Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807028012/bi2192sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807028012/bi2192Isup2.hkl |
CCDC reference: 654747
An aqueous solution of HI (57%; 0.1337 g, 0.596 mmol) was added to a solution of cyclooctatetraenedimethylplatinum(II) (0.2120 g, 0.644 mmol) in CH2Cl2 (20 ml) and MeOH (10 ml), and stirred for 10 h at room temperature. The solvent was removed under vacuum, the residue was washed with pentane, dissolved in ether, and filtered through a plug of Al2O3 (1 cm × 2 cm). Evaporation of the solvent gave a yellow powder (0.0171 g). Crystals suitable for X-ray analysis were obtained by slow evaporation from a CH2Cl2 solution.
H atoms were positioned geometrically and allowed to ride on their respective carrier atoms, with C—H = 0.98, 0.93 or 0.96 Å and with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C).
In the title complex, [PtI(CH3)(C8H8)], the central PtII ion lies in an essentially square-planar environment defined by the I and methyl C atoms and by the two midpoints (M1, M2) of the π-coordinated double bonds of the 1,3,5,7-cyclooctatetraene (cot) ligand (M1 and M2 denote the midpoints of the olefinic bonds C1—C2 and C5—C6, respectively). The Pt, I, C9 atoms and the midpoints lie in a coordination plane with the largest deviation of 0.024 Å (M2) from the least-squares plane, and with bond angles in the range 85.9–94.5°.
Owing to the different trans influence of the I atom and methyl group, the Pt—C bondstrans to C9 are on average 0.142 Å longer than those trans to I (mean lengths: Pt—C1/C2 = 2.280 Å, Pt—C5/C6 = 2.138 Å). The distances between the Pt atom and the midpoints are 2.174 Å (M1) and 2.019 Å (M2). The cot ligand coordinates symmetrically to the Pt atom in the "tub" conformation, and displays some increase in the coordinated double-bond distances (1.376 (12) Å and 1.401 (13) Å) compared to the non-coordinated double bonds (1.325 (13) Å and 1.289 (15) Å). The four coordinating C atoms (C1, C2, C5 and C6) and the four non-coordinating C atoms (C3, C4, C7 and C8) lie on respective planes, with the torsion angles C1—C2—C5—C6 = 0.8 (7)° and C3—C4—C7—C8 = -1.6 (8)°. The Pt atom is displaced by 1.532 (5) Å from the plane C1/C2/C5/C6, and by 2.501 (5) Å from the plane C3/C4/C7/C8. The dihedral angle between these least-squares planes is 0.4 (7)°. In the complex, the cot ring angles lie in the range 121.2 (8)–123.7 (8)°.
For a related structure, see: Song et al. (2006).
Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997) and PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97.
Fig. 1. The structure of the title compound, with displacement ellipsoids drawn at the 30% probability level for non-H atoms. | |
Fig. 2. View of the unit-cell contents of the title compound. |
[Pt(CH3)I(C8H8)] | F(000) = 784 |
Mr = 441.17 | Dx = 2.941 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 3200 reflections |
a = 8.447 (2) Å | θ = 2.7–26.4° |
b = 10.181 (2) Å | µ = 17.12 mm−1 |
c = 13.504 (2) Å | T = 293 K |
β = 120.901 (3)° | Plate, yellow |
V = 996.5 (3) Å3 | 0.18 × 0.17 × 0.10 mm |
Z = 4 |
Bruker SMART 1000 CCD diffractometer | 2034 independent reflections |
Radiation source: fine-focus sealed tube | 1824 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.031 |
φ and ω scans | θmax = 26.4°, θmin = 2.7° |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | h = −5→10 |
Tmin = 0.063, Tmax = 0.181 | k = −12→12 |
5241 measured reflections | l = −16→14 |
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) = 0.095 | H-atom parameters constrained |
S = 1.04 | w = 1/[σ2(Fo2) + (0.0652P)2 + 0.318P] where P = (Fo2 + 2Fc2)/3 |
2034 reflections | (Δ/σ)max < 0.001 |
101 parameters | Δρmax = 2.04 e Å−3 |
0 restraints | Δρmin = −1.65 e Å−3 |
[Pt(CH3)I(C8H8)] | V = 996.5 (3) Å3 |
Mr = 441.17 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 8.447 (2) Å | µ = 17.12 mm−1 |
b = 10.181 (2) Å | T = 293 K |
c = 13.504 (2) Å | 0.18 × 0.17 × 0.10 mm |
β = 120.901 (3)° |
Bruker SMART 1000 CCD diffractometer | 2034 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | 1824 reflections with I > 2σ(I) |
Tmin = 0.063, Tmax = 0.181 | Rint = 0.031 |
5241 measured reflections |
R[F2 > 2σ(F2)] = 0.035 | 0 restraints |
wR(F2) = 0.095 | H-atom parameters constrained |
S = 1.04 | Δρmax = 2.04 e Å−3 |
2034 reflections | Δρmin = −1.65 e Å−3 |
101 parameters |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
x | y | z | Uiso*/Ueq | ||
Pt | −0.07706 (4) | 0.19134 (3) | 0.33127 (2) | 0.03353 (14) | |
I | −0.25885 (8) | 0.36453 (6) | 0.37576 (6) | 0.0554 (2) | |
C1 | 0.1744 (12) | 0.1904 (9) | 0.5146 (7) | 0.048 (2) | |
H1 | 0.1547 | 0.2215 | 0.5761 | 0.058* | |
C2 | 0.2011 (11) | 0.2851 (9) | 0.4519 (8) | 0.0438 (19) | |
H2 | 0.1965 | 0.3760 | 0.4743 | 0.053* | |
C3 | 0.3096 (11) | 0.2642 (9) | 0.3965 (7) | 0.0456 (19) | |
H3 | 0.4196 | 0.3097 | 0.4233 | 0.055* | |
C4 | 0.2537 (12) | 0.1815 (9) | 0.3090 (8) | 0.050 (2) | |
H4 | 0.3263 | 0.1694 | 0.2763 | 0.060* | |
C5 | 0.0784 (12) | 0.1079 (9) | 0.2621 (7) | 0.048 (2) | |
H5 | 0.0101 | 0.0950 | 0.1783 | 0.057* | |
C6 | 0.0489 (13) | 0.0121 (8) | 0.3254 (8) | 0.052 (2) | |
H6 | −0.0371 | −0.0580 | 0.2793 | 0.063* | |
C7 | 0.1911 (14) | −0.0256 (10) | 0.4420 (10) | 0.061 (2) | |
H7 | 0.2403 | −0.1099 | 0.4550 | 0.073* | |
C8 | 0.2505 (14) | 0.0547 (11) | 0.5277 (9) | 0.066 (3) | |
H8 | 0.3438 | 0.0272 | 0.6002 | 0.079* | |
C9 | −0.3222 (14) | 0.1393 (12) | 0.1861 (8) | 0.064 (3) | |
H9A | −0.3010 | 0.0683 | 0.1476 | 0.096* | |
H9B | −0.3711 | 0.2133 | 0.1350 | 0.096* | |
H9C | −0.4088 | 0.1122 | 0.2080 | 0.096* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Pt | 0.0312 (2) | 0.0354 (2) | 0.0346 (2) | −0.00195 (10) | 0.01736 (15) | −0.00058 (11) |
I | 0.0558 (4) | 0.0487 (4) | 0.0810 (4) | 0.0069 (3) | 0.0489 (3) | 0.0041 (3) |
C1 | 0.036 (4) | 0.074 (7) | 0.029 (4) | −0.008 (4) | 0.013 (3) | −0.005 (4) |
C2 | 0.037 (4) | 0.051 (5) | 0.045 (4) | −0.009 (3) | 0.022 (4) | −0.015 (4) |
C3 | 0.027 (4) | 0.050 (5) | 0.052 (5) | −0.003 (4) | 0.015 (3) | 0.010 (4) |
C4 | 0.045 (5) | 0.062 (6) | 0.057 (5) | 0.014 (4) | 0.036 (4) | 0.016 (4) |
C5 | 0.052 (5) | 0.052 (5) | 0.048 (4) | 0.004 (4) | 0.032 (4) | −0.007 (4) |
C6 | 0.063 (6) | 0.028 (4) | 0.067 (6) | −0.003 (4) | 0.034 (5) | −0.007 (4) |
C7 | 0.064 (6) | 0.041 (5) | 0.082 (7) | 0.012 (4) | 0.041 (5) | 0.020 (5) |
C8 | 0.053 (6) | 0.076 (7) | 0.062 (6) | 0.013 (5) | 0.025 (5) | 0.041 (6) |
C9 | 0.048 (5) | 0.081 (7) | 0.046 (5) | −0.014 (5) | 0.012 (4) | −0.009 (5) |
Pt—C9 | 2.060 (9) | C4—C5 | 1.481 (13) |
Pt—C6 | 2.135 (8) | C4—H4 | 0.930 |
Pt—C5 | 2.140 (8) | C5—C6 | 1.401 (13) |
Pt—C2 | 2.270 (8) | C5—H5 | 0.980 |
Pt—C1 | 2.289 (8) | C6—C7 | 1.459 (14) |
Pt—I | 2.6029 (7) | C6—H6 | 0.980 |
C1—C2 | 1.376 (12) | C7—C8 | 1.289 (15) |
C1—C8 | 1.495 (14) | C7—H7 | 0.930 |
C1—H1 | 0.980 | C8—H8 | 0.930 |
C2—C3 | 1.466 (12) | C9—H9A | 0.960 |
C2—H2 | 0.980 | C9—H9B | 0.960 |
C3—C4 | 1.325 (13) | C9—H9C | 0.960 |
C3—H3 | 0.930 | ||
C9—Pt—C6 | 91.2 (4) | C2—C3—H3 | 119.4 |
C9—Pt—C5 | 91.4 (4) | C3—C4—C5 | 121.6 (8) |
C6—Pt—C5 | 38.3 (3) | C3—C4—H4 | 119.2 |
C9—Pt—C2 | 162.8 (4) | C5—C4—H4 | 119.2 |
C6—Pt—C2 | 92.0 (3) | C6—C5—C4 | 122.9 (8) |
C5—Pt—C2 | 80.8 (3) | C6—C5—Pt | 70.7 (5) |
C9—Pt—C1 | 161.7 (4) | C4—C5—Pt | 108.4 (6) |
C6—Pt—C1 | 80.4 (3) | C6—C5—H5 | 115.4 |
C5—Pt—C1 | 91.9 (3) | C4—C5—H5 | 115.4 |
C2—Pt—C1 | 35.1 (3) | Pt—C5—H5 | 115.4 |
C9—Pt—I | 88.3 (3) | C5—C6—C7 | 122.4 (8) |
C6—Pt—I | 162.2 (3) | C5—C6—Pt | 71.1 (5) |
C5—Pt—I | 159.5 (2) | C7—C6—Pt | 109.5 (7) |
C2—Pt—I | 93.7 (2) | C5—C6—H6 | 115.2 |
C1—Pt—I | 94.8 (2) | C7—C6—H6 | 115.2 |
C2—C1—C8 | 121.6 (8) | Pt—C6—H6 | 115.2 |
C2—C1—Pt | 71.7 (5) | C8—C7—C6 | 121.8 (9) |
C8—C1—Pt | 103.6 (6) | C8—C7—H7 | 119.1 |
C2—C1—H1 | 116.6 | C6—C7—H7 | 119.1 |
C8—C1—H1 | 116.6 | C7—C8—C1 | 122.3 (9) |
Pt—C1—H1 | 116.6 | C7—C8—H8 | 118.8 |
C1—C2—C3 | 123.7 (8) | C1—C8—H8 | 118.8 |
C1—C2—Pt | 73.2 (5) | Pt—C9—H9A | 109.5 |
C3—C2—Pt | 105.1 (5) | Pt—C9—H9B | 109.5 |
C1—C2—H2 | 115.3 | H9A—C9—H9B | 109.5 |
C3—C2—H2 | 115.3 | Pt—C9—H9C | 109.5 |
Pt—C2—H2 | 115.3 | H9A—C9—H9C | 109.5 |
C4—C3—C2 | 121.2 (8) | H9B—C9—H9C | 109.5 |
C4—C3—H3 | 119.4 | ||
C9—Pt—C1—C2 | 171.3 (12) | I—Pt—C5—C6 | −179.1 (5) |
C6—Pt—C1—C2 | 107.5 (6) | C9—Pt—C5—C4 | 150.5 (7) |
C5—Pt—C1—C2 | 70.9 (6) | C6—Pt—C5—C4 | −119.3 (8) |
I—Pt—C1—C2 | −89.7 (5) | C2—Pt—C5—C4 | −14.1 (6) |
C9—Pt—C1—C8 | 52.1 (15) | C1—Pt—C5—C4 | −47.6 (6) |
C6—Pt—C1—C8 | −11.7 (6) | I—Pt—C5—C4 | 61.6 (10) |
C5—Pt—C1—C8 | −48.3 (6) | C4—C5—C6—C7 | −1.8 (14) |
C2—Pt—C1—C8 | −119.2 (9) | Pt—C5—C6—C7 | −101.6 (9) |
I—Pt—C1—C8 | 151.1 (6) | C4—C5—C6—Pt | 99.8 (8) |
C8—C1—C2—C3 | −2.2 (13) | C9—Pt—C6—C5 | 90.7 (6) |
Pt—C1—C2—C3 | −97.2 (8) | C2—Pt—C6—C5 | −72.4 (5) |
C8—C1—C2—Pt | 95.0 (8) | C1—Pt—C6—C5 | −105.7 (6) |
C9—Pt—C2—C1 | −170.8 (13) | I—Pt—C6—C5 | 178.9 (6) |
C6—Pt—C2—C1 | −70.2 (6) | C9—Pt—C6—C7 | −150.6 (7) |
C5—Pt—C2—C1 | −106.9 (6) | C5—Pt—C6—C7 | 118.7 (9) |
I—Pt—C2—C1 | 93.0 (5) | C2—Pt—C6—C7 | 46.3 (7) |
C9—Pt—C2—C3 | −49.5 (16) | C1—Pt—C6—C7 | 13.0 (6) |
C6—Pt—C2—C3 | 51.1 (6) | I—Pt—C6—C7 | −62.4 (11) |
C5—Pt—C2—C3 | 14.3 (6) | C5—C6—C7—C8 | 66.5 (14) |
C1—Pt—C2—C3 | 121.2 (9) | Pt—C6—C7—C8 | −13.0 (12) |
I—Pt—C2—C3 | −145.8 (6) | C6—C7—C8—C1 | 1.9 (16) |
C1—C2—C3—C4 | 66.9 (12) | C2—C1—C8—C7 | −67.4 (13) |
Pt—C2—C3—C4 | −12.8 (10) | Pt—C1—C8—C7 | 9.3 (12) |
C2—C3—C4—C5 | 0.9 (13) | C1—C2—C5—C6 | 0.8 (7) |
C3—C4—C5—C6 | −65.9 (12) | C3—C4—C7—C8 | −1.6 (8) |
C3—C4—C5—Pt | 12.6 (10) | C3—C2—C1—C8 | −2.2 (13) |
C9—Pt—C5—C6 | −90.2 (6) | C4—C5—C6—C7 | −1.8 (14) |
C2—Pt—C5—C6 | 105.2 (6) | C2—C3—C4—C5 | 0.9 (13) |
C1—Pt—C5—C6 | 71.8 (5) | C6—C7—C8—C1 | 1.9 (16) |
Experimental details
Crystal data | |
Chemical formula | [Pt(CH3)I(C8H8)] |
Mr | 441.17 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 293 |
a, b, c (Å) | 8.447 (2), 10.181 (2), 13.504 (2) |
β (°) | 120.901 (3) |
V (Å3) | 996.5 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 17.12 |
Crystal size (mm) | 0.18 × 0.17 × 0.10 |
Data collection | |
Diffractometer | Bruker SMART 1000 CCD |
Absorption correction | Multi-scan (SADABS; Bruker, 2000) |
Tmin, Tmax | 0.063, 0.181 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5241, 2034, 1824 |
Rint | 0.031 |
(sin θ/λ)max (Å−1) | 0.625 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.035, 0.095, 1.04 |
No. of reflections | 2034 |
No. of parameters | 101 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 2.04, −1.65 |
Computer programs: SMART (Bruker, 2000), SAINT (Bruker, 2000), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 (Farrugia, 1997) and PLATON (Spek, 2003), SHELXL97.
In the title complex, [PtI(CH3)(C8H8)], the central PtII ion lies in an essentially square-planar environment defined by the I and methyl C atoms and by the two midpoints (M1, M2) of the π-coordinated double bonds of the 1,3,5,7-cyclooctatetraene (cot) ligand (M1 and M2 denote the midpoints of the olefinic bonds C1—C2 and C5—C6, respectively). The Pt, I, C9 atoms and the midpoints lie in a coordination plane with the largest deviation of 0.024 Å (M2) from the least-squares plane, and with bond angles in the range 85.9–94.5°.
Owing to the different trans influence of the I atom and methyl group, the Pt—C bondstrans to C9 are on average 0.142 Å longer than those trans to I (mean lengths: Pt—C1/C2 = 2.280 Å, Pt—C5/C6 = 2.138 Å). The distances between the Pt atom and the midpoints are 2.174 Å (M1) and 2.019 Å (M2). The cot ligand coordinates symmetrically to the Pt atom in the "tub" conformation, and displays some increase in the coordinated double-bond distances (1.376 (12) Å and 1.401 (13) Å) compared to the non-coordinated double bonds (1.325 (13) Å and 1.289 (15) Å). The four coordinating C atoms (C1, C2, C5 and C6) and the four non-coordinating C atoms (C3, C4, C7 and C8) lie on respective planes, with the torsion angles C1—C2—C5—C6 = 0.8 (7)° and C3—C4—C7—C8 = -1.6 (8)°. The Pt atom is displaced by 1.532 (5) Å from the plane C1/C2/C5/C6, and by 2.501 (5) Å from the plane C3/C4/C7/C8. The dihedral angle between these least-squares planes is 0.4 (7)°. In the complex, the cot ring angles lie in the range 121.2 (8)–123.7 (8)°.