Francesca
Forti
ab,
Cristiana
Cesari
*ab,
Marco
Bortoluzzi
c,
Cristina
Femoni
a,
Maria Carmela
Iapalucci
a and
Stefano
Zacchini
ab
aDipartimento di Chimica Industriale “Toso Montanari”, Università di Bologna, Viale Risorgimento 4 – 40136, Bologna, Italy. E-mail: cristiana.cesari2@unibo.it
bCenter for Chemical Catalysis – C3, Viale Risorgimento 4 – 40136, University of Bologna, Bologna, Italy
cDipartimento di Scienze Molecolari e Nanosistemi, Ca’ Foscari University of Venice, Via Torino 155 – 30175, Mestre (Ve), Italy
First published on 22nd September 2023
Reaction of [HRu3(CO)11]− (1) with [Ir(COD)Cl]2 in CH2Cl2 under a H2 atmosphere afforded dihydride [H2Ru3Ir(CO)12]− (2), which was quantitatively protonated to H3Ru3Ir(CO)12 (3) by strong acids such as HBF4·Et2O. The related mono-hydride [HRu3Ir(CO)12]2− (4) was obtained by deprotonation of 2 with a strong base such as KOtBu, or by the reaction of 1 with [Ir(CO)4]− in refluxing THF. Hydride carbonyl clusters 2–4 were fully characterized by IR and 1H NMR spectroscopies, and the molecular structures of 2 and 3 were determined by single-crystal X-ray diffraction (SC-XRD). The location of the hydride ligands within the tetrahedral cages of these clusters was further corroborated by computational studies employing DFT methods. Clusters 2–4 were tested as catalyst precursors for transfer hydrogenation on the model substrate 4-fluoroacetophenone, using iPrOH as a solvent and a hydrogen source. The results obtained using these heterometallic Ru–Ir clusters were compared to those using homometallic 1, evidencing a significant difference, particularly regarding the effect of the base on catalysis. Heterometallic cluster 2 was also tested in the hydrogenation of trans-cinnamaldehyde in iPrOH at refluxing temperature both under N2 and H2 atmospheres, and H2 pressure.
[Ru3Ir(CO)13]− showed high catalytic activity for the carbonylation of methanol.26,27 HRu3Ir(CO)13 acted as an effective catalyst in the hydrogenation of diphenylacetylene to stilbene.28 Several Ru–Ir complexes were employed in homogeneous catalysis for the hydrogenation of alkenes, alkynes, aldehydes and ketones.25 Supported heterometallic Ru–Ir catalysts have been shown to produce C2 oxygenates from syngas29,30 and also to exhibit unusually high catalytic activity for the oxygen evolution reaction in the electrolysis of water.31–34 Ru–Ir nanoparticles were employed for the catalytic hydrogenation of carbonyl compounds at room temperature and H2 pressure.35 Carbon-supported heterometallic Ru–Ir catalysts were used for selective and stable hydrodebromination of dibromomethane.36 Hydrogenation of CO2 was accomplished over mixed Ru–Ir catalysts.37 Overall, it seems that Ru–Ir complexes and clusters might have very interesting catalytic properties, in view of synergistic effects between these two metals that are employed in catalysis often also as homometallic species.
Within this framework, we report an improved synthesis of the cluster [H2Ru3Ir(CO)12]−,26,27,38 as well as the study of its protonation and deprotonation reactions, which resulted in a [H3−nRu3Ir(CO)12]n− (n = 0–2) series of clusters. All the species were characterized by IR and 1H NMR spectroscopies, and their structures were determined by single-crystal X-ray diffraction (SC-XRD). The location of hydride ligands was complemented by computational studies. These heterometallic Ru–Ir clusters were tested as catalyst precursors for transfer hydrogenation of 4-fluoroacetophenone using iPrOH as a solvent and a hydrogen source. [H2Ru3Ir(CO)12]− was also employed as the catalyst precursor in hydrogenation of trans-cinnamaldehyde under both hydrogen transfer and direct H2 hydrogenation conditions.
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Scheme 1 Synthesis of 2–4. H+ is added using strong acids, such as HBF4·Et2O; H+ is removed using strong bases, such as KOtBu. |
Compound 2 was identified by ESI-MS, IR spectroscopy and 1H NMR spectroscopy, and its structure was determined by SC-XRD as the [NEt4] [2] salt.
The molecular structure of 2 found in [NEt4][2] is comparable to that previously determined as the [PPN]+ salt.26,27,38 A similar structure was also adopted for the related Ru–Rh cluster [H2Ru3Rh(CO)12]−.39 It consists of a Ru3Ir tetrahedron, where the edges of one Ru2Ir triangle are bridged by three μ-CO ligands (Fig. 1 and Table 1). The two μ-H hydride ligands are bridging the two Ru–Ru edges of the unique Ru3 triangle not bearing μ-CO. This location of the hydride ligands is in agreement with the elongation of the μ-H bridged Ru–Ru edges (Table 1). One Ru atom is bonded to two μ-H and three terminal CO ligands. Ir and the two remaining Ru atoms are bonded to two terminal CO ligands, in addition to two μ-CO ligands, as well as one hydride in the case of the two Ru atoms. The presence of both terminal and edge bridging carbonyls is supported by IR analysis (νCO 2078(w), 2041(m), 2005(vs), 1973(m) cm−1, and 1797(m) cm−1 in the CH2Cl2 solution; Fig. S1 in the ESI†). The cluster displays pseudo-C2v symmetry and the two hydride ligands are equivalent, as also demonstrated by the presence of a singlet in the hydride region of the 1H NMR spectrum (δH −20.7 ppm in CD2Cl2; Fig. S6 in the ESI†). The nature of [H2Ru3Ir(CO)12]− in solution has been further corroborated by ESI-MS analysis, which shows a peak at m/z 835 for the molecular mono-anion (Fig. S10 in the ESI†).
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Fig. 1 Two views of the molecular structure of [H2Ru3Ir(CO)12]− (2) (orange: Ru; yellow: Ir; red O; grey: C; white: H). All Ru–H distances were restrained to be same. |
[H2Ru3Ir(CO)12]− (2) | H3Ru3Ir(CO)12 (3) | |
---|---|---|
Ir(1)–Ru(1) | 2.7508(16) | 2.7401(6) |
Ir(1)–Ru(2) | 2.7255(12) | 2.7414(6) |
Ir(1)–Ru(3) | 2.7254(12) | 2.7454(6) |
Ru(1)–Ru(2) | 2.9206(17) | 2.9193(8) |
Ru(1)–Ru(3) | 2.9206(17) | 2.9093(8) |
Ru(2)–Ru(3) | 2.760(2) | 2.9210(8) |
Ir(1)–COt | 1.84(2)–1.931(19) | 1.908(7)–1.918(7) |
Ir(1)–COb | 2.151(16) | — |
Ru(1)–COt | 1.895(17)–1.99(2) | 1.899(7)–1.940(8) |
Ru(2)–COt | 1.870(18)–1.914(16) | 1.910(8)–1.931(7) |
Ru(2)–COb | 2.042(17)–2.1127(16) | — |
Ru(3)–COt | 1.870(18)–1.914(16) | 1.895(7)–1.944(8) |
Ru(3)–COb | 2.042(17)–2.1127(16) | — |
Ru(1)–H(1) | 1.60(6) | 1.80(3) |
Ru(1)–H(2) | 1.60(6) | 1.80(3) |
Ru(2)–H(2) | 1.60(6) | 1.79(3) |
Ru(2)–H(3) | — | 1.79(3) |
Ru(3)–H(1) | 1.60(6) | 1.79(3) |
Ru(3)–H(3) | — | 1.79(3) |
The position of the hydrides in 2 was further corroborated by DFT calculations. The {Ru3Ir} tetrahedral structure with two hydrides bridging two Ru–Ru edges was also obtained starting from initial geometries with Ir–H interactions. The differences among the stationary points obtained from different initial structures are negligible. The computationally optimized ground state is in good agreement with the experimental data, and the RMSD is 0.178 Å. The greatest variation concerns the hydride positions, predicted to be slightly more far from the Ru centres with respect to the X-ray data (Fig. S11 in the ESI†). The unscaled simulated IR spectrum is shown in Fig. S16 in the ESI.† The vibrational frequencies are overestimated (about 7%) with respect to the experimental ones, as commonly occurs with IR simulations carried out at the DFT level with the harmonic approximation.
As previously reported for other hydride metal carbonyl clusters,40–432 undergoes reversible protonation/deprotonation reactions (Scheme 3). Thus, 2 is quantitatively converted into H3Ru3Ir(CO)12 (3) upon the addition of a slight excess of a strong acid such as HBF4·Et2O or HCl·Et2O. By using HCl·Et2O, [Ru2Ir2Cl6(CO)9]2− (5) is obtained as a side product and, thus, a better yield of 3 is achieved with HBF4·Et2O. The protonation may be reversed upon the addition of a strong base such as KOtBu. Further addition of a 3 equivalent excess of KOtBu to 2 affords the mono-hydride di-anion [HRu3Ir(CO)12]2− (4). The process is reversed upon addition of a strong acid.
The mono-hydride di-anion 4 may be alternatively obtained from the reaction of 1 with [Ir(CO)4]− in refluxing THF (Scheme 1). The structures of the new clusters 3 and 5 have been determined by SC-XRD as their 3 and [NEt4]2[5] crystals. Crystals of [PPN]2[4] were of low quality and displayed high disorder, which hampered the full SC-XRD analysis of the structure of 4. Preliminary data (crystal system, space group, and unit cell parameters) are included in the Experimental Section. These allowed the identification of the tetrahedral Ru3Ir metal cage of 4, as well as the presence of twelve CO ligands and two [PPN]+ cations. The structure of 4 was further investigated using computational methods (see below).
The protonation/deprotonation reactions of 2 were studied in solution by IR and 1H NMR spectroscopies (Fig. 2, and Fig. S1–S8 in the ESI†).
![]() | ||
Fig. 2 IR spectra in the νCO region of [H3−nRu3Ir(CO)12]n− (n = 0–2) in CH2Cl2. H+ is added as HBF4·Et2O or HCl·Et2O, and removed with KOtBu. See Scheme 3 for the stoichiometry. |
The molecular structure of 3 is based on the same Ru3Ir tetrahedral metal core of 2 (Fig. 3 and Table 1). Nonetheless, the stereochemistry of the ligands is rather different. The tri-hydride 3, in view of its neutral charge and reduced π-back donation, contains only terminal carbonyls, three per each metal atom. The three hydrides are edge-bridging on the three basal Ru–Ru edges. Cluster 3 possesses idealized C3v symmetry and, therefore, just a singlet is present in the hydride region of its 1H NMR spectrum at δH −17.8 ppm (Fig. S8 in the ESI†). A similar structure was previously reported for H3Ru3Rh(CO)12.44 Even if the structure of 3 is unprecedented, a few phosphine derivatives of 3 have been previously reported.38
![]() | ||
Fig. 3 Molecular structure of H3Ru3Ir(CO)12 (3) (orange: Ru; yellow: Ir; red: O; grey: C; white: H). All Ru–H distances were restrained to be the same. |
The DFT-optimized structure of 3 agrees well with the experimental outcomes, with a RMSD of 0.107 Å. The computed and experimental structures are superimposed in Fig. S12 in the ESI.† The simulated IR spectrum is reported in Fig. S16 in the ESI.† The investigation on other possible isomers of 3 afforded other two stationary points, where one of the hydrides is μ3-coordinated at the centre of a {Ru2Ir} face or it is bridging a Ru–Ir edge. As shown in Fig. S13 in the ESI,† both these isomers resulted however less stable than that experimentally observed.
The molecular structure of the mono-hydride di-anion 4 was only preliminarily determined by SC-XRD and, then, further optimized and investigated using DFT methods (Fig. 4). Based on this hybrid approach, the most likely structure of 4 consists of a Ru3Ir tetrahedron, as in the parent 2. After some attempts, the computed structure depicted in Fig. 4 was selected as the most probable because it was the only one maintaining the same disposition of the carbonyl ligands deducted from the preliminary X-ray outcomes, i.e. three terminal carbonyls on the Ir centre, two terminal carbonyls for each Ru atom and three edge-bridging carbonyls located on the Ru3 triangle. The superposition of the {Ru3Ir(CO)12} fragments between the computed and preliminary X-ray structures is quite good, as observed in Fig. S14 in the ESI,† with a RMSD of 0.133 Å. The Cartesian coordinates of other possible isomers obtained from DFT calculations, with different dispositions of the CO ligands, are provided in the ESI† (Fig. S15). In the stationary point considered (Fig. 4), the unique hydride caps the Ru3 face with an average Ru–H distance of 1.902 Å, as in the case of [HRu4(CO)12]3−41 and [HFe4(CO)12]3−.45 The optimized geometry of 4 roughly belongs to the C3v point group (R = 0.096). The presence of the hydride ligand has been supported by 1H NMR spectroscopy which shows a singlet at δH −19.9 ppm (Fig. S7 in the ESI†).
As in the case of 2, 4 also contains nine terminal and three μ-CO ligands. Nonetheless, the three edge-bridging carbonyls are located on the Ru3 triangle of 4, and in a Ru2Ir triangle in the case of 2. This further supports different numbers and locations of the hydride ligands in the two clusters.
It must be remarked that the related [HFe3M(CO)12]2− (M = Co, Rh, Ir) clusters adopt different structures. In the case of [HFe3Co(CO)12]2− and [HFe3Rh(CO)12]2−,46,47 three μ-CO ligands are located on a Fe2M triangle, with fourth μ-CO bridging the basal M and the apical Fe. The unique hydride is capping the Fe2M triangle. Conversely, [HFe3Ir(CO)12]2− displays only three μ-CO ligands on a Fe2Ir triangle, and the unique hydride bridges between the basal Ir and the apical Fe(CO)3.46
The unscaled computed IR spectrum, reported in Fig. S16 in the ESI,† is in agreement with the experimental data. The simulated IR spectra of 2, 3, and 4 follow the trend observed in Fig. 2, with a shift towards higher frequencies of the CO stretching vibrations on reducing the negative charge of the clusters because of a lower degree of π-back-donation.
The Hirshfeld population analysis on 2, 3 and 4 indicated that the partial charge on the hydrides is not directly related to the global charge of the clusters. The computed partial charge of the unique hydride in the doubly negatively charged cluster 4 is −0.102 a.u., while slightly more negative values were obtained for dihydride 2 (average value −0.118 a.u.) and neutral trihydride 3 (−0.117 a.u.).
It is worth noting that the structure shown in Fig. 4 is not the most stable isomer computationally found for 4. Another stationary point with a completely different disposition of the carbonyl ligands and much lower symmetry resulted more stable by about 2.9 kcal mol−1 (Gibbs free energy). As observed in Fig. S15 in the ESI,† in the energetically lowest isomer, the Ir centre is bonded to two terminal and two bridging carbonyl ligands. Another carbonyl bridges two Ru centres, each one bearing two terminal CO ligands. The last Ru centre interacts with three terminal CO. The hydride bridges {Ru(CO)3} and {Ru(CO)2} fragments. The energy gap with respect to the experimentally observed structure (based on the preliminary SC-XRD data) is however quite small, while the superimposition with the preliminary X-ray data is very poor. It is possible that the relative stability could be affected by anion–cation contacts and intramolecular interactions not accounted using in vacuo calculations. Another stationary point for 4, where Ir is bonded only to one terminal carbonyl ligand and the hydride is μ3-briding two Ru and the Ir centres, is less stable than the other isomers (Fig. S15 in the ESI†).
In view of the fact that 2 and 3 are isostructural with [H2Ru3Rh(CO)12]− and H3Ru3Rh(CO)12, respectively, it was of interest to compare the structure of 4 with the related [HRu3Rh(CO)12]2−. Since its structure was not previously reported in the literature, [HRu3Rh(CO)12]2− (6) was prepared from 1 and [Rh(CO)4]− (Scheme 4) and its molecular structure was determined by SC-XRD as the [NEt4]2 [6] salt (Fig. 5). The structure of 6 is different from that of 4 and similar to those of [HFe3Co(CO)12]2− and [HFe3Rh(CO)12]2−.46,47 Thus, the unique hydride is μ3-coordinated to a Ru2Rh triangle, whose three edges are bridged by three μ-CO ligands. A fourth μ-CO is bridging the basal Rh and apical Ru. The two Ru–Ru edges not bridged by μ-CO ligands are somehow hindered by terminal carbonyls, and this makes very unlikely that the unique hydride could be edge bridging rather than face capping. The location of the hydride on the Ru2Rh face is also in agreement with the fact that a doublet at δH −15.7 ppm with 1JH-Rh = 17 Hz is present in the 1H NMR spectrum of 6. A similar 1JH-Rh coupling constant was observed in [HFe3Rh(CO)12]2−, where the hydride is located on a Fe2Rh face.47
The DFT-optimized structure of 6 agrees with the X-ray structure, as observed in Fig. S17 in the ESI† (RMSD = 0.161 Å). The computed hydride position is a bit more far from the {Ru2Rh} plane with respect to the X-ray data. The simulated IR spectrum confirms the good overlap between the experimental and computed data (Fig. S17 in the ESI†). As previously occurred for the related Ir derivative 4, the computational investigation afforded other stationary points for 6, and, in particular, one is slightly more stable than the others (about 1.6 kcal mol−1, Fig. S18 in the ESI†). The disposition of the carbonyl ligands is however different with respect to the experimental geometry (ruling out the possibility that this computed structure is present in the solid state), since two terminal CO are bonded to the Rh centre and only one CO bridges a Ru–Ru edge. In this case, the hydride bridges two Ru centres without a direct interaction with Rh. This disagrees with the 1JH-Rh coupling constant observed in solution, which is typical for μ3-H with direct coupling to Rh,47 as experimentally observed. Finally, a structure geometrically analogous to that observed for 4 resulted less stable than the experimental one by about 4.6 kcal mol−1.
It seems that the structures of [HRu3M(CO)12]2− and [HFe3M(CO)12]2− (M = Co, Rh, Ir) clusters result from a subtle balance between the sizes of the metals and their affinities for CO and hydride ligands.
The molecular structure of 5 is rather peculiar and may be viewed as composed of a Ru2(μ-Cl)2(μ-CO)(CO)4 core where the two Ru atoms are directly bonded to two square–planar [IrCl2(CO)2]− complexes (Fig. 6).
The computed structure of 5 is in good agreement with the experimental one, with the RMSD being 0.361 Å. The superposition of the two structures is shown in Fig. S19 in the ESI.† The nature of the Ru–Ir interactions in 5 was investigated by means of AIM analysis. Comparable (3,−1) bond critical points were localized for both the Ru–Ir interactions, with an average electron density value of 0.245 e A−3 and a potential energy density of −0.223 Hartree A−3. The energy density is slightly negative, −0.044 Hartree A−3, while the Laplacian of electron density is positive, 3.852 e A−5, according to Bianchi's definition of the metal–metal bond.48 The two critical points are shown in Fig. 7, together with the occupied molecular orbital showing the best superposition between Ir and Ru. On the other hand, no (3,−1) bond critical point was localized between the Ru centres. The formal electron count for each Ru in a neutral Ru2(μ-Cl)2(μ-CO)(CO)4 core without the Ru–Ru bond is 16 electrons; thus, two [IrCl2(CO)2]− fragments formally behave in 5 as ligands to saturate the coordination sphere of the Ru centres. The possible behaviour as the electron donor of [IrCl2(CO)2]− towards the Ru centre was supported by the charge decomposition analysis on 5,49 partitioned as composed by the fragments [Ru2IrCl4(CO)7]− and [IrCl2(CO)2]−. No negative charge donation from [Ru2IrCl4(CO)7]− to [IrCl2(CO)2]− was calculated, while 0.17 electrons are transferred in the reverse process.
Entry | Cat | Cat (mol%) | KOtBu (mol%) | Conversion (%) 1 h | Conversion (%) 3 h | Conversion (%) 5 h | Conversion (%) 24 h |
---|---|---|---|---|---|---|---|
General conditions: catalyst (3, 7.5 or 15 μmol, 1, 2.5 or 5 mol%), iPrOH (5 mL), KOtBu (4, 10 or 20 mol% when added), and 4-fluoroacetophenone (36.5 μL, 300 μmol), T = 82 °C, N2 atmosphere; the conversions were determined by 19F NMR spectroscopy. All entries are the average of at least three independent catalytic runs. | |||||||
1-2 | 5 | 10 | 0 | 16 | 20 | 84 | |
2-2 | 5 | — | 0 | 0 | 0 | 52 | |
3-2 | 2.5 | 10 | 24 | 42 | 58 | 87 | |
4-2 | [NEt4][2] | 1 | 4 | 10 | 24 | 34 | 54 |
5-2 | 1 | 10 | 13 | 34 | 46 | 86 | |
6-2 | 1 | — | 0 | 5 | 12 | 42 | |
7-2 | 1 | 20 | 0 | 27 | 46 | 92 | |
1-1 | 5 | 10 | 0 | 7 | 10 | 50 | |
2-1 | 5 | — | 0 | 19 | 37 | 92 | |
3-1 | [NEt4][1] | 2.5 | — | 0 | 17 | 24 | 82 |
4-1 | 1 | 10 | 0 | <5 | 11 | 19 | |
5-1 | 1 | — | 0 | 0 | 18 | 80 |
Control experiments include reactions without any catalyst (with and without a base), as well as reactions with RuCl3, IrCl3, [PPN][Ir(CO)4] and [Ir(COD)Cl]2 as potential catalyst precursors. All these control tests resulted in almost zero conversion after 5 and 24 h, ruling out the presence of any background reaction under the experimental conditions adopted for the catalytic tests (Table S1 in the ESI†). The homometallic cluster [NEt4][1] was previously tested as the catalyst precursor under similar experimental conditions, and the results are summarized in Table 2 for the sake of comparison.50
Conversions recorded after 5 h (0–58%) and 24 h (42–92%) indicate some catalytic activity under all the experimental conditions considered, but a long induction period (Table 2). Moreover, spectroscopic analyses (IR spectroscopy, 1H NMR spectroscopy and ESI-MS) of the reaction mixtures at the end of the catalytic tests showed the presence in solution of mixtures of carbonyl clusters (Fig. S20–S28 in the ESI†), including hydrides and heterometallic Ru–Ir clusters, ruling out cluster breakdown to mononuclear complexes or nanoparticles as the major event.
Using [NEt4][2] as the catalyst precursor, there is a clear beneficial effect after the addition of KOtBu. Indeed, the conversion at 24 h increases from 42 to 52% (no base) to 54 to 92% (KOtBu, 4–10–20 mol % respect to the substrate). Heterometallic Ru–M (M = Cu, Ag, Au) carbonyl clusters displayed a similar improvement of the conversion after addition of a base,50 whereas the opposite trend was observed with the homometallic Ru precursor [NEt4][1]. This is somehow indicative of the fact that [NEt4][2] and [NEt4][1] follow different activation and/or catalytic paths. It is noteworthy that the highest conversion recorded with the heterometallic precursor (92%) was obtained after 24 h employing 1 mol% of [NEt4][2] and 20 mol% of KOtBu. In the case of the homometallic precursor, the same conversion was obtained after 24 h with 5 mol% of [NEt4][1] and no base. The results obtained with [NEt4][2] are comparable to those previously reported for heterometallic Ru–Cu and Ru–Ag carbonyl clusters, and superior to Ru–Au ones.50
It seems that the catalytic process employing [NEt4][2] as the catalyst precursor requires a strong base. Indeed, similar results were obtained using NaOMe instead of KOtBu (Table 3), whereas employing a weaker base such as NEt3 resulted in a conversion comparable to that observed without a base.
Entry | Cat | Cat (mol%) | Base (10 mol%) | Conversion (%) 1 h | Conversion (%) 3 h | Conversion (%) 5 h | Conversion (%) 24 h |
---|---|---|---|---|---|---|---|
General conditions: catalyst (3 μmol, 1% mol/mol), iPrOH (5 mL), KOtBu or NEt3 or NaOMe (10 mol %), and 4-fluoroacetophenone (36.5 μL, 300 μmol), T = 82 °C, and N2 atmosphere; the conversions were determined by 19F NMR spectroscopy. All entries are the average of at least three independent catalytic runs. | |||||||
1-2 | 1 | NaOMe | 35 | 49 | 61 | 88 | |
2-2 | [NEt4][2] | 1 | NEt3 | 0 | 0 | 0 | 42 |
3-2 | 1 | KOtBu | 13 | 34 | 46 | 86 |
Some catalytic tests with [NEt4][2] have been repeated adding metallic mercury (Table S3 in the ESI†). This is a well-known method described in the literature in order to remove metal particles and eliminate the heterogeneous contribution to catalysis. It resulted that mercury had a limited effect on catalytic tests in the presence of [NEt4][2], suggesting that catalysis is mainly homogeneous. When the base KOtBu is not used, the results are comparable to those without mercury, if not better, while in the presence of 10 mol% of base, the conversion of the substrate is below expectations. This anomaly in the yield could be expected due to the presence of the metallic Hg itself, more than to the heterogeneous inhibition's role of the mercury, because the latter should cause no activities at all.
Further catalytic tests were performed using 3 and [NEt4]2[4] instead of [NEt4][2] as the catalyst precursors (Table 4). In the absence of any base, both 3 and [NEt4]2[4] displayed very poor conversions (13–15%) compared to [NEt4][2] (42%). Conversely, in the presence of KOtBu (10 mol % per mol of substrate), high conversions were observed for all the three catalyst precursors. Nonetheless, in the case of [NEt4]2[4], several unknown resonances were present in the 19F NMR spectra after catalysis. These are likely to be due to condensation products, in addition to the main hydrogenation reaction. It is noteworthy that such selectivity problems have been observed only by using [NEt4]2[4] as the catalyst precursor, whereas complete selectivity to 4-F-α-methylbenzylalcohol was usually observed for all other Ru-based carbonyl clusters employed, both heterometallic and homometallic.
Entry | Cat | Cat (mol %) | KOtBu (mol %) | Conversion (%) 1 h | Conversion (%) 3 h | Conversion (%) 5 h | Conversion (%) 24 h |
---|---|---|---|---|---|---|---|
General conditions: catalyst (3 μmol, 1% mol/mol), iPrOH (5 mL), KOtBu (10 mol % when needed), and 4-fluoroacetophenone (36.5 μL, 300 μmol), T = 82 °C, and N2 atmosphere; the conversions were determined by 19F NMR spectroscopy. All entries are the average of at least three independent catalytic runs.a The selectivity of the product is 80%; there is evidence of other fluorinated compounds, in contrast with all the other experiments. | |||||||
1-2 | [NEt4][2] | 1 | 10 | 13 | 34 | 46 | 86 |
2-2 | 1 | / | 0 | 5 | 12 | 42 | |
1-3 | 3 | 1 | 10 | 0 | 16 | 24 | 81 |
2-3 | 1 | / | 0 | 0 | 0 | 13 | |
1-4 | [NEt4]2[4] | 1 | 10 | 29 | 45 | 52 | 100(80)a |
2-4 | 1 | / | 0 | 4 | 6 | 15 |
Combined IR spectroscopy, 1H NMR spectroscopy and ESI-MS analyses were performed after heating the catalyst precursors in iPrOH at refluxing temperature, with and without bases, as well as with and without substrates in stoichiometric amounts, in order to gain some insights into the carbonyl species present in solution at the end of catalysis (Fig. S20–S28 in the ESI†). These experiments showed the presence of mixtures of products, including heterometallic carbonyl clusters and carbonyl hydrides. During all these experiments, there was no evidence of any stoichiometric product between the catalyst precursors and the substrate, or of the formation of unsaturated species. Thus, it was not possible to devise any plausible reaction pathway for the catalytic process.
Further reactivity tests conducted in a iPrOH solution showed, thanks to IR spectroscopy and 1H NMR spectroscopy, that all the three [H3−nRu3Ir(CO)12]n− (n = 0–2) species are quickly deprotonated at room temperature to give quantitatively cluster 4 when 10 mol % of KOtBu is added. Further experiments carried out under the same conditions but with 24 hours of reflux also showed the formation of [H3Ru4(CO)12]− (see below). It must be remarked that [H3Ru4(CO)12]− displays poorer catalytic activity than 2, 3 and 4 in the presence of a base (Table 5), further supporting the involvement of heterometallic species during catalysis. However, in the presence of the substrate, the composition of the reaction mixture after 24 h diverges for the three compounds 4, 2 and 3, evidencing a completely different reaction path, according to the results obtained (Table 4).
Entry | Cat | Cat (mol %) | KOtBu (mol %) | Conversion (%) 1 h | Conversion (%) 3 h | Conversion (%) 5 h | Conversion (%) 24 h |
---|---|---|---|---|---|---|---|
General conditions: catalyst (3 μmol, 1 mol %), iPrOH (5 mL), KOtBu (10 mol % when needed), and 4-fluoroacetophenone (36.5 μL, 300 μmol), T = 82 °C, and N2 atmosphere; the conversions were determined by 19F NMR spectroscopy. All entries are the average of at least three independent catalytic runs. | |||||||
1 | [NEt4][H3Ru4(CO)12] | 1 | / | 0 | 0 | 10 | 44 |
2 | 1 | 10 | 13 | 44 | 45 | 48 |
When [NEt4][2] was employed, it was possible to identify the same species among the carbonyl hydrides species present at the end of the catalytic process. Some homometallic species such as 1 and [H3Ru4(CO)12]− were51 identified in some experiments, as mentioned above; however, the main compound at the end of the catalytic experiments is [NEt4][2] (Fig. S24 in the ESI†), and no mononuclear fragments were detected from the ESI-MS analysis. Overall, it seems that the catalyst precursor 2 is in part transformed and in part recovered intact at the end of the process. All the not yet identified species, found at the end of the reactivity experiments, have a molecular mass compatible with at least a bi or trimetallic metal core cluster. In addition, control experiments (Table S1 in the ESI†), using ruthenium and iridium salts, have been conducted to prove the little or no influence of oxidised metal ions in the catalytic activity, since their formation can arise from the decomposition of the clusters structures. In all cases, these results seem to indicate that cluster breakdown to monometallic species or metal nanoparticles is not the major event in solution during catalysis.
Heterometallic cluster [NEt4] [2] was also tested in the hydrogenation of trans-cinnamaldehyde in iPrOH at refluxing temperature under both a N2 atmosphere and a H2 atmosphere. Catalytic tests were performed without a base in order to avoid side reactions, such as aldol condensation. Under these conditions, three different hydrogenation products can be obtained (Table 6), depending on the hydrogenation site: the saturated aldehyde (a), if hydrogenation occurs on the CC bond; the unsaturated alcohol (b), if the C
O bond is hydrogenated; the saturated alcohol (c), which is formed when both C
C and C
O are hydrogenated. Conversions and yields were determined by 1H NMR spectroscopy at the end of the catalytic tests.
Entry | Time (h) | Pressure (bar) | Substrate conversion (%) | Yield (a) (%) | Yield (b) (%) | Yield (c) (%) |
---|---|---|---|---|---|---|
General conditions entries 1–6: catalyst (18 μmol, 1 mol%), iPrOH (30 mL) and trans-cinnamaldehyde (228 μL, 1800 μmol), T = 82 °C, and H2 atmosphere; the conversions were determined by 1H NMR spectroscopy. All entries are the average of at least three independent catalytic runs. Catalytic tests were performed using the autoclave Parr reactor.General conditions entries 7–10: catalyst (3 μmol, 1 mol%), iPrOH (5 mL) and trans-cinnamaldehyde (38 μL, 300 μmol), T = 82 °C, and N2 or H2 atmosphere; the conversions were determined by 1H NMR spectroscopy. All entries are the average of at least three independent catalytic runs. | ||||||
1-2 | 24 | 60 H2 | >99 | 0 | 0 | >99 |
2-2 | 24 | 30 H2 | >99 | 6 | 0 | 94 |
3-2 | 24 | 10 H2 | >99 | 4 | 20 | 76 |
4-2 | 3 | 60 H2 | >99 | 17 | 8 | 75 |
5-2 | 3 | 30 H2 | >99 | 23 | <5 | 77 |
6-2 | 3 | 10 H2 | 81 | 27 | 10 | 44 |
7-2 | 24 | 1 H2 | 85 | 26 | 24 | 35 |
8-2 | 3 | 1H2 | 49 | <5 | <5 | 49 |
9-2 | 24 | 1 N2 | 43 | 0 | 40 | 3 |
10-2 | 3 | 1 N2 | 54 | 0 | 54 | 0 |
Performing the reaction under a N2 atmosphere, the conversion is moderate but the selectivity is very high towards (b). This is consistent with the fact that, under these conditions, hydrogenation occurs via hydrogen transfer from iPrOH, which is more selective for the polar CO bond. The low conversion observed is probably due to the fact that no base has been added. Indeed, as shown by using 4-F-acetophenone as the substrate, the catalytic performances of [NEt4][2] for H-transfer to C
O bonds seem to be enhanced by strong bases.
The conversion is considerably increased under H2 at atmospheric pressure, but the selectivity is low, since a mixture of (a), (b) and (c) is obtained. This is due to the fact that, under these experimental conditions, both H-transfer from iPrOH and hydrogenation from H2 occur, the former targeting preferentially the polar CO bond and the latter the C
C bond. Indeed, by performing the catalytic test under H2 (1 bar) in toluene (entries 1 and 2 in Table 7), the conversion is again low, but the major product is (a).
Entry | Time (h) | Pressure (bar) | Substrate conversion (%) | Yield (a) (%) | Yield (b) (%) | Yield (c) (%) |
---|---|---|---|---|---|---|
General conditions entries 1 and 2: catalyst (3 μmol, 1 mol%), toluene (5 mL) and trans-cinnamaldehyde (38 μL, 300 μmol), T = 82 °C, and H2 atmosphere; the conversions were determined by 1H NMR spectroscopy. All entries are the average of at least three independent catalytic runs.General conditions entries 3 and 4: catalyst (18 μmol, 1 mol%), toluene (30 mL) and trans-cinnamaldehyde (228 μL, 1800 μmol), T = 82 °C, and H2 atmosphere; the conversions were determined by 1H NMR spectroscopy. All entries are the average of at least three independent catalytic runs. Catalytic tests were performed using the autoclave Parr reactor. | ||||||
1-2 | 24 | 1 H2 | 31 | 21 | <5 | 10 |
2-2 | 3 | 1 H2 | 19 | 10.5 | <5 | <5 |
3-2 | 3 | 30 H2 | 92 | 16 | 13 | 63 |
4-2 | 24 | 30 H2 | >95 | 8 | <5 | 87 |
Further catalytic tests were performed in iPrOH at a H2 pressure (10–60 bar) for 24 h (Table 6). At a high H2 pressure (30–60 bar), the conversion is almost quantitative, and selectivity towards the fully hydrogenated product (c) is observed, for both long short reaction times (3 and 24 h). Lowering the H2 pressure to 10 bar results in a decreased conversion just a 3 h of reaction, and a mixture of the three hydrogenation and H-transfer products.
Performing the catalytic test for 3 h at 60 bar H2 results in 80% conversion and (a) is the major product (46% yield) followed by (c) (25%) and traces of (b) (9%). These results suggest that hydrogenation mainly occurs via H2 at a high pressure, whereas H-transfer becomes more significant at lower H2 pressures.
This point was further supported by performing the reactions in toluene rather than iPrOH (Table 7). Significant amounts of (a) are formed, especially operating at a low H2 pressure and/or with a short reaction time. Increasing the H2 pressure and reaction time, (c) becomes the major products, whereas the formation of (b) is always limited.
Clusters 2–4 display some activities as catalyst precursors in the transfer hydrogenation of 4-fluoroacetophenone. The fact that catalyst loading and addition of a base have a different effect on 2–4 as compared to that on the homometallic cluster 1 suggests that their heterometallic nature somehow aids the catalytic process, as also found previously for Ru–M (M = Cu, Ag, Au) clusters.50 Cluster 2 is also active as the catalyst precursor in the hydrogenation of trans-cinnamaldehyde. Depending on the solvent, atmosphere (N2 or H2) and H2 pressure, both a hydrogen transfer mechanism and direct hydrogenation by H2 are observed.
As a final remark, the present findings seem to confirm the synergistic effects of Ru–Ir systems evidenced in the Introduction section. These might be, at least in part, due to the capacity of Ir to form stronger bonds than Ru and/or to some slight polarization of the heterometallic Ru–Ir bonds.
[NEt4]4[2]·CH3CN: C20H22IrNO12Ru3 (963.79): calcd (%): C 24.92, H 2.30, N 1.45; found: C 25.09, H 2.17, N 1.58. IR (CH2Cl2, 298 K) νCO: 2078(w), 2041(m), 2005(vs), 1973(m), 1797(w) cm−1. IR (Nujol, 298 K) νCO: 2077(w), 2034(s), 2001(vs), 1935(m), 1792(w) cm−1. 1H NMR (400 MHz, CD2Cl2, 298 K) δ: −20.7 ppm. ESI-MS (m/z): ES- 835 [M]−; ES+ 130 [NEt4]+.
3: C12H3IrO12Ru3 (834.55): calcd (%): C 17.27, H 0.36; found: C 17.42, H 0.59. IR (THF, 298K) νCO: 2078(vs), 2064(m), 2049(s), 2029(m), 2018(m) cm−1. IR (Nujol, 298 K) νCO: 2075(m), 2048(s), 2023(vs), 2003(vs) cm−1. 1H NMR (400 MHz, CD2Cl2, 298 K) δ(ppm): −17.8 ppm. ESI-MS (m/z): 3 is deprotonated to 2 during ESI-MS analysis.
[PPN]2[4]: C84H61IrN2O12P4Ru3 (1909.63): calcd (%): C 52.83, H 3.22, N 1.47; found: C 52.64, H 2.87, N 1.78. IR (CH2Cl2, 298 K) νCO: 2023(w), 1976(s), 1961(vs), 1917(m), 1767(m), 1751(m) cm−1. IR (Nujol, 298 K) νCO: 2025(w), 2020(w), 1971(s), 1950(vs), 1915(s), 1760(m), 1755(m) cm−1. 1H NMR (400 MHz, acetone d6, 298 K) δ: −19.9 ppm. ESI-MS (m/z): 4 is protonated to 2 during ESI-MS analysis.
[NEt4]2[4]: C28H41IrN2O12Ru3 (1093.06): calcd (%): C 30.77, H 3.78, N 2.56; found: C 30.52, H 3.94, N 2.34. IR (CH3CN, 298 K) νCO: 1979(s), 1959(vs), 1910(m), 1759(m) cm−1. 1H NMR (400 MHz, CD2Cl2, 298 K) δ(ppm): −19.4 ppm.
[NEt4]2[4]: C28H41IrN2O12Ru3 (1093.06): calcd (%): C 30.77, H 3.78, N 2.56; found: C 30.91, H 3.62, N 2.29. IR (CH2Cl2, 298 K) νCO: 2023(w), 1976(s), 1961(vs), 1917(m), 1767(m), 1751(m) cm−1. 1H NMR (400 MHz, acetone d6, 298 K) δ: −19.9 ppm.
[NEt4]2[4]: C28H41IrN2O12Ru3 (1093.06): calcd (%): C 30.77, H 3.78, N 2.56; found: C 30.91, H 3.62, N 2.29. IR (CH2Cl2, 298 K) νCO: 2023(w), 1976(s), 1961(vs), 1917(m), 1767(m), 1751(m) cm−1. 1H NMR (400 MHz, acetone d6, 298 K) δ: −19.9 ppm.
[NEt4]2[6]: C28H41N2O12RhRu3 (1003.75): calcd (%): C 33.50, H 4.12, N 2.79; found: C 33.21, H 4.35, N 2.50. IR (acetone, 298 K) νCO: 2014(w), 1956(vs), 1936(m), 1903(w). IR (Nujol, 298 K) νCO: 2015(w), 1957(vs), 1923(s), 1903(s), 1808(w), 1783(m), 1769(m), 1727(m) cm−1. 1H NMR (400 MHz, acetone d6, 298 K) δ: −15.7 ppm (d, 1JH-Rh = 17 Hz).
[NEt4]2[5]: C25H40Cl6Ir2N2O9Ru2 (1311.83): calcd (%): C 22.89, H 3.07, N 2.14; found: C 23.05, H 2.89, N 2.38. IR (THF, 298K) νCO: 2048(vs), 2038(m), 2024(s), 2010(s), 1965(s) cm−1.
As noticed by one referee during revision, there are some problems with these structures. Something has gone seriously wrong with data collection and/or date reduction steps. Nonetheless, there is no question regarding the overall connectivity of the heavy elements. These problems are mainly due to absorption effects. Multi-scan absorption corrections have been applied to all the structures. Indeed, all the crystals are irregular making face indexing very difficult. Despite several attempts, it was not possible to obtain better crystals. Face index corrections instead of multi-scan have sometimes been attempted, without any improvement. Therefore, in some cases, residual electron densities close to heavy atoms are still present after refinement, due to the above mentioned problems in applying absorption corrections to irregular thin plates and needles. In order to help the reader assessing the quality of these structures and related problems, images of residual electron densities, observed and calculated structure factors (Fobsvs. Fcalc plot), and fractal dimension plots are included as Fig. S42–S51 in the ESI.†
Footnote |
† Electronic supplementary information (ESI) available: Supplementary experimental and computational figures and tables. Crystal data and collection details (PDF). DFT-optimized coordinates in the XYZ format (xyz). CCDC 2256428 ([NEt4][2]), 2256429 (3), 2256431 ([NEt4]2[5]), and 2256432 ([NEt4]2[6]), contain the supplementary crystallographic data for this paper. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d3nj03478j |
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