) and Q(0,1) bands and the ϕf values of our two cobaltous derivatives are very close to those of the related [CoII(TPBP)(4,4′-bipy)] (TPBP = meso-tetra[4-(benzoyloxy)phenyl]porphyrinato) compound7 (Table 3). The fluorescent lifetime (τf) values of our synthetic cobalt(II) metalloporphyrins are smaller than those of the free meso-porphyrins H2TMPP and H2TClPP, as expected (Table 3).
The ORTEP drawings of these two cobaltous metalloporphyrins 1–2 are illustrated in Fig. 5 and 6, respectively. For both complexes 1–2, the cobalt(II) central ion are chelated by the four pyrrole N atoms of the porphyrinate anion and the 4-CNpy axial ligand occupies the apical site of the distorted square-pyramidal coordination polyhedral (Fig. SI-5†). The 4-CNpy is coordinated to the Co(II) center ion through the N-pyridyl cycle as is the case for all known 4-cyanopyridine metalloporphyrins. Fig. SI-5† represents the coordination polyhedral of the cobaltous center ion of the two 4-cyanopyridine porphyrin derivatives 1–2 which shows that the angles and distances of both two “Co-4-CNpy–porphyrin” systems are very close. Nevertheless, the Co-N(4-CNpy) value for the TClPP derivative (2) [2.196(3) Å] is smaller than that of the TMPP species (1) [2.209(3) Å]. These distances are very close to the [2.159–2.202 Å] range of the related Co(II)-4-CNpy non-porphyrinic complexes (Table 4). For 1–2, as expected, the C–C–N group of the 4-CNpy ligand is linear where the C51–C54–N6 and C47–C50–N6 angles values are 178.7(5)° and 179.1(5)°, respectively. The C–C and CN distances values of the same C–C–N moiety are 1.449(5) Å and 1.139(5) Å, respectively, for complex 1 and 1.446(5) Å and 1.146(5) for complex 2, respectively.
Fig. 5 ORTEP diagram of [CoII(TMPP)(4-CNpy)] (1). Only the major disorder fragments are shown and the hydrogen atoms are not represented for clarity. The ellipsoids are drawn at 40%. |
Fig. 6 ORTEP diagram of [CoII(TClPP)(4-CNpy)] (2). Only the major disorder fragments are shown and the hydrogen atoms are not represented for clarity. The ellipsoids are drawn at 40%. |
Complex | Porphyrin core deformation typea | M–Npb | M–XLc | M–PCd | Ref. |
---|---|---|---|---|---|
a See the description of different types of the porphyrin core deformation in the text, planar designate a planar porphyrin core. +: moderate, ++: important, +++: very important and “−”: weak deformation.b M–Np = average equatorial distance between the center metal and the nitrogen atoms of the pyrroles.c M–XL = distance between the metal atom and the coordinated atoms of the axial ligands.d M–PC = distance between the metal atom and the mean plane made by the 24-atom core of the porphyrin (PC).e TPP = meso-tetraphenylporphyrinato.f Lut = 2,6-lutidine.g 1-MeIm = 1-methylimidazole.h pip = piperidine.i TCPP = meso-tetra(4-carboxyphenyl)porphyrinato.j OEP = octaethylporphyrin.k DMAP = 4-(dimethylamino)pyridine.l pipz-S = (piperazin-1-yl)sulfonyl)naphthalen-1-amine.m PFPP = meso-tetra(pentafluorophenyl)porphyrinato.n TMP = meso-tetramesitylporphyrinato.o TPBP = meso-{tetrakis-[4-(benzoyloxy)phenyl]porphyrinato}.p L1 = 3,5-di-t-butylbenzosemiquinonato. | |||||
Co(II) porphyrin complexes | |||||
[CoII(TPP)]e | +++Ruf | 1.923 | — | 0.050 | 48 |
[CoII(TPP)]e | +++Ruf | 1.949 | — | 0.009 | 51 |
[CoII(TPP)(NO2)(Lut)]−e,f | ++Ruf | 1.959(2) | 2.017(2)(Lut), 1.925(2) (NO2) | 0.044 | 49 |
[CoII(TPP)(1-MeIm)] e,g | −Ruf | 1.978(3) | 2.157(3) | 0.139 | 52 |
[CoII(TPP)(pip)2]e,h | Planar | 1.987 | 2.436(2) | 0.000 | 50 |
[CoII(TCPP)(py)2]i | ++Ruf | 1.961 | 1.958 | 0.000 | 53 |
[CoII(OEP)(DMAP)]j,k | Planar | 1.981(3) | 2.191(2) | 0.156 | 54 |
[CoII(TPP)(pipz-S)]l | ++−Sad, −Ruf | 1.989(5) | 2.241(5) | 0.134 | 55 |
[CoII(TMPP)(4-CNpy)]·CHCl3 (1) | Ruf, +sad | 1.984(3) | 2.209(3) | 0.1404(8) | This work |
[CoII(TClPP)(4-CNpy)] (2) | ++Ruf, +sad | 1.977(3) | 2.196(3) | 0.1440(7) | This work |
4-Cyanopyridine metalloporphyrins | |||||
[NiII(PFPP)(4-CNpy)2]m | Planar | 2.283 | 2.220 | — | 56 |
[FeIII(TPP)(4-CNpy)2]e | +++Ruf, sad | 1.952(4) | 1.996/2.008 | — | 21 |
[FeII(TMP)(4-CNpy)2]n | Planar | 1.992 | 1.996 | — | 22 |
[{RhIII(OEP)}2(μ2-4-CNpy)]j | Planar | 2.032(4) | 2.273(4) | — | 22 |
[ZnII(TBAP)(4-CNpy)]o | +Ruf, +sad | 2.060(6) | 2.159(2) | — | 57 |
4-Cyanopyridine-Co(II) non-porphyrinic complexes | |||||
[CoII(SO4)(4-CNpy)2(H2O)3] | — | — | 2.135(1)/2.200(1) | — | 58 |
[CoII(L1)2(4-CNpy)2]p | — | — | 2.159 | — | 59 |
{[CoII(μ-Br)2(4-CNpy)2]}n | — | — | 2.202 | — | 60 |
For the case of the Co-TMPP derivative (1), the projection of the 4-CNpy plane is very close to the trans Np–Co–Np vector with an angle (φ) of 3.0(2)° while for the Co-TClPP species (2), the value of dihedral angle between the projection of the 4-CNpy and the closest cis Np–Co–Np angle is 20.5(2)°. It should be noted that for hemoproteins and the majority of metalloporphyrins, the planar axial ligand (type imidazole or pyridine) is located parallel to the trans meso-positions with a φ dihedral angle value of about 45°. For our TMPP-4-CNpy cobaltous derivative (1) the very short φ angle value could be explained by the intermolecular interaction between the nitrogen N6 of the 4-CNpy ligand and the hydrogen H17 of a pyrrole group of an adjacent [CoII(TMPP)(4-CNpy)] molecule (see the crystal packing description below).
Iimura et al.,47 reported that the value of the mean equatorial distance between the cobalt cation and the four nitrogen atoms of the porphyrin macrocycle (Co–Np) is directly related to the ruffling deformation of the porphyrin core (Fig. 7) where the Co–Np bond length decreases as the ruffling of the porphyrin cycle increases. The ruffling deformation of the porphyrin core is indicated by the high values of the displacement of the meso-carbon atoms above and below the porphyrin mean plane. The shortest Co–Np distance (1.923 Å) reported in Table 4, corresponds to the [Co(TPP)] complex48 for which the ruffling is the most important among all the known Co(II) porphyrins. The correlation between the Co–Np distance and the ruffling deformation is also observed for the pentacoordinated cobaltous metalloporphyrins (Table 4). For instance, the Co–Np bond length of [CoII(TPP)(NO2)(lut)] (lut: 2,2-luthidine)49 is 1.959(2) Å while for [CoII(TPP)(pip)2]50 (pip = piperidine), the Co–Np distance is 1.987 Å. Thus, the former complex exhibits high ruffling deformation while the later one presents a planar porphyrin core. For our two Co(II) derivatives 1–2, the displacements of each atom from the 24-atom core plane in units of 0.01 Å are given in Fig. 8. It has been reported that high ruffling of the porphyrin core could originate from strong π-acid axial ligands such as 4-cyanopyridine24 which can explain the short Co–Np distance for the TClPP derivative (2) with a value of 2.977(2) Å. Nevertheless, for the TMPP-4-CNpy derivative (1), the Co–Np distance is quite high with a value of 2.985(2) Å. This could be because in the TMPP porphyrinate, the donor effect of the methoxy group in the para-positions of the porphyrin phenyls (which is more important than those of the chlorine atoms in the para-positions of the TClPP moiety) destabilizes the π orbitals of the porphyrin core.21 It is noteworthy, that the Co–Np bond length values of 1–2 are not affected by the saddling deformation of the porphyrin macrocycle (Table 4).
Fig. 7 Schematic representation of the porphyrin core ruffling (ruf) deformation (a) and the saddle (sad) deformation (b). |
Fig. 8 Formal diagrams of the porphyrinato cores of 1 (left) and 2 (right). The displacement of each atom from the mean plane of the 24-atom porphyrin macrocycle in given in units of 0.01 Å. |
A part of the crystal packing of the [CoII(TMPP)(4-CNpy)] complex (1) is illustrated by Fig. SI-6.† The [CoII(TMPP)(4-CNpy)] molecules are located up-side-down in the lattice where the chloroform solvent molecules are located in channels parallel to the [010] direction. The C52 aromatic carbon of the 4-CNpy axial ligand of one [CoII(TMPP)(4-CNpy)] molecule is hydrogen bonded to the nitrogen N6 of the 4-CNpy axial ligand of a nearby up-side-down [CoII(TMPP)(4-CNpy)] molecule with a C52–H52⋯N6 distance of 3.553(6) Å. The crystal lattice of complex 1 is also sustained by weak C–H⋯O (oxygen of the OMe group in the para position of the TMPP) and C–H⋯Cg where Cg is the centroid of a TMPP phenyl ring (Tables SI-3, SI-4 and Fig. SI-6†). Additionally, the chloroform solvent molecule is involved in weak intermolecular interactions of type C–H⋯Cl between a phenyl carbon of one TMPP porphyrinato and one chlorine atom of the CHCl3 solvent molecule (Tables SI-2, SI-3 and Fig. SI-6).†
A three-dimensional non-conventional hydrogen-bonded network is formed in the crystal lattice of the [CoII(TClPP)(4-CNpy)] (2) by C–H⋯N and C–H⋯Cg where Cg is the centroid of a pyrrole ring of the TClPP moiety. Indeed, the carbon C48 of one [CoII(TClPP)(4-CNPy)] molecule is weakly H-bonded to the nitrogen N6 of the CN moiety of the 4-CNpy on an up-side-down neighboring [CoII(TClPP)(4-CNpy)] with a C48–H48⋯N6 distance of 3.527(6) Å (Fig. SI-7, Table SI-3 and SI-4†). The carbon C23 of a phenyl ring of one TClPP-Co(II) derivative is linked to the centroid Cg1 of the N1/C1–C4 pyrrole ring of a nearby [CoII(TClPP)(4-CNpy)] with a C23–H23⋯Cg1 distance of 3.613(4) Å. The crystal packing of 2 is further consolidated by π–π stacking Cg1⋯Cg2 interactions where Cg2 is the centroid of the N2/C6–C9 pyrrole ring (Fig. SI-7†).
The [CoII(TClPP)(4-CNpy)] complex (2) exhibits short Co⋯Co distance with a value of 5.663 Å with a distance value between two adjacent 24-atom mean plan porphyrin rings (PC) of 3.643 Å leading to a supramolecular dimer (Fig. 9). However, this is not the case for [Co(TMPP)(4-CNpy)] (1) with a much longer Co⋯Co distance value of 8.636 Å.
The β-substituted octaethylporphyrin (H2OEP) complexes in solid state can also form supramolecular dimers known as π–π dimers.61 The stability of these species is consolidated by π interaction between the two 24-atom plans (porphyrin cores) of one supramolecular dimer, e.g. in the case of the [FeIII(OEP)(O2C2Cl3)]·CHCl3 (ref. 62) species, the Fe⋯Fe distance is 5.45 Å. Although the meso-arylporphyrin complexes were originally synthesized to prevent porphyrin aggregation, the phenyl groups are not sufficiently sterically bulky to completely prevent the formation of supramolecular dimers. Thus, as reported by Scheidt and Lee,63 there are a number of “dimeric” TPP (meso-tetraphenylporphyrinato) metalloporphyrins observed in the solid state. In 2017, Nasri et al.,64 reported the molecular structures of two meso-arylporphyrin manganese(III) complexes: [MnIII(TPP)(TBA)] (TPP = meso-tetraphenylporphyrinato and TBA = trichloroacetato axial ligand) and [MnIII(TBrPP)(TCA)] (TBrPP = meso-tetra-(para-bromophenylporphyrinato)). The Mn⋯Mn distance values are 5.57 Å and 4.80 Å for the TPP and TBrPP derivatives, respectively. For these two species, the smaller Mn⋯Mn distance values, in the case of the TBrPP derivative, are related to its smaller deformation of the porphyrin core leading to a close contact between the two center ions.
For our two 4-CNpy derivatives 1–2, the high value of the Co⋯Co distance in the case of the [CoII(TMPP)(4-CNpy)] complex (1), which is 8.636 Å, could be related to the bulky methoxy groups of the TMPP porphyrinato which is not the case of the [CoII(TClPP)(4-CNpy)] species (2). This coordination compound presents a much smaller Co⋯Co distance of 5.693 Å, therefore enabling the formation of a supramolecular dimer. Additionally, the electron withdrawing effect of the Cl compared to the OMe causes a more efficient π–π stacking and results in a shorter Co⋯Co distance.
The π–π supramolecular dimer in the case of (2) is stabilized, as mentioned above, by C–H⋯Cg intermolecular interactions (Cg is the centroid of a pyrrole ring) and also by the Cg1⋯Cg2 π–π interactions where Cg1 and Cg2 are the centroids of pyrrole rings of two adjacent [CoII(TClPP)(4-CNpy)] molecules forming the supramolecular dimer (Fig. SI-7†).
In the case of the Co-TClPP-4-CNpy species (2), the H⋯H contacts represents 36.3% of the total intermolecular interactions with the following proportions: C⋯H/H⋯C of 17%, N⋯N/H⋯N of 8.5% and a very weak Cl⋯H/H⋯Cl of 22.6% between the chlorine atoms of one TClPP moiety and several phenyl carbons of an adjacent TClPP species.
Scheme 1 Electrochemical reduction reactions of [CoII(TPP)] in dichloromethane solvent.62,63 |
The CV of the two starting materials [CoII(TMPP)] and [CoII(TClPP)] and complexes 1–2 were recorded in the non-coordinating dichloromethane solvent under argon using the tetra-n-butylammonium perchlorate (TBAP) as the supporting electrolyte (0.2 M) and all potential values are given in volt versus SCE. For [CoII(TClPP)] and [CoII(TMPP)] (Table 5), the values of the half potential first reversible Co(II)/Co(I) reduction (eqn (I)) (MR1,MO1) are −0.88 and −0.70 V respectively. The anodic irreversible wave shown at −0.29 V for [CoII(TClPP)], which is not seen for [CoII(TMPP)], could be explained, as just mentioned above,66 by the reduction involving the [CoI(TClPP)(CH2Cl)] and [CoI(TClPP)(CH2Cl)]− intermediates. The first porphyrin ring reduction (eqn (VI)) of the TClPP and TMPP cobaltous tetracoordinated species present E1/2[R4,O4] values of −1.40 and −1.36 V, respectively.
Oxidations | Reductions | Ref. | ||||||
---|---|---|---|---|---|---|---|---|
1st Porph oxid. (O1,R1) | 2nd Porph oxid. (O2,R2) | 3rd Porph oxid. (O3,R3) | Oxid. Co(II)/Co(III) (MO2) | 1st Porph red. (R4,O4) | 2nd Porph red. (R5,O5) | Red Co(II)/Co(I) (MR1,MO1) | ||
E1/2b | E1/2 | E1/2 | E1/2 | E1/2 | E1/2 | E1/2 | ||
a The potentials are reported versus SCE.b E1/2 = half wave potential.c Irreversible wave. | ||||||||
H2TPP | 1.02 | 1.26 | — | — | −1.20 | −1.55 | — | 68 |
H2TPBP | 0.95 | 1.36 | 1.48 | — | −1.12 | −1.53 | — | 5 |
H2TMPP | 1.02 | 1.19 | 1.67c | — | −1.19 | −1.52 | — | This work |
H2TClPP | 1.00 | 1.23 | 1.53 | — | −1.09 | −1.41 | — | This work |
[CoII(TPP)] | 1.16 | — | — | 0.98 | −1.40c | — | −0.83 | 69 |
[CoII(TPP)] | 0.97 | — | — | 0.78 | — | — | −0.85 | 70 |
[CoII(TPP)] | 0.91 | — | — | 0.75 | — | — | — | 17 |
[CoII(TClPP)] | 1.00 | 1.26 | 1.85 | 0.60c | −1.40 | — | −0.88 | This work |
[CoII(TMPP)] | 0.93 | 1.20 | — | 0.70c | −1.36 | — | −0.70 | This work |
[CoII(TPP)(py)x] | — | — | — | −0.12 | — | — | −1.16 | 69 |
[CoII(TMPP)(4-CNpy)] (1) | 0.89 | 1.25 | 1.78 | 0.47 | −1.43 | — | −0.94 | This work |
[CoII(TClPP)(4-CNpy)] (2) | 1.13 | 1.31 | — | 0.42 | −1.32 | — | −0.92 | This work |
The anodic region of the cyclic voltammograms of [CoII(TClPP)] and [CoII(TMPP)] (Table 5, the voltammograms of these species are not reported), presents: (1) an oxidation of the center ion [Co(II)/Co(III)] (MO2) with Eap (Eap = anodic peak potential) values of 0.60 for the TClPP derivative 0.65 V for the TMPP species, (2) a first oxidation of the porphyrin ring (O1,R1) with E1/2 values of 1.02 and 0.92 V for the TClPP and TMPP derivatives, respectively, (3) these two cobaltous complexes exhibit a reversible second ring oxidation waves (O2,R2) with E1/2 values of 0.26 and 1.20 V, respectively, (4) unlike [CoII(TMPP)], complex [CoII(TClPP)] presents a third irreversible oxidation of the porphyrin core (O3,R3) with E1/2 value of 1.85 V and (5) an irreversible oxidation wave (O5) for both two cobaltous tetracoordinated TClPP and TMPP complexes are shown which Eap values ∼2.29 V for both species which can be attributed to the phenyl rings oxidation of the meso-porphyrin.67 For the [CoII(TMPP)] complex, the irreversibility of this oxidation is probably due to chemical reactions involving unstable electrogenerated radicals leading to an unidentified species reduced at about 0.18 V (R5). The cyclic voltammograms of complexes [CoII(TMPP)(4-CNpy)] and [CoII(TClPP)(4-CNpy)] (1–2) are illustrated in Fig. 11 and 12 and the CV data of these two cobaltous 4-CNpy derivatives are reported in Table 5 along with those of several reported porphyrinic species. The CV data of 1–2 are similar to those of the [CoII(TMPP)], [CoII(TClPP)] and other reported cobalt(II) meso-porphyrins (Table 5). The first one-electron reversible reduction of 1–2 correspond to the Co(II)/Co(I) center metal reduction (RM1,OM1) with E1/2 values of −0.94 and −0.92 V, respectively. Then a first ring reduction (R4,O4) occurs with E1/2 values of −1.35 and −1.32 V for 1–2, respectively. An irreversible wave with Eap values of −0.31 and −0.35 V for 1–2 respectively, could be attributed to the reduction involving the [CoI(Porph)(CH2Cl)] and [CoI(TClPP)(CH2Cl)]− (Porph = TClPP or TMPP) intermediates. A first irreversible oxidation wave of 1–2 corresponding to Co(II)/Co(III) oxidation (MO2,MR2) are shown with Eap values of 0.47 and 0.42 V, respectively and a first reversible ring oxidation (O1,R1) of these derivatives present E1/2 values of 0.89 and 1.18 V, respectively. Then, a second reversible ring oxidation wave (O2,R2) occurs at E1/2 values of 1.25 and 1.31 V for 1–2 respectively. The [CoII(TMPP)(4-CNpy)] (1) and unlike the complex [CoII(TClPP)(4-CNpy)] (2) shows a quasi-reversible third ring oxidation wave (O3,R3) with E1/2 value of 1.78 V. Both cyclic voltammograms of complexes 1–2 present an irreversible oxidation wave with Epa = 2.29 for 1 and 2.01 V for 2 attributed to the phenyl rings oxidation (O5) of the meso-porphyrins.
Fig. 11 Cyclic voltammogram of 1. The solvent is CH2Cl2 and the concentration is ca. 10−3 M in 0.2 M TBAP, 100 mV s−1, vitreous carbon working electrode (Ø = 2 mm). The inset shows enlarged view. |
Fig. 12 Cyclic voltammogram of 2. The solvent is CH2Cl2 and the concentration is ca. 10−3 M in 0.2 M TBAP, 100 mV s−1, vitreous carbon working electrode (Ø = 2 mm). The inset shows enlarged view. |
Thus, summarizing the CV investigation: (i) the values of the potential of the center metal Co(II)/Co(I) reduction and especially the values of the potential of the center metal oxidation Co(II)/Co(III) of the cobaltous 4-CNpy derivatives (1–2) are shifted to more negative values compared to those of the starting material of tetracoordinated complexes [CoII(Porph)] (Porph = TMPP or TClPP), (ii) the values of oxidation and reduction potential do not depend on the nature of the meso-porphyrin (TMPP or TClPP porphyrinato ligands). Notably, the fact that the larger shift to more negative potential values observed for the Co(II)/Co(III) oxidation compared to those of the Co(II)/Co(I) reduction suggests that Co(III) complexes are stabilized to a greater degree than the cobalt(II) metalloporphyrin complexes.67
Fig. 14 illustrates the adsorption capacities (qt) and the decolorization yields (R%) of the MB dye in the presence of 1–2 as a function of time under the following experimental conditions: room temperature, Co = 10 mg l−1 (of the MB dye) at pH = 6. Using the relationship (Ao and At are the absorption at t = 0 and at the t instant), the color removal yield values of 1–2 are 16.1% and 14.8%, respectively.
Fig. 14 Variation of the adsorption capacity (qt) (left) and the yield removal yield (R%) (right) vs. time for the MB dye using 1–2. |
One explanation of the adsorption phenomenon of the MB dye on complexes 1–2, could be the intermolecular interactions occurring between the nitrogen atoms, the methoxy groups and the chlorine atoms present on the surface of the porphyrin complexes 1–2 and the MB organic dye molecule.
The slightly higher qt and R(%) values in the case of the Co-TMPP-4-CNpy derivative (1) compared to those of the Co-TClPP-4-CNpy species (2), could be explained by the fact that for the TMPP derivative (1) the adsorption involves both the C–H bonds and the oxygen atoms of the methoxy groups while for the TClPP species (2) only the chlorine atom of this meso-porphyrin is involved (Fig. SI-10†).
A theoretical kinetic approach was used in order to understand the adsorption process between the MB dye and our two cobaltous derivatives 1–2. This include, the Lagergren pseudo first order, the pseudo second order, the Elovich and the intra-particular diffusion.71 The plots corresponding to the four kinetic models are reported in Fig. 15.
The results obtained using the four models which were evaluated based on the regression coefficient R2 values are given in Table 6. In reference to the high R2 values, the experimental results are better fitted using the intra-particular diffusion model for both complexes 1–2. Complex 1 exhibits a better fit than that of complex 2.
Kinetic equations | Calculated parameters | 1 | 2 |
---|---|---|---|
a K1: is the pseudo first order kinetic constant (min−1), K2: is the pseudo-second order kinetic constant (g mg−1 min−1), Kd: is the intra-particular-diffusion kinetic constant (g mg−1 min−1/2), α: is the initial adsorption rate (mg g−1 min−1), β: is the desorption constant (g mg−1) during any experiment. | |||
Lagergren pseudo first order | K1 (min−1) | 0.142 | 0.144 |
q (mg g−1) | 0.87 | 0.86 | |
R2 | 0.98 | 0.97 | |
Pseudo-second order | K2 (g mg−1 min−1) | 0.009 | 0.008 |
q (mg g−1) | 1.07 | 1.01 | |
R2 | 0.9863 | 0.9860 | |
Elovich | α (mg g−1 min−1) | 0.022 | 0.019 |
β (mg g−1 min−1) | 4.16 | 4.4 | |
R2 | 0.9785 | 0.9825 | |
Intra-particular-diffusion | Kd (mg g−1 min−1/2) | 0.048 | 0.044 |
C (mg g−1) | 0.994 | 0.996 | |
R2 | 0.013 | 0.004 |
The first step of the adsorption process is usually described by the first order model and then one or more of the three other models are applicable depending mainly on the adsorbent–adsorbate system used. Weber et al.,72 reported that for well mixed suspensions, rate-controlling step is the intra-particular diffusion model. This model is based on the following equation (eqn (4)):
qt = Kdt1/2 + C | (4) |
The intra-particular diffusion model requires that the corresponding qt versus t1/2 curve is linear and must pass through the origin.73 Therefore, as already mentioned, the intra-particular diffusion model describes our adsorbent–adsorbate system the best.
In order to improve the ability of the two cobaltous-4-CNpy porphyrins to catalyze the color degradation of the MB dye, the addition of an aqueous hydrogen peroxide solution to the previous used MB dye-1–2 systems was investigated. As expected,74 in the presence of the H2O2 aqueous solution alone (4 ml l−1) without the addition of our two Co(II) coordination compounds, no degradation of the MB dye was observed (Fig. 16). Thus, for a dye concentration of 10 mg l−1 and a pH = 6, the color degradation yields are 80% and 78% in the presence of complexes 1–2, respectively. These values are much higher than those obtained without the use of the hydrogen peroxide as an oxidant reagent were the degradation yield values are 16.1% and 14.8% for 1–2, respectively (Fig. 16). Complex 1 gives better catalytic results than complex 2.
The important role of the use of the H2O2 could be explained by the activation of this oxidant species by the 4-CNpy cobaltous porphyrins complexes 1–2. The plots corresponding to the change of the Ct/Co versus time in the case of the MB dye with H2O2 only, the dye with complexes 1–2 and the dye with 1–2 and H2O2 are given in Fig. 17.
We calculated the kinetic constants of degradation of the MB dye (Ko) when 1–2 are used in the presence of the H2O2 using the following equation (eqn (5)):75
(5) |
Fig. 18 Fitting data of the intra-particular-diffusion curves for the “MB dye-H2O2-complexes 1–2” systems. |
Footnote |
† Electronic supplementary information (ESI) available. CCDC 1950658 and 1950659. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c9ra08504a |
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