Mikhail N.
Khrizanforov
a,
Svetlana V.
Fedorenko
a,
Sofia O.
Strekalova
a,
Kirill V.
Kholin
a,
Asiya R.
Mustafina
a,
Mikhail Ye.
Zhilkin
a,
Vera V.
Khrizanforova
a,
Yuri N.
Osin
b,
Vadim V.
Salnikov
b,
Tatyana V.
Gryaznova
a and
Yulia H.
Budnikova
*a
aA.E.Arbuzov Institute of Organic and Physical Chemistry, Kazan Scientific Center, Russian Academy of Sciences, 8 Arbuzov Str., 420088 Kazan, Russian Federation. E-mail: yulia@iopc.ru; Fax: +7(843)275-22-53; Tel: +7(843)279-53-35
bKazan Federal University, 18 Kremlevskaya St., Kazan 420018, Russian Federation
First published on 22nd June 2016
We have developed NiIII-doped silica nanoparticles ([(bpy)xNiIII]@SiO2) as a recyclable, low-leaching, and efficient oxidative functionalization nanocatalyst for aromatic C–H bonds. The catalyst is obtained by doping the complex [(bpy)3NiII] on silica nanoparticles along with its subsequent electrooxidation to [(bpy)xNiIII] without an additional oxidant. The coupling reaction of arenes with perfluoroheptanoic acid occurs with 100% conversion of reactants in a single step at room temperature under nanoheterogeneous conditions. The catalyst content is only 1% with respect to the substrates under electrochemical regeneration conditions. The catalyst can be easily separated from the reaction mixture and reused a minimum of five times. The results emphasize immobilization on the silica support and the electrochemical regeneration of NiIII complexes as a facile route for developing an efficient nanocatalyst for oxidative functionalization.
Interest in nickel compounds of higher oxidation states (III, IV) has now grown considerably, especially given the prospects of using them in oxidation catalysis.10–15 Although the first reports on the complexes and salts of nickel in oxidation states (III) and (IV) appeared a relatively long time ago,16,17 there have thus far been few examples of fully characterized, isolated, and relatively stable structures demonstrated.18–26 This is due to the great difficulty in obtaining Ni(III, IV) and their stabilization, as highly oxidized nickel derivatives are very sensitive to moisture and light, and usually feature a high level of reactivity. Recently, we have demonstrated the examples of successful applications involving catalytic NiIII derivatives under electrochemical oxidation conditions27,28 as well as other electrochemically induced transformation involving nickel complexes under homogeneous conditions.29–33 Careful ligand selection is crucial in obtaining stable metal complexes in high oxidation states. Thus, fluoro-, oxo-ligands and certain macrocyclic N-donor ligands are usually preferred for the stabilization of the highest oxidation states, both in main-group and transition-metal chemistry.10–26 A recent report34 on the isolated Ni(III) complex [(tpy)NiIII(C4F8)](BF4) with an identified structure exemplifies the effect of perfluoro cyclic alkyl substituents (–C4F8–) of ligands on stabilization of nickel in high oxidation states.
An attractive goal would be to obtain nickel derivatives in higher oxidation states, stabilized by a special environment so that they are highly effective in catalytic reactions, meanwhile easy to handle as well, and their separation from the reaction mixture, suitable for regeneration and reactivation. In this study, we consider one of the possible solutions to this problem, namely the stabilization of a nickel(III) complex generated electrochemically using a silicate shell in order to obtain a temporarily stable system, but nonetheless active in C–H substitution reactions for various aromatic model systems.
Electrochemically induced nanoheterogeneous catalysis using nickel immobilized on nanoparticles has previously only been investigated for reduction conditions, where the working pair is Ni(II)/Ni(0).36 We know only of a few successful examples of solid-supported, non-metallic mediators that are easily separable and recycled in electrochemical processes.37,38 It is worth noting that the encapsulation of transition metal complexes in silica nanoparticles is not as widely applied in heterogeneous catalysis as silica surface decoration by transition metal complexes. Moreover, the accessibility of nickel complexes within silica nanoparticles for both oxidation and catalysis seems questionable. Nevertheless, a silica matrix with solvent-exposed Si–OH and Si–O− groups is a prerequisite for the extra-stabilization of Ni(III) for the purposes of both electrostatic interactions and coordination bonds.
It seems sensible to combine the advantages of two different approaches – nanoheterogeneous catalysis (easy catalyst recycling) and electrocatalysis (the generation and regeneration of the catalyst active form on the electrode surface without any additional molecular oxidant) – in order to develop a new effective catalytic technique that is both green and atom economical.
Interest in C–H activation has grown due to the fact that the direct functionalization of hydrocarbons presents several potential advantages over traditional cross-coupling in which prefunctionalization of the substrate, for example with a halogen, is not required. Though examples of nickel-mediated C–H activation date back to at least 1963,35 the development of catalytic C–H activation methods using nickel is a more recent development.10,27 Perfluoroalkyl groups are of special interest among fluorine-containing functional groups and new methods are necessary for incorporating them into organic substrates.39–42
The purpose of this study is to provide stable nano-sized nickel complexes(III) with 2,2′-bipyridine ligands stabilized by a silica matrix while active during the fluoroalkylation reaction of the C–H bonds of aromatic substrates based on the examples of some model compounds (caffeine, 2-phenylpyridine). C–H substitution reactions will be examined as chemically variant with primarily obtained and isolated NiIII particles taken in a stoichiometric ratio as well as under electrocatalytic NiIII regeneration conditions on an anode.
The encapsulation of tris-bipyridine complexes into silica nanoparticles is well documented in the literature by [(bpy)3Ru]II.43–47
The previously documented Stöber procedure48 was thus optimized for the synthesis of Ni(II)-doped silica nanoparticles. Scheme 1 shows the fundamental steps in the synthesis (for further details on synthesis, see the ESI†). Fig. 1 exemplifies the SEM image of 90 ± 7 nm sized nanoparticles.
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Fig. 1 SEM (scanning electron microscopy) image of silica nanoparticles doped with [(bpy)3Ni](BF4)2. |
The Ni:
Si weight ratio of 1
:
74 was evaluated by plasma atomic emission spectrometry of the nanoparticles with a standard deviation not greater than 10%.
With the assumption that each nanoparticle weight is determined by its average size, formula (1) was then used to calculate the average weight of a nanoparticle (1.1 × 10−7 g). Thus, about 4 × 1012 Ni(II) ions are packed into each nanoparticle.
m = 4/3ρπr3, | (1) |
The transparency of silica nanoparticles enables one to apply the electronic absorption spectra of their aqueous colloids and reveal chromophores doped in silica nanoparticles.49,50 Thus, electronic absorption spectra can reveal the presence of bipyridine ligands in silica nanoparticles. This is greatly significant, since the lability of [(bpy)3Ni]II complexes is a reason for their degradation under the conditions of alkali-catalyzed TEOS hydrolysis. Fig. 2a presents the electronic absorption spectra of Ni(II)-doped silica nanoparticles in acetonitrile. The spectra of bpy, [(bpy)NiII], and [(bpy)3NiII] in acetonitrile are presented in Fig. 2b as well for comparison. The spectra in Fig. 2a indicate the presence of bpy molecules in the silica nanoparticles. These molecules can be either coordinated with Ni(II) ions or adsorbed by the silica matrix. Fig. 2b presents different spectral patterns of “free” bpy and its complexes [(bpy)NiII] and [(bpy)3NiII]. Comparison of the spectral patterns with the spectrum of Ni(II)-doped silica nanoparticles (Fig. 2a) indicates a predominance of coordinated bpy in the synthesized nanoparticles. Nevertheless, the complex stoichiometry in silica nanoparticles cannot be accurately evaluated. Thus, the synthesized nanoparticles will continue to be designated as [(bpy)xNi]@SiO2, where x ≤ 3.
The electrochemical oxidation of [(bpy)xNiII]@SiO2 first calls for additional studies aimed at the evaluation of [(bpy)xNi]II leakage from the silica matrix into a solution. Electronic absorption spectra were applied to reveal the presence of bpy (either coordinated with Ni(II) or free) in the supernatant after continuously (1 hour) stirring [(bpy)xNi]@SiO2 in the acetonitrile solution with further phase separation by centrifugation. The spectra of the supernatant fit the spectral mode of “free” bpy with a small contribution of [(bpy)xNiII] (Fig. 3). These data point to a rather small [(bpy)xNiII] leakage from the silica nanoparticles into acetonitrile in an hour of stirring. It is worth noting that this time duration is optimal for electrochemical or catalytic experiments, while the leakage tends to increase in the course of 2 days (Fig. 3).
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Fig. 3 The absorption spectra of the supernatants after 1 hour (1) and 2 days of continuous stirring (2) followed by the separation of [(bpy)xNi]@SiO2 (0.2 g L−1) in CH3CN. |
The appearance of “free” bpy in the supernatant provides yet another confirmation of the partial degradation of [(bpy)3NiII] under alkaline synthetic conditions, while no detectable amounts of NiII ions (less than 0.001 mg L−1) are revealed in supernatants. The poor leaching of [(bpy)xNiII] from [(bpy)xNiII]@SiO2 into the acetonitrile (Fig. 3) confirms the above-presented assumption that the unsaturated coordinating sphere of [(bpy)xNiII] can be a reason for its coordination via Si–O− groups of the silica matrix. Thus, the loading of silica nanoparticles by [(bpy)3NiII] differs from [(bpy)3RuII]. In the latter case, the kinetic inertness of [(bpy)3RuII] prevents its degradation under synthetic conditions. Thus, the binding of [(bpy)3RuII] in the silica matrix is contributed by electrostatic and van der Waals interactions only, while [(bpy)xNiII] can be bound with silica via coordination bonds. These coordination bonds should have an effect on the redox properties of [(bpy)xNiII]@SiO2.
Complex | Conditions | Potentials, V | ||
---|---|---|---|---|
E p a/Epc | ΔEpa–c | E 1/2 | ||
[(bpy)xNi]@SiO2 | CPE | 1.92/1.77 | 0.15 | 1.84 |
CH3CN suspension | 1.94/1.88 | 0.06 | 1.91 | |
[(bpy)3Ni](BF4)2 | CPE | 1.83/1.70 | 0.13 | 1.77 |
CH3CN solution | 1.85/1.78 | 0.07 | 1.82 |
The ratio of cathodic to anodic ic/ia currents is approximately equal to 1 for both [(bpy)3NiII] in the solution and doped into silica nanoparticles in the paste electrode (Fig. 4). This fact indicates the NiIII stability in cyclic voltammetry for both solutions and colloids in the time scale of voltammetry.
[(bpy)xNiIII]@SiO2 − 1e ⇌ [(bpy)xNiIII]@SiO2 | (1) |
The size of the isolated [(bpy)xNiIII]@SiO2 particles is almost identical to the original [(bpy)xNiII]@SiO2 (Fig. 5).
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Fig. 5 Scheme of an oxidized [(bpy)xNiIII]@SiO2 complex electrochemically obtained and an SEM image of the nanoparticles. |
Fig. 2b illustrates the spectra of [(bpy)3NiII] and electrochemically generated [(bpy)3NiIII] in acetonitrile solutions. The difference in their spectral modes (spectra 1, 2 in Fig. 2b) is not great, but still detectable. Nevertheless, the difference between [(bpy)xNi]@SiO2 before and after electrochemical oxidation (spectra 1, 2 in Fig. 2a) is not as obvious as in the solution (Fig. 2b) due to the light scattering phenomenon in the colloids. Thus, ESR spectroscopy must be applied in order to confirm the electrochemical generation of [(bpy)xNiIII] in the silica nanoparticles.
The presence of a NiIII center in an electrogenerated [(bpy)xNiIII]@SiO2 was confirmed by ESR spectroscopy. The ESR spectra were compared with those of [(bpy)3NiIII] in the CH3CN solution, as well as their stability over time was analyzed. The electrochemically generated [(bpy)3NiIII] complex in the acetonitrile solution at ambient temperature yields an isotropic ESR spectrum, the intensity of which exhibits a two-fold decrease within 4.5 hours (Fig. 6). This decrease results from the instability of [(bpy)3NiIII] in acetonitrile solutions, which is the reason for NiIII to NiII transfer. This instability is the reason for unsuccessful doping of the electrochemically generated [(bpy)3NiIII] in acetonitrile solution into the silica nanoparticles according to the applied procedure.
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Fig. 6 The ESR spectra of the [(bpy)3NiIII](BF4)3 complex in CH3CN and its parameters: g = 2.097; dH = 62G (left) along with the reducing signal intensity over time (right). |
The powder of the electrochemically generated nanoparticles [(bpy)xNiIII]@SiO2 separated from either the background solutions or phosphonium salt was studied by ESR spectroscopy. The single band with g = 2.18 revealed in the ESR spectra of the nanoparticles (Fig. 7) indicates paramagnetic Ni(III) complexes within silica nanoparticles. Although the main band is reproduced in the repeated measurements, the ESR spectral pattern is somewhat affected by the ampoule rotation (Fig.1S†). The observed anisotropy can be explained by the nanoparticle aggregation in the concentrating and drying processes. Moreover, the presence of the preferred directions for nanoparticle aggregates in the ampoule demonstrates asymmetrically formed aggregates, such as “chain” aggregation. It should be noted that the experimentally observed ESR signal does not correspond to the [(bpy)3NiIII] complex signal in a frozen solution with g = 2.10, which is followed in both of our experiments, as well as stated in the literature.53 This observation confirms the hypothesis that the first coordination sphere of the nickel complex inside the nanoparticles has changed. At the same time, there are many examples of complexes with low-spin NiIII 3d7 (S = 1/2) (including those doped in silica) with g-factors, close to the one we observed, g = 2.18.54–56 The intensity of the ESR [(bpy)xNiIII]@SiO2 spectrum does not change to any great extent within a few months (error ±10%), indicating the stability of the obtained NiIII complexes inside the nanoparticles. Thus, for the first time, we have succeeded in obtaining a NiIII complex that remains stable for a long time due to stabilization of the silica matrix. Moreover, it was kept in a closed flask in the dark, but not under argon, and all operations were performed without the use of special protective measures, without a Schlenk system.
It has been discovered that an effective coupling of the selected arenes and perfluoroheptanoic acid can be carried out under electrochemically generated conditions and regenerate an active catalyst from [(bpy)xNiIII]@SiO2 when the nickel content is small in relation to the reagents, 1 mol% (eqn (3), Scheme 2). This reaction has also been successful. As a result of the initial substrate's 100% conversion, a perfluoroalkylation product is formed with an isolated yield of 75–85%. Interestingly, CO2 gas evolution was observed at room temperature. The yields of the substituted products, namely phenylpyridine, are higher than the previously described methods for obtaining them under homogeneous conditions27 and for caffeine they are comparable with better results.42
It is worth noting the insignificant leaching of [(bpy)xNiIII] from [(bpy)xNi]@SiO2 during the reaction. The low leaching enabled [(bpy)xNi]@SiO2 to be recycled and reused 5 times for C(sp2)–H bond functionalization (Table 2). The conversion of caffeine in the fifth synthesis with the same portion of the nanocatalyst has decreased by 6–8% according to the NMR spectra and the preparative yield for fluoroalkylated caffeine decreased by about the same amount. Moreover, the reaction cannot be repeated when the catalyst is extracted from the synthetic mixture by phase separation. We examined catalytic activities of both blank silica particles and nickel ions and complexes in the supernatant solution after their leaching over 24 hours from [(bpy)xNi]@SiO2. The supernatant solution was obtained by separation through the centrifugation of [(bpy)xNi]@SiO2 from the solution. Experiments with blank (empty) silica particles under electrolysis oxidative conditions reveal the lack of target products of C–H bond fluoroalkylation for both substrates (Table 2). Also, only a trace amount of a coupling product could be found in the reaction mixture after electrolysis of the electrolyte solution from which [(bpy)xNi]@SiO2 has been removed by phase separation (Table 2).
Compound | Conditiona | Product yields | ||||
---|---|---|---|---|---|---|
NMR yieldb (isolated yield)c, [%] | ||||||
1st | 2nd | 3rd | 4th | 5th | ||
a Condition details are described in the ESI. b NMR yields obtained by 19F NMR analysis of the crude reaction mixtures. c Isolated yields with a RFCOOH base and 100% conversion using 19F NMR spectroscopy. | ||||||
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Condition 1 | 95(76) | 95 | 95 | 95 | 94 |
Condition 2 | 100(85) | 95(80) | 87(74) | 82(69) | 77(63) | |
Blank silica nanoparticles | 0 (0) | |||||
Ni(II) leached over 24 h from[(bpy)xNiII]@SiO2 | Traces | |||||
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Condition 1 | 85(68) | 85 | 85 | 85 | 85 |
Condition 2 | 86(75) | 81(68) | 77(65) | 73(62) | 69(58) | |
Blank silica nanoparticles | 0 (0) | |||||
Ni(II) leached over 24 h from[(bpy)xNiII]@SiO2 | Traces |
Thus, for the first time, Ni(III) complex-catalyst particles were obtained by means of silica matrix stabilization, which are highly effective in oxidative functionalization reactions of C–H bonds of aromatic compounds. The advantage of the developed catalyst is the high level of activity, the facile separation from the reaction mass, and the ability to be used multiple times. Moreover, applying conditions of the electrochemical regeneration in situ is the route to get high product yields under the low catalyst content, which is only 1% with respect to the substrates.
Footnote |
† Electronic supplementary information (ESI) available: Synthesis and electrosynthesis conditions, physico-chemical characterization of catalysts and products, and other experimental details. See DOI: 10.1039/c6dt01492e |
This journal is © The Royal Society of Chemistry 2016 |