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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Dec 7;68(Pt 1):o44. doi: 10.1107/S160053681105183X

trans-(Ethene-1,2-di­yl)bis­(diphenyl­phosphine selenide)

Zanele Phasha a,*, Sizwe Makhoba a, Alfred Muller a,*
PMCID: PMC3254404  PMID: 22259547

Abstract

In the title mol­ecule, C26H22P2Se2, both P atoms have distorted tetra­hedral environments, resulting in effective cone angles of 177 and 174°. Inversion twinning was detected and refined to a ratio of 0.35:0.65. Weak inter­molecular C—H⋯Se inter­actions are observed.

Related literature

For background to the steric and electronic effects of group 15 ligands, see: Roodt et al. (2003); Muller et al. (2008). For information on cone angles, see: Tolman (1977); Otto (2001).graphic file with name e-68-00o44-scheme1.jpg

Experimental

Crystal data

  • C26H22P2Se2

  • M r = 554.3

  • Orthorhombic, Inline graphic

  • a = 9.0604 (9) Å

  • b = 14.3239 (14) Å

  • c = 17.9617 (18) Å

  • V = 2331.1 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 3.32 mm−1

  • T = 100 K

  • 0.26 × 0.21 × 0.04 mm

Data collection

  • Bruker APEX DUO 4K CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2008) T min = 0.479, T max = 0.879

  • 14567 measured reflections

  • 5814 independent reflections

  • 5356 reflections with I > 2σ(I)

  • R int = 0.028

Refinement

  • R[F 2 > 2σ(F 2)] = 0.025

  • wR(F 2) = 0.053

  • S = 1.01

  • 5814 reflections

  • 272 parameters

  • H-atom parameters constrained

  • Δρmax = 0.51 e Å−3

  • Δρmin = −0.48 e Å−3

  • Absolute structure: Flack (1983), 2517 Friedel pairs

  • Flack parameter: 0.354 (6)

Data collection: APEX2 (Bruker, 2011); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT and XPREP (Bruker, 2008); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2005); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S160053681105183X/fj2485sup1.cif

e-68-00o44-sup1.cif (30.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681105183X/fj2485Isup2.hkl

e-68-00o44-Isup2.hkl (278.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C3—H3⋯Se2i 0.95 3.02 3.953 (2) 168
C21—H21⋯Se1ii 0.95 3.06 3.812 (2) 138
C17—H17⋯Se2iii 0.95 3.01 3.885 (3) 155

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

Acknowledgments

Research funds of the University of Johannesburg are gratefully acknowledged.

supplementary crystallographic information

Comment

The study of the transition metal phosphorous bond spans over several decades using various techniques such as crystallography, multi nuclear NMR and IR (Roodt et al., 2003). As part of this systematic investigation we have extended this study to selenium derivatives of the phosphorus ligands (see Muller et al., 2008). Reported as part of the above continuing study, the single-crystal structure of the bis-phosphorus containing compound, (SePPh2)2C2H2 where Ph = C6H5, is reported here.

The structure of the title compound (see Figure 1, Table 1) shows distorted tetrahedral environments for both the phosphorus centers. The P═Se bond distances (2.1026 (6), 2.1054 (6) Å for Se1 and Se2 respectively) are marginally statistically different, possibly due to the weak C—H···Se intermolecular hydrogen bonding observed (see Figure 2, Table 2; comparison based on 1% normal distribution coefficient).

The phosphorus ligand bulkiness was evaluated by using an adaptation of the well known Tolman cone angle model (Tolman, 1977). Instead of using a CPK model, the actual geometry from the crystal structure was taken to determine an 'effective cone angle' (Otto et al. 2001). The Se═P distances were also adjusted to 2.28 Å (the default value used by Tolman) to remove the effect of bond distance variation. Two different cone angles of 177° and 174° were obtained for P1and P2 respectively. The difference in cone angles may also be attributed to the weak interactions mentioned previously.

Experimental

Trans-1,2-bis(diphenylphosphino)ethylene and KSeCN were purchased from Sigma-Aldrich and used without purification. Eqimolar amounts of KSeCN and the trans-1,2-bis(diphenylphosphino)ethylene compound (ca 0.04 mmol) were dissolved in the minimum amounts of methanol (10 - 20 ml). The KSeCN solution was added drop wise (5 min.) to the phosphine solution with stirring at room temperature. The final solution was left to evaporate slowly until dry to give crystals suitable for a single-crystal X-ray study.

Refinement

All hydrogen atoms were positioned in geometrically idealized positions with C—H = 0.95 Å and allowed to ride on their parent atoms with Uiso(H) = 1.2Ueq. The Flack parameter (based on 2517 Friedel pairs) indicates racemic twinning of the compound. This refined to a 35.4:64.6 racemic twin. The highest residual electron density of 0.51 e.Å-3 is 0.98 Å from Se1 representing no physical meaning.

Figures

Fig. 1.

Fig. 1.

: View of the title compound indicating labelling and displacement ellipsoids (drawn at a 50% probability level).

Fig. 2.

Fig. 2.

: Partial packing diagram of the title compound illustrating the weak C–H···Se interactions stabilizing the crystal packing.

Crystal data

C26H22P2Se2 F(000) = 1104
Mr = 554.3 Dx = 1.579 Mg m3
Orthorhombic, P212121 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2ab Cell parameters from 5956 reflections
a = 9.0604 (9) Å θ = 2.3–28.2°
b = 14.3239 (14) Å µ = 3.32 mm1
c = 17.9617 (18) Å T = 100 K
V = 2331.1 (4) Å3 Plate, colourless
Z = 4 0.26 × 0.21 × 0.04 mm

Data collection

Bruker APEX DUO 4K CCD diffractometer 5814 independent reflections
graphite 5356 reflections with I > 2σ(I)
Detector resolution: 8.4 pixels mm-1 Rint = 0.028
φ and ω scans θmax = 28.5°, θmin = 1.8°
Absorption correction: multi-scan (SADABS; Bruker, 2008) h = −10→12
Tmin = 0.479, Tmax = 0.879 k = −12→19
14567 measured reflections l = −24→22

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.025 H-atom parameters constrained
wR(F2) = 0.053 w = 1/[σ2(Fo2) + (0.0268P)2] where P = (Fo2 + 2Fc2)/3
S = 1.01 (Δ/σ)max = 0.001
5814 reflections Δρmax = 0.51 e Å3
272 parameters Δρmin = −0.48 e Å3
0 restraints Absolute structure: Flack (1983), 2517 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.354 (6)

Special details

Experimental. The intensity data was collected on a Bruker Apex DUO 4 K CCD diffractometer using an exposure time of 20 s/frame. A total of 588 frames were collected with a frame width of 0.5° covering up to θ = 28.49° with 99.2% completeness accomplished.Analytical data: 1H NMR (CDCl3, 400 MHz) δ 7.50–7.70 (m, 10H), 7.51–7.42 (m, 10H), 7.89 (t, 3J = 22.8 Hz, 2H); 13C {H} NMR (CDCl3, 100 MHz) δ 142.4 (ethylene), 132.1, 131.8, 129.0 (Ar); 31P {H} NMR (CDCl3, 160 MHz):δ = 28.58 (dd, 1JSe—P = 694.9, 814.8 Hz, 2P).
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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)

x y z Uiso*/Ueq
C1 1.0685 (2) 0.72411 (15) 0.64399 (13) 0.0134 (4)
C2 1.0826 (3) 0.62874 (15) 0.62917 (14) 0.0185 (5)
H2 0.9975 0.5921 0.619 0.022*
C3 1.2215 (3) 0.58774 (15) 0.62938 (15) 0.0226 (5)
H3 1.231 0.5228 0.6198 0.027*
C4 1.3460 (3) 0.64076 (16) 0.64339 (15) 0.0197 (5)
H4 1.4407 0.6123 0.6434 0.024*
C5 1.3321 (3) 0.73551 (16) 0.65749 (14) 0.0186 (5)
H5 1.4175 0.7721 0.6668 0.022*
C6 1.1940 (3) 0.77686 (15) 0.65806 (13) 0.0173 (5)
H6 1.185 0.8417 0.6681 0.021*
C7 0.9158 (2) 0.89938 (15) 0.62504 (14) 0.0158 (5)
C8 0.9380 (3) 0.92399 (16) 0.55117 (14) 0.0198 (5)
H8 0.939 0.8771 0.5138 0.024*
C9 0.9588 (3) 1.01653 (18) 0.53168 (17) 0.0265 (6)
H9 0.9743 1.033 0.481 0.032*
C10 0.9571 (3) 1.08522 (17) 0.58612 (17) 0.0278 (6)
H10 0.9707 1.1488 0.5726 0.033*
C11 0.9357 (3) 1.06180 (17) 0.65944 (18) 0.0282 (6)
H11 0.935 1.1091 0.6965 0.034*
C12 0.9150 (3) 0.96844 (16) 0.67974 (16) 0.0221 (5)
H12 0.9004 0.9522 0.7305 0.027*
C13 0.4690 (2) 0.81404 (15) 0.84948 (14) 0.0156 (5)
C14 0.4717 (3) 0.90052 (16) 0.81243 (15) 0.0212 (5)
H14 0.5622 0.9242 0.7935 0.025*
C15 0.3430 (3) 0.95120 (17) 0.80341 (16) 0.0252 (6)
H15 0.3451 1.0095 0.7782 0.03*
C16 0.2105 (3) 0.91681 (17) 0.83126 (15) 0.0250 (6)
H16 0.1221 0.9516 0.825 0.03*
C17 0.2075 (3) 0.83228 (17) 0.86790 (15) 0.0244 (5)
H17 0.1169 0.8088 0.8869 0.029*
C18 0.3369 (3) 0.78136 (17) 0.87717 (14) 0.0211 (5)
H18 0.3343 0.7234 0.9029 0.025*
C19 0.5966 (2) 0.63390 (15) 0.88948 (14) 0.0145 (5)
C20 0.6670 (3) 0.59705 (15) 0.95104 (14) 0.0192 (5)
H20 0.737 0.6336 0.9775 0.023*
C21 0.6355 (3) 0.50619 (16) 0.97447 (16) 0.0245 (6)
H21 0.6852 0.4806 1.0164 0.029*
C22 0.5324 (3) 0.45375 (16) 0.93677 (16) 0.0230 (6)
H22 0.5092 0.3925 0.9534 0.028*
C23 0.4621 (3) 0.49016 (17) 0.87437 (17) 0.0243 (6)
H23 0.3923 0.4535 0.8479 0.029*
C24 0.4944 (3) 0.58029 (17) 0.85093 (16) 0.0214 (5)
H24 0.4464 0.6053 0.8084 0.026*
C25 0.7048 (2) 0.74177 (14) 0.76513 (12) 0.0142 (4)
H25 0.6431 0.711 0.7301 0.017*
C26 0.8328 (2) 0.77552 (14) 0.74213 (13) 0.0147 (4)
H26 0.8992 0.8002 0.778 0.018*
P1 0.88646 (6) 0.77673 (4) 0.64539 (3) 0.01278 (11)
P2 0.64250 (6) 0.75184 (4) 0.86038 (3) 0.01338 (12)
Se1 0.73133 (2) 0.712573 (15) 0.574954 (15) 0.01794 (6)
Se2 0.79614 (2) 0.821665 (14) 0.928447 (14) 0.01582 (5)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0146 (10) 0.0147 (10) 0.0108 (10) 0.0023 (8) 0.0025 (9) 0.0012 (8)
C2 0.0186 (11) 0.0144 (11) 0.0226 (14) −0.0001 (9) 0.0022 (11) −0.0013 (9)
C3 0.0248 (12) 0.0135 (11) 0.0295 (14) 0.0039 (9) 0.0034 (12) −0.0008 (9)
C4 0.0178 (11) 0.0191 (11) 0.0224 (13) 0.0056 (9) −0.0008 (11) 0.0032 (10)
C5 0.0155 (11) 0.0190 (11) 0.0213 (13) −0.0012 (9) −0.0027 (10) −0.0005 (9)
C6 0.0200 (11) 0.0127 (10) 0.0193 (12) 0.0014 (9) 0.0001 (10) −0.0049 (9)
C7 0.0123 (10) 0.0174 (11) 0.0178 (13) 0.0019 (8) −0.0017 (10) 0.0017 (9)
C8 0.0250 (12) 0.0168 (11) 0.0176 (13) 0.0007 (10) −0.0004 (11) 0.0001 (9)
C9 0.0265 (14) 0.0257 (14) 0.0274 (16) −0.0004 (11) 0.0010 (13) 0.0078 (11)
C10 0.0263 (12) 0.0147 (12) 0.0423 (19) −0.0005 (9) −0.0028 (14) 0.0064 (11)
C11 0.0316 (14) 0.0149 (12) 0.0379 (18) 0.0000 (11) −0.0067 (14) −0.0048 (11)
C12 0.0249 (12) 0.0184 (11) 0.0230 (14) 0.0000 (10) −0.0028 (12) −0.0010 (10)
C13 0.0182 (10) 0.0151 (11) 0.0136 (11) 0.0030 (9) 0.0024 (10) −0.0028 (9)
C14 0.0209 (12) 0.0174 (12) 0.0252 (14) −0.0010 (9) −0.0023 (11) 0.0023 (10)
C15 0.0269 (13) 0.0172 (11) 0.0317 (16) 0.0059 (10) −0.0039 (12) 0.0034 (10)
C16 0.0239 (12) 0.0254 (12) 0.0259 (14) 0.0100 (11) −0.0037 (12) −0.0062 (10)
C17 0.0193 (11) 0.0306 (13) 0.0232 (14) 0.0027 (11) 0.0034 (12) 0.0003 (10)
C18 0.0241 (12) 0.0227 (12) 0.0165 (12) 0.0032 (10) 0.0061 (11) 0.0039 (10)
C19 0.0153 (10) 0.0114 (11) 0.0168 (12) 0.0026 (8) 0.0044 (10) −0.0009 (9)
C20 0.0184 (11) 0.0187 (11) 0.0206 (13) −0.0023 (9) 0.0001 (10) 0.0001 (9)
C21 0.0328 (14) 0.0183 (12) 0.0225 (15) 0.0018 (11) −0.0029 (12) 0.0048 (10)
C22 0.0283 (12) 0.0149 (11) 0.0257 (15) −0.0027 (9) 0.0049 (12) 0.0054 (11)
C23 0.0233 (12) 0.0208 (12) 0.0288 (16) −0.0062 (10) 0.0010 (12) −0.0026 (11)
C24 0.0216 (12) 0.0219 (12) 0.0207 (13) −0.0009 (9) −0.0024 (11) 0.0029 (10)
C25 0.0189 (10) 0.0106 (9) 0.0130 (11) 0.0014 (9) 0.0008 (10) 0.0000 (8)
C26 0.0165 (10) 0.0135 (10) 0.0140 (11) 0.0019 (8) −0.0014 (9) −0.0001 (8)
P1 0.0135 (2) 0.0126 (3) 0.0122 (3) 0.0001 (2) 0.0011 (2) −0.0005 (2)
P2 0.0148 (3) 0.0124 (3) 0.0130 (3) 0.0017 (2) 0.0019 (2) 0.0009 (2)
Se1 0.01645 (10) 0.01938 (11) 0.01798 (12) −0.00169 (8) −0.00126 (11) −0.00443 (9)
Se2 0.01802 (10) 0.01372 (10) 0.01572 (11) 0.00030 (8) 0.00040 (11) −0.00065 (9)

Geometric parameters (Å, °)

C1—C6 1.388 (3) C14—H14 0.95
C1—C2 1.398 (3) C15—C16 1.391 (4)
C1—P1 1.813 (2) C15—H15 0.95
C2—C3 1.389 (3) C16—C17 1.378 (4)
C2—H2 0.95 C16—H16 0.95
C3—C4 1.383 (3) C17—C18 1.391 (3)
C3—H3 0.95 C17—H17 0.95
C4—C5 1.386 (3) C18—H18 0.95
C4—H4 0.95 C19—C20 1.381 (3)
C5—C6 1.384 (3) C19—C24 1.388 (3)
C5—H5 0.95 C19—P2 1.817 (2)
C6—H6 0.95 C20—C21 1.397 (3)
C7—C8 1.387 (3) C20—H20 0.95
C7—C12 1.394 (3) C21—C22 1.377 (4)
C7—P1 1.814 (2) C21—H21 0.95
C8—C9 1.384 (3) C22—C23 1.391 (4)
C8—H8 0.95 C22—H22 0.95
C9—C10 1.387 (4) C23—C24 1.389 (3)
C9—H9 0.95 C23—H23 0.95
C10—C11 1.373 (4) C24—H24 0.95
C10—H10 0.95 C25—C26 1.322 (3)
C11—C12 1.399 (3) C25—P2 1.807 (2)
C11—H11 0.95 C25—H25 0.95
C12—H12 0.95 C26—P1 1.804 (2)
C13—C18 1.377 (3) C26—H26 0.95
C13—C14 1.406 (3) P1—Se1 2.1026 (6)
C13—P2 1.818 (2) P2—Se2 2.1054 (6)
C14—C15 1.383 (3)
C6—C1—C2 119.4 (2) C17—C16—C15 120.0 (2)
C6—C1—P1 121.07 (16) C17—C16—H16 120
C2—C1—P1 119.47 (17) C15—C16—H16 120
C3—C2—C1 119.7 (2) C16—C17—C18 120.1 (2)
C3—C2—H2 120.1 C16—C17—H17 120
C1—C2—H2 120.1 C18—C17—H17 120
C4—C3—C2 120.5 (2) C13—C18—C17 120.7 (2)
C4—C3—H3 119.8 C13—C18—H18 119.6
C2—C3—H3 119.8 C17—C18—H18 119.6
C3—C4—C5 119.8 (2) C20—C19—C24 119.7 (2)
C3—C4—H4 120.1 C20—C19—P2 118.68 (18)
C5—C4—H4 120.1 C24—C19—P2 121.57 (19)
C6—C5—C4 120.1 (2) C19—C20—C21 120.2 (2)
C6—C5—H5 119.9 C19—C20—H20 119.9
C4—C5—H5 119.9 C21—C20—H20 119.9
C5—C6—C1 120.40 (19) C22—C21—C20 119.9 (2)
C5—C6—H6 119.8 C22—C21—H21 120
C1—C6—H6 119.8 C20—C21—H21 120
C8—C7—C12 119.6 (2) C21—C22—C23 120.2 (2)
C8—C7—P1 117.39 (19) C21—C22—H22 119.9
C12—C7—P1 123.0 (2) C23—C22—H22 119.9
C9—C8—C7 120.3 (2) C24—C23—C22 119.8 (2)
C9—C8—H8 119.8 C24—C23—H23 120.1
C7—C8—H8 119.8 C22—C23—H23 120.1
C8—C9—C10 120.0 (3) C19—C24—C23 120.2 (3)
C8—C9—H9 120 C19—C24—H24 119.9
C10—C9—H9 120 C23—C24—H24 119.9
C11—C10—C9 120.3 (2) C26—C25—P2 122.73 (18)
C11—C10—H10 119.8 C26—C25—H25 118.6
C9—C10—H10 119.8 P2—C25—H25 118.6
C10—C11—C12 120.2 (3) C25—C26—P1 122.73 (18)
C10—C11—H11 119.9 C25—C26—H26 118.6
C12—C11—H11 119.9 P1—C26—H26 118.6
C7—C12—C11 119.6 (3) C26—P1—C1 104.75 (11)
C7—C12—H12 120.2 C26—P1—C7 104.06 (11)
C11—C12—H12 120.2 C1—P1—C7 105.45 (10)
C18—C13—C14 119.0 (2) C26—P1—Se1 113.27 (8)
C18—C13—P2 123.07 (18) C1—P1—Se1 114.70 (8)
C14—C13—P2 117.87 (18) C7—P1—Se1 113.58 (8)
C15—C14—C13 120.2 (2) C25—P2—C19 105.65 (10)
C15—C14—H14 119.9 C25—P2—C13 101.97 (11)
C13—C14—H14 119.9 C19—P2—C13 106.79 (11)
C14—C15—C16 120.0 (2) C25—P2—Se2 112.39 (8)
C14—C15—H15 120 C19—P2—Se2 115.22 (8)
C16—C15—H15 120 C13—P2—Se2 113.68 (8)
C6—C1—C2—C3 0.6 (4) P2—C25—C26—P1 −173.15 (11)
P1—C1—C2—C3 −178.8 (2) C25—C26—P1—C1 −129.02 (19)
C1—C2—C3—C4 −0.7 (4) C25—C26—P1—C7 120.51 (19)
C2—C3—C4—C5 0.1 (4) C25—C26—P1—Se1 −3.3 (2)
C3—C4—C5—C6 0.4 (4) C6—C1—P1—C26 −84.4 (2)
C4—C5—C6—C1 −0.5 (4) C2—C1—P1—C26 95.0 (2)
C2—C1—C6—C5 0.0 (4) C6—C1—P1—C7 25.1 (2)
P1—C1—C6—C5 179.38 (19) C2—C1—P1—C7 −155.5 (2)
C12—C7—C8—C9 −0.2 (4) C6—C1—P1—Se1 150.79 (18)
P1—C7—C8—C9 179.00 (19) C2—C1—P1—Se1 −29.8 (2)
C7—C8—C9—C10 −0.2 (4) C8—C7—P1—C26 −170.97 (19)
C8—C9—C10—C11 0.4 (4) C12—C7—P1—C26 8.2 (2)
C9—C10—C11—C12 −0.2 (4) C8—C7—P1—C1 79.1 (2)
C8—C7—C12—C11 0.4 (4) C12—C7—P1—C1 −101.8 (2)
P1—C7—C12—C11 −178.79 (19) C8—C7—P1—Se1 −47.3 (2)
C10—C11—C12—C7 −0.2 (4) C12—C7—P1—Se1 131.83 (19)
C18—C13—C14—C15 −0.7 (4) C26—C25—P2—C19 −126.76 (19)
P2—C13—C14—C15 −179.2 (2) C26—C25—P2—C13 121.8 (2)
C13—C14—C15—C16 0.2 (4) C26—C25—P2—Se2 −0.3 (2)
C14—C15—C16—C17 0.1 (4) C20—C19—P2—C25 122.47 (19)
C15—C16—C17—C18 0.1 (4) C24—C19—P2—C25 −56.8 (2)
C14—C13—C18—C17 0.9 (4) C20—C19—P2—C13 −129.50 (19)
P2—C13—C18—C17 179.33 (19) C24—C19—P2—C13 51.2 (2)
C16—C17—C18—C13 −0.6 (4) C20—C19—P2—Se2 −2.2 (2)
C24—C19—C20—C21 0.0 (4) C24—C19—P2—Se2 178.50 (18)
P2—C19—C20—C21 −179.30 (19) C18—C13—P2—C25 125.2 (2)
C19—C20—C21—C22 −1.0 (4) C14—C13—P2—C25 −56.3 (2)
C20—C21—C22—C23 1.6 (4) C18—C13—P2—C19 14.6 (3)
C21—C22—C23—C24 −1.1 (4) C14—C13—P2—C19 −166.89 (19)
C20—C19—C24—C23 0.4 (4) C18—C13—P2—Se2 −113.6 (2)
P2—C19—C24—C23 179.7 (2) C14—C13—P2—Se2 64.9 (2)
C22—C23—C24—C19 0.1 (4)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C3—H3···Se2i 0.95 3.02 3.953 (2) 168
C21—H21···Se1ii 0.95 3.06 3.812 (2) 138
C17—H17···Se2iii 0.95 3.01 3.885 (3) 155

Symmetry codes: (i) −x+2, y−1/2, −z+3/2; (ii) −x+3/2, −y+1, z+1/2; (iii) x−1, y, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FJ2485).

References

  1. Altomare, A., Burla, M. C., Camalli, M., Cascarano, G. L., Giacovazzo, C., Guagliardi, A., Moliterni, A. G. G., Polidori, G. & Spagna, R. (1999). J. Appl. Cryst. 32, 115–119.
  2. Brandenburg, K. & Putz, H. (2005). DIAMOND Crystal Impact GbR, Bonn, Germany.
  3. Bruker (2008). SADABS, SAINT and XPREP Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Bruker (2011). APEX2 Bruker AXS Inc., Madison, Wisconsin, USA.
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  6. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
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  11. Tolman, C. A. (1977). Chem. Rev. 77, 313–348.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S160053681105183X/fj2485sup1.cif

e-68-00o44-sup1.cif (30.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681105183X/fj2485Isup2.hkl

e-68-00o44-Isup2.hkl (278.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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