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In the title compound, [Cr(C24H20P2S)(CO)5], the key bond lengths are P1-P2 2.2659 (15), P2-S 1.9531 (15), P1-C 1.830, 1.833 (3), P2-C 1.821, 1.822 (3) and P1-Cr 2.3921 (13) Å. The conformation about the P-P bond is defined by the torsion angle S-P2-P1-Cr of -58.60 (7)°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802014125/cv6136sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802014125/cv6136Isup2.hkl
Contains datablock I

CCDC reference: 197447

Key indicators

  • Single-crystal X-ray study
  • T = 178 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.040
  • wR factor = 0.108
  • Data-to-parameter ratio = 13.3

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry

General Notes

ABSTM_02 When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 0.884 Tmax scaled 0.877 Tmin scaled 0.708

Comment top

The title compound, (I), arose during studies (see Experimental) of thioureas substituted with phosphorus-containing groups (Farkens, 1991). It was characterized by this structure determination.

The molecule of (I) is shown in Fig. 1. A search of the Cambridge Structural Database (CSD, Version of April 2002; Allen & Kennard, 1993) revealed no other complexes of any tetra(organyl)diphosphine monosulfide (in the strict sense of a compound containing a P—P bond). The key bond lengths are P1—P2 2.2659 (15), P2—S 1.9531 (15), P1—C 1.830, 1.833 (3) and P2—C 1.821 1.822 (3) Å. These may be compared, although the two systems clearly differ chemically in many respects, with values for uncomplexed tetramethyldiphosphane monosulfide (Gruber et al., 1990): P—P 2.201 (1), P—S 1.970 (1), PIII—C 1.830 and 1.834 (1), and P(S)—C 1.803 and 1.803 (1) Å. The P—P bond in (I) may be regarded as long, and it is reasonable to propose steric effects as the cause. A CSD search revealed 57 structures with (C)2P—P(C)2 single bonds, involving 69 bonds in the range 2.104–2.310 Å (average 2.216 Å).

The P—Cr distance is 2.3921 (13) Å, and the Cr—C bond trans to Cr—P is by far the shortest at 1.865 (4) Å, cf. average 1.903 Å for the other four Cr—C bonds. The conformation about the P—P bond is defined by the torsion angle S—P2—P1—Cr of −58.60 (7)° (in the above-mentioned diphosphine monosulfide, the S atom is trans to the lone pair at the other phosphorus). As expected, the largest angles at phosphorus are those involving the Cr atom at P1 and the S atom at P2.

Two short H···O contacts could reasonably be interpreted as weak hydrogen bonds (Table 2).

Experimental top

The reaction between (norbornadiene)Cr(CO)4 and N,N'-bis(diphenylphosphino)-N,N'-dimethylthiourea in dichloromethane led to a complex mixture of products. The mixture was dissolved in diethyl ether, from which the title compound crystallized in 13% yield (Farkens, 1991). The decomposition of the thiourea to tetraphenyldiphosphine monosulfide has been observed before in our laboratory (Gruber, 1989).

Refinement top

H atoms were included using a riding model with fixed C—H bond lengths of 0.95 Å; Uiso(H) values were fixed at 1.2 times the Ueq of the parent atom.

Computing details top

Data collection: P3 (Nicolet, 1987); cell refinement: P3; data reduction: XDISK (Nicolet, 1987); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP (Siemens, 1994); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The molecule of compound (I) in the crystal. Displacement ellipsoids represent 30% probability levels. H-atom radii are arbitrary.
(Tetraphenyldiphosphinmonosulfide-P)pentacarbonylchromium(0) top
Crystal data top
[Cr(C24H20P2S)(CO)5]Z = 2
Mr = 594.45F(000) = 608
Triclinic, P1Dx = 1.466 Mg m3
a = 9.840 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.089 (5) ÅCell parameters from 50 reflections
c = 14.967 (6) Åθ = 10–11.5°
α = 77.90 (3)°µ = 0.66 mm1
β = 84.43 (3)°T = 178 K
γ = 68.02 (3)°Tablet, yellow
V = 1347.0 (10) Å30.5 × 0.5 × 0.2 mm
Data collection top
Nicolet R3
diffractometer
3476 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.038
Graphite monochromatorθmax = 25.1°, θmin = 3.1°
ω scansh = 1111
Absorption correction: ψ scan
(XEMP; Nicolet, 1987)
k = 1111
Tmin = 0.801, Tmax = 0.991l = 1217
5120 measured reflections3 standard reflections every 147 reflections
4578 independent reflections intensity decay: none
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)] = 0.040Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.108H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0464P)2 + 1.6663P]
where P = (Fo2 + 2Fc2)/3
4578 reflections(Δ/σ)max < 0.001
343 parametersΔρmax = 0.48 e Å3
0 restraintsΔρmin = 0.47 e Å3
Crystal data top
[Cr(C24H20P2S)(CO)5]γ = 68.02 (3)°
Mr = 594.45V = 1347.0 (10) Å3
Triclinic, P1Z = 2
a = 9.840 (3) ÅMo Kα radiation
b = 10.089 (5) ŵ = 0.66 mm1
c = 14.967 (6) ÅT = 178 K
α = 77.90 (3)°0.5 × 0.5 × 0.2 mm
β = 84.43 (3)°
Data collection top
Nicolet R3
diffractometer
3476 reflections with I > 2σ(I)
Absorption correction: ψ scan
(XEMP; Nicolet, 1987)
Rint = 0.038
Tmin = 0.801, Tmax = 0.9913 standard reflections every 147 reflections
5120 measured reflections intensity decay: none
4578 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0400 restraints
wR(F2) = 0.108H-atom parameters constrained
S = 1.03Δρmax = 0.48 e Å3
4578 reflectionsΔρmin = 0.47 e Å3
343 parameters
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 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cr0.12119 (5)0.22328 (5)0.40722 (3)0.02628 (15)
S0.06062 (9)0.57737 (10)0.15723 (6)0.0382 (2)
P10.23659 (8)0.21117 (8)0.25938 (5)0.02230 (19)
P20.25228 (8)0.42161 (8)0.17823 (5)0.02327 (19)
O10.3039 (3)0.0945 (3)0.47601 (17)0.0481 (7)
O20.3385 (3)0.3212 (3)0.48080 (17)0.0508 (7)
O30.0302 (3)0.2233 (3)0.59188 (18)0.0514 (7)
O40.1003 (3)0.1140 (3)0.35052 (18)0.0489 (7)
O50.0987 (3)0.5345 (3)0.3672 (2)0.0626 (8)
C10.4255 (3)0.0849 (3)0.2502 (2)0.0240 (6)
C20.4827 (3)0.0388 (3)0.1683 (2)0.0299 (7)
H20.42170.06910.11680.036*
C30.6278 (4)0.0508 (4)0.1620 (3)0.0378 (8)
H30.66660.08010.10560.045*
C40.7171 (4)0.0983 (4)0.2370 (3)0.0425 (9)
H40.81600.16200.23270.051*
C50.6619 (4)0.0527 (4)0.3175 (2)0.0400 (9)
H50.72350.08370.36880.048*
C60.5170 (3)0.0381 (4)0.3248 (2)0.0321 (7)
H60.47990.06870.38100.038*
C70.1355 (3)0.1573 (3)0.1860 (2)0.0237 (6)
C80.0092 (4)0.2571 (4)0.1432 (2)0.0365 (8)
H80.01710.35760.14350.044*
C90.0793 (4)0.2120 (4)0.0998 (3)0.0450 (9)
H90.16500.28150.06990.054*
C100.0430 (4)0.0660 (4)0.1002 (2)0.0407 (9)
H100.10360.03500.07040.049*
C110.0804 (4)0.0344 (4)0.1435 (2)0.0405 (9)
H110.10460.13500.14420.049*
C120.1698 (3)0.0107 (4)0.1862 (2)0.0322 (7)
H120.25540.05940.21590.039*
C130.3465 (3)0.3827 (3)0.0705 (2)0.0245 (6)
C140.2578 (4)0.3983 (4)0.0014 (2)0.0325 (7)
H140.15430.43100.00700.039*
C150.3201 (4)0.3664 (4)0.0847 (2)0.0397 (8)
H150.25930.37720.13340.048*
C160.4705 (4)0.3189 (4)0.0978 (2)0.0358 (8)
H160.51330.29680.15510.043*
C170.5573 (4)0.3040 (4)0.0273 (2)0.0378 (8)
H170.66070.27150.03620.045*
C180.4972 (3)0.3354 (4)0.0562 (2)0.0324 (7)
H180.55920.32450.10420.039*
C190.3649 (3)0.4636 (3)0.2496 (2)0.0265 (7)
C200.5115 (3)0.3782 (4)0.2695 (2)0.0311 (7)
H200.55860.29170.24550.037*
C210.5876 (4)0.4198 (4)0.3243 (3)0.0435 (9)
H210.68750.36230.33700.052*
C220.5201 (4)0.5442 (4)0.3606 (3)0.0466 (10)
H220.57370.57260.39760.056*
C230.3750 (4)0.6270 (4)0.3433 (2)0.0412 (9)
H230.32800.71190.36890.049*
C240.2971 (4)0.5864 (4)0.2883 (2)0.0336 (8)
H240.19660.64320.27710.040*
C250.2382 (4)0.0257 (4)0.4483 (2)0.0333 (8)
C260.2590 (4)0.2869 (4)0.4496 (2)0.0346 (8)
C270.0275 (4)0.2238 (4)0.5217 (2)0.0365 (8)
C280.0164 (4)0.1567 (4)0.3695 (2)0.0334 (8)
C290.0118 (4)0.4205 (4)0.3756 (2)0.0376 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cr0.0250 (3)0.0285 (3)0.0259 (3)0.0090 (2)0.0015 (2)0.0087 (2)
S0.0323 (5)0.0326 (5)0.0487 (5)0.0077 (4)0.0059 (4)0.0106 (4)
P10.0210 (4)0.0235 (4)0.0235 (4)0.0079 (3)0.0023 (3)0.0061 (3)
P20.0222 (4)0.0219 (4)0.0263 (4)0.0072 (3)0.0029 (3)0.0064 (3)
O10.0527 (16)0.0344 (15)0.0443 (15)0.0035 (13)0.0030 (12)0.0054 (12)
O20.0583 (17)0.076 (2)0.0383 (14)0.0420 (16)0.0004 (12)0.0207 (14)
O30.0471 (16)0.0629 (18)0.0383 (15)0.0131 (14)0.0133 (13)0.0162 (13)
O40.0420 (15)0.0630 (18)0.0549 (17)0.0323 (14)0.0076 (12)0.0182 (14)
O50.0576 (18)0.0338 (16)0.078 (2)0.0006 (14)0.0144 (15)0.0092 (14)
C10.0206 (15)0.0214 (16)0.0314 (17)0.0087 (13)0.0002 (12)0.0059 (13)
C20.0304 (17)0.0277 (17)0.0353 (18)0.0139 (14)0.0006 (14)0.0077 (14)
C30.038 (2)0.0325 (19)0.045 (2)0.0148 (16)0.0101 (16)0.0133 (16)
C40.0242 (17)0.0287 (19)0.065 (3)0.0028 (15)0.0035 (17)0.0037 (18)
C50.0281 (18)0.040 (2)0.042 (2)0.0064 (16)0.0068 (15)0.0037 (17)
C60.0257 (16)0.0367 (19)0.0304 (18)0.0091 (15)0.0002 (13)0.0033 (15)
C70.0258 (15)0.0263 (16)0.0232 (15)0.0137 (13)0.0018 (12)0.0049 (13)
C80.0358 (19)0.0293 (18)0.047 (2)0.0136 (15)0.0133 (16)0.0035 (16)
C90.044 (2)0.049 (2)0.048 (2)0.0264 (19)0.0226 (17)0.0054 (18)
C100.049 (2)0.057 (2)0.0329 (19)0.036 (2)0.0030 (16)0.0122 (17)
C110.047 (2)0.037 (2)0.050 (2)0.0229 (18)0.0062 (17)0.0222 (17)
C120.0280 (17)0.0294 (18)0.0408 (19)0.0107 (14)0.0000 (14)0.0102 (15)
C130.0306 (16)0.0176 (15)0.0275 (16)0.0090 (13)0.0035 (13)0.0071 (12)
C140.0287 (17)0.0345 (19)0.0322 (18)0.0090 (15)0.0038 (14)0.0053 (15)
C150.048 (2)0.044 (2)0.0318 (19)0.0170 (18)0.0074 (16)0.0127 (16)
C160.046 (2)0.0350 (19)0.0299 (18)0.0184 (17)0.0071 (15)0.0095 (15)
C170.0317 (18)0.044 (2)0.043 (2)0.0179 (16)0.0079 (15)0.0153 (17)
C180.0284 (17)0.041 (2)0.0309 (18)0.0162 (15)0.0004 (14)0.0076 (15)
C190.0298 (16)0.0250 (16)0.0279 (17)0.0120 (14)0.0020 (13)0.0078 (13)
C200.0294 (17)0.0322 (18)0.0329 (18)0.0104 (14)0.0046 (14)0.0088 (14)
C210.0330 (19)0.051 (2)0.048 (2)0.0134 (17)0.0117 (16)0.0115 (18)
C220.051 (2)0.061 (3)0.043 (2)0.029 (2)0.0081 (18)0.0207 (19)
C230.049 (2)0.048 (2)0.038 (2)0.0228 (19)0.0023 (17)0.0228 (17)
C240.0311 (17)0.0357 (19)0.0377 (19)0.0140 (15)0.0016 (14)0.0123 (15)
C250.0331 (18)0.041 (2)0.0270 (17)0.0135 (17)0.0063 (14)0.0108 (16)
C260.0401 (19)0.042 (2)0.0236 (17)0.0165 (17)0.0037 (14)0.0099 (15)
C270.0307 (18)0.036 (2)0.040 (2)0.0062 (15)0.0007 (16)0.0128 (16)
C280.0320 (18)0.037 (2)0.0316 (18)0.0138 (16)0.0048 (14)0.0075 (15)
C290.0373 (19)0.032 (2)0.042 (2)0.0111 (17)0.0073 (16)0.0123 (16)
Geometric parameters (Å, º) top
Cr—C271.865 (4)C8—H80.9500
Cr—C251.893 (4)C9—C101.378 (5)
Cr—C281.895 (4)C9—H90.9500
Cr—C261.909 (4)C10—C111.369 (5)
Cr—C291.916 (4)C10—H100.9500
Cr—P12.3921 (13)C11—C121.386 (5)
S—P21.9531 (15)C11—H110.9500
P1—C11.830 (3)C12—H120.9500
P1—C71.833 (3)C13—C181.387 (4)
P1—P22.2659 (15)C13—C141.399 (4)
P2—C131.821 (3)C14—C151.381 (5)
P2—C191.822 (3)C14—H140.9500
O1—C251.146 (4)C15—C161.382 (5)
O2—C261.135 (4)C15—H150.9500
O3—C271.144 (4)C16—C171.371 (5)
O4—C281.144 (4)C16—H160.9500
O5—C291.138 (4)C17—C181.376 (5)
C1—C61.391 (4)C17—H170.9500
C1—C21.394 (4)C18—H180.9500
C2—C31.382 (5)C19—C241.387 (4)
C2—H20.9500C19—C201.399 (4)
C3—C41.383 (5)C20—C211.381 (5)
C3—H30.9500C20—H200.9500
C4—C51.371 (5)C21—C221.380 (5)
C4—H40.9500C21—H210.9500
C5—C61.384 (5)C22—C231.376 (5)
C5—H50.9500C22—H220.9500
C6—H60.9500C23—C241.389 (5)
C7—C81.384 (4)C23—H230.9500
C7—C121.388 (4)C24—H240.9500
C8—C91.384 (5)
C27—Cr—C2588.48 (15)C10—C9—H9120.1
C27—Cr—C2888.55 (15)C8—C9—H9120.1
C25—Cr—C2887.44 (15)C11—C10—C9120.1 (3)
C27—Cr—C2689.65 (15)C11—C10—H10119.9
C25—Cr—C2691.50 (15)C9—C10—H10119.9
C28—Cr—C26177.94 (14)C10—C11—C12120.0 (3)
C27—Cr—C2985.89 (15)C10—C11—H11120.0
C25—Cr—C29173.94 (14)C12—C11—H11120.0
C28—Cr—C2990.19 (15)C11—C12—C7120.6 (3)
C26—Cr—C2990.69 (16)C11—C12—H12119.7
C27—Cr—P1176.55 (11)C7—C12—H12119.7
C25—Cr—P189.77 (10)C18—C13—C14118.7 (3)
C28—Cr—P188.40 (10)C18—C13—P2125.1 (2)
C26—Cr—P193.36 (10)C14—C13—P2116.2 (2)
C29—Cr—P195.75 (11)C15—C14—C13120.2 (3)
C1—P1—C7103.54 (14)C15—C14—H14119.9
C1—P1—P2101.21 (10)C13—C14—H14119.9
C7—P1—P2104.56 (10)C14—C15—C16120.4 (3)
C1—P1—Cr119.02 (11)C14—C15—H15119.8
C7—P1—Cr110.78 (10)C16—C15—H15119.8
P2—P1—Cr116.02 (5)C17—C16—C15119.3 (3)
C13—P2—C19110.90 (14)C17—C16—H16120.3
C13—P2—S111.01 (11)C15—C16—H16120.3
C19—P2—S111.67 (11)C16—C17—C18121.1 (3)
C13—P2—P1107.35 (10)C16—C17—H17119.4
C19—P2—P1103.03 (11)C18—C17—H17119.4
S—P2—P1112.55 (6)C17—C18—C13120.2 (3)
C6—C1—C2118.7 (3)C17—C18—H18119.9
C6—C1—P1119.9 (2)C13—C18—H18119.9
C2—C1—P1121.3 (2)C24—C19—C20118.9 (3)
C3—C2—C1120.1 (3)C24—C19—P2116.7 (2)
C3—C2—H2119.9C20—C19—P2124.4 (2)
C1—C2—H2119.9C21—C20—C19119.9 (3)
C2—C3—C4120.6 (3)C21—C20—H20120.0
C2—C3—H3119.7C19—C20—H20120.0
C4—C3—H3119.7C22—C21—C20120.7 (3)
C5—C4—C3119.6 (3)C22—C21—H21119.7
C5—C4—H4120.2C20—C21—H21119.7
C3—C4—H4120.2C23—C22—C21119.9 (3)
C4—C5—C6120.5 (3)C23—C22—H22120.1
C4—C5—H5119.7C21—C22—H22120.1
C6—C5—H5119.7C22—C23—C24120.0 (3)
C5—C6—C1120.5 (3)C22—C23—H23120.0
C5—C6—H6119.8C24—C23—H23120.0
C1—C6—H6119.8C19—C24—C23120.5 (3)
C8—C7—C12118.5 (3)C19—C24—H24119.7
C8—C7—P1121.0 (2)C23—C24—H24119.7
C12—C7—P1119.4 (2)O1—C25—Cr176.9 (3)
C9—C8—C7120.8 (3)O2—C26—Cr175.3 (3)
C9—C8—H8119.6O3—C27—Cr179.6 (3)
C7—C8—H8119.6O4—C28—Cr177.1 (3)
C10—C9—C8119.9 (3)O5—C29—Cr171.5 (3)
C25—Cr—P1—C129.32 (15)P2—P1—C7—C12145.4 (2)
C28—Cr—P1—C1116.76 (15)Cr—P1—C7—C1288.9 (2)
C26—Cr—P1—C162.17 (16)C12—C7—C8—C91.4 (5)
C29—Cr—P1—C1153.20 (15)P1—C7—C8—C9169.7 (3)
C25—Cr—P1—C790.49 (15)C7—C8—C9—C101.0 (6)
C28—Cr—P1—C73.04 (15)C8—C9—C10—C110.1 (6)
C26—Cr—P1—C7178.02 (15)C9—C10—C11—C120.7 (5)
C29—Cr—P1—C786.99 (15)C10—C11—C12—C70.2 (5)
C25—Cr—P1—P2150.53 (11)C8—C7—C12—C110.8 (5)
C28—Cr—P1—P2122.02 (11)P1—C7—C12—C11169.3 (3)
C26—Cr—P1—P259.04 (12)C19—P2—C13—C1823.4 (3)
C29—Cr—P1—P231.99 (12)S—P2—C13—C18148.1 (3)
C1—P1—P2—C1348.63 (15)P1—P2—C13—C1888.5 (3)
C7—P1—P2—C1358.72 (15)C19—P2—C13—C14158.7 (2)
Cr—P1—P2—C13178.96 (10)S—P2—C13—C1433.9 (3)
C1—P1—P2—C1968.50 (15)P1—P2—C13—C1489.5 (2)
C7—P1—P2—C19175.85 (14)C18—C13—C14—C150.2 (5)
Cr—P1—P2—C1961.83 (11)P2—C13—C14—C15177.8 (3)
C1—P1—P2—S171.07 (11)C13—C14—C15—C160.0 (5)
C7—P1—P2—S63.72 (11)C14—C15—C16—C170.1 (5)
Cr—P1—P2—S58.60 (7)C15—C16—C17—C180.1 (5)
C7—P1—C1—C6146.8 (3)C16—C17—C18—C130.1 (5)
P2—P1—C1—C6105.1 (2)C14—C13—C18—C170.3 (5)
Cr—P1—C1—C623.3 (3)P2—C13—C18—C17177.6 (3)
C7—P1—C1—C236.1 (3)C13—P2—C19—C24132.2 (3)
P2—P1—C1—C272.0 (2)S—P2—C19—C247.9 (3)
Cr—P1—C1—C2159.5 (2)P1—P2—C19—C24113.2 (2)
C6—C1—C2—C30.4 (4)C13—P2—C19—C2049.9 (3)
P1—C1—C2—C3176.8 (2)S—P2—C19—C20174.3 (2)
C1—C2—C3—C41.3 (5)P1—P2—C19—C2064.7 (3)
C2—C3—C4—C51.7 (5)C24—C19—C20—C212.4 (5)
C3—C4—C5—C61.2 (5)P2—C19—C20—C21179.8 (3)
C4—C5—C6—C10.2 (5)C19—C20—C21—C220.8 (5)
C2—C1—C6—C50.2 (5)C20—C21—C22—C230.8 (6)
P1—C1—C6—C5177.3 (3)C21—C22—C23—C240.8 (6)
C1—P1—C7—C8152.0 (3)C20—C19—C24—C232.4 (5)
P2—P1—C7—C846.4 (3)P2—C19—C24—C23179.7 (3)
Cr—P1—C7—C879.3 (3)C22—C23—C24—C190.8 (5)
C1—P1—C7—C1239.8 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C22—H22···O2i0.952.653.581 (4)166
C21—H21···O4ii0.952.573.426 (5)149
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+1, y, z.

Experimental details

Crystal data
Chemical formula[Cr(C24H20P2S)(CO)5]
Mr594.45
Crystal system, space groupTriclinic, P1
Temperature (K)178
a, b, c (Å)9.840 (3), 10.089 (5), 14.967 (6)
α, β, γ (°)77.90 (3), 84.43 (3), 68.02 (3)
V3)1347.0 (10)
Z2
Radiation typeMo Kα
µ (mm1)0.66
Crystal size (mm)0.5 × 0.5 × 0.2
Data collection
DiffractometerNicolet R3
diffractometer
Absorption correctionψ scan
(XEMP; Nicolet, 1987)
Tmin, Tmax0.801, 0.991
No. of measured, independent and
observed [I > 2σ(I)] reflections
5120, 4578, 3476
Rint0.038
(sin θ/λ)max1)0.596
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.040, 0.108, 1.03
No. of reflections4578
No. of parameters343
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.48, 0.47

Computer programs: P3 (Nicolet, 1987), P3, XDISK (Nicolet, 1987), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), XP (Siemens, 1994), SHELXL97.

Selected geometric parameters (Å, º) top
Cr—C271.865 (4)S—P21.9531 (15)
Cr—C251.893 (4)P1—C11.830 (3)
Cr—C281.895 (4)P1—C71.833 (3)
Cr—C261.909 (4)P1—P22.2659 (15)
Cr—C291.916 (4)P2—C131.821 (3)
Cr—P12.3921 (13)P2—C191.822 (3)
C27—Cr—C2588.48 (15)C29—Cr—P195.75 (11)
C27—Cr—C2888.55 (15)C1—P1—C7103.54 (14)
C25—Cr—C2887.44 (15)C1—P1—P2101.21 (10)
C27—Cr—C2689.65 (15)C7—P1—P2104.56 (10)
C25—Cr—C2691.50 (15)C1—P1—Cr119.02 (11)
C28—Cr—C26177.94 (14)C7—P1—Cr110.78 (10)
C27—Cr—C2985.89 (15)P2—P1—Cr116.02 (5)
C25—Cr—C29173.94 (14)C13—P2—C19110.90 (14)
C28—Cr—C2990.19 (15)C13—P2—S111.01 (11)
C26—Cr—C2990.69 (16)C19—P2—S111.67 (11)
C27—Cr—P1176.55 (11)C13—P2—P1107.35 (10)
C25—Cr—P189.77 (10)C19—P2—P1103.03 (11)
C28—Cr—P188.40 (10)S—P2—P1112.55 (6)
C26—Cr—P193.36 (10)
C1—P1—P2—C1348.63 (15)Cr—P1—P2—C1961.83 (11)
C7—P1—P2—C1358.72 (15)C1—P1—P2—S171.07 (11)
Cr—P1—P2—C13178.96 (10)C7—P1—P2—S63.72 (11)
C1—P1—P2—C1968.50 (15)Cr—P1—P2—S58.60 (7)
C7—P1—P2—C19175.85 (14)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C22—H22···O2i0.952.653.581 (4)166.4
C21—H21···O4ii0.952.573.426 (5)149.3
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+1, y, z.
 

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