Ethan A.
Hill
,
Margaret L.
Kelty
,
Alexander S.
Filatov
and
John S.
Anderson
*
Department of Chemistry, The University of Chicago, 5735 S. Ellis Ave, Chicago, IL 60637, USA. E-mail: jsanderson@uchicago.edu
First published on 23rd April 2018
We report an unusual series of discrete iodosyl- and iodoxyarene adducts of Co. The formation of these adducts was confirmed by a suite of techniques including single crystal X-ray diffraction. The reactivity of these adducts with O-atom acceptors and an H-atom donor has been investigated with particular focus on elucidating mechanistic details. Detailed kinetic analysis allows for discrimination between proposed oxo and adduct mediated mechanisms. In particular, these reactions have been interrogated by competition experiments with isotopically labelled mixtures which shows that all of the studied adducts display a large KIE. These studies suggest different mechanisms may be relevant depending on subtle substituent changes in the adduct complexes. Reactivity data are consistent with the involvement of a transient oxo complex in one case, while the two other systems appear to react with substrates directly as iodosyl- or iodoxyarene adducts. These results support that reactivity typically ascribed to metal-oxo complexes, such as O-atom transfer and C–H activation, can also be mediated by discrete transition metal iodosyl- or iodoxyarene adducts that are frequent intermediates in the generation of oxo complexes. The influence of additional Lewis acids such as Sc3+ on the reactivity of these systems has also been investigated.
Herein, we report the first isolable examples of Co iodosyl- and iodoxyarene adducts [Co(II)TpAd,Me(sPhIO)]+ (1), [Co(II)TptBu(sPhIO)]+ (2), and [Co(II)TptBu(sPhIO2)]+ (3) (Tp = hydrotris(pyrazolyl)borate and sPh = 2-(tert-butylsulfonyl)phenyl; Scheme 1). Complexes 1, 2, and 3 have been crystallographically characterized and detailed kinetic studies reveal a range of reactivity for these three adducts. Complex 1 shows unique behavior that may be consistent with transient oxo formation, but complexes 2 and 3 appear to react as adducts. The observed C–H activation kinetic isotope effect (KIE) is large in all cases, potentially consistent with proton tunnelling transition states.35–38 These observations, in addition to controls with redox-innocent Lewis acids, suggest that Lewis acid activation of iodosylarenes leads to H-atom abstraction with large KIEs.
Synthesis of the cobalt iodosylarene adducts was carried out by treatment of 4 and 5 with 1.1 equivalents of sPhIO and NaBArF4 (BArF4 = tetrakis(3,5-bis(trifluoromethyl)phenyl)borate) in diethyl ether (Et2O). This procedure resulted in the clean formation of new paramagnetic species that maintain C3-symmetry in solution as judged by 1H NMR. A new set of paramagnetically shifted signals consistent with a bound sPhIO ligand are also observed, which suggests the formation of a stable adduct in solution (see ESI†). These species were assigned as the cationic iodosylarene adducts 1 and 2 that can be isolated as blue powders in 76% and 83% yield, respectively (Scheme 1). Complex 3 was first observed as a by-product in 1H NMR spectra from the synthesis of 2. The identity of 3 as an sPhIO2 adduct was suspected due to literature reports that upon standing in solution, sPhIO will disproportionate into sPhI and sPhIO2.41 Treatment of 5 with independently prepared sPhIO2 in the presence of NaBArF4 in Et2O led to the isolation of the targeted sPhIO2 adduct 3 in 67% yield as a light blue powder. Solution 1H NMR spectra showed that complex 3 retains overall C3-symmetry with paramagnetically shifted resonances. The X-band EPR spectra of complexes 1–3 are consistent with S = 3/2 Co(II) centers.
Crystals of 1 were grown under the same conditions to those of 4 and 5, while crystals of 2 were grown from a concentrated solution of Et2O layered with hexamethyldisiloxane and stored at −35 °C for 7 days. The XRD structures of 1 and 2 confirm the expected pseudo-tetrahedral geometry at Co and furthermore confirm coordination of the sPhIO ligand in the solid state (Chart 1). The average Co–N bond distances are nearly identical to those in 4 and 5, suggesting the oxidation and spin state of Co is unchanged, which is also corroborated by the aforementioned spectroscopic data. The I–O bond lengths in 1 and 2 are 1.878(6) and 1.891(3) Å. When compared to the I–O distance of 1.848(5) Å for free sPhIO there appears to be minimal activation of the iodosylarene by the Co center in these complexes.39 The Co–O bond lengths are 1.920(6) and 1.934(3) Å, which are comparable with other Co(II)–O bonds as well as the OTf starting complexes 4 and 5.52 Complex 3 has also been structurally characterized with crystals grown from a layered Et2O/petroleum ether solution stored at −35 °C. The average Co–N bond lengths of 3 are nearly identical to those of the starting Co–OTf complex 5 and the I–O bond lengths of 1.814(3) and 1.780(3) Å are also similar to those in the structure of free sPhIO2 at 1.822(3) and 1.796(2) Å.41 Isolable iodoxyarene adducts are quite rare, and to our knowledge 3 represents the first structurally characterized example with a transition metal.30 While the I–O bond lengths in this series of complexes are all similar to those reported in the free hypervalent iodine reagents, suggestive of minimal activation, the SO⋯I interactions show more sensitivity to Co coordination. The SO⋯I distances are in fact shorter than those found in the structures of the free oxidants, suggesting some effect of binding the Lewis acidic Co(II) center. For 1 and 2 the distances have substantially shortened to 2.481(6) and 2.520(3) Å compared to 2.707(5) Å for free sPhIO.39 For 3, an analogous but smaller contraction from 2.693(2) Å to 2.662(3) Å is observed.41 In the case of 3, there is an unusual close interaction between a solvent THF molecule and the iodine center which may also speak to a more electron deficient adduct (see ESI†).30
The structural data for 1, 2, and 3 support the formation of well-defined adducts with no substantial change in the Co oxidation state, spin state, or activation of the hypervalent iodine unit. This series of complexes represents an unusual family of isolable, well-characterized hypervalent iodine adducts. These species are generally rare and, as mentioned in the introduction, there have been no examples to date of isolated Co adducts despite the use of iodosylarene reagents in Co-mediated oxidation reactivity.32–34
While complexes 1, 2, and 3 were stable enough to allow for their isolation, they do slowly decompose in solution at room temperature. Complex 1 decays with a rate constant of kobs = 1.4(±0.4) × 10−5 s−1 at room temperature in Et2O (Fig. 1, Table 1). Analysis of the resulting reaction mixture by 1H NMR spectroscopy indicated a complex array of peaks that were not easily assigned (see ESI†). Analysis by ESI-MS shows evidence of incorporation of oxygen into the ligand backbone suggesting ligand-based oxidation as a mode of decay for complex 1 (see ESI†). Attempts to react 1 with external substrates were carried out by addition of either 10 equivalents of thioanisole or up to 100 equivalents of 9,10-dihydroanthracene (DHA). In both cases no increase in the rate of decay was observed by UV-vis spectroscopy (see ESI†). Complex 1 does react rapidly with PMe3 in ∼120 s to generate what is assigned as an OPMe3 adduct. The assignment of the phosphine oxide adduct is supported by independent synthesis from OPMe3 (see ESI†).
a Reported rates are 10−6 s−1. Reaction conditions: 2.5 mM cobalt complex, 23 °C, 25 mM substrate (250 mM for DHA). b Monitored via UV-vis spectroscopy in Et2O. c Monitored via1H NMR spectroscopy in CDCl3. d 1:1 mixture of 125 mM each H4-DHA and D4-DHA in DCM. | |||
---|---|---|---|
Substrate | 1 | 2 | 3 |
Self-decay | 14(4) | 0.63(8) | 6.3(4) |
Thioanisole | No change | 1.12(9) | 16(8) |
9,10-DHA | No change | 1.2(3) | 10.3(2) |
9,10-DHA KIEd | >12 | 14(5) | 9(1) |
Complexes 2 and 3 were similarly unstable in solution and decayed with markedly slower rate constants than 1. The decay of 2 was monitored via UV-vis spectroscopy to obtain a rate of decay with kobs = 6.3(±0.8) × 10−7 s−1 at room temperature in Et2O. Complex 3 decayed with kobs = 6.3(±0.4) × 10−6 s−1 as monitored with 1H NMR spectroscopy at room temperature in CDCl3. In addition, the decay profiles of both complexes are much less complicated than that observed for 1; complex 2 decays to a single paramagnetic product and 3 decays to this same product while also producing some amount of 2 (see ESI†). Similar to 1, these species show rapid reactivity with phosphines to generate putative phosphine-oxide adducts (also supported by independent syntheses, see ESI†). Unlike 1, both 2 and 3 show distinct reactivity with other substrates. In the presence of 10 equivalents of thioanisole, the rate of disappearance of 2 or 3 increased by roughly two-fold. In the reactions of 2 and 3 with thioanisole, the adduct of the corresponding oxidized substrate, phenylmethylsulfoxide, was observed by 1H NMR spectroscopy. This assignment was again confirmed by independent synthesis of the adduct (see ESI†). Smaller, concentration dependent rate enhancements were observed for 2 and 3 treated with excess DHA (k2 = 2.4 × 10−6 and 1.4 × 10−5 M−1 s−1, Fig. 2 and ESI†). In this case, anthracene was detected by GCMS analysis of the reaction mixtures (see ESI†).
Fig. 2 Plots of observed rate constants for the reaction of 2 (left) and 3 (right) with varying concentrations of DHA to determine second order rate constants, k2. |
Control reactions were also performed to assess the relative reactivity of 1 and 2 compared to free sPhIO. The complementary study to compare 3 with sPhIO2 was hindered by the extremely poor solubility of sPhIO2 in organic solvents. The rate of decay of sPhIO monitored via1H NMR spectroscopy with either 50 equivalents of DHA or 10 equivalents of thioanisole gave rates of 1.7(±0.2) × 10−5 and 4.3(±0.1) × 10−4 s−1, respectively (see ESI†). The reaction of sPhIO with 10 equivalents of PPh3 was too rapid to monitor by this method; it was complete within 3 minutes of mixing. These data show that the rate of decay of sPhIO with thioanisole is at least an order of magnitude faster than for 1 and 2 under the same conditions and the rate with DHA is on the same order of magnitude as 1 and an order of magnitude faster than for 2 under similar conditions.
It has been previously shown for metal–porphyrin complexes that an equilibrium exists between metal iodosylarene adducts and the corresponding metal–oxo complexes.13,17 This equilibrium can be shifted towards the metal iodosylarene adduct by addition of a sufficient excess of the iodoarene. In order to test whether the Co complexes presented here may reversibly form high-valent Co–oxo species, we tested the effect of added iodoarene on reaction rates. For complex 1, an excess of sPhI (10 equivalents) was added and the self-decay monitored. Under these conditions, no change of the rate of self-decay was observed (see ESI†). The reactions of 2 and 3 with thioanisole or DHA were also investigated with the addition of excess iodoarene. In both cases, no inhibition was observed with additional sPhI. However, in the case of 2, increased rates were observed and for 3, a complex reaction occurred which produced unknown paramagnetic products in addition to the formation of 2 (see ESI†). While we do not have a concrete explanation for these observations, these experiments still oppose a simple reversible oxo formation pathway (see below).
Given a lack of reactivity studies that have been performed with discrete metal iodosyl- and iodoxyarene adducts, we sought to examine more carefully their C–H activation reactivity. As a mechanistic probe of C–H activation, KIEs for the reaction of 1–3 with DHA were measured. Due to the sluggish rates of reaction, we turned to a method reported in the literature for estimating KIE values using GCMS data from the relative ratio of the mass peaks of the H2- and D2-anthracene produced from the competition reaction of the oxidant with a 1:1 mixture of H4- and D4-DHA.53 In these experiments, relatively large KIEs were observed for complexes 1, 2, and 3 (Table 1). With this method, it was difficult to precisely determine the KIE value for 1 because there was no increase in the amount of D2-anthracene detected and instead a value is estimated with a lower bound of 12 using the variability in the instrument response for D2-anthracene in the control mixture (see ESI† for more details). The KIE values for 2 and 3 could be determined more precisely at 14 and 9, respectively. The KIE for free sPhIO was also determined using this method and was found to have a lower bound of 3, which is consistent with the value reported for PhIO.53 Additionally, controls were performed involving redox-innocent, diamagnetic Lewis acids to determine whether the higher KIE values for complexes 1–3 could be due to the influence of the paramagnetic Co ion. Oxidation reactions under the conditions described using sPhIO in the presence of either Sc(OTf)3 or NaBArF4 display a high selectivity for H4-DHA to give KIE values of >66 and >11, respectively. These results suggest that a paramagnetic Lewis acid is not essential for the observation of large KIE values under these conditions. Furthermore, all of the observed KIEs are larger than that measured for free sPhIO, supporting the agency of metal-based intermediates in the observed reactivity as opposed to simple dissociation of sPhIO.
As a final set of experiments to explore the reactivity of the Co iodosyl- and iodoxyarene complexes, we examined the effect of a Lewis acid on their stability and reactivity. Recently, there have been several reports suggesting that in the oxidation of a Co complex with sPhIO, strong Lewis acids such as Sc3+ can stabilize high valent, [Co–O–Sc]5+ moieties.33,34 However, there has been some debate about the nature of these species,54 prompting us to investigate the reactivity of our discrete adducts with Lewis acids. When complexes 2 and 3 were treated with excess Sc(OTf)3, the only observed reaction was slow conversion to complex 5, presumably from the coordination of OTf. When complex 1 was treated with excess Sc(OTf)3 under the same conditions a mixture of products was obtained. We have been unable to purify a single species from this mixture, but we have crystallographically characterized a new asymmetric Co(II) complex which appears to be the major product by 1H NMR analysis (6, see ESI†). Complex 6 shows a single Co center coordinated to two pyrazole arms from the Tp ligand, a free Ad,Me-pyrazole, and OTf with an outer sphere BArF4 ion. Notably, the mass spectrum of this solution did not show evidence of ligand oxidation that is typically observed in the self-decay of 1 (see ESI†). While there was no incorporation of Sc3+ or oxygen into the complex and we do not know the mechanism leading to ligand degradation, this new reaction product demonstrates an alternative pathway is operative for 1 when Sc3+ ions are added. These data do not allow us to definitively support or exclude the formation of transient, high-valent [Co–O–Sc]5+ species.
The data for complex 1 are consistent with a rate-determining, irreversible Co–oxo forming step (Fig. 3, pathway A). To be clear, we have no spectroscopic evidence for a Co–oxo species, but its potential involvement is proposed based on the observed reactivity and cannot be ruled out. The rate of decay of complex 1 was not inhibited by addition of excess sPhI, which argues against any equilibrium between 1 and a Co–oxo species as shown in pathway B of Fig. 3. If 1 were to follow pathway C, it is expected that the rate of decay would be dependent on substrate concentration. Instead, the rate of decay of 1 was not accelerated by external substrates, with the exception of phosphines. Furthermore, the decay of 1 results in a complicated mixture of paramagnetic products and some degree of ligand oxidation in the mixture can be inferred from the ESI-MS data. Finally, the large calculated KIE for 1 is comparable to other reported metal–oxo complexes.55–57 These data taken together are consistent with the involvement of a Co–oxo intermediate in the case of 1, but are certainly not conclusive on their own. At minimum the data support a distinct reactivity pathway for 1 compared with complexes 2 and 3.
For 2, there is an observed substrate dependence on the rate of decay, suggesting I–O bond scission is not rate-limiting; this observation argues against pathway A. Furthermore, the reactivity of 2 is not inhibited by the addition of excess sPhI, which argues against a reversible oxo formation mechanism as would be observed in pathway B. These combined data support the direct agency of adduct 2 in the observed oxidative activity rather than decomposition into a Co–oxo complex (Fig. 3, pathway C). The observed large KIE for 2 also suggests that this adduct is directly involved in reactivity, as opposed to a dissociative pathway where free sPhIO acts as the active oxidant. Given that the electrochemistry for both the Ad and the tBu systems shows similar electronic properties in both cases, the observed differences in reactivity between 1 and 2 are likely due to the differing steric profiles of these two systems.
The self-decay and observed substrate reactivity for 3 are similar to that of 2, suggesting that a related mechanism may be operative. However, because formation of 2 is frequently observed in the reactivity of 3, it is difficult to deconvolute relative contributions from these two species in certain experiments such as the KIE analysis and the inhibition of reactivity by added sPhI. These factors make it difficult to distinguish between pathways B and C, but the observed rate dependence on substrate concentration for 3 suggests that pathway A can be excluded.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 1818929–1818931 and 1818933–1818935. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c8sc01167b |
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