Reza Babadi Aghakhanpoura,
Mehdi Rashidi*a,
Fatemeh Niroomand Hosseinib,
Fatemeh Raoofa and
S. Masoud Nabavizadeh*a
aDepartment of Chemistry, College of Sciences, Shiraz University, Shiraz, 71454, Iran. E-mail: rashidi@chem.susc.ac.ir; nabavi@chem.susc.ac.ir
bDepartment of Chemistry, Shiraz Branch, Islamic Azad University, Shiraz, Iran
First published on 30th July 2015
The known rollover cycloplatinated(II) complex [Pt2Me2(PPh3)2(μ-bpy-2H)], 1, in which bpy-2H acts as a bridging rollover ligand, was reacted with MeI to give a new binuclear rollover cycloplatinated(IV) complex [Pt2Me4I2(PPh3)2(μ-bpy-2H)], 2. The stereochemistry of 2 was fully identified by NMR spectroscopy (1H and 31P) and confirmed by DFT calculations. To the best of our knowledge, 2 is the first example of a diplatinum(IV) complex having a bridging rollover bipyridine ligand. 1 has a 5dπ(Pt) → π*(bpy) MLCT band in the visible region which was used to easily follow the kinetics of its reaction with MeI; a double MeI oxidative addition was observed and classical SN2 mechanism was suggested for both steps of the reaction. The large negative entropy of activation (ΔS‡), found in each step, complies with an associative process. The rates are almost 3–5 times slower in the second step as compared to the first step, due the electronic effects transmitted through the rollover bpy ligand. The rates were also compared with that reported for the corresponding monomeric cyclometalated complex [PtMe(bpy-H)(PPh3)] and found to be higher (in step 1) and usually lower (in step 2). Theoretical computations of the geometry of the possible reaction transition states and intermediates revealed that each step of the reaction takes place via a transition state with a nearly linear arrangement of the I–CH3–Pt moiety. The computational results are in good agreement with the experimental findings, confirming the proposed mechanism.
Oxidative addition of MeI to platinum(II) centers is a fundamental process in organometallic chemistry with significant implications in catalysis. A classic example of such a system is the oxidative addition of MeI to [PtX4]2− complex in the Shilov process of activation of C–H bonds.7 It is well-known that electron-rich Pt(II) complexes (e.g. [PtMe2(NN)], in which NN are various diimine ligands such as 2,2′-bipyridine and 1,10-phenanthroline) undergo faster oxidative addition than electron-poor Pt(II) complexes.8–10 Electron density on the Pt(II) center of a [PtR2(LL)] complex can be manipulated by selecting R ligand, which has either electron-withdrawing or electron-donating ability.11–14
Our previous study has described in detail the effect of usual cyclometalated groups on rate of oxidative addition of MeI to the complexes of type [PtMe(C^N)L], in which C^N = 2-phenylpyridinate, 2-(p-tolyl)pyridinate or benzo[h]quinolate and L = PPh3 or PPh2Me.15 However, report on oxidative addition of alkyl halides on rollover cyclometalated platinum(II) complexes are very rare,9,16 with only one report existing on kinetic study of this type of complexes with MeI in which effect of rollover cyclometalated group on the rate of oxidative addition is investigated.9 There, a study of reaction between MeI and the monomeric Pt(II) complexes [PtMe(bpy-H)(L)] (bpy-H = κ2N,C-2,2′-bipyridine; L = PPh3 or PPh2Me)] led to formation of the Pt(IV) rollover complexes [PtMe2I(bpy-H)(L)]. Despite of this, any such reactions involving the related binuclear complexes are not reported. We report here, for the first time, on the reactivity toward oxidative addition of MeI with dimeric rollover cyclometalated Pt(II) complex, [Pt2Me2(PPh3)2(μ-bpy-2H)], 1, to investigate the cooperative steric or electronic effects between the two adjacent metal centers. Finally, using density functional theory for structure optimizations on the related complexes, geometries of transition states and intermediates in the complete reaction sequence are proposed.
The known starting rollover methylplatinum(II) [Pt2Me2(PPh3)2(μ-bpy-2H)], 1,17 was reacted cleanly with an excess of MeI in toluene at room temperature to give the air-stable solid product [Pt2Me4I2(PPh3)2(μ-bpy-2H)], 2. The synthesized Pt(IV) complex was fully characterized using 1H and 31P NMR spectroscopy and elemental analysis (full data are collected in the Experimental section). Thus, structure of product of the oxidative addition, 2, is proposed to adopt an octahedral geometry in which the rollover bpy ligand, iodide and Me groups are located in an equatorial plane with the methyl and PPh3 ligands in the axial positions. In 1H NMR spectrum of 2, the two equivalent Me groups trans to P were observed at δ 1.15 as a doublet with 3JPH = 12.0 and 2JPtH = 60.0 Hz, while the two equivalent Me groups locating trans to N ligating atoms were appeared at δ 1.64, with a considerably higher 2JPtH value of 75.0 Hz, due to lower trans influence of N atom as compared with that of P atom; these data are in agreement with those reported for the related monomeric complexes, such as [PtMe2I(bpy-H)(PPh3)] with chemical shift values of 1.12 (with 2JPtH = 61 Hz) and 1.64 ppm (with 2JPtH = 71 Hz) for Me groups trans to P and N atoms, respectively.21 Hydrogens related to CH groups adjacent to ligating N and C atoms of the rollover bpy-2H ligand each appeared as a doublet at δ = 8.80 (with 3JHH = 7.9 Hz) and 6.84 (with 3JHH = 12.0 Hz and 3JPtH = 64.0 Hz), respectively. In the 31P NMR spectrum of [Pt2Me4I2(PPh3)2(μ-bpy-2H)], 2, a singlet at δ 10.4 (with 1JPtP = 1004 Hz), assigned to the two equivalent P ligating atoms, was observed with its 1JPtP value, as expected, being much lower than the corresponding value of 1JPtP = 2347 Hz found for the starting Pt(II) complex 1.17 Although the data comply well with relative disposition of different ligands on each Pt center of the complex 2 (with chirality at each Pt center), it is not possible to use the present data to actually propose any “frozen” conformer(s) for complex 2 resulting from rotation around one or two of the Pt–P bonds. As twice the “expected” numbers of signals were observed in NMR spectra of 2, the formation of a statistical 1:
1 mixture of two stereoisomers may be a reasonable explanation.
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Fig. 1 Changes in the UV-vis spectrum during reaction of 1 with MeI in CHCl3; successive spectra were recorded at intervals of 150 s. |
Time-dependence curves of spectra of the reaction at this condition are shown in Fig. 2. The data failed to fit properly in equation Abst = Abs∞ + (Abs0 − Abs∞)[exp(−kobst)], which corresponds to a monophasic kinetic behavior. However, the data were successfully fitted in eqn (1) with two exponentials, showing the occurrence of two sequential first-order reactions. Thus, pseudo-first-order rate constants, kobs(1) and kobs(2), for the two steps of the reaction were calculated by nonlinear least-square fitting kinetic data to the biphasic first order equation (eqn (1) and Fig. 2).
Abst = α[exp(−kobs(1)t)] + β[exp(−kobs(2)t)] + Abs∞ | (1) |
The experimentally determined pseudo-first-order rate constants, kobs(1) and kobs(2), were converted to second order rate constants (k2 for the first step and k′2 for the second step) by determining slope of the linear plots of kobs(1) and kobs(2) against the concentration of MeI reagent (Fig. 3). Non-zero intercepts implied that kobs(1) = k2[MeI] + k1 for the first step and kobs(2) = k′2[MeI] + k′1 for the second step and that the k1 or k′1 step in the proposed reaction mechanism should exist. Thus, in addition to second-order terms k2 and k′2, which are suggested for the simple associative SN2-type mechanism, a much smaller terms, k1 and k′1, are also observed for associative substitutions by solvent. The results are given in Table 1. The findings are consistent with the two-step sequence shown in Scheme 3 for reaction of 1 with MeI. It should be noted that k2 > k′2. The same method was used at other temperatures and activation parameters were obtained from the Eyring equation (eqn (2)):
![]() | (2) |
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Fig. 3 Plots of first-order rate constants for the reaction of 1 with MeI at 25 °C versus [MeI] in CHCl3. |
Rate constants at different temperatures | |||||||
---|---|---|---|---|---|---|---|
15 °C | 20 °C | 25 °C | 30 °C | 40 °C | ΔH‡/kJ mol−1 | ΔS‡/J K−1 mol−1 | |
a Estimated error in k values are ±5%.b Obtained from the Eyring equation.c From ref. 9. | |||||||
103k2/(L mol−1 s−1) | 2.83 | 3.72 | 4.83 | 7.02 | 11.74 | 40.9 ± 1.5 | −152 ± 5 |
103k1/s−1 | 0.74 | 0.81 | 1.12 | — | — | 26.6 ± 9.9 | −210 ± 33 |
103k′2/(L mol−1 s−1) | 0.59 | 0.78 | 0.99 | 2.22 | 3.16 | 51.7 ± 7.5 | −127 ± 25 |
103k′1/s−1 | 0.20 | 0.25 | 0.39 | — | — | 44.9 ± 9.5 | −160 ± 33 |
103k2/(L mol−1 s−1) for [PtMe(bpy-H)(PPh3)]c | 0.70 | 0.90 | 1.50 | 2.00 | 4.60 | 55.1 ± 3.2 | −114 ± 10 |
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Scheme 3 Suggested mechanism for the two-step oxidative addition reaction of 1 with MeI (S = solvent). |
In this equation ΔH‡ = activation enthalpy, ΔS‡ = activation entropy, k = rate constant, kB = Boltzmann's constant, T = temperature, h = Planck's constant, R = universal gas constant (see Fig. 4). The data are shown in Table 1.
ΔS‡ values are large and negative for the both steps, complying with the classical SN2 type mechanism. Oxidative addition of organoplatinum(II) complexes with alkyl halides have been extensively investigated8,22 and we have also studied a secondary α-deuterium KIE study involving the reaction of MeI/CD3I to confirm operation of SN2 mechanism in the oxidative addition of MeI to some organoplatinum(II) complexes.23–25 So it is well established that these reactions proceed by an SN2 mechanism. Although a redox pathway is also a possibility, it has never been demonstrated by experimental evidence. On the basis of these kinetic data and the related DFT calculations (described in the next section) we propose that (see Scheme 3) in the first step, one of the electron rich Pt(II) centers of [Pt2Me2(PPh3)2(μ-bpy-2H)], 1 (as a nucleophile), attacks on carbon atom of MeI through an SN2 type mechanism (with rate constant k2) and the mix valence Pt(II)–Pt(IV) kinetic binuclear intermediate IM-A is formed, via the transition state TS1, which is then equilibrated with the analogous intermediate IM-B with Me and I being in cis disposition at Pt(IV) center. The latter intermediate, IM-B, is then converted to the Pt(II)–Pt(IV) compound [PtMe(PPh3)(μ-bpy-2H)PtMe2I(PPh3)], A. The complex A is then reacted with MeI in the second step, again by an SN2 type mechanism, with the rate constant k′2 being nearly 3–5 times smaller than value for rate constant of the first step (i.e. k2, see Table 1) and the Pt(IV)–Pt(IV) binuclear intermediate IM-C in equilibrium with the analogous intermediate IM-D is formed via the transition state TS2. The latter intermediate, IM-D, gives the final product [Pt2Me4I2(PPh3)2(μ-bpy-2H)], 2.
On the basis of the UV-vis data for the two-step oxidative addition reaction studied in this work (see Table 1) and using the Espenson's approach, in which the biphasic equation was used in evaluating the molar absorptivities of intermediates and the two rate constants,26–28 the second step seems to be slower than the first step by a factor of nearly 3 to 5. This is suggested to be due to the fact that in the first step one of the Pt(II) centers of Pt(II)–Pt(II) complex 1 attacks on methyl group of MeI, while in the second step, MeI reacts with the Pt(II) center of the Pt(II)–Pt(IV) complex A, in which the adjacent Pt(IV) reduces nucleophilicity of the Pt(II) center (through the bridging rollover bpy-2H ligand) when compared with situation in the first step during which the attack is performed on a Pt(II)–Pt(II) species.
For the purpose of comparison, the kinetic data for reaction of the related monomeric complex [PtMe(bpy-H)(PPh3)] with MeI9 are also included in Table 1. Thus, on reaction with MeI, 1 in the first step reacts nearly 3 time faster than the monomer [PtMe(bpy-H)(PPh3)]; we attribute this to less electron withdrawing ability of the neighboring Pt(II) center in 1 to increase the electron density of the attacking Pt(II) center in Pt(II)–Pt(II) complex 1 when compared with the case of monomer. As such, 1 in the second step is reacted with MeI with usually lower rate constant.
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Fig. 5 (a) HOMO−1 of rollover dimer 1, (b) LUMO of MeI, (c) interactions of dz2 orbital of electron-rich Pt(II) center of dimer 1 with σ* LUMO of MeI and (d) HOMO of TS1. |
A is then reacted with MeI in the second step, again by an SN2 type mechanism, upon which iodide separates from carbon of the MeI reagent and the transition state TS2 is formed (see Scheme 3 and Fig. 6 and 7), having an approximately collinear arrangement of the I–CH3–Pt moiety (the angle being 176.8°) with the Pt–CMe–H angle (91.8°) close to 90°, corresponding to an SN2 type of reaction. A similar trend is observed in the second step giving the transition state TS2 following by formation of the intermediate IM-C which is then equilibrate with the intermediate isomer IM-D,15 to finally give the thermodynamic isomer 2. Formation of the thermodynamic isomer 2 over the kinetic isomer (in which iodide groups are located trans to the incoming Me groups) is favored as in 2 the more sterically demanding PPh3 ligand is situated in “axial” position when compared with that in the kinetic isomer in which it is located in the “equatorial” position.
Although formation of 2 through a concerted pathway is a possibility, the theoretical suggested SN2 mechanism is consistent with the experimental finding.
Calculated structures and energies for the compounds, shown in Scheme 3, in chloroform solution (Fig. 6 and 7) indicate that, in consistent with the experimental observations, 1 is easily reacted with MeI to give A which is followed by a slower reaction to give 2. Calculated energies of the transition states TS1 (+45.5 kJ mol−1) and TS2 (+48.2 kJ mol−1) are in excellent agreement with the observed values of ΔH‡ = 40.9 and 51.7 kJ mol−1 for the first and second steps, respectively.
A summary of calculated atomic charges (based on Atomic Polar Tensors population (APT) analysis) for the selected compounds of Scheme 3 is given in Table 2. Charges on Pt(II) centers of 1 are significantly lower than those on the other compounds, supporting that 1 has the most potential to act as nucleophile in the reaction with MeI (Fig. 5). Atomic charges on Pt(IV) and Pt(II) centers of the mixed valence Pt(IV)–Pt(II) complex A are +0.553 and −0.201, respectively. As one moves from 1 to 2, the electron population on the iodide atom increases. These results confirm the fact that the oxidative addition reaction in such systems happens through transfer of electron density from Pt center to Me group and then to the iodide atom.
Compounds | qPt(1)/qPt(2) | qI(1)a/qI(2)b | qC(1)a/qC(2)b |
---|---|---|---|
a First incoming MeI.b Second incoming MeI. | |||
1 | −0.204/−0.204 | −0.236/−0.236 | +0.274/+0.274 |
IM-B | +0.440/−0.189 | −1/−0.236 | +0.203/+0.274 |
A | +0.553/−0.201 | −0.833/−0.236 | +0.306/+0.274 |
IM-D | +0.540/+0.469 | −0.788/−1 | +0.290/+0.211 |
2 | +0.544/+0.554 | −0.809/−0.809 | +0.298/+0.298 |
A further rationale of oxidative addition process in terms of nature of frontier molecular orbitals of the Pt compounds (Fig. 8) may be helpful. Composition and energy of HOMO and LUMO of 1 and A are also reported in Fig. 8. The highest occupied molecular orbitals 1 consist mainly of the Pt orbitals (42% and 84% for HOMO and HOMO−1, respectively) with some contribution from orbitals of the bridged bpy-2H ligand (53 and 8% for HOMO and HOMO−1, respectively). The LUMO in 1 is predominately localized on the bpy-2H unit orbitals. The HOMO and HOMO−1 of A consist of the iodide ligand and the LUMO of this complex is mainly localized on the bpy-2H ligand (see Fig. 8). Value of energy separations between the HOMO and LUMO of 1 is greater than that of A and are equal to 4.157 and 3.588 eV, respectively, meaning that the kinetic stability of A is lower than 1. Main contribution to Pt⋯CMeI in the transition state TS1 comes from overlap of dz2 HOMO−1 of the platinum center with the LUMO of MeI (which is the C–I σ* antibonding molecular orbital, see Fig. 5). So it is reasonable to view the oxidation process formally as removal of electrons from HOMO−1 of 1 into the LUMO of MeI. The second step including the reaction of A with a second incoming MeI shows similar frontier orbitals (see Fig. 8).
(1) In the first step, one of the electron rich Pt centers of Pt(II)–Pt(II) starting complex 1 attacks the carbon of MeI to form A (suggested to be a Pt(II)–Pt(IV) complex) via the transition state TS1. The Pt(II) center in A is then reacted with MeI with a rate considerably slower (by a factor of nearly 3–5) than that in the first step involving the starting complex 1, which is in consistent with a significant electronic effect transmitted through the rollover bpy bridging ligand. Less importantly, the fact that coordination around A seems to be more sterically hindered than that of 1 is probably responsible for the rate differences.
(2) MeI in the first step reacts with 1 in CHCl3 at 25 °C with a rate constant k2 = 4.83 × 10−3 L mol−1 s−1, which is some 3 times faster than that with the related mononuclear cycloplatinated(II) complex [PtMe(bpy-H)(PPh3)] at the same condition (with k2 = 1.50 × 10−3 L mol−1 s−1). This is attributed to less electron withdrawing ability of neighboring Pt(II) center in 1 to increase the electron density of the under attacking Pt(II) center in the Pt(II)–Pt(II) complex 1 as compared to that in monomer [PtMe(bpy-H)(PPh3)].
(3) Rate of MeI oxidative addition in the second step involving 1 (see Table 1) is found to be usually lower than that involving the mononuclear complex [PtMe(bpy-H)(PPh3)].
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