Abstract
The title molecular salt, C6H16N+·CH3SO3 −, has been determined at 150 K. Two diisopropylammonium cations (dipH) and two anions form N—H⋯O hydrogen-bonded cyclic dimers lying around centers of symmetry. Only two of the three O atoms of the methanesulfonate anion are involved in hydrogen bonding, resulting in slightly longer S—O bond lengths. The title structure represents an example of a sulfonate anion that is part of a hydrogen-bonding R 4 4(12) graph-set motif, which is well known for related dipH acetates. Additionally, the Raman and the IR spectroscopic data for the title compound are presented.
Related literature
For simple dipH salts, see: Bajorat & Reiss (2007 ▶); Reiss (1998 ▶, 2002 ▶); Reiss (2010a
▶,b
▶); Reiss & Engel (2004 ▶); Reiss & Meyer (2010 ▶); Sada et al. (2004 ▶), Summers et al. (1998 ▶). For spectroscopic data for sulfonate salts, see: Thomson (1972 ▶); Genceli Guner et al. (2010 ▶). For graph-set analysis, see: Etter et al. (1990 ▶).
Experimental
Crystal data
C6H16N+·CH3SO3 −
M r = 197.29
Monoclinic,
a = 8.88154 (13) Å
b = 8.53537 (13) Å
c = 14.5784 (2) Å
β = 101.8161 (15)°
V = 1081.73 (3) Å3
Z = 4
Mo Kα radiation
μ = 0.27 mm−1
T = 150 K
0.65 × 0.25 × 0.10 mm
Data collection
Oxford Diffraction Xcalibur Eos diffractometer
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009 ▶) T min = 0.951, T max = 1.000
25064 measured reflections
3149 independent reflections
2782 reflections with I > 2σ(I)
R int = 0.024
Refinement
R[F 2 > 2σ(F 2)] = 0.027
wR(F 2) = 0.060
S = 1.03
3149 reflections
146 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.34 e Å−3
Δρmin = −0.32 e Å−3
Data collection: CrysAlis PRO (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg, 2010 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811029382/qm2018sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811029382/qm2018Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811029382/qm2018Isup3.mol
Supplementary material file. DOI: 10.1107/S1600536811029382/qm2018Isup4.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected geometric parameters (Å, °).
| S1—O2 | 1.4433 (9) |
| S1—O1 | 1.4596 (8) |
| S1—O3 | 1.4600 (8) |
| S1—C1 | 1.7560 (12) |
Table 2. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H11⋯O1 | 0.885 (13) | 1.944 (13) | 2.8168 (11) | 168.5 (12) |
| N1—H12⋯O3i | 0.891 (13) | 1.919 (13) | 2.7944 (11) | 166.9 (12) |
Symmetry code: (i)
.
Acknowledgments
We thank E. Hammes for technical support.
supplementary crystallographic information
Comment
More than one hundred structures are listed to date in the Cambridge Crystallographic Database, which include a diisopropylammonium cation (dipH). In most cases the dipH cation is the counter cation of bigger anionic species e.g. anionic complexes and clusters. A limited number of structures are reported that are solely constructed by small classical anions and the dipH cation. In these cases the structure type is strongly dependent on the geometry and the ability of these anions to form hydrogen bonds. The structures reported so far range from a quasi-molecular (dipH)2[SiF6] (Reiss, 1998), over cyclic dimers for some acetates (e.g.: Sada et al., 2004) and e.g. a substituted phosphate (Summers et al., 1998), to one-dimensional polymers for the halogenides and some pseudo-halogenides (literature cited in Reiss & Meyer, 2010). Even a two-dimensional hydrogen bonded network for the (dipH)2SO4 (Reiss & Engel, 2004) and three-dimensional networks for dipH[IrCl6] (Reiss, 2002) and (dipH)2[CdCl4] (Reiss, 2010a) have been reported. The asymmetric unit of the title compound, which crystallizes in the centrosymmetric space group P21/n, consists of one formular unit. The structure is composed of centrosymmetric, hydrogen bonded, cyclic dimers which are composed of two dipH cations and two methanesulfonate anions arranged as rings (Fig. 1). The graph set (Etter et al., 1990) for these hydrogen bonded dimers is R44(12). All N–C, C–C, S–O, and S–C bond lengths are generally within the expected range. The two S–O bond lengths of the oxygen atoms involved in hydrogen bonding (O1 and O3) are longer than the third one which is in accord to our anticipation (Table 1). The N–H···O hydrogen bonds with donor-acceptor distances close to 2.79–2.82 Å (Table 2) are in the range of medium strong hydrogen bonds. The R44(12) hydrogen bonding motif is well known for dipH acetates (Reiss & Meyer, 2010, Sada et al. 2004). Combinations of the dipH cation with structurally similar anions like [NO3]– (Reiss, 2010b), [ClO4]- (Bajorat & Reiss, 2007) and various substituted carboxylate anions can be described as the generalized synthon: {dipH}+{O2XRy}- (X = C, Cl, N; y = 1,2, R = O, C). The title structure is a further example with this supramolecular synthon and the typical cyclic dimer.
Experimental
Diisopropylammonium methanesulfonate, ((CH3)2CH)2NH2[CH3SO3] was prepared by the reaction of 0.72 g (7.12 mmol) diisopropylamine and 1.48 g (15.40 mmol) methanesulfonic acid at room temperature. From colourless solution small block-shaped crystals were obtained within a few days. A Raman spectrum was measured using a Bruker MULTIRAM spectrometer; Nd:YAG-Laser at 1064 nm; RT-InGaAS-detector; 4000–70 cm-1: 3022(sh), 2986(ν(C–H), s), 2944(ν(C–H), vs), 2784(ν(N–H), w), 1462 (δ(C–H, m), 1429(δ(C–H, m), 1350(w), 1315(w), 1227(w), 1183(w), 1158(w), 1099 (w), 1044 (ν(S–O),vs), 958 (w), 914(w), 808(s), 778(ν(C–S), s), 558(δ(S–O), s), 528(m), 470(m), 392(w), 348(ρ(S–O), br), 83(m). IR data collected on a Digilab FT3400 spectrometer using a MIRacle ATR unit (Pike Technologies); 4000–560 cm-1: 3019(ν(C–H), s), 2988 (sh), 2941(m), 2870(ν(C–H), s), 2781(ν(N–H), m), 2514(m), 1625(w), 1601(w), 1483(δ(C–H, m), 1416(w), 1397(m), 1331(w), 1314(w), 1206(vs), 1177(sh), 1153(νs(S–O), vs), 1100(m), 1040(νa(S–O), vs), 977(w), 954(w), 837(w), 805(w), 776(ν(C–S), s), 551(δ(S–O)s). Band assignments for Raman and IR spectroscopic data were made by comparing results of earlier work done on sodium- and caesium methanesulfonate (Thomson, 1972), magnesium sulfonate (Genceli Guner et al., 2010) and dipHCl (Reiss & Meyer 2010).
Refinement
A single-crystal suitable for structure determination was harvested from the mother liquor and directly transferred into the cooling stream of an Oxford-Xcalibur diffractometer equipped with an EOS-CCD detector. Data collection was performed at 150 K. All hydrogen atoms were located via difference Fourier synthesis. Positional parameters of hydrogen atoms of the NH2 and the CH group were refined freely. All hydrogen atoms belonging to methyl groups were refined using a riding model with restrained angles and C–H distances but allowed to rotate about the C–C bond. Anisotrope displacement parameters of all non hydrogen atoms and individual isotropic displacement parameters for all hydrogen atoms were refined freely.
Figures
Fig. 1.
Hydrogen atoms are drawn with an arbitrary radius and the displacement ellipsoids are shown at the 50% probability level; ' = 1 - x,-y,-z.
Crystal data
| C6H16N+·CH3SO3− | F(000) = 432 |
| Mr = 197.29 | Dx = 1.211 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 18202 reflections |
| a = 8.88154 (13) Å | θ = 3.4–32.0° |
| b = 8.53537 (13) Å | µ = 0.27 mm−1 |
| c = 14.5784 (2) Å | T = 150 K |
| β = 101.8161 (15)° | Needle, colourless |
| V = 1081.73 (3) Å3 | 0.65 × 0.25 × 0.10 mm |
| Z = 4 |
Data collection
| Oxford Diffraction Xcalibur Eos diffractometer | 3149 independent reflections |
| Radiation source: fine-focus sealed tube | 2782 reflections with I > 2σ(I) |
| graphite | Rint = 0.024 |
| Detector resolution: 16.27 pixels mm-1 | θmax = 30.0°, θmin = 4.1° |
| ω scans | h = −12→12 |
| Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) | k = −12→12 |
| Tmin = 0.951, Tmax = 1.000 | l = −20→20 |
| 25064 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.027 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.060 | w = 1/[σ2(Fo2) + (0.01P)2 + 0.55P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.03 | (Δ/σ)max < 0.001 |
| 3149 reflections | Δρmax = 0.34 e Å−3 |
| 146 parameters | Δρmin = −0.32 e Å−3 |
| 0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0276 (9) |
Special details
| Experimental. CrysAlisPro, Oxford Diffraction Ltd., Version 1.171.33.52, Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK. |
| 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 | ||
| S1 | 0.38147 (3) | 0.02594 (3) | 0.180331 (16) | 0.01976 (7) | |
| O1 | 0.47025 (9) | 0.13813 (10) | 0.13749 (6) | 0.0355 (2) | |
| O2 | 0.47472 (10) | −0.09928 (12) | 0.22849 (6) | 0.0408 (2) | |
| O3 | 0.24712 (9) | −0.03058 (10) | 0.11340 (5) | 0.02989 (17) | |
| C1 | 0.30699 (15) | 0.12931 (19) | 0.26524 (9) | 0.0442 (3) | |
| H1A | 0.2477 | 0.0595 | 0.2955 | 0.065 (5)* | |
| H1B | 0.2424 | 0.2128 | 0.2357 | 0.062 (5)* | |
| H1C | 0.3901 | 0.1721 | 0.3109 | 0.066 (5)* | |
| N1 | 0.74609 (9) | 0.09843 (10) | 0.07323 (6) | 0.01840 (16) | |
| H11 | 0.6562 (15) | 0.0976 (15) | 0.0906 (9) | 0.028 (3)* | |
| H12 | 0.7329 (14) | 0.0729 (15) | 0.0128 (9) | 0.028 (3)* | |
| C2 | 0.84677 (11) | −0.02552 (12) | 0.12848 (7) | 0.02104 (18) | |
| H2 | 0.9413 (14) | −0.0236 (14) | 0.1056 (8) | 0.022 (3)* | |
| C3 | 0.76690 (13) | −0.18212 (12) | 0.10422 (8) | 0.0283 (2) | |
| H3A | 0.6709 | −0.1827 | 0.1248 | 0.036 (4)* | |
| H3B | 0.8313 | −0.2649 | 0.1349 | 0.039 (4)* | |
| H3C | 0.7480 | −0.1977 | 0.0376 | 0.037 (4)* | |
| C4 | 0.87442 (13) | 0.00990 (14) | 0.23269 (7) | 0.0286 (2) | |
| H4A | 0.9296 | 0.1069 | 0.2452 | 0.036 (4)* | |
| H4B | 0.9337 | −0.0731 | 0.2670 | 0.037 (4)* | |
| H4C | 0.7775 | 0.0183 | 0.2517 | 0.037 (4)* | |
| C5 | 0.80229 (12) | 0.26542 (12) | 0.08130 (7) | 0.02175 (19) | |
| H5 | 0.8146 (13) | 0.2921 (14) | 0.1445 (8) | 0.022 (3)* | |
| C6 | 0.67707 (14) | 0.36632 (13) | 0.02325 (8) | 0.0322 (2) | |
| H6A | 0.6606 | 0.3347 | −0.0412 | 0.041 (4)* | |
| H6B | 0.7081 | 0.4742 | 0.0286 | 0.049 (4)* | |
| H6C | 0.5834 | 0.3538 | 0.0457 | 0.041 (4)* | |
| C7 | 0.95364 (13) | 0.27936 (14) | 0.04905 (8) | 0.0296 (2) | |
| H7A | 1.0290 | 0.2129 | 0.0868 | 0.041 (4)* | |
| H7B | 0.9884 | 0.3861 | 0.0553 | 0.042 (4)* | |
| H7C | 0.9393 | 0.2479 | −0.0154 | 0.036 (4)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.01698 (10) | 0.02503 (12) | 0.01773 (10) | 0.00188 (9) | 0.00463 (8) | −0.00071 (9) |
| O1 | 0.0289 (4) | 0.0331 (4) | 0.0485 (5) | −0.0013 (3) | 0.0171 (4) | 0.0074 (4) |
| O2 | 0.0310 (4) | 0.0471 (5) | 0.0445 (5) | 0.0131 (4) | 0.0083 (4) | 0.0205 (4) |
| O3 | 0.0267 (4) | 0.0403 (4) | 0.0216 (3) | −0.0034 (3) | 0.0022 (3) | −0.0084 (3) |
| C1 | 0.0305 (6) | 0.0663 (9) | 0.0370 (6) | −0.0021 (6) | 0.0101 (5) | −0.0286 (7) |
| N1 | 0.0188 (4) | 0.0194 (4) | 0.0171 (4) | −0.0008 (3) | 0.0040 (3) | −0.0005 (3) |
| C2 | 0.0193 (4) | 0.0209 (4) | 0.0238 (4) | 0.0026 (4) | 0.0064 (3) | 0.0024 (4) |
| C3 | 0.0306 (5) | 0.0205 (5) | 0.0350 (6) | −0.0003 (4) | 0.0096 (4) | 0.0007 (4) |
| C4 | 0.0295 (5) | 0.0322 (6) | 0.0223 (5) | 0.0020 (4) | 0.0009 (4) | 0.0043 (4) |
| C5 | 0.0269 (5) | 0.0187 (4) | 0.0196 (4) | −0.0025 (4) | 0.0045 (4) | −0.0015 (3) |
| C6 | 0.0368 (6) | 0.0235 (5) | 0.0360 (6) | 0.0049 (4) | 0.0067 (5) | 0.0058 (4) |
| C7 | 0.0278 (5) | 0.0295 (6) | 0.0317 (5) | −0.0080 (4) | 0.0066 (4) | 0.0030 (4) |
Geometric parameters (Å, °)
| S1—O2 | 1.4433 (9) | C3—H3B | 0.9600 |
| S1—O1 | 1.4596 (8) | C3—H3C | 0.9600 |
| S1—O3 | 1.4600 (8) | C4—H4A | 0.9600 |
| S1—C1 | 1.7560 (12) | C4—H4B | 0.9600 |
| C1—H1A | 0.9600 | C4—H4C | 0.9600 |
| C1—H1B | 0.9600 | C5—C6 | 1.5196 (15) |
| C1—H1C | 0.9600 | C5—C7 | 1.5169 (14) |
| N1—C5 | 1.5068 (13) | C5—H5 | 0.934 (12) |
| N1—C2 | 1.5076 (12) | C6—H6A | 0.9600 |
| N1—H11 | 0.885 (13) | C6—H6B | 0.9600 |
| N1—H12 | 0.891 (13) | C6—H6C | 0.9600 |
| C2—C4 | 1.5189 (14) | C7—H7A | 0.9600 |
| C2—C3 | 1.5206 (14) | C7—H7B | 0.9600 |
| C2—H2 | 0.964 (12) | C7—H7C | 0.9600 |
| C3—H3A | 0.9600 | ||
| O2—S1—O1 | 112.80 (5) | N1—C2—C4 | 110.58 (8) |
| O2—S1—O3 | 112.92 (6) | N1—C2—C3 | 107.17 (8) |
| O1—S1—O3 | 111.71 (5) | C4—C2—C3 | 112.32 (9) |
| O2—S1—C1 | 106.90 (7) | N1—C2—H2 | 105.4 (7) |
| O1—S1—C1 | 106.65 (7) | C4—C2—H2 | 111.6 (7) |
| O3—S1—C1 | 105.24 (5) | C3—C2—H2 | 109.4 (7) |
| C5—N1—C2 | 118.12 (8) | N1—C5—C6 | 107.44 (8) |
| C5—N1—H11 | 106.8 (9) | N1—C5—C7 | 110.51 (8) |
| C2—N1—H11 | 108.2 (8) | C6—C5—C7 | 112.14 (9) |
| C5—N1—H12 | 106.4 (8) | N1—C5—H5 | 106.1 (8) |
| C2—N1—H12 | 107.5 (8) | C6—C5—H5 | 109.6 (7) |
| H11—N1—H12 | 109.6 (11) | C7—C5—H5 | 110.8 (7) |
| C5—N1—C2—C4 | 59.81 (11) | C2—N1—C5—C6 | −177.19 (8) |
| C5—N1—C2—C3 | −177.47 (8) | C2—N1—C5—C7 | 60.18 (11) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H11···O1 | 0.885 (13) | 1.944 (13) | 2.8168 (11) | 168.5 (12) |
| N1—H12···O3i | 0.891 (13) | 1.919 (13) | 2.7944 (11) | 166.9 (12) |
Symmetry codes: (i) −x+1, −y, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: QM2018).
References
- Bajorat, S. & Reiss, G. J. (2007). Acta Cryst. E63, o3144. [DOI] [PMC free article] [PubMed]
- Brandenburg, K. (2010). DIAMOND Crystal Impact GbR, Bonn, Germany.
- Etter, M. C., MacDonald, J. C. & Bernstein, J. (1990). Acta Cryst. B46, 256–262. [DOI] [PubMed]
- Genceli Guner, F. E., Martin Lutz, M., Sakurai, T., Spek, A. L. & Hondoh, T. (2010). Cryst. Growth Des. 10, 4327–4333.
- Oxford Diffraction (2009). CrysAlis PRO. Oxford Diffraction Ltd, Yarnton, England.
- Reiß, G. J. (1998). Acta Cryst. C54, 1489–1491.
- Reiß, G. J. (2002). Acta Cryst. E58, m47–m50.
- Reiss, G. J. (2010a). Private communication (deposition number: CCDC 771423). CCDC, Cambridge, England.
- Reiss, G. J. (2010b). Private communication (deposition number: CCDC 790195). CCDC, Cambridge, England.
- Reiß, G. J. & Engel, J. S. (2004). Acta Cryst. E60, o985–o987.
- Reiss, G. J. & Meyer, M. K. (2010). Z. Naturforsch. B, 65, 479–484.
- Sada, K., Watanabe, T., Miyamoto, J., Fukuda, T., Tohnai, N., Miyata, M., Kitayama, T., Maehara, K. & Ute, K. (2004). Chem. Lett. 33, 160–162.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Summers, J. S., Roe, D., Boyle, P. D., Colvin, M. & Ramsay Shaw, B. (1998). Inorg. Chem. 37, 4158–4159. [DOI] [PubMed]
- Thomson, W. K. (1972). Spectrochim. Acta Part A, 28, 1479–1484.
- Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
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/S1600536811029382/qm2018sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811029382/qm2018Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811029382/qm2018Isup3.mol
Supplementary material file. DOI: 10.1107/S1600536811029382/qm2018Isup4.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

