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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Sep 3;67(Pt 10):o2546. doi: 10.1107/S1600536811035057

Bis(triphenyl-λ5-phosphanylidene)ammonium hydrogen dichloride

Jorit Gellhaar a, Carsten Knapp a,*
PMCID: PMC3201248  PMID: 22058726

Abstract

In the title compound, [(Ph3P)2N]+·[Cl-H-Cl] or C36H30NP2 +·Cl2H, the H atom of the [Cl—H—Cl] anion and the N atom of the [(Ph3P)2N]+ cation are located on a twofold axis, yielding overall symmetry 2 for both the cation and the anion. The central P—N—P angle [144.12 (13)°] of the cation is in the expected range and indicates only weak cation–anion inter­actions. The almost linear [Cl—H—Cl] anion is a rare example of a symmetric hydrogen bridge in a hydrogen dichloride anion. The Cl⋯Cl distance and two equal Cl—H bonds are typical of such a symmetric hydrogen dichloride anion.

Related literature

For selected examples containing the [Cl—H—Cl] anion, see: Atwood et al. (1990); Mootz et al. (1981); Habtemariam et al. (2001); Swann et al. (1984); Neumüller et al. (2005). For other bis(triphenyl-λ5-phosphanylidene)ammonium halide structures, see: Knapp & Uzun (2010a,b ); Beckett et al. (2010). For a discussion of the [(Ph3P)2N]+ cation, see: Lewis & Dance (2000). For a description of the Cambridge Structural Database, see: Allen (2002). For the synthesis of [(Ph3P)2N]Cl, see: Ruff & Schlientz (1974).graphic file with name e-67-o2546-scheme1.jpg

Experimental

Crystal data

  • C36H30NP2 +·Cl2H

  • M r = 610.46

  • Orthorhombic, Inline graphic

  • a = 11.6467 (3) Å

  • b = 16.5474 (4) Å

  • c = 15.7584 (3) Å

  • V = 3037.00 (12) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.35 mm−1

  • T = 100 K

  • 0.18 × 0.14 × 0.09 mm

Data collection

  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2001) T min = 0.940, T max = 0.970

  • 28633 measured reflections

  • 2994 independent reflections

  • 2671 reflections with I > 2σ(I)

  • R int = 0.030

Refinement

  • R[F 2 > 2σ(F 2)] = 0.033

  • wR(F 2) = 0.085

  • S = 1.08

  • 2994 reflections

  • 189 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.61 e Å−3

  • Δρmin = −0.79 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2011); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811035057/su2304sup1.cif

e-67-o2546-sup1.cif (24.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811035057/su2304Isup2.hkl

e-67-o2546-Isup2.hkl (147KB, 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
Cl1—H1⋯Cl1i 1.56 (1) 1.56 (1) 3.1045 (9) 173 (3)

Symmetry code: (i) Inline graphic.

Acknowledgments

Financial support from the Deutsche Forschungsgemeinschaft (DFG) and Universität Freiburg is gratefully acknowledged.

supplementary crystallographic information

Comment

The Cambridge Structural Database (Allen, 2002) currently contains more than 1200 structures containing the [(Ph3P)2N]+ cation ([(Ph3P)2N]+ = [PNP]+). Usually this cation is partnered by a bulky anion, while crystal structures containing small anions and especially halides are rare. The crystal structures of some solvate-free halides, [(Ph3P)2N]I (Beckett et al., 2010) and [(Ph3P)2N]Cl (Knapp & Uzun, 2010a), and the acetontrile solvate [(Ph3P)2N]Br.CH3CN (Knapp & Uzun, 2010b), were published only very recently.

Bis(triphenyl-λ5-phosphanylidene)ammonium chloride [(Ph3P)2N]Cl was synthesized according to a published method (Ruff et al., 1974). Solvate-free single crystals suitable for X-ray diffraction of the title compound were obtained as a by-product by layering a CH3CN solution with diethyl ether. The H atom of the [Cl—H—Cl]- anion and the N atom of the [(Ph3P)2N]+ cation are located on a twofold axis, yielding overall symmetry 2 for the cation. The central P—N—P angle [144.12 (13)°] and the P—N [1.5762 (7) Å] and P—C distances [1.7940 (16)–1.8028 (15) Å] are in the expected range for the [(Ph3P)2N]+ cation (Lewis & Dance, 2000).

The number of structurally characterized hydrogen dichloride anions is still limited. Often disorder or low crystal quality does not allow to establish unequivically the position of the H atom. The Cl···Cl distances in all hydrogen dichloride anions deviate only slightly from an averaged distance of 3.10 Å. The anion in the title compound contains a symmetric hydrogen bridge with H—Cl distances of 1.56 (1) Å and a Cl···Cl distance of 3.1045 (9) Å. The anion is almost linear and a Cl—H—Cl angle of 173 (3)° is observed. A very similar hydrogen dichloride anion was found in the the crystal structure of [K(18 C-6)][Cl—H—Cl], where H—Cl is 1.56 Å and Cl···Cl 3.117 (1) Å (Atwood et al., 1990).

Experimental

Single crystals of the title compound, suitable for X-ray diffraction analysis, were obtained as a by-product by layering a CH3CN solution of [(Ph3P)2N]Cl with diethyl ether.

Refinement

The carbon-bonded hydrogen atoms were positioned geometrically and refined using a riding model. The same Uiso value was used for all H atoms, which refined to 0.0226 (13) Å2. The coordinates for the hydrogen atom in the [Cl—H—Cl]- anion were taken from the Fourier map and the atom was refined isotropically.

Figures

Fig. 1.

Fig. 1.

A view of the ionic unit of the title compound, showing the atom numbering and displacement ellipsoids drawn at the 50% probability level. H atoms are drawn with arbitrary radii. [Symmetry code: (i) -x+1, y, -z+0.5.]

Crystal data

C36H30NP2+·Cl2H F(000) = 1272
Mr = 610.46 Dx = 1.335 Mg m3
Orthorhombic, Pbcn Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2n 2ab Cell parameters from 9956 reflections
a = 11.6467 (3) Å θ = 2.5–30.8°
b = 16.5474 (4) Å µ = 0.35 mm1
c = 15.7584 (3) Å T = 100 K
V = 3037.00 (12) Å3 Block, colourless
Z = 4 0.18 × 0.14 × 0.09 mm

Data collection

Bruker APEXII CCD area-detector diffractometer 2994 independent reflections
Radiation source: microfocus sealed tube 2671 reflections with I > 2σ(I)
multilayer mirro optics Rint = 0.030
φ and ω scans θmax = 26.0°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Bruker, 2001) h = −14→14
Tmin = 0.940, Tmax = 0.970 k = −19→20
28633 measured reflections l = −19→16

Refinement

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)] = 0.033 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.085 H atoms treated by a mixture of independent and constrained refinement
S = 1.08 w = 1/[σ2(Fo2) + (0.0372P)2 + 2.5322P] where P = (Fo2 + 2Fc2)/3
2994 reflections (Δ/σ)max < 0.001
189 parameters Δρmax = 0.61 e Å3
0 restraints Δρmin = −0.79 e Å3

Special details

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)

x y z Uiso*/Ueq
P1 0.37492 (3) 0.47726 (2) 0.22743 (2) 0.01086 (11)
N1 0.5000 0.44792 (11) 0.2500 0.0142 (4)
C1 0.32847 (13) 0.42600 (9) 0.13289 (10) 0.0136 (3)
C2 0.37451 (13) 0.35003 (10) 0.11482 (10) 0.0163 (3)
H2 0.4320 0.3275 0.1505 0.0226 (13)*
C3 0.33594 (15) 0.30750 (10) 0.04441 (11) 0.0203 (4)
H3 0.3678 0.2561 0.0315 0.0226 (13)*
C4 0.25109 (16) 0.33988 (10) −0.00703 (11) 0.0227 (4)
H4 0.2247 0.3104 −0.0549 0.0226 (13)*
C5 0.20431 (15) 0.41512 (11) 0.01091 (11) 0.0224 (4)
H5 0.1460 0.4369 −0.0245 0.0226 (13)*
C6 0.24288 (14) 0.45863 (10) 0.08092 (10) 0.0173 (3)
H6 0.2112 0.5102 0.0933 0.0226 (13)*
C7 0.36204 (12) 0.58392 (9) 0.20936 (10) 0.0126 (3)
C8 0.43189 (13) 0.61829 (10) 0.14660 (10) 0.0171 (3)
H8 0.4784 0.5847 0.1118 0.0226 (13)*
C9 0.43306 (14) 0.70100 (10) 0.13533 (11) 0.0203 (4)
H9 0.4809 0.7243 0.0931 0.0226 (13)*
C10 0.36455 (14) 0.75028 (10) 0.18551 (11) 0.0204 (4)
H10 0.3661 0.8072 0.1778 0.0226 (13)*
C11 0.29393 (15) 0.71670 (10) 0.24675 (11) 0.0210 (4)
H11 0.2462 0.7505 0.2803 0.0226 (13)*
C12 0.29273 (14) 0.63361 (10) 0.25912 (10) 0.0169 (3)
H12 0.2447 0.6107 0.3015 0.0226 (13)*
C13 0.27637 (13) 0.44720 (9) 0.30980 (10) 0.0128 (3)
C14 0.15825 (13) 0.45901 (10) 0.30003 (10) 0.0162 (3)
H14 0.1295 0.4861 0.2513 0.0226 (13)*
C15 0.08307 (14) 0.43109 (10) 0.36169 (11) 0.0189 (3)
H15 0.0028 0.4391 0.3550 0.0226 (13)*
C16 0.12438 (14) 0.39159 (10) 0.43294 (10) 0.0179 (3)
H16 0.0724 0.3723 0.4748 0.0226 (13)*
C17 0.24172 (14) 0.38023 (10) 0.44327 (10) 0.0174 (3)
H17 0.2700 0.3534 0.4923 0.0226 (13)*
C18 0.31776 (13) 0.40806 (9) 0.38184 (10) 0.0149 (3)
H18 0.3980 0.4004 0.3890 0.0226 (13)*
Cl1 0.49306 (4) 0.14372 (3) 0.15163 (3) 0.03665 (15)
H1 0.5000 0.149 (3) 0.2500 0.087 (15)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
P1 0.0108 (2) 0.0097 (2) 0.0120 (2) −0.00044 (14) −0.00017 (14) −0.00049 (14)
N1 0.0123 (9) 0.0108 (9) 0.0196 (10) 0.000 −0.0001 (7) 0.000
C1 0.0144 (7) 0.0138 (8) 0.0127 (7) −0.0053 (6) 0.0026 (6) −0.0011 (6)
C2 0.0148 (7) 0.0154 (8) 0.0188 (8) −0.0027 (6) 0.0026 (6) −0.0021 (6)
C3 0.0231 (8) 0.0158 (8) 0.0219 (9) −0.0040 (7) 0.0065 (7) −0.0059 (7)
C4 0.0334 (9) 0.0200 (9) 0.0146 (8) −0.0099 (7) 0.0004 (7) −0.0030 (7)
C5 0.0300 (9) 0.0212 (9) 0.0160 (8) −0.0063 (7) −0.0066 (7) 0.0041 (7)
C6 0.0229 (8) 0.0135 (8) 0.0155 (8) −0.0021 (6) −0.0011 (6) 0.0015 (6)
C7 0.0126 (7) 0.0118 (7) 0.0134 (7) 0.0000 (6) −0.0044 (6) −0.0001 (6)
C8 0.0160 (7) 0.0169 (8) 0.0184 (8) 0.0015 (6) 0.0007 (6) 0.0006 (6)
C9 0.0187 (8) 0.0174 (9) 0.0247 (9) −0.0021 (7) −0.0007 (7) 0.0067 (7)
C10 0.0218 (8) 0.0118 (8) 0.0276 (9) 0.0007 (6) −0.0076 (7) 0.0019 (7)
C11 0.0231 (8) 0.0158 (8) 0.0240 (9) 0.0054 (7) −0.0021 (7) −0.0027 (7)
C12 0.0173 (8) 0.0166 (8) 0.0169 (8) 0.0019 (6) 0.0003 (6) 0.0001 (6)
C13 0.0148 (7) 0.0106 (7) 0.0130 (8) −0.0014 (6) 0.0006 (6) −0.0023 (6)
C14 0.0155 (7) 0.0185 (8) 0.0147 (8) −0.0014 (6) −0.0018 (6) 0.0002 (6)
C15 0.0133 (7) 0.0214 (9) 0.0219 (9) −0.0024 (6) 0.0001 (6) −0.0006 (7)
C16 0.0202 (8) 0.0153 (8) 0.0180 (8) −0.0039 (6) 0.0047 (6) 0.0001 (6)
C17 0.0230 (8) 0.0142 (8) 0.0149 (8) 0.0002 (6) −0.0009 (6) 0.0022 (6)
C18 0.0151 (7) 0.0127 (8) 0.0168 (8) 0.0008 (6) −0.0009 (6) −0.0005 (6)
Cl1 0.0363 (3) 0.0556 (3) 0.0181 (2) 0.0236 (2) −0.00128 (18) −0.0032 (2)

Geometric parameters (Å, °)

P1—N1 1.5762 (7) C9—C10 1.388 (2)
P1—C7 1.7940 (16) C9—H9 0.9500
P1—C1 1.7976 (16) C10—C11 1.384 (2)
P1—C13 1.8028 (15) C10—H10 0.9500
N1—P1i 1.5761 (7) C11—C12 1.389 (2)
C1—C2 1.396 (2) C11—H11 0.9500
C1—C6 1.399 (2) C12—H12 0.9500
C2—C3 1.389 (2) C13—C18 1.393 (2)
C2—H2 0.9500 C13—C14 1.398 (2)
C3—C4 1.386 (3) C14—C15 1.387 (2)
C3—H3 0.9500 C14—H14 0.9500
C4—C5 1.388 (3) C15—C16 1.386 (2)
C4—H4 0.9500 C15—H15 0.9500
C5—C6 1.392 (2) C16—C17 1.389 (2)
C5—H5 0.9500 C16—H16 0.9500
C6—H6 0.9500 C17—C18 1.390 (2)
C7—C12 1.394 (2) C17—H17 0.9500
C7—C8 1.401 (2) C18—H18 0.9500
C8—C9 1.380 (2) Cl1—H1 1.555 (3)
C8—H8 0.9500
N1—P1—C7 114.59 (8) C8—C9—C10 120.24 (16)
N1—P1—C1 108.65 (7) C8—C9—H9 119.9
C7—P1—C1 107.91 (7) C10—C9—H9 119.9
N1—P1—C13 109.93 (6) C11—C10—C9 120.19 (15)
C7—P1—C13 109.42 (7) C11—C10—H10 119.9
C1—P1—C13 105.96 (7) C9—C10—H10 119.9
P1i—N1—P1 144.12 (13) C10—C11—C12 120.08 (16)
C2—C1—C6 120.13 (14) C10—C11—H11 120.0
C2—C1—P1 118.58 (12) C12—C11—H11 120.0
C6—C1—P1 121.17 (12) C11—C12—C7 119.95 (16)
C3—C2—C1 119.67 (15) C11—C12—H12 120.0
C3—C2—H2 120.2 C7—C12—H12 120.0
C1—C2—H2 120.2 C18—C13—C14 119.68 (14)
C4—C3—C2 120.14 (16) C18—C13—P1 119.66 (11)
C4—C3—H3 119.9 C14—C13—P1 120.57 (12)
C2—C3—H3 119.9 C15—C14—C13 119.84 (15)
C3—C4—C5 120.49 (16) C15—C14—H14 120.1
C3—C4—H4 119.8 C13—C14—H14 120.1
C5—C4—H4 119.8 C16—C15—C14 120.37 (15)
C4—C5—C6 119.92 (16) C16—C15—H15 119.8
C4—C5—H5 120.0 C14—C15—H15 119.8
C6—C5—H5 120.0 C15—C16—C17 120.03 (15)
C5—C6—C1 119.63 (16) C15—C16—H16 120.0
C5—C6—H6 120.2 C17—C16—H16 120.0
C1—C6—H6 120.2 C16—C17—C18 120.02 (15)
C12—C7—C8 119.59 (15) C16—C17—H17 120.0
C12—C7—P1 122.65 (12) C18—C17—H17 120.0
C8—C7—P1 117.57 (12) C17—C18—C13 120.06 (14)
C9—C8—C7 119.94 (15) C17—C18—H18 120.0
C9—C8—H8 120.0 C13—C18—H18 120.0
C7—C8—H8 120.0
C7—P1—N1—P1i 8.50 (6) C12—C7—C8—C9 1.0 (2)
C1—P1—N1—P1i 129.26 (6) P1—C7—C8—C9 −174.15 (13)
C13—P1—N1—P1i −115.21 (6) C7—C8—C9—C10 −0.5 (2)
N1—P1—C1—C2 27.31 (14) C8—C9—C10—C11 −0.5 (3)
C7—P1—C1—C2 152.11 (12) C9—C10—C11—C12 1.0 (3)
C13—P1—C1—C2 −90.78 (13) C10—C11—C12—C7 −0.5 (2)
N1—P1—C1—C6 −156.65 (13) C8—C7—C12—C11 −0.5 (2)
C7—P1—C1—C6 −31.85 (15) P1—C7—C12—C11 174.41 (13)
C13—P1—C1—C6 85.26 (14) N1—P1—C13—C18 3.27 (15)
C6—C1—C2—C3 0.8 (2) C7—P1—C13—C18 −123.40 (13)
P1—C1—C2—C3 176.89 (12) C1—P1—C13—C18 120.50 (13)
C1—C2—C3—C4 −0.8 (2) N1—P1—C13—C14 −173.36 (13)
C2—C3—C4—C5 0.4 (3) C7—P1—C13—C14 59.97 (14)
C3—C4—C5—C6 0.2 (3) C1—P1—C13—C14 −56.13 (14)
C4—C5—C6—C1 −0.2 (2) C18—C13—C14—C15 −0.6 (2)
C2—C1—C6—C5 −0.3 (2) P1—C13—C14—C15 176.07 (12)
P1—C1—C6—C5 −176.29 (12) C13—C14—C15—C16 0.0 (2)
N1—P1—C7—C12 −118.52 (12) C14—C15—C16—C17 0.4 (3)
C1—P1—C7—C12 120.31 (13) C15—C16—C17—C18 −0.4 (2)
C13—P1—C7—C12 5.46 (15) C16—C17—C18—C13 −0.1 (2)
N1—P1—C7—C8 56.51 (13) C14—C13—C18—C17 0.6 (2)
C1—P1—C7—C8 −64.66 (13) P1—C13—C18—C17 −176.05 (12)
C13—P1—C7—C8 −179.52 (12)

Symmetry codes: (i) −x+1, y, −z+1/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
Cl1—H1···Cl1i 1.56 (1) 1.56 (1) 3.1045 (9) 173 (3)

Symmetry codes: (i) −x+1, y, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SU2304).

References

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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) I, global. DOI: 10.1107/S1600536811035057/su2304sup1.cif

e-67-o2546-sup1.cif (24.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811035057/su2304Isup2.hkl

e-67-o2546-Isup2.hkl (147KB, hkl)

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


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