Literature DB >> 21201968

1-Methyl-1-propyl-pyrrolidinium chloride.

Pamela M Dean1, Jennifer M Pringle, Douglas R Macfarlane.   

Abstract

The aymmetric unit of the title compound, C(8)H(18)N(+)·Cl(-), consists of one crystallographically independent 1-methyl-1-propyl-pyrrolidinium cation and one chloride anion, both of which lie in general positions. Minor hydrogen-bonded C-H⋯Cl inter-actions occur. However, no classical hydrogen bonding is observed.

Entities:  

Year:  2008        PMID: 21201968      PMCID: PMC2960766          DOI: 10.1107/S1600536808005229

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For bond-length data, see: Allen et al. (1987 ▶). For comparative thermal and crystallographic analysis of four crystallized N-alkyl-N-methyl­pyrrolidinium and piperidinium bis­(trifluoro­methane­sulfon­yl)imide salts and an insight into why these salts form room-temperature ionic liquids, see: Henderson et al. (2006 ▶). For the synthesis and analysis of N-butyl-N-methyl pyrrolidinium chloride, an analogue of the title compound, see: Lancaster et al. (2002 ▶). For the first synthesis and analysis of the new pyrrolidinium family of molten salts, see: MacFarlane et al. (1999 ▶). For the quanti­tative comparison of inter­molecular inter­actions using Hirshfeld surfaces, see: McKinnon et al. (2007 ▶). For the first synthesis and analysis of 1-alkyl-2-methyl pyrrolidinium ionic liquids involving the bis­(trifluoro­methane­sulfon­yl)imide anion, see: Sun et al. (2003 ▶).

Experimental

Crystal data

C8H18N+·Cl− M = 163.68 Orthorhombic, a = 14.5863 (5) Å b = 13.2196 (4) Å c = 9.9779 (3) Å V = 1923.99 (11) Å3 Z = 8 Mo Kα radiation μ = 0.33 mm−1 T = 123 (2) K 0.30 × 0.30 × 0.30 mm

Data collection

Bruker Kappa APEXII diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2005 ▶) T min = 0.907, T max = 0.907 11550 measured reflections 1982 independent reflections 1800 reflections with I > 2σ(I) R int = 0.030

Refinement

R[F 2 > 2σ(F 2)] = 0.031 wR(F 2) = 0.079 S = 1.04 1982 reflections 93 parameters H-atom parameters constrained Δρmax = 0.25 e Å−3 Δρmin = −0.20 e Å−3 Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: APEX2; data reduction: APEX2; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: POV-RAY (Persistence of Vision, 2003 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808005229/zl2101sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808005229/zl2101Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C8H18N+·ClDx = 1.130 Mg m3
Mr = 163.68Melting point: 323.5 K
Orthorhombic, PbcnMo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2n 2abCell parameters from 4825 reflections
a = 14.5863 (5) Åθ = 2.8–26.4º
b = 13.2196 (4) ŵ = 0.33 mm1
c = 9.9779 (3) ÅT = 123 (2) K
V = 1923.99 (11) Å3Cubic, colourless
Z = 80.30 × 0.30 × 0.30 mm
F000 = 720
Bruker X8 APEX KappaCCD diffractometer1982 independent reflections
Radiation source: fine-focus sealed tube1800 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.030
T = 123(2) Kθmax = 26.4º
0.5° frames in φ and ω scansθmin = 2.1º
Absorption correction: multi-scan(SADABS; Bruker, 2005)h = −18→18
Tmin = 0.907, Tmax = 0.907k = −15→16
11550 measured reflectionsl = −11→12
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.031H-atom parameters constrained
wR(F2) = 0.079  w = 1/[σ2(Fo2) + (0.0361P)2 + 0.834P] where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.001
1982 reflectionsΔρmax = 0.25 e Å3
93 parametersΔρmin = −0.20 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
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.
xyzUiso*/Ueq
Cl10.36024 (2)0.82436 (2)0.05218 (3)0.02423 (12)
N10.32912 (7)0.86923 (8)0.43497 (10)0.0179 (2)
C10.35707 (9)0.75928 (10)0.41992 (14)0.0241 (3)
H1A0.39390.74960.33760.029*
H1B0.30230.71520.41520.029*
C20.41390 (11)0.73488 (12)0.54424 (15)0.0323 (3)
H2A0.47930.72680.52020.039*
H2B0.39220.67140.58630.039*
C30.40131 (10)0.82444 (12)0.64053 (15)0.0309 (3)
H3A0.38840.80040.73260.037*
H3B0.45690.86740.64230.037*
C40.32014 (9)0.88251 (11)0.58455 (13)0.0242 (3)
H4A0.26160.85400.61740.029*
H4B0.32340.95490.60970.029*
C50.40372 (8)0.93610 (10)0.38042 (13)0.0209 (3)
H5A0.40450.93150.28240.031*
H5B0.46310.91410.41610.031*
H5C0.39221.00630.40720.031*
C60.23958 (8)0.88722 (10)0.36358 (13)0.0198 (3)
H6A0.19410.83740.39620.024*
H6B0.24870.87500.26660.024*
C70.20062 (9)0.99281 (11)0.38223 (14)0.0254 (3)
H7A0.19311.00730.47890.031*
H7B0.24331.04340.34420.031*
C80.10858 (10)0.99984 (12)0.31221 (18)0.0372 (4)
H8A0.11730.99260.21530.056*
H8B0.08061.06570.33130.056*
H8C0.06830.94580.34470.056*
U11U22U33U12U13U23
Cl10.02343 (18)0.02619 (19)0.02308 (18)−0.00399 (13)−0.00151 (13)−0.00178 (12)
N10.0162 (5)0.0191 (5)0.0185 (5)−0.0015 (4)−0.0013 (4)0.0004 (4)
C10.0246 (7)0.0178 (6)0.0299 (7)0.0005 (5)−0.0008 (6)0.0012 (5)
C20.0282 (7)0.0287 (8)0.0401 (9)0.0006 (6)−0.0051 (6)0.0123 (6)
C30.0273 (7)0.0406 (9)0.0247 (7)−0.0068 (6)−0.0067 (6)0.0100 (6)
C40.0232 (6)0.0322 (8)0.0172 (6)−0.0044 (6)−0.0004 (5)−0.0005 (5)
C50.0163 (6)0.0223 (7)0.0241 (6)−0.0031 (5)0.0008 (5)0.0023 (5)
C60.0157 (6)0.0231 (6)0.0206 (6)−0.0019 (5)−0.0035 (5)−0.0014 (5)
C70.0208 (6)0.0257 (7)0.0298 (7)0.0018 (5)−0.0037 (6)−0.0049 (6)
C80.0258 (7)0.0314 (8)0.0543 (10)0.0050 (6)−0.0138 (7)−0.0065 (7)
N1—C51.5038 (16)C4—H4B0.9900
N1—C61.5066 (16)C5—H5A0.9800
N1—C41.5085 (16)C5—H5B0.9800
N1—C11.5171 (17)C5—H5C0.9800
C1—C21.526 (2)C6—C71.5185 (18)
C1—H1A0.9900C6—H6A0.9900
C1—H1B0.9900C6—H6B0.9900
C2—C31.536 (2)C7—C81.5163 (19)
C2—H2A0.9900C7—H7A0.9900
C2—H2B0.9900C7—H7B0.9900
C3—C41.518 (2)C8—H8A0.9800
C3—H3A0.9900C8—H8B0.9800
C3—H3B0.9900C8—H8C0.9800
C4—H4A0.9900
C5—N1—C6111.31 (10)N1—C4—H4B111.0
C5—N1—C4110.64 (10)C3—C4—H4B111.0
C6—N1—C4111.98 (10)H4A—C4—H4B109.0
C5—N1—C1109.44 (10)N1—C5—H5A109.5
C6—N1—C1109.72 (10)N1—C5—H5B109.5
C4—N1—C1103.46 (10)H5A—C5—H5B109.5
N1—C1—C2105.54 (11)N1—C5—H5C109.5
N1—C1—H1A110.6H5A—C5—H5C109.5
C2—C1—H1A110.6H5B—C5—H5C109.5
N1—C1—H1B110.6N1—C6—C7114.30 (10)
C2—C1—H1B110.6N1—C6—H6A108.7
H1A—C1—H1B108.8C7—C6—H6A108.7
C1—C2—C3106.30 (12)N1—C6—H6B108.7
C1—C2—H2A110.5C7—C6—H6B108.7
C3—C2—H2A110.5H6A—C6—H6B107.6
C1—C2—H2B110.5C8—C7—C6109.34 (11)
C3—C2—H2B110.5C8—C7—H7A109.8
H2A—C2—H2B108.7C6—C7—H7A109.8
C4—C3—C2104.66 (11)C8—C7—H7B109.8
C4—C3—H3A110.8C6—C7—H7B109.8
C2—C3—H3A110.8H7A—C7—H7B108.3
C4—C3—H3B110.8C7—C8—H8A109.5
C2—C3—H3B110.8C7—C8—H8B109.5
H3A—C3—H3B108.9H8A—C8—H8B109.5
N1—C4—C3103.74 (11)C7—C8—H8C109.5
N1—C4—H4A111.0H8A—C8—H8C109.5
C3—C4—H4A111.0H8B—C8—H8C109.5
C5—N1—C1—C285.97 (12)C1—N1—C4—C340.98 (12)
C6—N1—C1—C2−151.63 (11)C2—C3—C4—N1−33.99 (14)
C4—N1—C1—C2−31.99 (13)C5—N1—C6—C7−63.82 (14)
N1—C1—C2—C310.96 (15)C4—N1—C6—C760.62 (14)
C1—C2—C3—C414.09 (15)C1—N1—C6—C7174.90 (11)
C5—N1—C4—C3−76.14 (13)N1—C6—C7—C8−177.02 (12)
C6—N1—C4—C3159.05 (10)
D—H···AD—HH···AD···AD—H···A
C1—H1B···Cl1i0.992.793.607 (1)141
C2—H2A···Cl1ii0.992.773.630 (2)146
C5—H5A···Cl10.982.773.648 (1)149
C5—H5C···Cl1iii0.982.713.656 (1)163
C6—H6A···Cl1i0.992.763.672 (1)153
C6—H6B···Cl10.992.773.666 (1)151
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C1—H1B⋯Cl1i0.992.793.607 (1)141
C2—H2A⋯Cl1ii0.992.773.630 (2)146
C5—H5A⋯Cl10.982.773.648 (1)149
C5—H5C⋯Cl1iii0.982.713.656 (1)163
C6—H6A⋯Cl1i0.992.763.672 (1)153
C6—H6B⋯Cl10.992.773.666 (1)151

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

  3 in total

1.  Nucleophilicity in ionic liquids. 2.(1) Cation effects on halide nucleophilicity in a series of bis(trifluoromethylsulfonyl)imide ionic liquids.

Authors:  N Llewellyn Lancaster; Paul A Salter; Tom Welton T; G Brent Young
Journal:  J Org Chem       Date:  2002-12-13       Impact factor: 4.354

2.  Towards quantitative analysis of intermolecular interactions with Hirshfeld surfaces.

Authors:  Joshua J McKinnon; Dylan Jayatilaka; Mark A Spackman
Journal:  Chem Commun (Camb)       Date:  2007-10-07       Impact factor: 6.222

3.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

  3 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.