Open Access Article
Maialen
Espinal-Viguri
,
Victor
Varela-Izquierdo
,
Fedor M.
Miloserdov
,
Ian M.
Riddlestone
,
Mary F.
Mahon
* and
Michael K.
Whittlesey
*
Department of Chemistry, University of Bath, Claverton Down, Bath BA2 7AY, UK. E-mail: m.k.whittlesey@bath.ac.uk
First published on 19th February 2019
The ruthenium–zinc heterobimetallic complexes, [Ru(IPr)2(CO)ZnMe][BArF4] (7), [Ru(IBiox6)2(CO)(THF)ZnMe][BArF4] (12) and [Ru(IMes)′(PPh3)(CO)ZnMe] (15), have been prepared by reaction of ZnMe2 with the ruthenium N-heterocyclic carbene complexes [Ru(IPr)2(CO)H][BArF4] (1), [Ru(IBiox6)2(CO)(THF)H][BArF4] (11) and [Ru(IMes)(PPh3)(CO)HCl] respectively. 7 shows clean reactivity towards H2, yielding [Ru(IPr)2(CO)(η2-H2)(H)2ZnMe][BArF4] (8), which undergoes loss of the coordinated dihydrogen ligand upon application of vacuum to form [Ru(IPr)2(CO)(H)2ZnMe][BArF4] (9). In contrast, addition of H2 to 12 gave only a mixture of products. The tetramethyl IBiox complex [Ru(IBioxMe4)2(CO)(THF)H][BArF4] (14) failed to give any isolable Ru–Zn containing species upon reaction with ZnMe2. The cyclometallated NHC complex [Ru(IMes)′(PPh3)(CO)ZnMe] (15) added H2 across the Ru–Zn bond both in solution and in the solid-state to afford [Ru(IMes)′(PPh3)(CO)(H)2ZnMe] (17), with retention of the cyclometallation.
Very recently, we reported that addition of GaMe3, InMe3 and ZnEt2 to the bulky N-heterocyclic carbene (NHC) stabilised cationic ruthenium hydride complex [Ru(IPr)2(CO)H][BArF4] (1; IPr = 1,3-bis(2,6-diisopropylphenyl)imidazol-2-ylidene; BArF4 = [B{C6H3(3,5-CF3)2}4]−)5 resulted in alkane elimination and formation of the Ru–Ga, Ru–In and Ru–Zn complexes 2–4 shown in Scheme 1.6 Of most relevance to this current paper was the ruthenium–zinc complex [Ru(IPr)2(CO)ZnEt][BArF4] (4) which, upon treatment with H2, both coordinated dihydrogen at Ru and added H2 across the Ru–Zn bond to give [Ru(IPr)2(CO)(η2-H2)(H)2ZnEt][BArF4] (5). Dissociation of the dihydrogen ligand from this highly fluxional species took place upon heating under vacuum to give the agostically stabilised dihydride complex, [Ru(IPr)2(CO)(H)2ZnEt][BArF4] (6, Scheme 1).7,8
Structural analysis showed that 4 (as well as 1) was also agostically stabilised, in this case through a bifurcated η3-H2C ξ-agostic interaction involving an iPr substituent of the IPr ligand. Thus, while 1 and 4 appear at first sight to be rare examples of isolable, four-coordinate Ru(II) complexes, the bifurcated agostic interactions impart formally 18-electron configurations. The participation of the bulky IPr ligand in forming agostic interactions seems to play a role in allowing 1, 4 and 6 to be isolated and structurally characterised, given that the less sterically crowded analogue [Ru(IMes)2(CO)H]+ (IMes = 1,3-bis(2,4,6-trimethylphenyl)imidazol-2-ylidene) is found only as an oil.9
Herein, we describe efforts to elaborate on the chemistry of 1 and 4–6 through studies in which (i) the reactivity of 1 towards other ZnR2 reagents (R = Me, Ph) is probed and (ii) analogues containing the bulky oxazoline-derived IBiox class of NHC ligands are investigated. We also show that the formation of coordinatively unsaturated and reactive (NHC)Ru–Zn complexes is not limited to just cationic Ru–H precursors.10
Upon exposure of a fluorobenzene solution of 7 to 1 atm H2, an instantaneous change in colour from red-orange to colourless was observed, resulting from the formation of the dihydrogen dihydride complex, [Ru(IPr)2(CO)(η2-H2)(H)2ZnMe][BArF4] (8, Scheme 2).11 This showed less fluxional behavior than the ZnEt analogue 5, exhibiting three low frequency hydride signals (δ −5.15, −7.83 and −12.16 in a 2
:
1
:
1 ratio) at room temperature compared to just two resonances for 5 (δ −5.33 and −12.13 in a 3
:
1 ratio). Cooling a THF solution of 8 to 238 K led to sharpening of the two lower frequency resonances, whereas that at ca. −5 ppm remained broader than the others even down to 218 K. Based upon the comparable chemical shifts and assignments in 5, the three signals were assigned to Ru(η2-H2), Ru–H–Zn trans to CO and Ru–H–Zn trans to η2-H2 in order of decreasing frequency.
The η2-H2 ligand in 8 could be removed simply by the application of vacuum to a solid sample of the compound (cf. vacuum and heat for 5, Scheme 1). The resulting product, [Ru(IPr)2(CO)(H)2ZnMe][BArF4] (9), was identified by the appearance of a low frequency (δ −25.77) doublet (2JHH = 7.7 Hz) resonance for Ru–H–Zn trans to the agostic Ru⋯H2C the IPr ligand (vide infra), together with a higher frequency doublet (δ −4.19, 2JHH = 7.7 Hz) arising from the Ru–H–Zn hydride trans to CO.
The Ru–Zn complexes 8 and 9 were characterised crystallographically (Fig. 2). As anticipated, a comparison of these two complexes to their ZnEt analogues 5 and 6 (Scheme 3) shows the same patterns i.e. elongation of the Ru⋯Zn distance relative to 4 and 7, less asymmetry of the Ru–H–Zn distances for H trans to CO and greater association with Ru for H trans to either an agostic interaction (6 and 9) or a dihydrogen ligand (5 and 8).
![]() | ||
| Scheme 3 Summary of key distances in [Ru(IPr)2(CO)(H)2ZnR][BArF4] and [Ru(IPr)2(CO)(η2-H2)(H)2ZnR][BArF4] (R = Et, Me). | ||
Employing previous methodology,15 the bis-carbene complexes [Ru(IBiox6)2(CO)HCl] (10; for structure of IBiox6, see Scheme 4) and [Ru(IBioxMe4)2(CO)HCl] (13; for structure of IBioxMe4, see Scheme 5) were isolated in ca. 50–70% yield after heating [Ru(AsPh3)3(CO)H2] with 2.5 equivalents of the free carbenes, followed by addition of dichloromethane. The 1H NMR spectra of these 16-electron species displayed a low frequency hydride resonance (10: δ −24.75; 13: δ −25.14) characteristic of [Ru(NHC)2(CO)HCl] complexes.15,16 Addition of NaBArF4 led to abstraction of the chloride ligand to give [Ru(IBiox6)2(CO)(THF)H][BArF4] (11, Scheme 4) and [Ru(IBioxMe4)2(CO)(THF)H][BArF4] (14, Scheme 5) respectively. The X-ray structures of neither 11 nor 14 (Fig. 3) showed any agostic interactions to the substituents on the IBiox ligands (e.g. shortest C–H⋯Ru in 11 is 3.182 Å).13a,c In order to relieve the electron-deficiency of the Ru(II) centres, a THF ligand resides in the metal coordination sphere of each complex trans to CO.17
The X-ray crystal structure of 10 and 13, along with those of the cations in 11 and 14, are shown in Fig. 3. A listing of metrical data for the compounds is given in Table 1. As expected, all four compounds exhibited square pyramidal geometries with the hydride ligand in an apical position. Analysis of the NHC tilting angle ΘNHC (Ru–CNHC–centroidNHC)18 revealed angles of >170° in all cases, showing that, despite the coordinative unsaturation at ruthenium, the IBiox ligands remain free of any structural distortions akin to those seen in some [M(IBiox)3]+ (M = Rh, Ir) species.13c
| 10 | 13 | 11 (X = H) | 14 (X = H) | 12 (X = ZnMe) | |
|---|---|---|---|---|---|
| Ru–CIBiox | 2.122(4) | 2.086(3) | 2.112(2), 2.116(3) | 2.093(3), 2.098(3) | 2.120(3), 2.127(3) |
| Ru–CO | 1.782(19) | 1.825(11) | 1.797(4) | 1.795(4) | 1.818(3) |
| Ru–Cl | 2.375(4) | 2.405(3) | — | — | — |
| Ru–O | — | — | 2.168(2) | 2.197(2) | — |
| Ru–Zn | — | — | — | — | 2.3819(4) |
| Ru–CIBiox–IBiox centroid18 | 175.87 | 176.96 | 174.07, 174.01 | N/A due to disorder | 170.84, 171.13 |
| Cl–Ru–CO | 170.0(8) | 179.2(5) | — | — | — |
| O–Ru–CO | — | — | 178.89(17) | 177.99(13) | 154.59(10) |
| Zn–Ru–CO | — | — | — | — | 134.11(6) |
Efforts to generate new Ru–Zn containing complexes through reaction of 11 and 14 with ZnMe2 was successful only in the case of the former,19 which generated [Ru(IBiox6)2(CO)(THF)ZnMe][BArF4] (12, Fig. 4 and Scheme 4). A comparison between the structures of 4 and 12 yield some superficial similarities and some interesting differences. Both structures contain two trans NHC ligands and coordination bonds in the equatorial plane of which two are common, namely, one to a zinc centre and one to a CO ligand. In 4, the remaining site is occupied by a bifurcated agostic interaction, while in 12, there is coordination of a THF molecule. In gross terms, the structures of both cations overlay reasonably well, but the biggest significant difference between them lies in the relative orientations of the NHC ligands. In 4, the angle between the mean planes based on the 5-membered NHC rings is relatively staggered at 102°, while the comparable angle in 12 (32°) reflects a more eclipsed carbene conformation. The arising steric ramifications are that the CNHC–Ru–CNHC angle of 177.32(19) Å in 4 is noticeably more linear than the 170.96(10)° angle observed in 12. It is possible that the significantly shorter Ru–Zn distance of 2.3819(4) Å in 12 (cf. 2.4069(7) Å in 4) may reflect the less encumbered access of the zinc ligand, towards the ruthenium centre, via the opposite face of the cation to the NHC ligand fold.
Upon exposure to either 1 or 5 atm H2, NMR spectra of fluorobenzene solutions of 12 exhibited signals for free IBiox6 as well as the salt [IBiox6·H][BArF4]. Any products of initial reaction with H2 therefore appear to be of only limited stability.
The similarity of chemical shifts and J values for both species (e.g. each exhibited a high frequency resonance for the carbenic carbon with a 2JCP value of >80 Hz, indicative of a trans IMes-Ru-PPh3 geometry) suggested that they were most likely conformers. There was a slight solvent dependence on the solution ratio of 15a
:
15b (88
:
12 and 82
:
18 in C6D6 and THF-d8 respectively). The two species were shown to be in exchange in THF-d8 by EXSY, although NOESY measurements failed to divulge any information as to the spatial difference between 15a and 15b. We were unable to establish any difference crystallographically as measurements of a number of different single crystals only ever afforded the same structure as shown in Fig. 5.
Upon addition of 1 atm H2 to a deep red-orange C6D6 solution of 15, an instant colour change to very pale ensued from formation of [Ru(IMes)′(PPh3)(CO)(H)2ZnMe] (17). The 1H NMR spectrum showed the presence of two doublet hydride resonances at δ −6.77 (2JHP = 14.9 Hz) and δ −9.19 (2JHP = 5.0 Hz), alongside a higher frequency doublet at δ 3.22 and doublet of doublets at δ 1.83, consistent with addition of H2 across the Ru–Zn bond rather than reversal of the IMes cyclometallation. This irreversibility contrasts with what we observed previously in the case of the related cyclometallated hydride derivative [Ru(IMes)′(PPh3)2(CO)H], which reacted with H2 to form [Ru(IMes)(PPh3)2(CO)H2].20a Equally surprisingly, monitoring of the reaction with H2 in the solid-state by IR spectroscopy showed complete depletion of νCO for 15 at 1860 cm−1 and appearance of a new carbonyl absorption band at 1941 cm−1 for 17 upon stirring a ground up microcrystalline sample of the former under 1 atm H2 for 2 days at room temperature.
The X-ray crystal structures of 15 and 17 (Fig. 5) show clearly the transformation of 5-coordinate 15 to six-coordinate 17 upon reaction with H2. As anticipated (vide supra), elongation of the Ru–Zn distance from 2.3677(3) Å to 2.4828(3) Å takes place upon H2 addition. Both bridging hydrogens were located and refined without restraints. As in 6 and 9, the hydride trans to CO was more evenly shared between Ru and Zn than that, which in the case of 17, lies trans to the methylene group of the activated IMes ligand. As a result of cyclometallation, neither 15 nor 17 showed a strictly linear CIMes′–Ru–P geometry (172.32(6) and 169.10(6)° respectively). 15 exhibited a particularly noticeable distortion of the angle at the cyclometallated methylene carbon (Ru(1)–C(3)–C(4) = 83.39(12)°).21
Preliminary studies to investigate the mechanism of formation of 17 revealed that exposure of 17 to D2 (1 atm) resulted in slow (1 day, room temperature) deuterium incorporation into both Ru–H–Zn positions, but no H/D exchange at RuCH2. This excludes exchange taking place via a reversible reductive elimination pathway involving both RuH and RuCH2.22 The viability of an alternative pathway through phosphine dissociation was probed by reaction of 17 with 5 equiv. P(p-tolyl)3. Slow PPh3/P(p-tolyl)3 was indeed observed, but the relevance of this to the H/D exchange was complicated by the appearance of other low frequency proton signals arising from the decomposition of 17 that can be seen in solution over 1–2 days.
NCH), 2.42 (sept, 3JHH = 6.8 Hz, 4H, CH(CH3)2), 2.32 (sept, 3JHH = 6.8 Hz, 4H, CH(CH3)2), 1.10 (d, 3JHH = 6.8 Hz, 12H, CH(CH3)2), 1.07 (d, 3JHH = 6.8 Hz, 12H, CH(CH3)2), 1.00 (d, 3JHH = 6.8 Hz, 12H, CH(CH3)2), 0.65 (d, 3JHH = 6.8 Hz, 12H, CH(CH3)2), −0.86 (s, 3H, ZnCH3). 13C{1H} NMR: δC (101 MHz, CD2Cl2, 298 K, [BArF4]− signals are omitted) 200.6 (s, RuCO), 188.0 (s, RuCNHC), 146.5 (s), 146.3 (s), 135.7 (s), 131.7 (s), 126.3 (s), 126.1 (s), 124.1 (s), 29.8 (s), 29.3 (s, CH(CH3)2), 25.9 (s), 24.7 (s), 24.2 (s), 23.7 (s, CH(CH3)2), −0.71 (s, ZnCH3). IR (CH2Cl2, cm−1): 1919 (νCO). Anal. calcd for C88H87BN4OF24ZnRu: C, 57.14, H, 4.74, N, 3.03. Found: C, 56.79, H, 4.70, N, 2.78.
NCH), 2.19 (sept, 3JHH = 6.8 Hz, 8H, CH(CH3)2), 1.10 (d, 3JHH = 6.8 Hz, 12H, CH(CH3)2), 1.01–0.98 (m, 36H, CH(CH3)2), −0.66 (s, 3H, ZnCH3), −5.15 (br s, 2H, Ru(η2-H2)), −7.83 (br s, 1H, RuHZn), −12.16 (s, 1H, RuHZn). 13C{1H} NMR: δC (126 MHz, CD2Cl2, 298 K, [BArF4]− signals are omitted) 196.8 (s, RuCO), 179.6 (s, RuCNHC), 146.3 (s), 145.0 (s), 137.2 (s), 131.7 (s), 126.4 (s), 126.0 (s), 125.9 (s), 29.5 (s), 29.2 (s, CH(CH3)2), 26.4 (s), 26.2 (s), 22.9 (s), 22.6 (s, CH(CH3)2), 1.38 (s, ZnCH3). IR (CD2Cl2, cm−1): 2005 (νCO). Anal. calcd for C88H91BN4OF24ZnRu·CH2Cl2: C, 55.13, H, 4.83, N, 2.89. Found: C, 55.6, H, 4.64, N, 2.48.
NCH), 2.35 (sept, 3JHH = 6.8 Hz, 4H, CH(CH3)2), 2.19 (sept, 3JHH = 6.8 Hz, 4H, CH(CH3)2), 1.04–0.99 (m, 36H, CH(CH3)2), 0.44 (d, 3JHH = 6.8 Hz, 12H, CH(CH3)2), −0.72 (s, 3H, ZnCH3), −4.19 (d, 2J = 7.7 Hz, 1H, RuHZn), −25.77 (d, 2JHH = 7.7 Hz, 1H, RuHZn). 13C{1H} NMR: δC (101 MHz, CD2Cl2, 298 K, [BArF4]− signals are omitted) 198.3 (s, RuCO), 182.2 (s, RuCNHC), 146.5 (s), 144.9 (s), 136.4 (s), 131.4 (s), 126.7 (s), 125.8 (s), 125.5 (s), 29.3 (s), 29.3 (s, CH(CH3)2), 26.1 (s), 24.9 (s), 23.1 (s), 22.2 (s, CH(CH3)2), 15.7 (s, ZnCH3). IR (CD2Cl2, cm−1): 2005 (νCO). Anal. calcd for C88H89BN4OF24ZnRu: C, 57.07, H, 4.84, N, 3.03. Found: C, 57.44, H, 4.62, N, 2.90.
NCH), 6.21 (d, 3JHH = 1.7 Hz, 1H, NCH
NCH), 6.00 (s, 1H, Ar), 3.17 (br t, 2JHH = 3JHP = 5.9 Hz, 1H, RuCHH), 2.27 (s, 3H, CH3), 2.23 (s, 3H, CH3), 2.08 (s, 6H, CH3), 1.99 (s, 6H, CH3), 1.59 (dd, 3JHP = 11.6 Hz, 2JHH = 6.5 Hz, 1H, RuCHH), −0.57 (s, 3H, ZnCH3). 31P{1H} NMR: δP (162 MHz, C6D6, 298 K) 52.1 (s). 13C{1H} NMR: δC (101 MHz, C6D6, 298 K) 206.7 (d, 2JCP = 11 Hz, RuCO), 196.2 (d, 2JCP = 83 Hz, RuCNHC), 139.1 (s, Ar), 138.9 (d, JCP = 12 Hz, PPh3), 137.5 (s, Ar), 136.6 (s, Ar), 136.3 (s, Ar), 135.2 (s, Ar), 134.4 (d, JCP = 12.0 Hz, PPh3), 133.1 (s, Ar), 131.6 (s, Ar), 130.5 (s, Ar), 130.2 (s, Ar), 129.1 (d, JCP = 1 Hz, PPh3), 128.9 (s, Ar), 128.1 (s, Ar), 125.7 (s, Ar), 122.3 (d, 4JCP = 3 Hz, NCH
CHN), 120.3 (d, 4JCP = 3 Hz, NCH
CHN), 31.6 (d, 2JCP = 7 Hz, RuCH2), 21.3 (s, CH3), 21.1 (s, CH3), 19.0 (s, CH3), 18.7 (s, CH3), 18.1 (s, CH3), −1.5 (d, 3JCP = 3 Hz, ZnCH3). 1H NMR: δH (500 MHz, THF-d8, 298 K) 7.47–7.13 (m, 17H, Ar + NCH
CHN), 7.00 (s, 1H, Ar) 6.99 (s, 1H, Ar), 6.62 (s, 1H, Ar), 5.55 (s, 1H, Ar), 2.61 (br t, 2JHH = 3JHP = 5.6 Hz, 1H, RuCHH), 2.34 (s, 3H, CH3), 2.30 (s, 3H, CH3), 2.25 (s, 3H, CH3), 2.17 (s, 3H, CH3), 1.87 (s, 3H, CH3), 0.98 (dd, 3JHP = 11.6 Hz, 2JHH = 6.7 Hz, 1H, RuCHH), −1.21 (s, 3H, ZnCH3). 31P{1H} NMR: δP (202 MHz, THF-d8, 298 K) 50.1 (s). Selected 13C{1H} NMR: δC (126 MHz, THF-d8, 298 K) 206.4 (d, 2JCP = 11 Hz, RuCO), 195.9 (d, 2JCP = 83 Hz, RuCNHC), 31.1 (d, 2JCP = 7 Hz, RuCH2), −2.4 (d, 3JCP = 4 Hz, ZnCH3). 15b: 1H NMR: δH (500 MHz, THF-d8, 298 K) 7.73 (s, 1H, NCH
NCH), 7.47–7.13 (m, 16 H, PPh3 and NCH
NCH), 6.95 (s, 1H, Ar), 6.92 (s, 1H, Ar), 6.46 (s, 1H, Ar), 6.03 (s, 1H, Ar), 2.28 (s, 3H, CH3), 2.26 (s, 3H, CH3), 2.16 (s, 3H, CH3), 2.12 (s, 3H, CH3), 1.86 (s, 3H, CH3), 1.52 (m, 1H, RuCHH), 1.40 (dd, 3JHP = 14.4 Hz, 2JHH = 8.6 Hz, 1H, RuCHH), −0.90 (s, 3H, ZnCH3). 31P{1H} NMR: δP (202 MHz, THF-d8, 298 K) 57.1 (s). Selected 13C{1H} NMR: δC (126 MHz, THF-d8, 298 K) 203.3 (d, 2JCP = 8 Hz, RuCO), 200.1 (d, 2JCP = 82 Hz, RuCNHC), 31.7 (d, 2JCP = 9 Hz, RuCH2), −4.0 (s, ZnCH3). IR (KBr, cm−1): 1860 (νCO). Anal. calcd for C41H41N2OPRuZn: C, 63.52, H, 5.33, N, 3.61. Found: C, 63.30, H, 5.30, N, 3.69.
CHN), 6.77 (s, 1H, Ar), 6.74 (s, 1H, Ar), 6.68 (s, 1H, Ar), 6.62 (s, 1H, Ar), 6.17 (d, 3JHH = 1.4 Hz, 1H, NCH
CHN), 3.22 (d, 2JHH = 9.2 Hz, 1H, RuCHH), 2.26 (s, 3H, CH3), 2.14 (s, 3H, CH3), 2.13 (s, 3H, CH3), 2.07 (s, 6H, CH3), 1.83 (dd, 3JHP = 12.3 Hz, 2JHH = 9.6 Hz, 1H, RuCHH), −1.29 (s, 3H, ZnCH3), −6.77 (d, 2JHP = 14.9 Hz, 1H, RuHZn), −9.19 (d, 2JHP = 5.0 Hz, RuHZn). 31P{1H} NMR: δP (202 MHz, C6D6, 298 K) 55.4 (s).13C{1H} NMR: δC (126 MHz, C6D6, 298 K) 203.0 (d, 2JCP = 14 Hz, RuCO), 194.6 (d, 2JCP = 83 Hz, RuCNHC), 156.0 (s, Ar), 139.9 (s, Ar), 138.7 (d, JCP = 38 Hz, PPh3), 137.8 (s, Ar), 137.1 (s, Ar), 136.7 (s, Ar), 135.4 (s, Ar), 135.1(s, Ar), 134.4 (d, JCP = 11 Hz, PPh3), 130.8 (s, Ar), 130.5 (s, Ar), 129.4 (s, PPh3), 128.8 (s, Ar), 125.2 (s, Ar), 121.8 (d, 4JCP = 2 Hz, NCH
CHN), 119.5 (d, 4JCP = 3 Hz, NCH
CHN), 21.3 (s, CH3), 21.1 (s, CH3), 19.8 (s, CH3), 18.7 (s, CH3), 18.4 (s, CH3), 7.7 (d, 2JCP = 7 Hz, RuCH2), −5.4 (s, ZnCH3). IR (KBr, cm−1): 1941 (νCO). Efforts to record elemental analyses repeatedly gave low %C values (e.g. Anal. calcd for C41H43N2OPRuZn: C, 63.36, H, 5.58, N, 3.60. Found: C, 61.23, H, 5.40, N, 3.65) which we attribute to the decomposition of the compound with time.
:
50 disorder ratio while F1–F3 exhibited 70
:
30 disorder. Moreover, the entire CF3 moieties based on C71 and C80 were refined to take account of 70
:
30 and 55
:
45 disorder levels, respectively.
| Identification code | 7 | 8 | 9 | 10 | 11 |
|---|---|---|---|---|---|
| Empirical formula | C88H87BF24N4ORuZn | C88H91BF24N4ORuZn | C89H91BCl2F24N4ORuZn | C41H55ClN4O5Ru | C77H74BF25N4O6Ru |
| Formula weight | 1849.86 | 1853.89 | 1936.80 | 820.41 | 1738.28 |
| Crystal system | Orthorhombic | Triclinic | Triclinic | Monoclinic | Triclinic |
| Space group | P212121 |
P![]() |
P![]() |
C2/c |
P![]() |
| a/Å | 16.4346(4) | 12.7837(2) | 13.1638(4) | 22.2537(14) | 14.9600(4) |
| b/Å | 21.1397(5) | 17.1267(3) | 17.7078(6) | 13.5448(8) | 15.8674(5) |
| c/Å | 24.5462(5) | 20.4172(3) | 19.6253(6) | 12.4203(7) | 16.5741(5) |
| α/° | 90 | 84.063(1) | 95.885(2) | 90 | 87.261(3) |
| β/° | 90 | 88.767(1) | 94.337(2) | 93.810(5) | 80.381(2) |
| γ/° | 90 | 85.402(1) | 98.208(2) | 90 | 75.276(2) |
| U/Å3 | 8527.9(3) | 4431.51(12) | 4485.0(2) | 3735.5(4) | 3751.5(2) |
| Z | 4 | 2 | 2 | 4 | 2 |
| ρ calc/g cm−3 | 1.441 | 1.389 | 1.434 | 1.459 | 1.539 |
| μ/mm−1 | 0.559 | 0.538 | 0.593 | 4.463 | 0.327 |
| F(000) | 3784.0 | 1900.0 | 1980.0 | 1720.0 | 1772.0 |
| Crystal size/mm3 | 0.528 × 0.38 × 0.378 | 0.317 × 0.132 × 0.103 | 0.577 × 0.493 × 0.41 | 0.324 × 0.214 × 0.167 | 0.56 × 0.542 × 0.434 |
| Radiation | MoKα | MoKα | MoKα | CuKα | MoKα |
| 2θ range for data collection/° | 6.668 to 54.968 | 5.164 to 61.016 | 6.794 to 54.968 | 10.28 to 145.568 | 6.87 to 54.968 |
| Index ranges | −20 ≤ h ≤ 18 | −18 ≤ h ≤ 18 | −17 ≤ h ≤ 17 | −26 ≤ h ≤ 27 | −17 ≤ h ≤ 19 |
| −27 ≤ k ≤ 27 | −24 ≤ k ≤ 24 | −22 ≤ k ≤ 19 | −16 ≤ k ≤ 16 | −18 ≤ k ≤ 20 | |
| −31 ≤ l ≤ 31 | −29 ≤ l ≤ 28 | −24 ≤ l ≤ 22 | −15 ≤ l ≤ 9 | −21 ≤ l ≤ 21 | |
| Reflections collected | 77 177 |
159 961 |
40 172 |
16 638 |
46 082 |
| Independent reflections, Rint | 19 171, 0.0429 |
26 703, 0.0629 |
19 792, 0.0362 |
3649, 0.0935 | 16 803, 0.0392 |
| Data/restraints/parameters | 19 171/67/1136 |
26 703/157/1267 |
19 792/240/1246 |
3649/0/249 | 16 803/334/1188 |
| Goodness-of-fit on F2 | 1.077 | 1.042 | 1.037 | 1.074 | 1.063 |
| Final R1, wR2, I ≥ 2σ(I) | 0.0511, 0.1112 | 0.0503, 0.1188 | 0.0467, 0.1017 | 0.0512, 0.1314 | 0.0617, 0.1407 |
| Final R1, wR2, all data | 0.0680, 0.1206 | 0.0694, 0.1298 | 0.0675, 0.1136 | 0.0531, 0.1326 | 0.0813, 0.1516 |
| Largest diff. peak/hole/e Å−3 | 0.83/−0.86 | 0.76/−1.18 | 0.88/−0.57 | 0.68/−0.64 | 2.80/−0.68 |
| Flack parameter | 0.017(4) | — | — | — | — |
| Identification code | 12 | 13 | 14 | 15 | 17 |
|---|---|---|---|---|---|
| Empirical formula | C72H71BF24N4O6RuZn | C23H32ClN4O5Ru | C59H52BF24N4O6Ru | C41H41N2OPRuZn | C41H43N2OPRuZn |
| Formula weight | 1721.57 | 581.04 | 1480.92 | 775.17 | 777.18 |
| Crystal system | Triclinic | Monoclinic | Triclinic | Monoclinic | Triclinic |
| Space group |
P![]() |
P21/n |
P![]() |
P21/c |
P![]() |
| a/Å | 12.9608(4) | 10.2772(2) | 9.9024(1) | 10.5880(1) | 9.8428(2) |
| b/Å | 13.1449(4) | 11.4391(2) | 18.4531(2) | 25.6243(2) | 11.4984(3) |
| c/Å | 21.6148(7) | 10.8292(2) | 19.4882(3) | 13.6538(1) | 17.9210(3) |
| α/° | 94.981(3) | 90 | 112.078(1) | 90 | 87.163(2) |
| β/° | 91.296(3) | 99.331(2) | 103.002(1) | 103.780(1) | 81.171(2) |
| γ/° | 97.163(3) | 90 | 96.389(1) | 90 | 65.917(2) |
| U/Å3 | 3637.8(2) | 1256.26(4) | 3138.80(7) | 3597.79(5) | 1829.55(7) |
| Z | 2 | 2 | 2 | 4 | 2 |
| ρ calc/g cm−3 | 1.572 | 1.536 | 1.567 | 1.431 | 1.411 |
| μ/mm−1 | 0.654 | 6.375 | 3.144 | 4.896 | 4.814 |
| F(000) | 1748.0 | 598.0 | 1494.0 | 1592.0 | 800.0 |
| Crystal size/mm3 | 0.561 × 0.375 × 0.27 | 0.072 × 0.058 × 0.019 | 0.283 × 0.229 × 0.094 | 0.471 × 0.095 × 0.092 | 0.116 × 0.08 × 0.05 |
| Radiation | MoKα | CuKα | CuKα | CuKα | CuKα |
| 2θ range for data collection/° | 6.678 to 54.966 | 11.012 to 146.588 | 5.636 to 147.162 | 6.9 to 146.304 | 4.99 to 146.094 |
| Index ranges | −16 ≤ h ≤ 16 | −12 ≤ h ≤ 12 | −9 ≤ h ≤ 12 | −13 ≤ h ≤ 9 | −12 ≤ h ≤ 12 |
| −17 ≤ k ≤ 16 | −14 ≤ k ≤ 11 | −22 ≤ k ≤ 22 | −31 ≤ k ≤ 31 | −14 ≤ k ≤ 14 | |
| −27 ≤ l ≤ 28 | −11 ≤ l ≤ 13 | −24 ≤ l ≤ 24 | −16 ≤ l ≤ 16 | −20 ≤ l ≤ 22 | |
| Reflections collected | 33 375 |
13 001 |
62 311 |
47 648 |
21 138 |
| Independent reflections, Rint | 16 641, 0.0262 |
2531, 0.0392 | 12 599, 0.0418 |
7195, 0.0440 | 7307, 0.0340 |
| Data/restraints/parameters | 16 641/264/1097 |
2531/0/173 | 12 599/2804/1493 |
7195/2/438 | 7307/2/446 |
| Goodness-of-fit on F2 | 1.027 | 1.194 | 1.039 | 1.056 | 1.020 |
| Final R1, wR2, I ≥ 2σ(I) | 0.0441, 0.1015 | 0.0343, 0.0721 | 0.0530, 0.1471 | 0.0279, 0.0729 | 0.0274, 0.0650 |
| Final R1, wR2, all data | 0.0580, 0.1096 | 0.0378, 0.0736 | 0.0573, 0.1523 | 0.0294, 0.0740 | 0.0311, 0.0672 |
| Largest diff. peak/hole/e Å−3 | 0.98/−0.65 | 0.50/−0.55 | 1.46/−1.04 | 1.02/−0.62 | 0.61/−0.52 |
In 9, the asymmetric unit contains one cation, one anion and one molecule of CH2Cl2. H1 and H2 in the cation were located a refined without restraints. The hydrogens attached to C26 were similarly located and refined subject to being located at a distance of 0.98 Å from C26. Fluoride disorder was modelled for two of the [BArF4] CF3 moieties. In particular, F1–F3 were disordered over two sites in a 75
:
25 ratio while F13–15 were disordered over three sites in a 50
:
40
:
10 ratio. The solvent molecule exhibited 55
:
45 disorder and C–Cl distances were restrained to being similar in both moieties. ADP restraints were included for fractional occupancy atoms. The asymmetric unit in 10 equates to half of one molecule of the complex, and half of a benzene molecule. The chloride and carbonyl ligands within the metal complex are disordered with each other in a 50
:
50 ratio. The hydride ligand (which is likely to be disordered over 2 sites) could not be reliably located and, hence, was omitted from the refinement. One cation, one anion and two independent fluorobenzene halves constitute the asymmetric unit in 11. The solvent moieties are proximate to crystallographic inversion centres which serve, in each case, to generate the remaining molecule portions. The halides in these solvent moieties are necessarily disordered and, hence, exhibit half site-occupancies. 75
:
25 disorder was also modelled for C22 in the cation, with chemically similar distances in each disordered component being restrained to being similar. The hydride was also located and is disordered in a 50
:
50 ratio. The associated metal-hydride distances were refined subject to a 1.6 Å, Ru–H, distance restraint. Anion disorder was limited to the halides in five of the CF3 functionalities. Specifically, the fluorines attached to C46, C54, C55, C63 and C70 exhibited disorder ratios of 65
:
35, 55
:
45, 50
:
50, 75
:
25 and 75
:
25, respectively.
Some disorder modelling was necessary in both that cation and the anion present in the asymmetric unit of compound 12. In the cation, this pertained to 55
:
45 disorder confined to atoms C37 and C38 in the THF ligand. Chemically equivalent distances involving the partial occupancy atoms were restrained to being similar in the final least-squares and some ADP restraints were also included for same. Four of the CF3 groups in the anion were seen to exhibit disorder. In particular, the fluorine atoms attached to C47, C56, C63 and C72 were each modelled over 2 sites, in ratios of 55
:
45, 60
:
40, 55
:
45 and 75
:
25, respectively. The asymmetric unit in 13 comprises half of a molecule, with the central ruthenium located at a crystallographic inversion centre. This necessarily means that the chloride and carbonyl ligands are disordered in a 50
:
50 ratio. An exemplary diffraction pattern was observed for crystal of compound 14 where the asymmetric unit was seen to contain one cation and one anion. There was no evident twinning but, yet, the structural motif itself is riddled with disorder. While this was successfully modelled, it has inevitably resulted in the addition of a large number of restraints to the model, as both carbene ligands in the cation were seen to be disordered in a 50
:
50 ratio. The carbene carbons are, in each ligand, common to both components. In addition, C26 in the THF ligand was also seen to exhibit disorder, which optimally refined to a 60
:
40 ratio. Distance similarity restraints and ADP restraints were added to the model for the cation, on merit, in the final refinement cycles. In the BArF4 anion, three of the rings were seen to be disordered in an 80
:
20 ratio. The moiety based on C36 did not exhibit disorder to a level that could be credibly modelled, although the CF3 group based on C42 was treated for 70
:
30 disorder.
In 15, both H3a and H3b were located and subsequently refined subject to each being a distance of 0.98 Å from C3. In a similar vein, the hydrogens attached to C3 were also readily located in 17, and each refined subject to being situated at distance of 0.95 Å from the parent atom. Finally, the bridging hydride ligands were also located in this compound and refined without restraints.
Crystallographic data for all compounds have been deposited with the Cambridge Crystallographic Data Centre as supplementary publications CCDC 1882150 (compound 7), 1882152 (8), 1882151 (9), 1882153 (10), 1882154 (11), 1882155 (12), 1882156 (13), 1882157 (14), 1882158 (15) and 1882159 (17).†
Footnote |
| † Electronic supplementary information (ESI) available: CCDC 1882150–1882159. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c8dt05023f |
| This journal is © The Royal Society of Chemistry 2019 |