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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Dec 18;70(Pt 1):o72. doi: 10.1107/S1600536813033734

N,N,2,4,6-Penta­methyl­anilinium hexa­fluoro­phosphate–1,4,7,10,13,16-hexa­oxa­cyclo­octa­decane (2/1)

Yi Qi Chang a, Yuan Zhang a,*, Huo Lin Lian a
PMCID: PMC3914100  PMID: 24527005

Abstract

In the title compound, 2C11H18N+·2PF6 ·C12H24O6, the 18-crown-6 mol­ecule has crystallographically imposed inversion symmetry. In the crystal, it inter­acts with the cation through weak C—H⋯O hydrogen bonds. The cations and anions are further linked via N—H⋯F and C—H⋯F hydrogen bonds, leading to a sandwich structure .

Related literature  

For background to the development of ferroelectric pure organic or inorganic compounds, see: Haertling (1999); Homes et al. (2001). For the structure of a related compound, see: Zhang (2013).graphic file with name e-70-00o72-scheme1.jpg

Experimental  

Crystal data  

  • 2C11H18N+·2PF6 ·C12H24O6

  • M r = 882.78

  • Monoclinic, Inline graphic

  • a = 8.9122 (18) Å

  • b = 16.775 (3) Å

  • c = 15.136 (3) Å

  • β = 103.71 (3)°

  • V = 2198.4 (8) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.19 mm−1

  • T = 293 K

  • 0.40 × 0.30 × 0.20 mm

Data collection  

  • Rigaku Mercury2 (2x2 bin mode) diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) T min = 0.832, T max = 1.000

  • 18170 measured reflections

  • 3858 independent reflections

  • 2524 reflections with I > 2σ(I)

  • R int = 0.053

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.083

  • wR(F 2) = 0.195

  • S = 1.20

  • 3858 reflections

  • 253 parameters

  • H-atom parameters constrained

  • Δρmax = 0.49 e Å−3

  • Δρmin = −0.30 e Å−3

Data collection: CrystalClear (Rigaku, 2005); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536813033734/rz5098sup1.cif

e-70-00o72-sup1.cif (20.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813033734/rz5098Isup2.hkl

e-70-00o72-Isup2.hkl (189.1KB, hkl)

Supporting information file. DOI: 10.1107/S1600536813033734/rz5098Isup3.cml

Additional supporting information: crystallographic information; 3D view; checkCIF report

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

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1C⋯F4 0.91 2.38 3.077 (5) 134
C16—H16A⋯O3i 0.96 2.52 3.334 (5) 143
C16—H16B⋯O2ii 0.96 2.51 3.443 (5) 164
C16—H16C⋯O1i 0.96 2.57 3.381 (5) 143
C17—H17B⋯F4 0.96 2.54 3.122 (6) 119

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

supplementary crystallographic information

1. Comment

As a continuation of our studies on the development of novel ferroelectric pure organic or inorganic compounds (Haertling et al., 1999; Homes et al., 2001), we investigated the physical properties of the title compound. Recently the crystal structure of the strictly related compound N,N,2,4,6-pentamethylanilinium hexafluorophosphate was reported by our group (Zhang, 2013). The dielectric constant of the title compound as a function of the temperature indicates that the permittivity is basically temperature-independent (dielectric constant equaling to 4.1 to 6.1), suggesting that this compound should be not a real ferroelectrics or there may be no distinct phase transition occurring within the measured temperature range. Similarly, below the melting point (180°C) of the compound, the dielectric constant as a function of temperature also goes smoothly, and there is no dielectric anomaly observed (dielectric constant equaling to 4.1 to 6.1). Herein, we report the synthesis and crystal structure of the title compound.

The asymmetric unit of the title compound (Fig. 1) consists of one N,N,2,4,6-pentamethylanilinium cation, one hexafluorophosphate anion and one half of a 1,4,7,10,13,16-hexaoxacyclooctadecane molecule. Bond distances and bond angles are not unusual. In the crystal structure (Fig. 2), the 18-crown-6 molecule interacts with the cation through weak C—H···O hydrogen bonds (Table 1). Cation and anion are further linked via N—H···F and C—H···F hydrogen bonds. Dipole–dipole and van der Waals interactions are effective in stabilizing the molecular packing.

2. Experimental

A mixture of N,N,2,4,6-pentamethylbenzenamine (1.36 g, 10 mmol), hexafluorophosphoric acid(1.90 g, 10 mmol) and 1,4,7,10,13,16-hexaoxacyclooctadecane (2.64, 10 mmol) in methanol(30 ml) was stirred until clear. After several days, the title compound was formed and recrystallized from a methanol solution to afford colourless prismatic crystals suitable for X-ray analysis.

3. Refinement

H atoms were positioned geometrically and refined using a riding model, with C—H = 0.97 Å, N—H = 0.91 Å, and Uiso(H) = 1.2 Ueq(C, N) or 1.5 Ueq(C) for methyl H atoms

Figures

Fig. 1.

Fig. 1.

Perspective view of the title compound, showing the displacement ellipsoids drawn at the 30% probability level. Atoms with the suffix A are generated by symmetry code -x, 2-y, 1-z.

Fig. 2.

Fig. 2.

Crystal packing of the title compound viewed along the b axis, showing the hydrogen bonding network (dashed lines).

Crystal data

2C11H18N+·2PF6·C12H24O6 F(000) = 928
Mr = 882.78 Dx = 1.334 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 3858 reflections
a = 8.9122 (18) Å θ = 2.6–25.0°
b = 16.775 (3) Å µ = 0.19 mm1
c = 15.136 (3) Å T = 293 K
β = 103.71 (3)° Prism, colourless
V = 2198.4 (8) Å3 0.40 × 0.30 × 0.20 mm
Z = 2

Data collection

Rigaku Mercury2 (2x2 bin mode) diffractometer 3858 independent reflections
Radiation source: fine-focus sealed tube 2524 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.053
Detector resolution: 13.6612 pixels mm-1 θmax = 25.0°, θmin = 3.0°
CCD_Profile_fitting scans h = −10→10
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) k = −19→19
Tmin = 0.832, Tmax = 1.000 l = −17→17
18170 measured reflections

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)] = 0.083 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.195 H-atom parameters constrained
S = 1.20 w = 1/[σ2(Fo2) + (0.0528P)2 + 2.P] where P = (Fo2 + 2Fc2)/3
3858 reflections (Δ/σ)max = 0.003
253 parameters Δρmax = 0.49 e Å3
0 restraints Δρmin = −0.30 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 0.47256 (14) 0.24011 (8) 0.74636 (8) 0.0722 (4)
F6 0.4805 (5) 0.2762 (2) 0.6529 (2) 0.1280 (12)
F5 0.3159 (4) 0.2840 (2) 0.7412 (3) 0.1289 (12)
F4 0.3770 (4) 0.16651 (18) 0.6942 (2) 0.1268 (12)
F3 0.4597 (5) 0.2030 (2) 0.8388 (2) 0.1461 (15)
F2 0.5602 (5) 0.3133 (2) 0.7981 (3) 0.1507 (15)
F1 0.6268 (5) 0.1971 (3) 0.7510 (3) 0.1725 (19)
O3 0.2823 (3) 1.00490 (16) 0.45178 (17) 0.0589 (7)
O2 0.1340 (3) 0.85340 (16) 0.45499 (17) 0.0612 (7)
O1 −0.1059 (3) 0.85014 (16) 0.55077 (17) 0.0609 (7)
C6 0.2987 (5) 1.0742 (3) 0.4023 (3) 0.0651 (11)
H6A 0.2276 1.0722 0.3429 0.078*
H6B 0.4029 1.0771 0.3936 0.078*
C4 0.2945 (5) 0.8633 (3) 0.4624 (3) 0.0673 (11)
H4A 0.3358 0.8166 0.4386 0.081*
H4B 0.3480 0.8696 0.5257 0.081*
C5 0.3191 (5) 0.9355 (3) 0.4095 (3) 0.0647 (11)
H5A 0.4261 0.9378 0.4056 0.078*
H5B 0.2548 0.9321 0.3482 0.078*
C2 −0.0682 (5) 0.7856 (2) 0.5001 (3) 0.0616 (11)
H2A −0.1249 0.7899 0.4371 0.074*
H2B −0.0961 0.7357 0.5243 0.074*
C3 0.1010 (5) 0.7875 (2) 0.5061 (3) 0.0630 (11)
H3A 0.1573 0.7927 0.5691 0.076*
H3B 0.1329 0.7384 0.4821 0.076*
C1 −0.2661 (5) 0.8535 (3) 0.5475 (3) 0.0664 (11)
H1A −0.2971 0.8060 0.5751 0.080*
H1B −0.3247 0.8560 0.4848 0.080*
C7 0.0742 (4) 0.0080 (2) 0.7882 (2) 0.0501 (9)
N1 0.1899 (4) 0.0220 (2) 0.7330 (2) 0.0679 (10)
H1C 0.1970 0.0761 0.7327 0.081*
C9 −0.1049 (5) 0.0657 (3) 0.8628 (3) 0.0647 (11)
H9A −0.1532 0.1104 0.8797 0.078*
C12 0.0381 (5) −0.0678 (2) 0.8125 (3) 0.0616 (11)
C11 −0.0714 (6) −0.0732 (3) 0.8639 (3) 0.0726 (13)
H11A −0.0971 −0.1235 0.8816 0.087*
C8 0.0030 (4) 0.0760 (2) 0.8112 (2) 0.0537 (10)
C10 −0.1433 (5) −0.0085 (3) 0.8899 (3) 0.0675 (12)
C13 0.0349 (6) 0.1585 (2) 0.7817 (3) 0.0774 (13)
H13A −0.0270 0.1963 0.8049 0.116*
H13B 0.0099 0.1611 0.7164 0.116*
H13C 0.1422 0.1709 0.8048 0.116*
C16 0.1342 (6) 0.0025 (3) 0.6344 (3) 0.0709 (12)
H16A 0.2140 0.0142 0.6035 0.106*
H16B 0.0443 0.0338 0.6087 0.106*
H16C 0.1085 −0.0531 0.6277 0.106*
C17 0.3506 (5) −0.0026 (3) 0.7753 (4) 0.0873 (15)
H17A 0.3774 0.0142 0.8377 0.131*
H17B 0.4196 0.0217 0.7433 0.131*
H17C 0.3588 −0.0595 0.7724 0.131*
C15 0.1046 (7) −0.1451 (3) 0.7880 (4) 0.1037 (18)
H15A 0.0592 −0.1889 0.8131 0.156*
H15B 0.2144 −0.1452 0.8123 0.156*
H15C 0.0827 −0.1503 0.7230 0.156*
C14 −0.2611 (6) −0.0173 (4) 0.9466 (3) 0.109 (2)
H14A −0.2989 0.0344 0.9579 0.164*
H14B −0.2137 −0.0423 1.0034 0.164*
H14C −0.3455 −0.0496 0.9144 0.164*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
P1 0.0737 (8) 0.0786 (9) 0.0619 (7) 0.0147 (7) 0.0115 (6) −0.0153 (6)
F6 0.166 (3) 0.134 (3) 0.090 (2) −0.004 (2) 0.044 (2) 0.010 (2)
F5 0.105 (2) 0.129 (3) 0.155 (3) 0.044 (2) 0.035 (2) −0.003 (2)
F4 0.177 (3) 0.088 (2) 0.106 (2) −0.022 (2) 0.017 (2) −0.0247 (18)
F3 0.202 (4) 0.166 (4) 0.074 (2) 0.046 (3) 0.041 (2) 0.022 (2)
F2 0.155 (3) 0.151 (3) 0.140 (3) −0.030 (3) 0.023 (2) −0.065 (3)
F1 0.126 (3) 0.232 (5) 0.158 (3) 0.101 (3) 0.031 (3) −0.019 (3)
O3 0.0604 (17) 0.0714 (18) 0.0509 (15) −0.0010 (14) 0.0253 (13) −0.0022 (14)
O2 0.0529 (16) 0.0711 (18) 0.0599 (16) 0.0049 (14) 0.0138 (12) 0.0084 (14)
O1 0.0557 (17) 0.0676 (18) 0.0605 (16) −0.0109 (14) 0.0164 (13) −0.0133 (14)
C6 0.053 (2) 0.090 (3) 0.057 (2) −0.012 (2) 0.0249 (19) 0.003 (2)
C4 0.054 (3) 0.079 (3) 0.070 (3) 0.011 (2) 0.019 (2) −0.001 (2)
C5 0.050 (2) 0.092 (3) 0.058 (2) 0.004 (2) 0.0234 (19) −0.004 (2)
C2 0.076 (3) 0.054 (2) 0.054 (2) −0.009 (2) 0.013 (2) 0.0014 (19)
C3 0.075 (3) 0.055 (2) 0.056 (2) 0.007 (2) 0.011 (2) −0.003 (2)
C1 0.061 (3) 0.074 (3) 0.066 (3) −0.019 (2) 0.018 (2) 0.000 (2)
C7 0.054 (2) 0.059 (2) 0.0350 (18) −0.0008 (19) 0.0063 (16) 0.0018 (17)
N1 0.065 (2) 0.083 (3) 0.055 (2) 0.0083 (18) 0.0140 (17) 0.0001 (18)
C9 0.067 (3) 0.078 (3) 0.046 (2) 0.014 (2) 0.006 (2) −0.008 (2)
C12 0.081 (3) 0.053 (2) 0.046 (2) 0.001 (2) 0.005 (2) −0.0007 (19)
C11 0.089 (3) 0.069 (3) 0.052 (2) −0.019 (3) 0.002 (2) 0.008 (2)
C8 0.061 (2) 0.055 (2) 0.040 (2) 0.0030 (19) 0.0023 (18) −0.0010 (17)
C10 0.052 (2) 0.105 (4) 0.040 (2) −0.010 (3) 0.0013 (18) 0.006 (2)
C13 0.110 (4) 0.049 (3) 0.075 (3) 0.005 (2) 0.026 (3) 0.001 (2)
C16 0.087 (3) 0.085 (3) 0.045 (2) −0.004 (2) 0.023 (2) −0.006 (2)
C17 0.067 (3) 0.090 (4) 0.100 (4) 0.011 (3) 0.010 (3) 0.010 (3)
C15 0.164 (6) 0.057 (3) 0.091 (4) 0.021 (3) 0.032 (4) 0.001 (3)
C14 0.073 (3) 0.187 (6) 0.070 (3) −0.025 (4) 0.024 (3) 0.011 (3)

Geometric parameters (Å, º)

P1—F1 1.539 (3) C7—C8 1.390 (5)
P1—F6 1.556 (3) C7—N1 1.492 (5)
P1—F3 1.560 (3) N1—C17 1.482 (5)
P1—F2 1.562 (4) N1—C16 1.493 (5)
P1—F5 1.564 (3) N1—H1C 0.9100
P1—F4 1.598 (3) C9—C10 1.380 (6)
O3—C5 1.404 (5) C9—C8 1.385 (6)
O3—C6 1.409 (5) C9—H9A 0.9300
O2—C4 1.418 (4) C12—C11 1.389 (6)
O2—C3 1.419 (4) C12—C15 1.507 (6)
O1—C2 1.412 (4) C11—C10 1.364 (6)
O1—C1 1.418 (4) C11—H11A 0.9300
C6—C1i 1.495 (6) C8—C13 1.503 (5)
C6—H6A 0.9700 C10—C14 1.512 (6)
C6—H6B 0.9700 C13—H13A 0.9600
C4—C5 1.497 (6) C13—H13B 0.9600
C4—H4A 0.9700 C13—H13C 0.9600
C4—H4B 0.9700 C16—H16A 0.9600
C5—H5A 0.9700 C16—H16B 0.9600
C5—H5B 0.9700 C16—H16C 0.9600
C2—C3 1.490 (6) C17—H17A 0.9600
C2—H2A 0.9700 C17—H17B 0.9600
C2—H2B 0.9700 C17—H17C 0.9600
C3—H3A 0.9700 C15—H15A 0.9600
C3—H3B 0.9700 C15—H15B 0.9600
C1—C6i 1.495 (6) C15—H15C 0.9600
C1—H1A 0.9700 C14—H14A 0.9600
C1—H1B 0.9700 C14—H14B 0.9600
C7—C12 1.382 (5) C14—H14C 0.9600
F1—P1—F6 89.5 (2) C12—C7—C8 122.7 (4)
F1—P1—F3 91.6 (2) C12—C7—N1 122.0 (4)
F6—P1—F3 178.3 (2) C8—C7—N1 115.4 (3)
F1—P1—F2 90.6 (3) C17—N1—C7 116.1 (3)
F6—P1—F2 91.4 (2) C17—N1—C16 115.4 (4)
F3—P1—F2 89.9 (2) C7—N1—C16 114.5 (3)
F1—P1—F5 179.7 (2) C17—N1—H1C 102.6
F6—P1—F5 90.2 (2) C7—N1—H1C 102.6
F3—P1—F5 88.7 (2) C16—N1—H1C 102.6
F2—P1—F5 89.4 (2) C10—C9—C8 122.3 (4)
F1—P1—F4 91.5 (2) C10—C9—H9A 118.9
F6—P1—F4 89.15 (19) C8—C9—H9A 118.9
F3—P1—F4 89.5 (2) C7—C12—C11 116.6 (4)
F2—P1—F4 177.8 (2) C7—C12—C15 126.6 (4)
F5—P1—F4 88.5 (2) C11—C12—C15 116.9 (4)
C5—O3—C6 112.2 (3) C10—C11—C12 123.4 (4)
C4—O2—C3 112.6 (3) C10—C11—H11A 118.3
C2—O1—C1 112.3 (3) C12—C11—H11A 118.3
O3—C6—C1i 110.0 (3) C9—C8—C7 117.3 (4)
O3—C6—H6A 109.7 C9—C8—C13 119.2 (4)
C1i—C6—H6A 109.7 C7—C8—C13 123.5 (4)
O3—C6—H6B 109.7 C11—C10—C9 117.7 (4)
C1i—C6—H6B 109.7 C11—C10—C14 121.5 (5)
H6A—C6—H6B 108.2 C9—C10—C14 120.7 (5)
O2—C4—C5 109.0 (3) C8—C13—H13A 109.5
O2—C4—H4A 109.9 C8—C13—H13B 109.5
C5—C4—H4A 109.9 H13A—C13—H13B 109.5
O2—C4—H4B 109.9 C8—C13—H13C 109.5
C5—C4—H4B 109.9 H13A—C13—H13C 109.5
H4A—C4—H4B 108.3 H13B—C13—H13C 109.5
O3—C5—C4 110.4 (3) N1—C16—H16A 109.5
O3—C5—H5A 109.6 N1—C16—H16B 109.5
C4—C5—H5A 109.6 H16A—C16—H16B 109.5
O3—C5—H5B 109.6 N1—C16—H16C 109.5
C4—C5—H5B 109.6 H16A—C16—H16C 109.5
H5A—C5—H5B 108.1 H16B—C16—H16C 109.5
O1—C2—C3 108.6 (3) N1—C17—H17A 109.5
O1—C2—H2A 110.0 N1—C17—H17B 109.5
C3—C2—H2A 110.0 H17A—C17—H17B 109.5
O1—C2—H2B 110.0 N1—C17—H17C 109.5
C3—C2—H2B 110.0 H17A—C17—H17C 109.5
H2A—C2—H2B 108.4 H17B—C17—H17C 109.5
O2—C3—C2 108.7 (3) C12—C15—H15A 109.5
O2—C3—H3A 109.9 C12—C15—H15B 109.5
C2—C3—H3A 109.9 H15A—C15—H15B 109.5
O2—C3—H3B 109.9 C12—C15—H15C 109.5
C2—C3—H3B 109.9 H15A—C15—H15C 109.5
H3A—C3—H3B 108.3 H15B—C15—H15C 109.5
O1—C1—C6i 109.3 (3) C10—C14—H14A 109.5
O1—C1—H1A 109.8 C10—C14—H14B 109.5
C6i—C1—H1A 109.8 H14A—C14—H14B 109.5
O1—C1—H1B 109.8 C10—C14—H14C 109.5
C6i—C1—H1B 109.8 H14A—C14—H14C 109.5
H1A—C1—H1B 108.3 H14B—C14—H14C 109.5

Symmetry code: (i) −x, −y+2, −z+1.

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N1—H1C···F4 0.91 2.38 3.077 (5) 134
C16—H16A···O3ii 0.96 2.52 3.334 (5) 143
C16—H16B···O2iii 0.96 2.51 3.443 (5) 164
C16—H16C···O1ii 0.96 2.57 3.381 (5) 143
C17—H17B···F4 0.96 2.54 3.122 (6) 119

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ5098).

References

  1. Haertling, G. H. (1999). J. Am. Ceram. Soc. 82, 797–810.
  2. Homes, C. C., Vogt, T., Shapiro, S. M., Wakimoto, S. & Ramirez, A. P. (2001). Science, 293, 673–676. [DOI] [PubMed]
  3. Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Zhang, Y. (2013). Acta Cryst. E69, o31.

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, New_Global_Publ_Block. DOI: 10.1107/S1600536813033734/rz5098sup1.cif

e-70-00o72-sup1.cif (20.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813033734/rz5098Isup2.hkl

e-70-00o72-Isup2.hkl (189.1KB, hkl)

Supporting information file. DOI: 10.1107/S1600536813033734/rz5098Isup3.cml

Additional supporting information: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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