research communications
η)-cycloocta-1,5-diene]iridium(I)
of chloridobis[(1,2,5,6-aDepartment of Chemistry, University of Rochester, Rochester, NY 14627, USA
*Correspondence e-mail: william.jones@rochester.edu
The title complex, [IrCl(C8H12)2], was synthesized directly from the reaction of IrCl3·3H2O with a large excess of cod (cod = cycloocta-1,5-diene) in alcoholic solvent. Large yellow needles were obtained by the slow cooling of a hot solution. Based on the positions of the chloride ligand and the mid-points of the four C=C bonds, the molecule adopts a five-coordinate geometry that is midway between square pyramidal and trigonal bipyramidal. The material crystallizes in the orthorhombic Pbca with one molecule per in a general position and shows no significant intermolecular interactions. Individual molecules are aligned along [010], and these rows form a pseudo-hexagonal packing arrangement.
Keywords: crystal structure; iridium; 1,5-cyclooctadiene; five-coordinate complex.
CCDC reference: 1527918
1. Chemical context
First reported in 1966 (Winkhaus & Singer, 1966) [Ir(cod)(μ-Cl)]2 (cod = 1,5-cyclooctadiene, C8H12) is perhaps the most common organometallic precursor used in the synthesis of a variety of organoiridium compounds (Leigh & Richards, 1982). [Ir(cod)(μ-Cl)]2 can be prepared using either Na2IrCl6·6H2O or IrCl3·3H2O as the metal-containing precursor (Herde et al., 1974). A few years later it was reported that a cyclooctene-ligated dimer [Ir(C8H14)2(μ-Cl)]2 had been synthesized from the reaction of ammonium hexachloridoiridiate(III) hydrate, (NH4)3IrCl6·H2O, with cyclooctene in a mixture of 2-propanol and water (Onderdelinden & van der Ent, 1972). In all three cases, IrIV or IrIII is reduced to IrI by oxidation of the alcoholic solvent. Upon suspension in pure cod, [Ir(C8H14)2(μ-Cl)]2 reacted to form mononuclear IrCl(cod)2, which was then characterized by infra-red spectroscopy and elemental analysis (Onderdelinden & van der Ent, 1972). Analogous to thermally unstable IrCl(C2H4)4, which releases ethylene to form the (slightly) more stable dimer [Ir(C2H4)2(μ-Cl)]2 (Onderdelinden & van der Ent, 1972), IrCl(cod)2 readily generates stable [Ir(cod)(μ-Cl)]2 with the loss of one equivalent of cod per iridium. We have found that if Herde's preparation using IrCl3·3H2O is carried out with a large excess of cod (10 ×), the product isolated after removal of the alcoholic solvent is IrCl(cod)2 (Fig. 1). This was apparent as the red–orange reaction mixture, which contained a mixture of red [Ir(cod)(μ-Cl)]2 and yellow IrCl(cod)2, became pale yellow. Recrystallization from refluxing methanol/cod (7:1, v:v) followed by cooling produced yellow needles of IrCl(cod)2 suitable for diffraction studies.
Herein we report the isolation and results of the single 2 and compare it to related IrX(diene)2 (X = Cl, SnMe3, SnCl3) complexes.
of mononuclear IrCl(cod)2. Structural commentary
Our single-crystal X-ray diffraction study confirmed the molecule to be mononuclear IrCl(cod)2, in which the two cod ligands are bound in an η2:η2 fashion (Fig. 2). The material crystallizes in the orthorhombic Pbca, with one molecule per in a general position. The five-coordinate complex adopts a geometry that is midway between square pyramidal (SP) and trigonal bipyramidal (TBP), with a τ5 parameter of 0.52 (Addison et al., 1984), calculated using the mid-points of the C=C double bonds and the axial chlorido ligand. The elongation of the cod double bonds (Table 1) compared to those of non-coordinating cod, 1.333 (4) and 1.334 (4) Å (Byrn et al., 1990), or to that of free ethylene, 1.333 Å (Lide, 2002–2003), is consistent with back donation to the π* orbitals from a low-valent iridium atom, formally IrI. The elongations are asymmetric, with one double bond from each cod ligand being larger than the other by 0.048 (6) and 0.029 (6) Å, respectively, for cod ligands C1—C8 and C9—C16. Likewise the distances between Ir and the mid-points of the C=C bonds also show this asymmetry with two shorter distances, Ir—(C1/C2) = 2.047 (4) and Ir—(C9/C10) = 2.069 (4) Å, and two longer distances, Ir—(C5/C6) = 2.138 (4) and Ir—(C13/C14) = 2.141 (4) Å (Table 2). This is likely due to its intermediacy between the geometric extremes of SP and TBP. Ideal SP geometry (τ5 = 0) would have very similar Ir–mid-point(C=C) distances as they would involve the same metal and ligand orbitals, while ideal TBP geometry (τ5 = 1) would involve different orbitals, dependent upon on whether the ligand's C=C bond lay in an axial or an equatorial position. We see the former (SP) in Ir(SnCl3)(nbd)2 (nbd = norbornadiene; Malosh et al., 2013), for which τ5 = 0.06 and the Ir–mid-point(C=C) distances are similar, ranging from 2.067 (4) to 2.089 (4) Å. An example towards TBP is found in [IrCl(cod)(CC*)]+ (CC* = [(η5-C5H5)Fe(η6-(1,1-di(2-propenyl)-3-butenyl)benzene)]; Marcén et al., 2002), for which τ5 = 0.76.
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3. Supramolecular features
Although there are no significant intermolecular interactions, the packing has adopted a supramolecular arrangement. Individual molecules are aligned in columns parallel to [010], which are then arranged in an overall pseudo-hexagonal packing (Fig. 4).
4. Database survey
A survey of the Cambridge Structural Database (CSD, Version 5.38, update No. 1, November 2016, Groom et al., 2016) revealed just a few related five-coordinate iridium complexes with four unconjugated substituted ethylene ligands and a halido or stannato ligand in the fifth coordination site: Ir(SnCl3)(cod)2 (CSD refcode COIRSN; Porta et al., 1967), Ir(SnMe3)(cod)2 (refcode DIVPAB), Ir(SnCl3)(nbd)2 (refcode DIVPIJ), Ir(SnMe3)(nbd)2 (refcode DIVNUT); Malosh et al., 2013), and [IrCl(cod)(CC*)]+ (refcode PUYCOB; Marcén et al., 2002). A report on the structure of IrCl(C2H4)4 exists, but no positional parameters were given (van der Ent & van Soest, 1970), which is unfortunate because a comparison of this species with IrCl(cod)2 would ostensibly show how the bite-angle restrictions imposed by the cod rings affect the overall geometry. The geometries of the two tin-containing compounds with cod are closely related to that of the title complex. Both Ir(SnCl3)(cod)2 and Ir(SnMe3)(cod)2 exhibit the same long–short variation of the Ir–mid-point(C=C) bond lengths within each cod ligand and have similar τ5 parameters of 0.53 and 0.55, respectively (Table 2). Malosh and coworkers concluded that the bulk of the cod ligands relative to that of the nbd ligands was responsible for the geometric distortion from SP geometry, specifically due to CH2⋯Me and CH2⋯Cl repulsions (Malosh et al., 2013). And indeed the two nbd complexes have near-perfect SP τ5 values of 0.10 and 0.06. In complex [IrCl(cod)(CC*)]+, the non-cod diene is part of a 1,1-di(2-propenyl)-3-butenyl)benzene unit that is η6-coordinating to an [Fe(C5H5)]+ cationic fragment. The pentacoordinated saturated (18 electron) iridium atom approaches a TBP geometry more than the other complexes mentioned (τ5 = 0.76), with the two apical positions being occupied by one C=C bond of the cod ligand and the chlorido ligand. The angles in the equatorial plane range between 109.73 (17) and 126.61 (16)°. The restriction of the cod ligand with its bite angle of 84.9 (2)° prevents the structure from ever achieving perfect TBP geometry, and this holds more so for structures with nbd ligands whose bite angles are even more acute. The Ir–mid-point(C=C) bond lengths differ, showing significantly longer bond lengths to the allylic C=C centroids [avg. 2.144 (11) Å] than to the cod C=C diolefin centroids [avg. 2.052 (11) Å]. The terminal Ir—Cl distance in IrCl(cod)2 of 2.5573 (8) Å is longer than all of the 214 structures with five-coordinate iridium in the CSD containing an IrCl(η2:η2-cod) fragment (avg. 2.368 Å), which may be attributable to its tendency to form the well-known stable cationic complex, [Ir(cod)2]+, whose structure (refcode TUQWOS) displays the anticipated d8 square-planar geometry with [BArF]− {tetrakis[3,5-bis(trifluoromethyl)phenyl]borate} as the non-coordinating anion (Woodmansee et al., 2010).
5. Synthesis and crystallization
All operations and routine manipulations were performed under a nitrogen atmosphere, either on a high-vacuum line using modified Schlenk techniques or in a Vacuum Atmospheres Company Dri-Lab. A preparation of IrCl(cod)2 via a cyclooctene-ligated dimer has been reported previously (Onderdelinden & van der Ent, 1972).
A two-necked round-bottom flask was charged with IrCl3·3H2O (6.0 g, 0.017 mol) and cod (20 g, 0.18 mol) in 80 ml of ethanol under nitrogen. The reaction mixture was refluxed for 24 h, followed by removal of the solvent under vacuum. As the ethanol evaporated, the red–orange solution became more yellow as the cod concentration increased, leading to the isolation of a yellow solid (5.32 g, 70.5%). The product was recrystallized by refluxing in a mixture 35 ml of methanol and 5 ml of cod, followed by cooling to obtain shiny yellow needles of IrCl(cod)2 (5.06 g, 67.0%).
6. Refinement
Crystal data, data collection and structure . H atoms were treated in the riding-model approximation, with C(methine)—H = 1.00 Å, C(methylene)—H = 0.99 Å, and with Uiso(H) = 1.2Ueq(C). The maximum and minimum electron densities are found 1.09 and 0.55 Å, respectively, from the iridium atom.
details are summarized in Table 3
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Supporting information
CCDC reference: 1527918
https://doi.org/10.1107/S2056989017000809/wm5359sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989017000809/wm5359Isup2.hkl
Data collection: APEX3 (Bruker, 2016); cell
SAINT (Bruker, 2016); data reduction: SAINT (Bruker, 2016); program(s) used to solve structure: SHELXT2014 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2016 (Sheldrick, 2015b); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).[IrCl(C8H12)2] | Dx = 2.154 Mg m−3 |
Mr = 444.00 | Mo Kα radiation, λ = 0.71073 Å |
Orthorhombic, Pbca | Cell parameters from 5121 reflections |
a = 12.8756 (8) Å | θ = 2.5–29.0° |
b = 13.3719 (8) Å | µ = 9.93 mm−1 |
c = 15.9033 (10) Å | T = 100 K |
V = 2738.1 (3) Å3 | Block, yellow |
Z = 8 | 0.24 × 0.20 × 0.20 mm |
F(000) = 1712 |
Bruker SMART APEXII CCD platform diffractometer | 5394 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.112 |
ω scans | θmax = 38.9°, θmin = 2.5° |
Absorption correction: multi-scan (SADABS; Krause et al., 2015) | h = −22→22 |
Tmin = 0.173, Tmax = 0.278 | k = −23→23 |
83189 measured reflections | l = −27→27 |
7755 independent reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.035 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.072 | H-atom parameters constrained |
S = 1.01 | w = 1/[σ2(Fo2) + (0.0214P)2] where P = (Fo2 + 2Fc2)/3 |
7755 reflections | (Δ/σ)max = 0.001 |
163 parameters | Δρmax = 1.34 e Å−3 |
0 restraints | Δρmin = −1.86 e Å−3 |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
x | y | z | Uiso*/Ueq | ||
Ir1 | 0.27908 (2) | 0.39530 (2) | 0.59862 (2) | 0.00769 (3) | |
Cl1 | 0.13983 (6) | 0.50996 (6) | 0.66069 (5) | 0.01377 (14) | |
C1 | 0.1656 (3) | 0.2813 (2) | 0.5723 (2) | 0.0116 (5) | |
H1A | 0.145496 | 0.241248 | 0.622824 | 0.014* | |
C2 | 0.2626 (2) | 0.2509 (2) | 0.5357 (2) | 0.0123 (6) | |
H2A | 0.296862 | 0.194607 | 0.566472 | 0.015* | |
C3 | 0.2855 (3) | 0.2514 (3) | 0.4419 (2) | 0.0143 (6) | |
H3A | 0.219685 | 0.241850 | 0.410691 | 0.017* | |
H3B | 0.331572 | 0.194314 | 0.428387 | 0.017* | |
C4 | 0.3373 (3) | 0.3486 (3) | 0.4120 (2) | 0.0157 (6) | |
H4A | 0.413620 | 0.341604 | 0.416347 | 0.019* | |
H4B | 0.319781 | 0.360032 | 0.352151 | 0.019* | |
C5 | 0.3028 (3) | 0.4380 (2) | 0.4632 (2) | 0.0126 (6) | |
H5A | 0.347039 | 0.498657 | 0.455193 | 0.015* | |
C6 | 0.2005 (2) | 0.4593 (2) | 0.4845 (2) | 0.0114 (6) | |
H6A | 0.186019 | 0.532519 | 0.489222 | 0.014* | |
C7 | 0.1063 (3) | 0.3986 (2) | 0.4565 (2) | 0.0142 (6) | |
H7A | 0.122928 | 0.363524 | 0.403371 | 0.017* | |
H7B | 0.047558 | 0.444498 | 0.445506 | 0.017* | |
C8 | 0.0736 (3) | 0.3211 (3) | 0.5234 (2) | 0.0157 (6) | |
H8A | 0.023939 | 0.352582 | 0.562866 | 0.019* | |
H8B | 0.037702 | 0.264779 | 0.495361 | 0.019* | |
C9 | 0.4463 (2) | 0.4276 (2) | 0.5992 (2) | 0.0129 (5) | |
H9A | 0.476894 | 0.435608 | 0.541763 | 0.015* | |
C10 | 0.3907 (2) | 0.5127 (2) | 0.6275 (2) | 0.0127 (6) | |
H10A | 0.390267 | 0.569889 | 0.587016 | 0.015* | |
C11 | 0.3863 (3) | 0.5434 (2) | 0.7186 (2) | 0.0145 (6) | |
H11A | 0.334721 | 0.597717 | 0.724955 | 0.017* | |
H11B | 0.454933 | 0.570368 | 0.735239 | 0.017* | |
C12 | 0.3573 (3) | 0.4571 (2) | 0.7786 (2) | 0.0143 (6) | |
H12A | 0.421967 | 0.428574 | 0.802348 | 0.017* | |
H12B | 0.316321 | 0.484671 | 0.825894 | 0.017* | |
C13 | 0.2957 (3) | 0.3738 (2) | 0.7378 (2) | 0.0122 (6) | |
H13A | 0.228508 | 0.359314 | 0.766834 | 0.015* | |
C14 | 0.3391 (3) | 0.2906 (2) | 0.6990 (2) | 0.0121 (5) | |
H14A | 0.296863 | 0.228253 | 0.705481 | 0.014* | |
C15 | 0.4533 (3) | 0.2717 (2) | 0.6889 (2) | 0.0143 (6) | |
H15A | 0.463587 | 0.216505 | 0.648278 | 0.017* | |
H15B | 0.482493 | 0.250336 | 0.743567 | 0.017* | |
C16 | 0.5120 (2) | 0.3639 (2) | 0.6581 (2) | 0.0132 (6) | |
H16A | 0.533137 | 0.404768 | 0.707119 | 0.016* | |
H16B | 0.575745 | 0.342441 | 0.628395 | 0.016* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ir1 | 0.00792 (5) | 0.00752 (5) | 0.00763 (5) | −0.00044 (4) | −0.00014 (4) | 0.00038 (4) |
Cl1 | 0.0124 (3) | 0.0145 (3) | 0.0144 (4) | 0.0035 (3) | 0.0018 (3) | 0.0005 (3) |
C1 | 0.0128 (13) | 0.0107 (13) | 0.0111 (13) | −0.0039 (11) | −0.0013 (11) | 0.0010 (10) |
C2 | 0.0142 (14) | 0.0104 (13) | 0.0123 (14) | −0.0015 (11) | −0.0020 (11) | −0.0017 (11) |
C3 | 0.0144 (14) | 0.0176 (14) | 0.0109 (14) | −0.0007 (12) | −0.0019 (12) | −0.0048 (11) |
C4 | 0.0157 (14) | 0.0192 (15) | 0.0124 (15) | 0.0007 (12) | 0.0012 (12) | −0.0017 (12) |
C5 | 0.0131 (13) | 0.0136 (14) | 0.0112 (14) | −0.0016 (11) | 0.0016 (11) | 0.0035 (11) |
C6 | 0.0152 (14) | 0.0103 (13) | 0.0088 (13) | 0.0003 (10) | −0.0017 (11) | 0.0034 (10) |
C7 | 0.0114 (13) | 0.0173 (14) | 0.0138 (14) | −0.0011 (12) | −0.0040 (11) | 0.0007 (12) |
C8 | 0.0131 (14) | 0.0182 (15) | 0.0157 (16) | −0.0057 (12) | −0.0012 (12) | −0.0014 (12) |
C9 | 0.0117 (13) | 0.0132 (13) | 0.0137 (14) | 0.0000 (10) | 0.0007 (12) | −0.0007 (12) |
C10 | 0.0136 (13) | 0.0109 (13) | 0.0137 (15) | −0.0019 (11) | 0.0017 (12) | −0.0002 (11) |
C11 | 0.0163 (14) | 0.0125 (14) | 0.0148 (16) | −0.0018 (11) | −0.0025 (12) | −0.0040 (11) |
C12 | 0.0153 (14) | 0.0170 (15) | 0.0106 (14) | 0.0025 (12) | −0.0018 (11) | −0.0025 (11) |
C13 | 0.0145 (14) | 0.0146 (14) | 0.0076 (13) | 0.0001 (11) | 0.0011 (11) | −0.0005 (10) |
C14 | 0.0159 (14) | 0.0109 (13) | 0.0094 (13) | −0.0004 (11) | −0.0012 (12) | 0.0043 (10) |
C15 | 0.0150 (14) | 0.0121 (14) | 0.0158 (16) | 0.0046 (11) | −0.0035 (12) | −0.0004 (11) |
C16 | 0.0106 (13) | 0.0153 (14) | 0.0137 (15) | 0.0026 (11) | −0.0026 (11) | −0.0022 (12) |
Ir1—C1 | 2.152 (3) | C7—H7A | 0.9900 |
Ir1—C10 | 2.178 (3) | C7—H7B | 0.9900 |
Ir1—C2 | 2.185 (3) | C8—H8A | 0.9900 |
Ir1—C9 | 2.196 (3) | C8—H8B | 0.9900 |
Ir1—C13 | 2.242 (3) | C9—C10 | 1.418 (5) |
Ir1—C6 | 2.248 (3) | C9—C16 | 1.522 (5) |
Ir1—C5 | 2.249 (3) | C9—H9A | 1.0000 |
Ir1—C14 | 2.260 (3) | C10—C11 | 1.506 (5) |
Ir1—Cl1 | 2.5573 (8) | C10—H10A | 1.0000 |
C1—C2 | 1.437 (5) | C11—C12 | 1.543 (5) |
C1—C8 | 1.514 (5) | C11—H11A | 0.9900 |
C1—H1A | 1.0000 | C11—H11B | 0.9900 |
C2—C3 | 1.521 (5) | C12—C13 | 1.514 (5) |
C2—H2A | 1.0000 | C12—H12A | 0.9900 |
C3—C4 | 1.537 (5) | C12—H12B | 0.9900 |
C3—H3A | 0.9900 | C13—C14 | 1.389 (4) |
C3—H3B | 0.9900 | C13—H13A | 1.0000 |
C4—C5 | 1.512 (5) | C14—C15 | 1.500 (4) |
C4—H4A | 0.9900 | C14—H14A | 1.0000 |
C4—H4B | 0.9900 | C15—C16 | 1.527 (5) |
C5—C6 | 1.389 (4) | C15—H15A | 0.9900 |
C5—H5A | 1.0000 | C15—H15B | 0.9900 |
C6—C7 | 1.525 (4) | C16—H16A | 0.9900 |
C6—H6A | 1.0000 | C16—H16B | 0.9900 |
C7—C8 | 1.543 (5) | ||
C1—Ir1—C10 | 178.38 (12) | C5—C6—C7 | 125.0 (3) |
C1—Ir1—C2 | 38.68 (12) | C5—C6—Ir1 | 72.04 (18) |
C10—Ir1—C2 | 142.92 (12) | C7—C6—Ir1 | 113.0 (2) |
C1—Ir1—C9 | 143.67 (12) | C5—C6—H6A | 113.3 |
C10—Ir1—C9 | 37.84 (12) | C7—C6—H6A | 113.3 |
C2—Ir1—C9 | 105.71 (12) | Ir1—C6—H6A | 113.3 |
C1—Ir1—C13 | 99.56 (12) | C6—C7—C8 | 111.9 (3) |
C10—Ir1—C13 | 79.68 (12) | C6—C7—H7A | 109.2 |
C2—Ir1—C13 | 110.35 (12) | C8—C7—H7A | 109.2 |
C9—Ir1—C13 | 85.84 (12) | C6—C7—H7B | 109.2 |
C1—Ir1—C6 | 78.85 (12) | C8—C7—H7B | 109.2 |
C10—Ir1—C6 | 101.16 (12) | H7A—C7—H7B | 107.9 |
C2—Ir1—C6 | 85.57 (12) | C1—C8—C7 | 112.1 (3) |
C9—Ir1—C6 | 111.72 (12) | C1—C8—H8A | 109.2 |
C13—Ir1—C6 | 152.77 (12) | C7—C8—H8A | 109.2 |
C1—Ir1—C5 | 94.89 (12) | C1—C8—H8B | 109.2 |
C10—Ir1—C5 | 85.98 (12) | C7—C8—H8B | 109.2 |
C2—Ir1—C5 | 78.39 (12) | H8A—C8—H8B | 107.9 |
C9—Ir1—C5 | 79.69 (12) | C10—C9—C16 | 122.2 (3) |
C13—Ir1—C5 | 164.79 (12) | C10—C9—Ir1 | 70.37 (18) |
C6—Ir1—C5 | 36.00 (11) | C16—C9—Ir1 | 115.9 (2) |
C1—Ir1—C14 | 86.02 (12) | C10—C9—H9A | 113.8 |
C10—Ir1—C14 | 94.13 (12) | C16—C9—H9A | 113.8 |
C2—Ir1—C14 | 78.99 (12) | Ir1—C9—H9A | 113.8 |
C9—Ir1—C14 | 77.53 (12) | C9—C10—C11 | 122.9 (3) |
C13—Ir1—C14 | 35.94 (11) | C9—C10—Ir1 | 71.79 (18) |
C6—Ir1—C14 | 163.81 (12) | C11—C10—Ir1 | 112.0 (2) |
C5—Ir1—C14 | 141.95 (12) | C9—C10—H10A | 114.3 |
C1—Ir1—Cl1 | 91.36 (9) | C11—C10—H10A | 114.3 |
C10—Ir1—Cl1 | 87.07 (9) | Ir1—C10—H10A | 114.3 |
C2—Ir1—Cl1 | 129.69 (8) | C10—C11—C12 | 113.6 (3) |
C9—Ir1—Cl1 | 124.61 (9) | C10—C11—H11A | 108.8 |
C13—Ir1—Cl1 | 76.29 (8) | C12—C11—H11A | 108.8 |
C6—Ir1—Cl1 | 76.57 (9) | C10—C11—H11B | 108.8 |
C5—Ir1—Cl1 | 108.22 (9) | C12—C11—H11B | 108.8 |
C14—Ir1—Cl1 | 109.78 (9) | H11A—C11—H11B | 107.7 |
C2—C1—C8 | 124.9 (3) | C13—C12—C11 | 114.3 (3) |
C2—C1—Ir1 | 71.90 (18) | C13—C12—H12A | 108.7 |
C8—C1—Ir1 | 112.5 (2) | C11—C12—H12A | 108.7 |
C2—C1—H1A | 113.5 | C13—C12—H12B | 108.7 |
C8—C1—H1A | 113.5 | C11—C12—H12B | 108.7 |
Ir1—C1—H1A | 113.5 | H12A—C12—H12B | 107.6 |
C1—C2—C3 | 124.4 (3) | C14—C13—C12 | 124.7 (3) |
C1—C2—Ir1 | 69.42 (18) | C14—C13—Ir1 | 72.71 (18) |
C3—C2—Ir1 | 115.3 (2) | C12—C13—Ir1 | 112.3 (2) |
C1—C2—H2A | 113.5 | C14—C13—H13A | 113.4 |
C3—C2—H2A | 113.5 | C12—C13—H13A | 113.4 |
Ir1—C2—H2A | 113.5 | Ir1—C13—H13A | 113.4 |
C2—C3—C4 | 113.0 (3) | C13—C14—C15 | 125.1 (3) |
C2—C3—H3A | 109.0 | C13—C14—Ir1 | 71.35 (18) |
C4—C3—H3A | 109.0 | C15—C14—Ir1 | 111.3 (2) |
C2—C3—H3B | 109.0 | C13—C14—H14A | 113.8 |
C4—C3—H3B | 109.0 | C15—C14—H14A | 113.8 |
H3A—C3—H3B | 107.8 | Ir1—C14—H14A | 113.8 |
C5—C4—C3 | 112.0 (3) | C14—C15—C16 | 112.6 (3) |
C5—C4—H4A | 109.2 | C14—C15—H15A | 109.1 |
C3—C4—H4A | 109.2 | C16—C15—H15A | 109.1 |
C5—C4—H4B | 109.2 | C14—C15—H15B | 109.1 |
C3—C4—H4B | 109.2 | C16—C15—H15B | 109.1 |
H4A—C4—H4B | 107.9 | H15A—C15—H15B | 107.8 |
C6—C5—C4 | 124.9 (3) | C9—C16—C15 | 112.0 (3) |
C6—C5—Ir1 | 71.96 (18) | C9—C16—H16A | 109.2 |
C4—C5—Ir1 | 110.8 (2) | C15—C16—H16A | 109.2 |
C6—C5—H5A | 113.9 | C9—C16—H16B | 109.2 |
C4—C5—H5A | 113.9 | C15—C16—H16B | 109.2 |
Ir1—C5—H5A | 113.9 | H16A—C16—H16B | 107.9 |
C8—C1—C2—C3 | −2.0 (5) | C16—C9—C10—C11 | −4.0 (5) |
Ir1—C1—C2—C3 | −107.2 (3) | Ir1—C9—C10—C11 | 104.9 (3) |
C8—C1—C2—Ir1 | 105.2 (3) | C16—C9—C10—Ir1 | −108.9 (3) |
C1—C2—C3—C4 | 93.2 (4) | C9—C10—C11—C12 | −49.6 (4) |
Ir1—C2—C3—C4 | 11.7 (4) | Ir1—C10—C11—C12 | 32.3 (3) |
C2—C3—C4—C5 | −31.5 (4) | C10—C11—C12—C13 | −24.8 (4) |
C3—C4—C5—C6 | −46.1 (4) | C11—C12—C13—C14 | 89.4 (4) |
C3—C4—C5—Ir1 | 35.8 (3) | C11—C12—C13—Ir1 | 5.6 (3) |
C4—C5—C6—C7 | −2.8 (5) | C12—C13—C14—C15 | −2.1 (5) |
Ir1—C5—C6—C7 | −106.0 (3) | Ir1—C13—C14—C15 | 103.4 (3) |
C4—C5—C6—Ir1 | 103.2 (3) | C12—C13—C14—Ir1 | −105.5 (3) |
C5—C6—C7—C8 | 95.7 (4) | C13—C14—C15—C16 | −45.8 (4) |
Ir1—C6—C7—C8 | 12.1 (3) | Ir1—C14—C15—C16 | 35.9 (3) |
C2—C1—C8—C7 | −44.6 (4) | C10—C9—C16—C15 | 97.1 (4) |
Ir1—C1—C8—C7 | 38.5 (3) | Ir1—C9—C16—C15 | 14.8 (4) |
C6—C7—C8—C1 | −32.5 (4) | C14—C15—C16—C9 | −33.3 (4) |
Feature | IrCl(cod)2 | COIRSNa | DIVPABb | DIVNUTc | DIVPIJd | PUYCOBe |
M—Xf | 2.5573 (8) | 2.642 (2) | 2.7090 (4) | 2.6606 (4) | 2.5850 (9) | 2.3883 (15) |
M—[A] | 2.047 (4) | 2.068 (31) | 2.062 (4) | 2.067 (4) | 2.101 (5) | 2.048 (8) |
M—[B] | 2.138 (4) | 2.135 (26) | 2.114 (4) | 2.089 (4) | 2.119 (5) | 2.057 (8) |
M—[C] | 2.069 (4) | 2.053 (34) | 2.069 (4) | 2.076 (4) | 2.104 (5) | 2.118 (8) |
M—[D] | 2.141 (4) | 2.134 (24) | 2.126 (4) | 2.089 (4) | 2.109 (5) | 2.170 (8) |
C═C[A] | 1.437 (5) | 1.320 (40) | 1.425 (5) | 1.408 (6) | 1.415 (8) | 1.395 (9) |
C═C[B] | 1.389 (4) | 1.450 (44) | 1.416 (5) | 1.415 (7) | 1.389 (7) | 1.372 (12) |
C═C[C] | 1.418 (5) | 1.361 (44) | 1.411 (5) | 1.400 (7) | 1.394 (7) | 1.393 (8) |
C═C[D] | 1.389 (4) | 1.375 (41) | 1.407 (5) | 1.423 (7) | 1.404 (8) | 1.386 (9) |
τ5g | 0.52 | 0.53 | 0.55 | 0.10 | 0.06 | 0.76 |
Notes: (a) Ir(SnCl3)(cod)2 (Porta et al., 1967); (b) Ir(SnMe3)(cod)2 (Malosh et al., 2013); (c) Ir(SnMe3)(nbd)2 (Malosh et al., 2013); (d) Ir(SnCl3)(nbd)2 (Malosh et al., 2013); (e) [IrCl(cod)(CC*)]+ (Marcén et al., 2002); (f) X = Sn or Cl; (g) Addison et al. (1984). |
Acknowledgements
The authors acknowledge support by the NSF under the CCI Center for Enabling New Technologies through Catalysis (CENTC), CHE-1205189. AKFR thanks the NSF CENTC REU program for support.
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