Abstract
The title compound, C10H11N4 +·Cl−, has been synthesized by the reaction of 8-aminoquinoline and cyanamide. The dihedral angle between the plane of the guanidine group and the quinoline ring system is 68.64 (13)°. The crystal structure is stabilized by intermolecular N—H⋯Cl hydrogen bonds.
Related literature
For related literature, see: Hughes & Liu (1976 ▶); Juyal & Anand (2003 ▶); Knhla et al. (1986 ▶); Orner & Hamilton (2001 ▶).
Experimental
Crystal data
C10H11N4 +·Cl−
M r = 222.68
Orthorhombic,
a = 8.7410 (17) Å
b = 9.0230 (18) Å
c = 13.942 (3) Å
V = 1099.6 (4) Å3
Z = 4
Mo Kα radiation
μ = 0.32 mm−1
T = 293 (2) K
0.20 × 0.20 × 0.20 mm
Data collection
Siemens P4 diffractometer
Absorption correction: multi-scan (XPREP in SHELXTL; Sheldrick, 2008 ▶) T min = 0.939, T max = 0.969
3398 measured reflections
2398 independent reflections
2340 reflections with I > 2σ(I)
R int = 0.0301
3 standard reflections every 97 reflections intensity decay: 2.1%
Refinement
R[F 2 > 2σ(F 2)] = 0.062
wR(F 2) = 0.108
S = 0.99
2398 reflections
136 parameters
H-atom parameters constrained
Δρmax = 0.17 e Å−3
Δρmin = −0.28 e Å−3
Absolute structure: Flack (1983 ▶), 500 Friedel pairs
Flack parameter: 0.02 (10)
Data collection: XSCANS (Bruker, 2000 ▶); cell refinement: XSCANS; data reduction: SHELXTL (Sheldrick, 2008 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808013640/rz2213sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808013640/rz2213Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1A⋯Cl1i | 0.86 | 2.34 | 3.171 (3) | 162 |
| N2—H2A⋯Cl1i | 0.86 | 2.65 | 3.401 (3) | 146 |
| N2—H2B⋯Cl1ii | 0.86 | 2.64 | 3.405 (3) | 149 |
| N3—H3A⋯Cl1ii | 0.86 | 2.39 | 3.198 (3) | 158 |
| N3—H3B⋯Cl1 | 0.86 | 2.46 | 3.269 (3) | 156 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The author is grateful to the Science Foundation of Jiangsu Education Bureau (05KJD 150039), the Professor Foundation of Huaiyin Teachers College (05 HSJS018) and the Science Foundation of Jangsu Key Laboratory for the Chemistry of Low-Dimensional Materials (JSKC 06028) for financial support.
supplementary crystallographic information
Comment
Guanidine is used in variety of supramolecular recognition processes across the spectrum of organic, biological and medicinal chemistry (Orner & Hamilton, 2001). Guanidine compounds containing a quinolyl ring are used as decongestive agents (Hughes & Liu, 1976) and in the treatment of gastrointestinal motility disorders (Knhla et al., 1986). Guanidine derivatives are also employed as inhibitors of the reactions responsible for sedimentation in fuels as they efficiently disperse the gum and sediments formed (Juyal & Anand, 2003). These important compounds are therefore of interest from a structural viewpoint. In this paper, we report the crystal structure of the title compound, (I), which, to our knowledge, represents the first structure containing the 8-quinolylguanidium cation. A perspective view of (I) is shown in Fig.1. In (I), bond lengths and angles within the 8-quinolylguanidium cation (Table 1) indicate a partial conjugation between the guanidine group and the quinoline ring. The dihedral angle formed by the plane of the guanidine group and the quinoline ring is 68.64 (13)°. In the crystal packing, The chloride anion interacts with the cations though N—H···Cl hydrogen bonds forming a three dimensions network (Fig. 2, Table 2).
Experimental
The title compound was synthesized as following. A mixture of 8-aminoquinoline (68.06 mmol), cyanamide (83.3 mmol) and ethanol (50 ml) was heated under reflux for 3 h with stirring. The reaction mixture was evaporated to give a residue. Singles crystals suitable for X-ray analysis were obtained by slow evaporation of an aqueous solution.
Refinement
All H atoms were placed in calculated positions with C—H = 0.93 Å, N—H = 0.86 Å, and refined as riding with Uiso(H) = 1.2 Ueq(C, N).
Figures
Fig. 1.
The molecular structure drawing for (I) showing 50% probability of displacement ellipsoids and the atom-numbering scheme.
Fig. 2.
The molecular packing diagram in the crystal for (I).
Crystal data
| C10H11N4+·Cl– | Dx = 1.345 Mg m−3 |
| Mr = 222.68 | Melting point = 533–534 K |
| Orthorhombic, P2(1)2(1)2(1) | Mo Kα radiation λ = 0.71073 Å |
| a = 8.7410 (17) Å | Cell parameters from 25 reflections |
| b = 9.0230 (18) Å | θ = 2.1–25.6º |
| c = 13.942 (3) Å | µ = 0.32 mm−1 |
| V = 1099.6 (4) Å3 | T = 293 (2) K |
| Z = 4 | Block, yellow |
| F000 = 464 | 0.20 × 0.20 × 0.20 mm |
Data collection
| Siemens P4 diffractometer | Rint = 0.030 |
| Radiation source: fine-focus sealed tube | θmax = 27.0º |
| Monochromator: graphite | θmin = 2.7º |
| T = 293(2) K | h = −11→11 |
| 2θ/ω scans | k = −11→11 |
| Absorption correction: multi-scan(XPREP in SHELXTL; Sheldrick, 2008) | l = −17→17 |
| Tmin = 0.939, Tmax = 0.969 | 3 standard reflections |
| 3398 measured reflections | every 97 reflections |
| 2398 independent reflections | intensity decay: 2.1% |
| 2340 reflections with I > 2σ(I) |
Refinement
| Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
| Least-squares matrix: full | H-atom parameters constrained |
| R[F2 > 2σ(F2)] = 0.062 | w = 1/[σ2(Fo2) + (0.0513P)2 + 0.585P] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.108 | (Δ/σ)max = 0.001 |
| S = 0.99 | Δρmax = 0.18 e Å−3 |
| 2398 reflections | Δρmin = −0.28 e Å−3 |
| 136 parameters | Extinction correction: none |
| Primary atom site location: structure-invariant direct methods | Absolute structure: Flack (1983), 500 Friedel pairs |
| Secondary atom site location: difference Fourier map | Flack parameter: 0.02 (10) |
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 | ||
| Cl1 | 0.87040 (9) | 0.86783 (8) | 0.66733 (5) | 0.04274 (19) | |
| N1 | 0.7592 (3) | 0.9935 (3) | 0.97479 (18) | 0.0385 (5) | |
| H1A | 0.7204 | 1.0096 | 1.0305 | 0.046* | |
| N2 | 0.8958 (3) | 1.1997 (3) | 0.99486 (19) | 0.0470 (6) | |
| H2A | 0.8569 | 1.2079 | 1.0513 | 0.056* | |
| H2B | 0.9600 | 1.2646 | 0.9745 | 0.056* | |
| N3 | 0.9244 (3) | 1.0767 (3) | 0.85594 (17) | 0.0424 (6) | |
| H3A | 0.9918 | 1.1397 | 0.8371 | 0.051* | |
| H3B | 0.8995 | 1.0037 | 0.8195 | 0.051* | |
| N4 | 0.4631 (3) | 0.9657 (3) | 0.90750 (19) | 0.0424 (6) | |
| C1 | 0.7557 (4) | 0.6150 (4) | 0.8683 (2) | 0.0451 (7) | |
| H1 | 0.8235 | 0.5370 | 0.8586 | 0.054* | |
| C2 | 0.6087 (3) | 0.6031 (3) | 0.8407 (2) | 0.0435 (7) | |
| H2 | 0.5741 | 0.5145 | 0.8144 | 0.052* | |
| C3 | 0.5062 (4) | 0.7226 (3) | 0.8511 (2) | 0.0437 (7) | |
| C4 | 0.3507 (4) | 0.7159 (3) | 0.8217 (2) | 0.0455 (7) | |
| H4A | 0.3118 | 0.6310 | 0.7929 | 0.055* | |
| C5 | 0.2599 (4) | 0.8362 (3) | 0.8366 (2) | 0.0479 (7) | |
| H5 | 0.1583 | 0.8351 | 0.8169 | 0.057* | |
| C6 | 0.3210 (4) | 0.9621 (4) | 0.8819 (2) | 0.0463 (7) | |
| H6 | 0.2585 | 1.0436 | 0.8936 | 0.056* | |
| C7 | 0.5564 (4) | 0.8547 (4) | 0.8952 (2) | 0.0426 (7) | |
| C8 | 0.7119 (3) | 0.8643 (4) | 0.92611 (19) | 0.0398 (6) | |
| C9 | 0.8061 (4) | 0.7491 (3) | 0.9126 (2) | 0.0434 (7) | |
| H9 | 0.9072 | 0.7566 | 0.9327 | 0.052* | |
| C10 | 0.8584 (3) | 1.0921 (3) | 0.9418 (2) | 0.0392 (6) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cl1 | 0.0583 (4) | 0.0381 (3) | 0.0318 (3) | 0.0130 (3) | −0.0029 (3) | 0.0014 (3) |
| N1 | 0.0418 (13) | 0.0343 (12) | 0.0395 (12) | −0.0066 (10) | −0.0012 (10) | −0.0012 (10) |
| N2 | 0.0490 (15) | 0.0475 (15) | 0.0445 (14) | −0.0093 (13) | 0.0009 (12) | −0.0055 (12) |
| N3 | 0.0438 (14) | 0.0413 (13) | 0.0420 (14) | −0.0112 (11) | 0.0029 (10) | −0.0047 (10) |
| N4 | 0.0424 (14) | 0.0408 (14) | 0.0440 (14) | −0.0057 (11) | −0.0028 (11) | 0.0004 (11) |
| C1 | 0.0506 (17) | 0.0380 (17) | 0.0468 (15) | −0.0019 (15) | 0.0020 (13) | −0.0019 (13) |
| C2 | 0.0483 (17) | 0.0376 (15) | 0.0446 (15) | −0.0059 (12) | 0.0004 (14) | −0.0005 (13) |
| C3 | 0.0496 (17) | 0.0398 (16) | 0.0418 (17) | −0.0083 (13) | 0.0030 (13) | −0.0009 (13) |
| C4 | 0.0478 (17) | 0.0423 (15) | 0.0464 (16) | −0.0071 (13) | −0.0045 (15) | 0.0004 (13) |
| C5 | 0.0498 (17) | 0.0454 (17) | 0.0485 (16) | −0.0079 (14) | −0.0006 (16) | 0.0026 (15) |
| C6 | 0.0493 (17) | 0.0444 (17) | 0.0452 (17) | −0.0024 (14) | 0.0000 (14) | −0.0008 (13) |
| C7 | 0.0456 (16) | 0.0396 (16) | 0.0426 (15) | −0.0060 (14) | 0.0010 (12) | 0.0002 (14) |
| C8 | 0.0455 (15) | 0.0357 (14) | 0.0382 (14) | −0.0090 (14) | −0.0028 (12) | 0.0011 (13) |
| C9 | 0.0460 (16) | 0.0379 (15) | 0.0462 (16) | −0.0013 (14) | 0.0020 (13) | −0.0006 (13) |
| C10 | 0.0387 (15) | 0.0367 (14) | 0.0423 (14) | −0.0079 (12) | −0.0001 (13) | −0.0009 (11) |
Geometric parameters (Å, °)
| N1—C10 | 1.324 (4) | C1—H1 | 0.9300 |
| N1—C8 | 1.411 (4) | C2—C3 | 1.410 (4) |
| N1—H1A | 0.8600 | C2—H2 | 0.9300 |
| N2—C10 | 1.263 (4) | C3—C7 | 1.411 (4) |
| N2—H2A | 0.8600 | C3—C4 | 1.420 (4) |
| N2—H2B | 0.8600 | C4—C5 | 1.361 (4) |
| N3—C10 | 1.337 (4) | C4—H4A | 0.9300 |
| N3—H3A | 0.8600 | C5—C6 | 1.406 (4) |
| N3—H3B | 0.8600 | C5—H5 | 0.9300 |
| N4—C6 | 1.293 (4) | C6—H6 | 0.9300 |
| N4—C7 | 1.303 (4) | C7—C8 | 1.429 (4) |
| C1—C2 | 1.345 (5) | C8—C9 | 1.339 (5) |
| C1—C9 | 1.429 (4) | C9—H9 | 0.9300 |
| C10—N1—C8 | 125.4 (3) | C5—C4—H4A | 120.6 |
| C10—N1—H1A | 117.3 | C3—C4—H4A | 120.6 |
| C8—N1—H1A | 117.3 | C4—C5—C6 | 119.5 (3) |
| C10—N2—H2A | 120.0 | C4—C5—H5 | 120.3 |
| C10—N2—H2B | 120.0 | C6—C5—H5 | 120.3 |
| H2A—N2—H2B | 120.0 | N4—C6—C5 | 120.6 (3) |
| C10—N3—H3A | 120.0 | N4—C6—H6 | 119.7 |
| C10—N3—H3B | 120.0 | C5—C6—H6 | 119.7 |
| H3A—N3—H3B | 120.0 | N4—C7—C3 | 120.8 (3) |
| C6—N4—C7 | 123.1 (3) | N4—C7—C8 | 120.6 (3) |
| C2—C1—C9 | 119.0 (3) | C3—C7—C8 | 118.6 (3) |
| C2—C1—H1 | 120.5 | C9—C8—N1 | 121.9 (3) |
| C9—C1—H1 | 120.5 | C9—C8—C7 | 119.7 (3) |
| C1—C2—C3 | 121.1 (3) | N1—C8—C7 | 118.3 (3) |
| C1—C2—H2 | 119.4 | C8—C9—C1 | 122.0 (3) |
| C3—C2—H2 | 119.4 | C8—C9—H9 | 119.0 |
| C2—C3—C7 | 119.5 (3) | C1—C9—H9 | 119.0 |
| C2—C3—C4 | 123.1 (3) | N2—C10—N1 | 118.8 (3) |
| C7—C3—C4 | 117.3 (3) | N2—C10—N3 | 119.5 (3) |
| C5—C4—C3 | 118.7 (3) | N1—C10—N3 | 121.6 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···Cl1i | 0.86 | 2.34 | 3.171 (3) | 162 |
| N2—H2A···Cl1i | 0.86 | 2.65 | 3.401 (3) | 146 |
| N2—H2B···Cl1ii | 0.86 | 2.64 | 3.405 (3) | 149 |
| N3—H3A···Cl1ii | 0.86 | 2.39 | 3.198 (3) | 158 |
| N3—H3B···Cl1 | 0.86 | 2.46 | 3.269 (3) | 156 |
Symmetry codes: (i) −x+3/2, −y+2, z+1/2; (ii) −x+2, y+1/2, −z+3/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2213).
References
- Bruker, (2000). XSCANS Bruker AXS Inc., Madison, Wisconsin, USA.
- Flack, H. D. (1983). Acta Cryst. A39, 876–881.
- Hughes, J. L. & Liu, R. C. H. (1976). US Patent No. 4 000 279.
- Juyal, P. & Anand, O. N. (2003). Fuel, 82, 97–103.
- Knhla, D. E., Studt, W. L., Campbell, H. F. & Yelnosky, J. (1986). US Patent No. 4 563 460.
- Orner, B. P. & Hamilton, A. D. (2001). J. Inclusion Phenom. Macrocycl. Chem.41, 141–147.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808013640/rz2213sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808013640/rz2213Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


