Literature DB >> 21580354

3-(1-Methyl-3-imidazolio)propane-sulfonate: a precursor to a Brønsted acid ionic liquid.

W Matthew Reichert, Paul C Trulove, Hugh C De Long.   

Abstract

The title compound, C(7)H(12)N(2)O(3)S, is a zwitterion precursor to a Brønsted acid ionic liquid with potential as an acid catalyst. The C-N-C-C torsion angle of 100.05 (8)° allows the positively charged imidazolium head group and the negatively charged sulfonate group to inter-act with neighboring zwitterions, forming a C-H⋯O hydrogen-bonding network; the shortest among these inter-actions is 2.9512 (9) Å. The C-H⋯O inter-actions can be described by graph-set notation as two R(2) (2)(16) and one R(2) (2)(5) hydrogen-bonded rings.

Entities:  

Year:  2010        PMID: 21580354      PMCID: PMC2983509          DOI: 10.1107/S1600536810004344

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


Related literature

For the use of functionalized ionic liquids (ILs) as Brønsted acid catalysts for organic reactions, see: Cole et al. (2002 ▶); Yoshizawa et al. (2001 ▶). The local structure of ILs is often conserved on transition from the solid state to the liquid state, see: Henderson et al. (2007 ▶); Reichert et al. (2007 ▶); Triolo et al. (2006 ▶). For a related structure, see: Pringle et al. (2003 ▶). For polymorphs of ionic liquids, see: Holbrey et al. (2003 ▶) and for the applications of ionic liquids, see: Plechkova & Seddon (2008 ▶).

Experimental

Crystal data

C7H12N2O3S M = 204.25 Monoclinic, a = 9.8164 (4) Å b = 11.7421 (5) Å c = 7.9769 (3) Å β = 94.878 (2)° V = 916.13 (6) Å3 Z = 4 Mo Kα radiation μ = 0.33 mm−1 T = 296 K 0.29 × 0.28 × 0.13 mm

Data collection

Bruker SMART CCD area-detector diffractometer Absorption correction: for a sphere (SADABS; Bruker, 2007 ▶) T min = 0.910, T max = 0.958 21327 measured reflections 8299 independent reflections 5726 reflections with I > 2σ(I) R int = 0.033

Refinement

R[F 2 > 2σ(F 2)] = 0.041 wR(F 2) = 0.120 S = 1.03 8299 reflections 166 parameters All H-atom parameters refined Δρmax = 0.55 e Å−3 Δρmin = −0.47 e Å−3 Data collection: SMART (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: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablocks I, New_Global_Publ_Block. DOI: 10.1107/S1600536810004344/kp2241sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810004344/kp2241Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C7H12N2O3SF(000) = 432
Mr = 204.25Dx = 1.481 Mg m3
Monoclinic, P21/cMelting point: 482 K
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 9.8164 (4) ÅCell parameters from 4851 reflections
b = 11.7421 (5) Åθ = 3.1–41.1°
c = 7.9769 (3) ŵ = 0.33 mm1
β = 94.878 (2)°T = 296 K
V = 916.13 (6) Å3Plate, colourless
Z = 40.29 × 0.28 × 0.13 mm
Bruker SMART CCD area-detector diffractometer8299 independent reflections
Radiation source: fine-focus sealed tube5726 reflections with I > 2σ(I)
graphiteRint = 0.033
phi and ω scansθmax = 47.1°, θmin = 3.1°
Absorption correction: for a sphere (SADABS; Bruker, 2007)h = −20→13
Tmin = 0.910, Tmax = 0.958k = −19→24
21327 measured reflectionsl = −16→16
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.041Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.120All H-atom parameters refined
S = 1.03w = 1/[σ2(Fo2) + (0.0574P)2 + 0.0483P] where P = (Fo2 + 2Fc2)/3
8299 reflections(Δ/σ)max = 0.002
166 parametersΔρmax = 0.55 e Å3
0 restraintsΔρmin = −0.47 e Å3
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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
S10.288447 (16)0.459431 (14)0.711035 (19)0.01929 (4)
O10.18103 (7)0.54452 (5)0.71911 (8)0.02993 (12)
O20.42331 (6)0.50523 (8)0.76230 (9)0.03616 (15)
O30.25705 (8)0.35528 (5)0.79823 (8)0.03407 (14)
N30.17238 (6)0.51000 (5)0.16133 (7)0.01989 (9)
N10.28516 (6)0.65793 (5)0.08981 (8)0.02208 (9)
C20.29151 (7)0.54584 (6)0.11322 (8)0.02096 (10)
H2A0.3704 (14)0.5037 (13)0.1080 (19)0.037 (3)*
C40.08588 (8)0.60254 (6)0.16753 (10)0.02580 (12)
H4A−0.0036 (14)0.5991 (11)0.2077 (16)0.034 (3)*
C50.15675 (8)0.69513 (7)0.12222 (11)0.02724 (13)
H5A0.1323 (14)0.7688 (12)0.1137 (17)0.037 (3)*
C60.39573 (9)0.72763 (8)0.03336 (12)0.03149 (15)
H6A0.3932 (15)0.8024 (14)0.0813 (19)0.044 (4)*
H6B0.4809 (19)0.6923 (15)0.063 (2)0.061 (5)*
H6C0.3820 (17)0.7417 (17)−0.081 (2)0.067 (5)*
C70.14604 (8)0.39419 (6)0.21968 (8)0.02303 (11)
H7A0.0552 (13)0.3717 (11)0.1696 (15)0.027 (3)*
H7B0.2156 (12)0.3490 (11)0.1741 (15)0.026 (3)*
C80.15267 (7)0.38976 (6)0.41105 (8)0.02112 (10)
H8A0.0853 (14)0.4389 (12)0.4510 (18)0.033 (3)*
H8B0.1301 (13)0.3105 (12)0.4405 (17)0.036 (3)*
C90.29159 (7)0.42456 (8)0.49418 (9)0.02574 (12)
H9A0.3243 (16)0.4859 (13)0.444 (2)0.043 (4)*
H9B0.3600 (16)0.3658 (13)0.4885 (18)0.043 (4)*
U11U22U33U12U13U23
S10.01791 (6)0.02075 (7)0.01894 (6)−0.00086 (5)0.00002 (4)0.00099 (4)
O10.0309 (3)0.0258 (2)0.0325 (3)0.0079 (2)−0.0007 (2)−0.00600 (19)
O20.0218 (2)0.0569 (4)0.0287 (3)−0.0109 (3)−0.0044 (2)−0.0016 (3)
O30.0510 (4)0.0231 (2)0.0281 (2)−0.0029 (2)0.0032 (2)0.00664 (19)
N30.0201 (2)0.01929 (19)0.02006 (19)0.00022 (16)0.00055 (16)−0.00017 (15)
N10.0208 (2)0.0222 (2)0.0233 (2)−0.00089 (18)0.00185 (17)0.00077 (17)
C20.0201 (2)0.0225 (2)0.0204 (2)0.00164 (19)0.00209 (18)0.00037 (18)
C40.0200 (3)0.0237 (3)0.0339 (3)0.0023 (2)0.0034 (2)0.0011 (2)
C50.0245 (3)0.0214 (3)0.0361 (3)0.0030 (2)0.0042 (2)0.0014 (2)
C60.0295 (4)0.0310 (3)0.0347 (4)−0.0069 (3)0.0068 (3)0.0048 (3)
C70.0289 (3)0.0190 (2)0.0207 (2)−0.0029 (2)−0.0008 (2)−0.00147 (18)
C80.0208 (2)0.0220 (2)0.0204 (2)−0.00162 (19)0.00092 (18)−0.00033 (18)
C90.0180 (2)0.0392 (4)0.0200 (2)0.0002 (2)0.00188 (18)−0.0015 (2)
S1—O31.4529 (6)C5—H5A0.899 (14)
S1—O21.4550 (6)C6—H6A0.959 (16)
S1—O11.4580 (6)C6—H6B0.945 (19)
S1—C91.7805 (7)C6—H6C0.924 (19)
N3—C21.3298 (9)C7—C81.5233 (9)
N3—C41.3825 (9)C7—H7A0.982 (13)
N3—C71.4673 (9)C7—H7B0.961 (12)
N1—C21.3301 (9)C8—C91.5207 (10)
N1—C51.3791 (10)C8—H8A0.952 (14)
N1—C61.4607 (10)C8—H8B0.990 (14)
C2—H2A0.923 (14)C9—H9A0.898 (16)
C4—C51.3562 (11)C9—H9B0.967 (16)
C4—H4A0.961 (14)
O3—S1—O2113.68 (5)H6A—C6—H6B110.8 (14)
O3—S1—O1111.84 (4)N1—C6—H6C110.7 (11)
O2—S1—O1112.24 (5)H6A—C6—H6C102.9 (15)
O3—S1—C9107.06 (4)H6B—C6—H6C112.0 (15)
O2—S1—C9105.52 (4)N3—C7—C8110.85 (5)
O1—S1—C9105.84 (4)N3—C7—H7A107.3 (7)
C2—N3—C4108.62 (6)C8—C7—H7A111.0 (7)
C2—N3—C7124.60 (6)N3—C7—H7B104.0 (7)
C4—N3—C7126.28 (6)C8—C7—H7B112.9 (7)
C2—N1—C5108.65 (6)H7A—C7—H7B110.4 (10)
C2—N1—C6124.78 (7)C9—C8—C7112.84 (6)
C5—N1—C6126.54 (7)C9—C8—H8A108.3 (8)
N3—C2—N1108.77 (6)C7—C8—H8A110.0 (8)
N3—C2—H2A127.3 (9)C9—C8—H8B111.1 (8)
N1—C2—H2A123.6 (9)C7—C8—H8B106.2 (8)
C5—C4—N3106.86 (7)H8A—C8—H8B108.4 (11)
C5—C4—H4A128.8 (8)C8—C9—S1113.36 (5)
N3—C4—H4A124.1 (8)C8—C9—H9A111.2 (10)
C4—C5—N1107.09 (7)S1—C9—H9A106.8 (10)
C4—C5—H5A130.7 (9)C8—C9—H9B112.9 (9)
N1—C5—H5A122.2 (9)S1—C9—H9B106.2 (9)
N1—C6—H6A110.2 (9)H9A—C9—H9B105.9 (13)
N1—C6—H6B110.1 (11)
C2—N3—C7—C8100.05 (8)C4—N3—C7—C8−70.97 (8)
N3—C7—C8—C9−60.48 (8)N3—C7—C8—C9−60.48 (8)
C7—C8—C9—S1163.00 (5)
D—H···AD—HH···AD···AD—H···A
C2—H2A···O2i0.923 (14)2.197 (14)2.9512 (9)138.4 (12)
C5—H5A···O1ii0.899 (14)2.381 (15)3.1573 (10)144.6 (12)
C4—H4A···O1iii0.961 (14)2.528 (14)3.3268 (11)140.5 (11)
C4—H4A···O3iii0.961 (14)2.541 (14)3.4364 (11)155.0 (11)
C7—H7B···O3iv0.961 (12)2.613 (12)3.1693 (10)117.2 (9)
C8—H8B···O3iv0.990 (14)2.621 (13)3.2086 (9)118.1 (9)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C2—H2A⋯O2i0.923 (14)2.197 (14)2.9512 (9)138.4 (12)
C5—H5A⋯O1ii0.899 (14)2.381 (15)3.1573 (10)144.6 (12)
C4—H4A⋯O1iii0.961 (14)2.528 (14)3.3268 (11)140.5 (11)
C4—H4A⋯O3iii0.961 (14)2.541 (14)3.4364 (11)155.0 (11)
C7—H7B⋯O3iv0.961 (12)2.613 (12)3.1693 (10)117.2 (9)
C8—H8B⋯O3iv0.990 (14)2.621 (13)3.2086 (9)118.1 (9)

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

  4 in total

1.  Applications of ionic liquids in the chemical industry.

Authors:  Natalia V Plechkova; Kenneth R Seddon
Journal:  Chem Soc Rev       Date:  2007-11-30       Impact factor: 54.564

2.  A short history of SHELX.

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

3.  Thermodynamics, structure, and dynamics in room temperature ionic liquids: the case of 1-butyl-3-methyl imidazolium hexafluorophosphate ([bmim][PF6]).

Authors:  Alessandro Triolo; Andrea Mandanici; Olga Russina; Virginia Rodriguez-Mora; Maria Cutroni; Christopher Hardacre; Mark Nieuwenhuyzen; Hans-Jurgen Bleif; Lukas Keller; Miguel Angel Ramos
Journal:  J Phys Chem B       Date:  2006-10-26       Impact factor: 2.991

4.  Novel Brønsted acidic ionic liquids and their use as dual solvent-catalysts.

Authors:  Amanda C Cole; Jessica L Jensen; Ioanna Ntai; Kim Loan T Tran; Kristin J Weaver; David C Forbes; James H Davis
Journal:  J Am Chem Soc       Date:  2002-05-29       Impact factor: 15.419

  4 in total
  2 in total

1.  1-(5,5-Di-meth-oxy-pent-yl)-3-methyl-imidazolium-2-carboxyl-ate.

Authors:  Olaf Walter
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2013-10-05

2.  Tuning anhydrous proton conduction in single-ion polymers by crystalline ion channels.

Authors:  Onnuri Kim; Kyoungwook Kim; U Hyeok Choi; Moon Jeong Park
Journal:  Nat Commun       Date:  2018-11-28       Impact factor: 14.919

  2 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.