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The crystal structure of (2-chloro­phenyl)­di­phenyl­phosphine, C18H14ClP, has been determined at 295 (1) K. The conform­ation of the mol­ecule is similar to that of the analogous 2-bromo and 2-methyl compounds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802004440/tk6057sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802004440/tk6057Isup2.hkl
Contains datablock I

CCDC reference: 183799

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.039
  • wR factor = 0.115
  • Data-to-parameter ratio = 19.2

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry








Computing details top

Data collection: MSC/AFC7 Diffractometer Control Software for Windows (Molecular Structure Corporation, 1999); cell refinement: MSC/AFC7 Diffractometer Control Software for Windows; data reduction: TEXSAN (Molecular Structure Corporation, 1997-2001); program(s) used to solve structure: TEXSAN; program(s) used to refine structure: TEXSAN and SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: TEXSAN and PLATON (Spek, 2001).

(2-Chlorophenyl)diphenylphosphine top
Crystal data top
C18H14ClPZ = 2
Mr = 296.71F(000) = 308
Triclinic, P1Dx = 1.293 Mg m3
Hall symbol: -P 1Melting point: 377 - 380 K K
a = 10.646 (8) ÅMo Kα radiation, λ = 0.71069 Å
b = 10.702 (6) ÅCell parameters from 25 reflections
c = 8.530 (6) Åθ = 12.6–16.6°
α = 105.53 (6)°µ = 0.34 mm1
β = 99.88 (6)°T = 295 K
γ = 119.27 (4)°Prismatic, colorless
V = 762.1 (11) Å30.30 × 0.30 × 0.30 mm
Data collection top
Rigaku AFC-7R
diffractometer
Rint = 0.021
Radiation source: Rigaku rotating anodeθmax = 27.5°, θmin = 2.7°
Graphite monochromatorh = 1313
ω–2θ scansk = 1313
4248 measured reflectionsl = 611
3483 independent reflections3 standard reflections every 150 reflections
2452 reflections with I > 2σ(I) 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)] = 0.039Hydrogen site location: constr
wR(F2) = 0.115H-atom parameters not refined
S = 1.04 w = 1/[σ2(Fo2) + (0.0519P)2 + 0.1312P]
where P = (Fo2 + 2Fc2)/3
3483 reflections(Δ/σ)max < 0.001
181 parametersΔρmax = 0.36 e Å3
0 restraintsΔρmin = 0.22 e Å3
Special details top

Experimental. The scan width was (1.79 + 0.30tanθ)° with an ω scan speed of 16° per minute (up to 5 scans to achieve I/σ(I) > 10). Stationary background counts were recorded at each end of the scan, and the scan time:background time ratio was 2:1.

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All e.s.d.'s are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles

Refinement. Refinement on F2 for ALL reflections except those 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*/Ueq
Cl0.16286 (7)0.06764 (6)0.07477 (8)0.0644 (2)
P0.18038 (6)0.32646 (6)0.19819 (7)0.0468 (2)
C110.2241 (2)0.3628 (2)0.0340 (2)0.0467 (6)
C120.2166 (2)0.2465 (2)0.0838 (3)0.0508 (6)
C130.2477 (3)0.2626 (3)0.2551 (3)0.0658 (8)
C140.2906 (3)0.4007 (3)0.3822 (3)0.0743 (9)
C150.2993 (3)0.5193 (3)0.3397 (3)0.0763 (9)
C160.2663 (3)0.5006 (3)0.1667 (3)0.0619 (7)
C210.0311 (2)0.2002 (2)0.2793 (2)0.0459 (6)
C220.1076 (3)0.0858 (3)0.4496 (3)0.0565 (7)
C230.2663 (3)0.0190 (3)0.5154 (3)0.0675 (8)
C240.3500 (3)0.0104 (3)0.4128 (4)0.0685 (8)
C250.2771 (3)0.1034 (3)0.2456 (4)0.0661 (9)
C260.1183 (2)0.2079 (2)0.1782 (3)0.0558 (7)
C310.2212 (2)0.5143 (2)0.1954 (2)0.0477 (6)
C320.3758 (2)0.6357 (3)0.1446 (3)0.0610 (8)
C330.4170 (3)0.7767 (3)0.1531 (3)0.0714 (9)
C340.3057 (3)0.7994 (3)0.2154 (3)0.0692 (9)
C350.1523 (3)0.6810 (3)0.2674 (3)0.0669 (9)
C360.1100 (2)0.5392 (2)0.2575 (3)0.0562 (7)
H130.239500.179700.283900.0790*
H140.314600.414600.500700.0890*
H150.327800.614100.428500.0920*
H160.272600.583000.138600.0740*
H220.050000.079600.521400.0680*
H230.317100.096900.631700.0810*
H240.458900.083300.457500.0820*
H250.336000.110300.175800.0790*
H260.068700.285400.061800.0670*
H320.454100.620900.103300.0730*
H330.522900.858700.115700.0860*
H340.334200.896200.222600.0830*
H350.074900.696500.310300.0800*
H360.003800.458400.293800.0680*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl0.0834 (4)0.0569 (3)0.0682 (4)0.0456 (3)0.0299 (3)0.0323 (3)
P0.0515 (3)0.0507 (3)0.0476 (3)0.0311 (2)0.0227 (2)0.0251 (2)
C110.0431 (10)0.0514 (11)0.0464 (10)0.0258 (8)0.0164 (8)0.0225 (9)
C120.0465 (10)0.0576 (12)0.0514 (11)0.0289 (9)0.0184 (9)0.0268 (10)
C130.0684 (14)0.0820 (16)0.0592 (13)0.0440 (13)0.0242 (11)0.0413 (13)
C140.0722 (16)0.0960 (19)0.0476 (13)0.0409 (14)0.0195 (11)0.0341 (13)
C150.0763 (16)0.0711 (16)0.0481 (13)0.0296 (13)0.0153 (12)0.0082 (12)
C160.0689 (14)0.0553 (12)0.0538 (12)0.0314 (11)0.0207 (11)0.0200 (10)
C210.0519 (10)0.0456 (10)0.0462 (10)0.0292 (9)0.0175 (8)0.0234 (8)
C220.0670 (13)0.0598 (13)0.0476 (11)0.0399 (11)0.0159 (10)0.0230 (10)
C230.0675 (14)0.0556 (13)0.0600 (14)0.0321 (12)0.0003 (12)0.0170 (11)
C240.0513 (12)0.0577 (13)0.0884 (18)0.0252 (11)0.0114 (12)0.0388 (13)
C250.0566 (13)0.0655 (14)0.0867 (17)0.0329 (12)0.0339 (12)0.0431 (13)
C260.0549 (12)0.0535 (12)0.0582 (12)0.0284 (10)0.0243 (10)0.0235 (10)
C310.0525 (11)0.0517 (11)0.0456 (10)0.0292 (9)0.0231 (9)0.0256 (9)
C320.0519 (12)0.0622 (13)0.0749 (14)0.0300 (10)0.0263 (11)0.0382 (12)
C330.0668 (15)0.0589 (14)0.0794 (17)0.0242 (12)0.0293 (13)0.0369 (13)
C340.0876 (17)0.0527 (13)0.0715 (15)0.0364 (13)0.0316 (13)0.0355 (12)
C350.0790 (16)0.0647 (14)0.0705 (15)0.0466 (13)0.0247 (13)0.0349 (12)
C360.0571 (12)0.0558 (12)0.0603 (13)0.0324 (10)0.0212 (10)0.0286 (10)
Geometric parameters (Å, º) top
Cl—C121.760 (3)C32—C331.377 (4)
P—C111.840 (2)C33—C341.371 (5)
P—C211.834 (3)C34—C351.377 (5)
P—C311.830 (3)C35—C361.388 (4)
C11—C121.391 (3)C13—H130.9505
C11—C161.393 (3)C14—H140.9502
C12—C131.385 (3)C15—H150.9506
C13—C141.371 (4)C16—H160.9489
C14—C151.376 (4)C22—H220.9500
C15—C161.392 (4)C23—H230.9507
C21—C221.392 (3)C24—H240.9501
C21—C261.387 (3)C25—H250.9503
C22—C231.383 (5)C26—H260.9505
C23—C241.369 (5)C32—H320.9499
C24—C251.373 (4)C33—H330.9498
C25—C261.383 (4)C34—H340.9498
C31—C321.396 (4)C35—H350.9503
C31—C361.386 (3)C36—H360.9499
Cl···P3.153 (3)C31···H14vii3.0476
Cl···C213.503 (3)C32···H162.8974
Cl···Cli3.653 (3)C32···H14vii3.0266
Cl···H22ii3.1007C35···H26viii3.0719
Cl···H33iii3.0533H13···C23i3.0073
P···Cl3.153 (3)H13···C24i2.9296
C16···C323.460 (5)H14···C31ix3.0476
C21···Cl3.503 (3)H14···C32ix3.0265
C24···C24iv3.421 (6)H16···C312.6281
C26···C363.515 (4)H16···C322.8974
C32···C163.460 (5)H22···Clii3.1007
C36···C263.515 (4)H22···C22ii2.9701
C11···H262.7035H22···H22ii2.4785
C12···H32iii3.0233H24···C24iv2.8610
C16···H263.0002H24···H24iv2.5437
C21···H362.6427H26···C112.7035
C22···H22ii2.9701H26···C163.0002
C23···H34v3.0318H26···C35viii3.0719
C23···H13i3.0073H32···C12iii3.0233
C24···H24iv2.8610H33···C25x3.0871
C24···H13i2.9296H33···Cliii3.0533
C25···H33vi3.0871H34···C23v3.0318
C26···H362.8804H36···C212.6427
C31···H162.6281H36···C262.8804
C11—P—C21100.23 (11)C12—C13—H13120.69
C11—P—C31102.47 (10)C14—C13—H13120.74
C21—P—C31103.26 (12)C13—C14—H14119.66
P—C11—C12118.67 (16)C15—C14—H14119.73
P—C11—C16124.73 (18)C14—C15—H15120.04
C12—C11—C16116.59 (19)C16—C15—H15119.91
Cl—C12—C11119.92 (17)C11—C16—H16119.45
Cl—C12—C13117.0 (2)C15—C16—H16119.48
C11—C12—C13123.1 (2)C21—C22—H22119.57
C12—C13—C14118.6 (3)C23—C22—H22119.60
C13—C14—C15120.6 (2)C22—C23—H23120.01
C14—C15—C16120.1 (3)C24—C23—H23120.10
C11—C16—C15121.1 (3)C23—C24—H24119.88
P—C21—C22118.0 (2)C25—C24—H24119.91
P—C21—C26123.65 (15)C24—C25—H25119.86
C22—C21—C26118.3 (2)C26—C25—H25119.84
C21—C22—C23120.8 (3)C21—C26—H26119.85
C22—C23—C24119.9 (3)C25—C26—H26119.72
C23—C24—C25120.2 (3)C31—C32—H32119.42
C24—C25—C26120.3 (3)C33—C32—H32119.36
C21—C26—C25120.4 (2)C32—C33—H33119.98
P—C31—C32117.1 (2)C34—C33—H33119.74
P—C31—C36124.68 (17)C33—C34—H34120.22
C32—C31—C36117.8 (2)C35—C34—H34120.19
C31—C32—C33121.2 (3)C34—C35—H35119.78
C32—C33—C34120.3 (3)C36—C35—H35119.79
C33—C34—C35119.6 (3)C31—C36—H36119.71
C34—C35—C36120.4 (3)C35—C36—H36119.65
C31—C36—C35120.6 (2)
C21—P—C11—C1278.5 (2)C12—C13—C14—C151.4 (5)
C21—P—C11—C16102.2 (3)C13—C14—C15—C160.8 (5)
C31—P—C11—C12175.3 (2)C14—C15—C16—C110.0 (5)
C31—P—C11—C164.0 (3)P—C21—C22—C23176.3 (2)
C11—P—C21—C22148.2 (2)C26—C21—C22—C231.0 (4)
C11—P—C21—C2628.9 (2)P—C21—C26—C25176.6 (2)
C31—P—C21—C22106.3 (2)C22—C21—C26—C250.4 (4)
C31—P—C21—C2676.6 (2)C21—C22—C23—C240.3 (5)
C11—P—C31—C3278.48 (18)C22—C23—C24—C250.9 (5)
C11—P—C31—C36108.81 (19)C23—C24—C25—C261.5 (5)
C21—P—C31—C32177.69 (16)C24—C25—C26—C210.8 (4)
C21—P—C31—C365.0 (2)P—C31—C32—C33174.24 (19)
P—C11—C12—Cl1.1 (3)C36—C31—C32—C331.0 (3)
P—C11—C12—C13179.9 (2)P—C31—C36—C35173.01 (19)
C16—C11—C12—Cl179.5 (2)C32—C31—C36—C350.3 (3)
C16—C11—C12—C130.4 (4)C31—C32—C33—C341.3 (4)
P—C11—C16—C15179.2 (3)C32—C33—C34—C350.8 (4)
C12—C11—C16—C150.2 (4)C33—C34—C35—C360.2 (4)
Cl—C12—C13—C14179.7 (3)C34—C35—C36—C310.1 (4)
C11—C12—C13—C141.2 (5)
Symmetry codes: (i) x, y, z; (ii) x, y, z1; (iii) x+1, y+1, z; (iv) x1, y, z1; (v) x, y+1, z1; (vi) x1, y1, z; (vii) x, y, z1; (viii) x, y+1, z; (ix) x, y, z+1; (x) x+1, y+1, z.
 

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