organic compounds
N-Chloromethyl-4-(dimethylamino)-N,N-dimethylanilinium chloride
aDepartment of Chemistry, University of Durham, South Road, Durham DH1 3LE, England
*Correspondence e-mail: a.s.batsanov@durham.ac.uk
In the cation of the title compound C11H18ClN2+·Cl−, the quaternary N atom has a distorted tetrahedral geometry, and the other N a nearly planar-trigonal (owing to conjugation with the benzene ring) bonding geometry.
Comment
The title compound, (I), was obtained as an accidental by-product while co-crystallizing N,N,N′,N′-tetramethyl-1,4-phenylenediamine (TMPD) and octafluoronaphthalene (OFN) from CH2Cl2 (Collings et al., 2004). The comprises one chloride anion and one Me2(ClCH2)N+–C6H4–NMe2 cation. This cation has been structurally studied earlier as its tetraphenylborate salt dichloromethane solvate (II) by Winter (2001), and the non-chlorinated analogue trimethyl{4-(dimethylamino)phenyl}ammonium cation as its ozonide salt (III) by Assenmacher & Jansen (1995). Unfortunately, the precision of both structure determinations was limited (R = 0.09), in (III) owing to disorder of the ozonide anion and to chemical instability (the compound explodes at 303 K), and in (II) probably because of some unrecognized disorder, as indicated by the discrepant N+—CH3 bond lengths of 1.50 (1) and 1.62 (1) Å.
The atom N2 has nearly planar geometry, the sum of the bond angles being 358.1°. The C10/N2/C11 plane forms an angle of 11.9 (1)° with the benzene ring plane, so that the pπ orbitals of N2 and C4 are nearly coplanar. This and the N2—C4 bond distance of 1.371 (2) Å are indicative of strong π-conjugation. The quaternary atom N1 has a distorted tetrahedral environment. The chloride anion is surrounded by eight H atoms of four different cations at Cl⋯H distances of 2.46 (2) to 2.60 (2) Å (calculated for the idealized C—H bond lengths of 1.08 Å).
Experimental
Slow evaporation at room temperature of a dichloromethane solution of equimolar amounts of TMPD and OFN yielded mainly co-crystals of TMPD and OFN (1:1) and a few smaller crystals of different habit, which were identified by the present study as (I).
Crystal data
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Data collection
Refinement
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Methyl groups bonded to N2 were refined as rigid bodies rotating around the N2—C bonds, and other H atoms were treated as riding on the corresponding C atoms in idealized positions. The C—H distances were fixed at 0.98 Å for methyl, 0.99 Å for methylene, 0.95 Å for benzene H atoms, with Uiso(H) = 1.5Ueq(C) for methyl H atoms and 1.2Ueq(C) for the rest.
Data collection: SMART (Bruker, 2001a); cell SMART; data reduction: SAINT (Bruker, 2001a); program(s) used to solve structure: SHELXTL (Bruker, 2001b); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Supporting information
https://doi.org/10.1107/S1600536804033860/bt6570sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536804033860/bt6570Isup2.hkl
Data collection: SMART (Bruker, 2001a); cell
SMART; data reduction: SAINT (Bruker, 2001a); program(s) used to solve structure: SHELXTL (Bruker, 2001b); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL (Bruker, 2001b); software used to prepare material for publication: SHELXTL.C11H18ClN2+·Cl− | F(000) = 528 |
Mr = 249.17 | Dx = 1.306 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 977 reflections |
a = 15.121 (3) Å | θ = 10.2–26.9° |
b = 7.234 (1) Å | µ = 0.48 mm−1 |
c = 12.773 (2) Å | T = 120 K |
β = 114.95 (1)° | Parallelepiped, colourless |
V = 1266.8 (4) Å3 | 0.22 × 0.15 × 0.10 mm |
Z = 4 |
Bruker SMART 6000 CCD area-detector diffractometer | 3689 independent reflections |
Radiation source: fine-focus sealed tube | 2994 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.047 |
Detector resolution: 5.6 pixels mm-1 | θmax = 30.0°, θmin = 1.5° |
ω scans | h = −21→21 |
Absorption correction: integration (XPREP;SHELXTL), R(int) = 0.053 before correction | k = −10→10 |
Tmin = 0.923, Tmax = 0.962 | l = −17→17 |
17336 measured reflections |
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)] = 0.037 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.115 | H-atom parameters constrained |
S = 1.05 | w = 1/[σ2(Fo2) + (0.0621P)2 + 0.4607P] where P = (Fo2 + 2Fc2)/3 |
3689 reflections | (Δ/σ)max = 0.001 |
138 parameters | Δρmax = 0.48 e Å−3 |
0 restraints | Δρmin = −0.51 e Å−3 |
Experimental. The data collection nominally covered full sphere of reciprocal space, by a combination of 4 sets of ω scans; each set at different φ and/or 2θ angles and each scan (30 sec exposure) covering 0.3° in ω. Crystal to detector distance 4.83 cm. |
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. |
x | y | z | Uiso*/Ueq | ||
Cl1 | 0.13260 (3) | 0.94831 (6) | 0.50991 (4) | 0.03711 (13) | |
N1 | 0.14834 (9) | 0.61049 (18) | 0.42545 (11) | 0.0191 (2) | |
N2 | 0.56069 (10) | 0.6864 (2) | 0.65487 (13) | 0.0270 (3) | |
C1 | 0.25717 (10) | 0.6300 (2) | 0.48375 (13) | 0.0196 (3) | |
C2 | 0.30675 (11) | 0.5631 (2) | 0.59580 (13) | 0.0212 (3) | |
H2 | 0.2715 | 0.5060 | 0.6335 | 0.025* | |
C3 | 0.40730 (11) | 0.5796 (2) | 0.65257 (14) | 0.0233 (3) | |
H3 | 0.4403 | 0.5332 | 0.7289 | 0.028* | |
C4 | 0.46152 (11) | 0.6645 (2) | 0.59844 (14) | 0.0216 (3) | |
C5 | 0.40898 (11) | 0.7286 (2) | 0.48480 (14) | 0.0237 (3) | |
H5 | 0.4433 | 0.7837 | 0.4454 | 0.028* | |
C6 | 0.30805 (11) | 0.7133 (2) | 0.42875 (14) | 0.0233 (3) | |
H6 | 0.2741 | 0.7602 | 0.3527 | 0.028* | |
C7 | 0.10071 (11) | 0.7136 (2) | 0.49168 (14) | 0.0232 (3) | |
H72 | 0.1205 | 0.6556 | 0.5685 | 0.028* | |
H73 | 0.0290 | 0.7026 | 0.4497 | 0.028* | |
C8 | 0.11909 (11) | 0.4104 (2) | 0.42498 (14) | 0.0226 (3) | |
H81 | 0.0478 | 0.4009 | 0.3904 | 0.034* | |
H82 | 0.1455 | 0.3639 | 0.5044 | 0.034* | |
H83 | 0.1450 | 0.3368 | 0.3798 | 0.034* | |
C9 | 0.10507 (12) | 0.6747 (3) | 0.30206 (14) | 0.0285 (4) | |
H91 | 0.0338 | 0.6671 | 0.2703 | 0.043* | |
H92 | 0.1287 | 0.5960 | 0.2568 | 0.043* | |
H93 | 0.1245 | 0.8030 | 0.2987 | 0.043* | |
C10 | 0.61542 (12) | 0.5952 (3) | 0.76493 (16) | 0.0328 (4) | |
H101 | 0.6052 | 0.4614 | 0.7555 | 0.049* | |
H102 | 0.5930 | 0.6403 | 0.8219 | 0.049* | |
H103 | 0.6850 | 0.6226 | 0.7915 | 0.049* | |
C11 | 0.61399 (12) | 0.7603 (3) | 0.59259 (16) | 0.0292 (4) | |
H111 | 0.6829 | 0.7744 | 0.6457 | 0.044* | |
H112 | 0.5869 | 0.8810 | 0.5599 | 0.044* | |
H113 | 0.6081 | 0.6754 | 0.5302 | 0.044* | |
Cl2 | 0.13930 (3) | 0.37737 (6) | 0.70918 (3) | 0.02326 (11) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0342 (2) | 0.0226 (2) | 0.0516 (3) | 0.00034 (16) | 0.0153 (2) | −0.00322 (18) |
N1 | 0.0148 (5) | 0.0219 (6) | 0.0193 (6) | −0.0002 (5) | 0.0059 (4) | 0.0022 (5) |
N2 | 0.0160 (6) | 0.0309 (7) | 0.0293 (7) | −0.0019 (5) | 0.0046 (5) | −0.0022 (6) |
C1 | 0.0136 (6) | 0.0208 (7) | 0.0223 (7) | 0.0000 (5) | 0.0055 (5) | 0.0012 (5) |
C2 | 0.0191 (7) | 0.0227 (7) | 0.0216 (7) | 0.0000 (5) | 0.0083 (6) | 0.0011 (5) |
C3 | 0.0187 (7) | 0.0251 (8) | 0.0220 (7) | 0.0013 (6) | 0.0048 (6) | 0.0008 (6) |
C4 | 0.0162 (6) | 0.0192 (7) | 0.0272 (7) | −0.0006 (5) | 0.0070 (6) | −0.0023 (6) |
C5 | 0.0174 (7) | 0.0227 (7) | 0.0306 (8) | −0.0004 (5) | 0.0097 (6) | 0.0046 (6) |
C6 | 0.0187 (7) | 0.0241 (7) | 0.0248 (7) | 0.0005 (6) | 0.0071 (6) | 0.0065 (6) |
C7 | 0.0191 (7) | 0.0220 (7) | 0.0279 (8) | 0.0005 (6) | 0.0093 (6) | −0.0028 (6) |
C8 | 0.0213 (7) | 0.0213 (7) | 0.0232 (7) | −0.0037 (5) | 0.0076 (6) | −0.0041 (5) |
C9 | 0.0180 (7) | 0.0426 (10) | 0.0208 (7) | 0.0005 (7) | 0.0043 (6) | 0.0102 (7) |
C10 | 0.0199 (8) | 0.0352 (10) | 0.0332 (9) | 0.0005 (7) | 0.0013 (7) | 0.0002 (7) |
C11 | 0.0167 (7) | 0.0258 (8) | 0.0415 (10) | −0.0033 (6) | 0.0090 (7) | −0.0016 (7) |
Cl2 | 0.01681 (17) | 0.0308 (2) | 0.02126 (18) | 0.00192 (13) | 0.00712 (13) | 0.00527 (14) |
Cl1—C7 | 1.7532 (17) | C5—H5 | 0.9500 |
N1—C1 | 1.4995 (19) | C6—H6 | 0.9500 |
N1—C9 | 1.5027 (19) | C7—H72 | 0.9900 |
N1—C8 | 1.513 (2) | C7—H73 | 0.9900 |
N1—C7 | 1.518 (2) | C8—H81 | 0.9800 |
N2—C4 | 1.372 (2) | C8—H82 | 0.9800 |
N2—C11 | 1.452 (2) | C8—H83 | 0.9800 |
N2—C10 | 1.454 (2) | C9—H91 | 0.9800 |
C1—C6 | 1.380 (2) | C9—H92 | 0.9800 |
C1—C2 | 1.392 (2) | C9—H93 | 0.9800 |
C2—C3 | 1.386 (2) | C10—H101 | 0.9800 |
C2—H2 | 0.9500 | C10—H102 | 0.9800 |
C3—C4 | 1.416 (2) | C10—H103 | 0.9800 |
C3—H3 | 0.9500 | C11—H111 | 0.9800 |
C4—C5 | 1.407 (2) | C11—H112 | 0.9800 |
C5—C6 | 1.390 (2) | C11—H113 | 0.9800 |
C1—N1—C9 | 113.14 (12) | Cl1—C7—H72 | 109.1 |
C1—N1—C8 | 110.47 (12) | N1—C7—H73 | 109.1 |
C9—N1—C8 | 107.13 (12) | Cl1—C7—H73 | 109.1 |
C1—N1—C7 | 110.87 (12) | H72—C7—H73 | 107.9 |
C9—N1—C7 | 109.47 (12) | N1—C8—H81 | 109.5 |
C8—N1—C7 | 105.42 (11) | N1—C8—H82 | 109.5 |
C4—N2—C11 | 119.40 (14) | H81—C8—H82 | 109.5 |
C4—N2—C10 | 120.39 (14) | N1—C8—H83 | 109.5 |
C11—N2—C10 | 118.40 (14) | H81—C8—H83 | 109.5 |
C6—C1—C2 | 120.06 (14) | H82—C8—H83 | 109.5 |
C6—C1—N1 | 121.26 (13) | N1—C9—H91 | 109.5 |
C2—C1—N1 | 118.68 (13) | N1—C9—H92 | 109.5 |
C3—C2—C1 | 120.26 (14) | H91—C9—H92 | 109.5 |
C3—C2—H2 | 119.9 | N1—C9—H93 | 109.5 |
C1—C2—H2 | 119.9 | H91—C9—H93 | 109.5 |
C2—C3—C4 | 121.00 (14) | H92—C9—H93 | 109.5 |
C2—C3—H3 | 119.5 | N2—C10—H101 | 109.5 |
C4—C3—H3 | 119.5 | N2—C10—H102 | 109.5 |
N2—C4—C5 | 121.36 (14) | H101—C10—H102 | 109.5 |
N2—C4—C3 | 121.55 (14) | N2—C10—H103 | 109.5 |
C5—C4—C3 | 117.08 (14) | H101—C10—H103 | 109.5 |
C6—C5—C4 | 121.64 (14) | H102—C10—H103 | 109.5 |
C6—C5—H5 | 119.2 | N2—C11—H111 | 109.5 |
C4—C5—H5 | 119.2 | N2—C11—H112 | 109.5 |
C1—C6—C5 | 119.95 (14) | H111—C11—H112 | 109.5 |
C1—C6—H6 | 120.0 | N2—C11—H113 | 109.5 |
C5—C6—H6 | 120.0 | H111—C11—H113 | 109.5 |
N1—C7—Cl1 | 112.42 (11) | H112—C11—H113 | 109.5 |
N1—C7—H72 | 109.1 | ||
Cl1—C7—N1—C1 | 56.59 (14) | C5—C4—N2—C11 | −6.2 (2) |
C7—N1—C1—C2 | 61.05 (18) | C3—C4—N2—C10 | 10.5 (2) |
C6—C1—N1—C9 | 4.9 (2) |
References
Assenmacher, W. & Jansen, M. (1995). Z. Kristallogr. 210, 704–706. CrossRef CAS Web of Science Google Scholar
Bruker (2001a). SMART (Version 5.625) and SAINT (Version 6.02A). Bruker AXS, Madison, Wisconsin, USA. Google Scholar
Bruker (2001b). SHELXTL. Versions 5.10 & 6.12. Bruker AXS, Madison, Wisconsin, USA. Google Scholar
Collings, J. C., Batsanov, A. S. & Marder, T. B. (2004). Unpublished results. Google Scholar
Winter, R. (2001). PhD Thesis, Institut für Anorganische Chemie, University of Stuttgart, Germany. Cited from CCDC-175408, refcode XILVET. Google Scholar
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