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In the title compound, [Mo{(C2F3)PPh2}(CO)5], the Mo atom occupies the center of a slightly distorted octahedral environment, bound to five carbonyl groups and one phosphine ligand, so that the local symmetry of the Mo(CO)4P portion of the mol­ecule is approximately C4v. The P atom sits in a distorted-tetrahedral environment; the C—P—Mo angles are much larger than the C—P—C angles. The C2F3 group is rotationally disordered by ∼180°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803026333/bt6384sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803026333/bt6384Isup2.hkl
Contains datablock I

CCDC reference: 227778

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.006 Å
  • R factor = 0.034
  • wR factor = 0.077
  • Data-to-parameter ratio = 11.9

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT242_ALERT_2_C Check Low U(eq) as Compared to Neighbors .... C19A PLAT301_ALERT_3_C Main Residue Disorder ......................... 12.00 Perc. PLAT764_ALERT_4_C Overcomplete CIF Bond list Detected (Rep/Expd) . 1.21 Ratio
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: XSCANS (Bruker, 1996); cell refinement: XSCANS (Bruker, 1996); data reduction: XSCANS (Bruker, 1996); program(s) used to solve structure: SHELXS90 (Sheldrick, 1990a); program(s) used to refine structure: SHELXL93 (Sheldrick, 1993); molecular graphics: SHELXTL/PC (Sheldrick, 1990b); software used to prepare material for publication: SHELXTL/PC (Sheldrick, 1990b) and SHELXL93 (Sheldrick, 1993).

Pentacarbonyl[diphenyl(perfluorovinyl)phosphine]molybdenum(0) top
Crystal data top
[Mo(C14H10F3P)(CO)5]F(000) = 1984
Mr = 502.18Dx = 1.647 Mg m3
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 100 reflections
a = 10.2463 (4) Åθ = 7.7–16.7°
b = 16.1386 (9) ŵ = 0.78 mm1
c = 24.5021 (13) ÅT = 293 K
V = 4051.7 (3) Å3Parallelepiped, light blue
Z = 80.58 × 0.55 × 0.27 mm
Data collection top
Siemens Bruker P4
diffractometer
2675 reflections with I > 2σ(I)
Radiation source: normal-focus sealed tubeRint = 0.030
Graphite monochromatorθmax = 25.0°, θmin = 2.5°
θ/2θ scansh = 121
Absorption correction: integration
(XSHELL; Bruker, 1999)
k = 191
Tmin = 0.684, Tmax = 0.806l = 129
4476 measured reflections3 standard reflections every 100 reflections
3555 independent reflections intensity decay: 1.8%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.034Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.077H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.042P)2 + 0.3244P]
where P = (Fo2 + 2Fc2)/3
3547 reflections(Δ/σ)max < 0.001
299 parametersΔρmax = 0.22 e Å3
0 restraintsΔρmin = 0.28 e Å3
Special details top

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 on F2 for ALL reflections except for 8 with very negative F2 or flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating R factor obs 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Mo10.23006 (3)0.35087 (2)0.460350 (11)0.04649 (12)
P10.27613 (8)0.40695 (5)0.36646 (3)0.0467 (2)
O10.3249 (4)0.1728 (2)0.42318 (14)0.1017 (11)
O20.1561 (3)0.5296 (2)0.50596 (12)0.0909 (9)
O30.5224 (3)0.3853 (2)0.49815 (13)0.0982 (10)
O40.0624 (3)0.3093 (2)0.42760 (12)0.0871 (8)
O50.1632 (3)0.2806 (2)0.57681 (11)0.0887 (9)
C10.2897 (4)0.2361 (2)0.4358 (2)0.0655 (9)
C20.1805 (4)0.4668 (2)0.48843 (14)0.0599 (9)
C30.4188 (4)0.3744 (2)0.48401 (14)0.0624 (9)
C40.0416 (4)0.3253 (2)0.43890 (14)0.0573 (9)
C50.1896 (4)0.3056 (2)0.5343 (2)0.0626 (9)
C60.2728 (3)0.3347 (2)0.30866 (13)0.0542 (8)
C70.1835 (4)0.2710 (3)0.3094 (2)0.0729 (11)
H7A0.13210.26290.34180.080*
C80.1664 (5)0.2201 (3)0.2648 (2)0.0907 (14)
H8A0.10320.17620.26570.080*
C90.2390 (5)0.2302 (4)0.2201 (2)0.100 (2)
H9A0.22730.19390.18940.080*
C100.3300 (5)0.2934 (4)0.2180 (2)0.101 (2)
H10A0.38030.30000.18530.080*
C110.3476 (5)0.3449 (3)0.2623 (2)0.0833 (12)
H11A0.41140.38840.26060.080*
C120.4330 (3)0.4592 (2)0.36217 (13)0.0514 (8)
C130.5455 (4)0.4124 (3)0.3615 (2)0.0745 (11)
H13A0.53980.35330.35820.080*
C140.6669 (4)0.4505 (3)0.3656 (2)0.0849 (13)
H14A0.74500.41770.36630.080*
C150.6750 (5)0.5344 (3)0.3698 (2)0.0823 (12)
H15A0.75850.56140.37070.080*
C160.5648 (5)0.5806 (3)0.3705 (2)0.0850 (13)
H16A0.57060.63970.37450.080*
C170.4443 (4)0.5439 (2)0.3673 (2)0.0657 (10)
H17A0.36760.57800.36780.080*
C180.1654 (5)0.4847 (3)0.3398 (3)0.0839 (15)
C19A0.0698 (8)0.5221 (5)0.3490 (4)0.062 (4)0.53 (2)
F1A0.2187 (15)0.5147 (9)0.2849 (4)0.083 (2)0.53 (2)
F2A0.0044 (9)0.5763 (7)0.3220 (5)0.101 (3)0.53 (2)
F3A0.0114 (11)0.5077 (8)0.3952 (5)0.079 (2)0.53 (2)
C19B0.1381 (15)0.5208 (8)0.3063 (7)0.095 (6)0.47 (2)
F1B0.0424 (15)0.4886 (11)0.3827 (7)0.111 (4)0.47 (2)
F2B0.0394 (17)0.5750 (8)0.2929 (8)0.131 (4)0.47 (2)
F3B0.232 (2)0.5232 (11)0.2663 (5)0.099 (3)0.47 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Mo10.0487 (2)0.0475 (2)0.0433 (2)0.00176 (12)0.00053 (12)0.00180 (12)
P10.0500 (5)0.0443 (5)0.0458 (5)0.0052 (4)0.0019 (4)0.0011 (4)
O10.131 (3)0.054 (2)0.121 (3)0.022 (2)0.006 (2)0.011 (2)
O20.114 (2)0.069 (2)0.090 (2)0.017 (2)0.004 (2)0.022 (2)
O30.060 (2)0.150 (3)0.084 (2)0.010 (2)0.016 (2)0.013 (2)
O40.058 (2)0.104 (2)0.099 (2)0.019 (2)0.007 (2)0.010 (2)
O50.100 (2)0.108 (2)0.058 (2)0.014 (2)0.005 (2)0.017 (2)
C10.077 (2)0.057 (2)0.062 (2)0.001 (2)0.008 (2)0.002 (2)
C20.063 (2)0.062 (2)0.055 (2)0.001 (2)0.002 (2)0.001 (2)
C30.064 (2)0.072 (2)0.051 (2)0.001 (2)0.002 (2)0.003 (2)
C40.061 (2)0.056 (2)0.055 (2)0.001 (2)0.001 (2)0.003 (2)
C50.062 (2)0.069 (2)0.057 (2)0.006 (2)0.002 (2)0.000 (2)
C60.062 (2)0.056 (2)0.045 (2)0.012 (2)0.004 (2)0.0029 (15)
C70.087 (3)0.078 (3)0.054 (2)0.010 (2)0.001 (2)0.014 (2)
C80.115 (4)0.081 (3)0.075 (3)0.011 (3)0.011 (3)0.028 (2)
C90.127 (4)0.103 (4)0.069 (3)0.030 (3)0.015 (3)0.036 (3)
C100.118 (4)0.127 (4)0.059 (3)0.019 (4)0.024 (3)0.026 (3)
C110.089 (3)0.091 (3)0.069 (3)0.002 (2)0.016 (2)0.011 (2)
C120.057 (2)0.050 (2)0.047 (2)0.001 (2)0.0009 (15)0.008 (2)
C130.059 (2)0.065 (2)0.099 (3)0.004 (2)0.002 (2)0.005 (2)
C140.055 (2)0.094 (4)0.105 (3)0.005 (2)0.007 (2)0.000 (3)
C150.070 (3)0.098 (4)0.079 (3)0.026 (3)0.004 (2)0.001 (3)
C160.092 (3)0.062 (3)0.100 (3)0.020 (2)0.010 (3)0.003 (2)
C170.064 (2)0.058 (2)0.075 (2)0.004 (2)0.004 (2)0.002 (2)
C180.088 (4)0.065 (3)0.099 (4)0.022 (3)0.042 (3)0.007 (3)
C19A0.050 (5)0.072 (6)0.065 (7)0.009 (4)0.005 (5)0.011 (5)
F1A0.108 (5)0.099 (5)0.041 (5)0.029 (4)0.022 (5)0.042 (5)
F2A0.087 (4)0.111 (4)0.103 (6)0.042 (3)0.002 (4)0.045 (5)
F3A0.068 (5)0.090 (6)0.079 (5)0.027 (4)0.011 (4)0.012 (4)
C19B0.107 (11)0.090 (9)0.089 (12)0.011 (8)0.008 (10)0.007 (8)
F1B0.099 (8)0.112 (8)0.123 (10)0.058 (5)0.039 (6)0.034 (7)
F2B0.137 (9)0.114 (6)0.144 (10)0.042 (6)0.051 (8)0.060 (8)
F3B0.142 (7)0.104 (6)0.049 (7)0.023 (5)0.022 (7)0.037 (6)
Geometric parameters (Å, º) top
Mo1—P12.5168 (9)C12—C171.378 (5)
Mo1—C12.042 (4)C13—C141.391 (6)
Mo1—C22.057 (4)C13—H13A0.96
Mo1—C32.055 (4)C14—C151.360 (6)
Mo1—C42.044 (4)C14—H14A0.96
Mo1—C51.996 (4)C15—C161.354 (6)
P1—C61.834 (3)C15—H15A0.96
P1—C121.818 (3)C16—C171.372 (6)
P1—C181.814 (5)C16—H16A0.96
O1—C11.126 (4)C17—H17A0.96
O2—C21.130 (4)C18—C19B1.043 (13)
O3—C31.130 (4)C18—C19A1.173 (9)
O4—C41.131 (4)C18—F1A1.529 (10)
O5—C51.150 (4)C18—F1B1.643 (15)
C6—C71.377 (5)C19A—F1B1.03 (2)
C6—C111.379 (5)C19A—C19B1.26 (2)
C7—C81.380 (5)C19A—F2A1.285 (14)
C7—H7A0.96C19A—F3A1.30 (2)
C8—C91.334 (7)C19A—F2B1.65 (2)
C8—H8A0.96F1A—C19B0.98 (2)
C9—C101.383 (7)F2A—F2B0.798 (15)
C9—H9A0.96F2A—C19B1.68 (2)
C10—C111.379 (6)F3A—F1B0.537 (14)
C10—H10A0.96C19B—F3B1.37 (2)
C11—H11A0.96C19B—F2B1.38 (2)
C12—C131.378 (5)
P1—Mo1—C190.02 (11)C16—C15—C14119.9 (4)
P1—Mo1—C291.43 (10)C16—C15—H15A119.5
P1—Mo1—C390.86 (10)C14—C15—H15A120.6
P1—Mo1—C490.85 (10)C15—C16—C17120.8 (4)
P1—Mo1—C5178.72 (11)C15—C16—H16A119.8
C1—Mo1—C2176.24 (14)C17—C16—H16A119.4
C1—Mo1—C388.23 (15)C16—C17—C12120.6 (4)
C1—Mo1—C491.34 (14)C16—C17—H17A119.3
C1—Mo1—C589.9 (2)C12—C17—H17A120.1
C2—Mo1—C388.27 (15)C19B—C18—C19A69.0 (10)
C2—Mo1—C492.11 (14)C19A—C18—F1A107.8 (9)
C2—Mo1—C588.73 (14)C19B—C18—F1B106.0 (13)
C3—Mo1—C4178.24 (14)F1A—C18—F1B145.6 (9)
C3—Mo1—C590.41 (15)C19B—C18—P1146.8 (12)
C4—Mo1—C587.88 (15)C19A—C18—P1144.0 (8)
Mo1—P1—C6118.28 (11)F1A—C18—P1108.2 (6)
Mo1—P1—C12112.66 (10)F1B—C18—P1106.0 (7)
Mo1—P1—C18117.4 (2)F1B—C19A—C1896.5 (11)
C6—P1—C12105.4 (2)F1B—C19A—C19B144.3 (13)
C6—P1—C1898.6 (2)C18—C19A—C19B50.7 (7)
C12—P1—C18102.2 (2)F1B—C19A—F2A129.1 (12)
O1—C1—Mo1178.3 (3)C18—C19A—F2A133.3 (11)
O2—C2—Mo1177.0 (3)C19B—C19A—F2A82.7 (11)
O3—C3—Mo1177.8 (4)C18—C19A—F3A117.4 (9)
O4—C4—Mo1178.4 (3)C19B—C19A—F3A167.3 (11)
O5—C5—Mo1178.3 (3)F2A—C19A—F3A109.3 (9)
C7—C6—C11118.0 (3)F1B—C19A—F2B153.2 (13)
C7—C6—P1118.4 (3)C18—C19A—F2B105.2 (11)
C11—C6—P1123.3 (3)C19B—C19A—F2B54.6 (12)
C6—C7—C8121.2 (4)F3A—C19A—F2B137.0 (11)
C6—C7—H7A118.5F2B—F2A—C19A102.0 (15)
C8—C7—H7A120.2F2B—F2A—C19B54.3 (13)
C9—C8—C7120.5 (5)C19A—F2A—C19B48.0 (7)
C9—C8—H8A119.1F1A—C19B—C1897.9 (16)
C7—C8—H8A120.4F1A—C19B—C19A155.8 (17)
C8—C9—C10119.7 (4)C18—C19B—C19A60.4 (10)
C8—C9—H9A119.9C18—C19B—F3B112.9 (14)
C10—C9—H9A120.4C19A—C19B—F3B169.0 (15)
C11—C10—C9120.3 (4)F1A—C19B—F2B123.6 (16)
C11—C10—H10A121.4C18—C19B—F2B137.6 (18)
C9—C10—H10A118.3C19A—C19B—F2B77.3 (14)
C10—C11—C6120.2 (4)F3B—C19B—F2B109.0 (15)
C10—C11—H11A119.7F1A—C19B—F2A149.3 (14)
C6—C11—H11A120.1C18—C19B—F2A109.7 (14)
C13—C12—C17118.4 (3)C19A—C19B—F2A49.3 (9)
C13—C12—P1119.1 (3)F3B—C19B—F2A135.9 (13)
C17—C12—P1121.9 (3)F3A—F1B—C19A109 (4)
C12—C13—C14120.3 (4)F3A—F1B—C18147 (4)
C12—C13—H13A119.7C19A—F1B—C1845.2 (6)
C14—C13—H13A120.0F2A—F2B—C19B97.6 (15)
C15—C14—C13120.0 (4)F2A—F2B—C19A49.7 (11)
C15—C14—H14A119.8C19B—F2B—C19A48.2 (8)
C13—C14—H14A120.2
 

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