organic compounds
8-Quinolylguanidinium chloride
aDepartment of Chemistry of Huaiyin Teachers College, Jangsu Key Laboratory for the Chemistry of Low-Dimensional Materials, Huaian 223300, People's Republic of China
*Correspondence e-mail: weichangmei@sina.com
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 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
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Data collection: XSCANS (Bruker, 2000); cell 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.
Supporting information
10.1107/S1600536808013640/rz2213sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536808013640/rz2213Isup2.hkl
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.
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).
Data collection: XSCANS (Bruker, 2000); cell
XSCANS (Bruker, 2000); 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 (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).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). |
C10H11N4+·Cl− | Dx = 1.345 Mg m−3 |
Mr = 222.68 | Melting point = 533–534 K |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
a = 8.7410 (17) Å | Cell parameters from 25 reflections |
b = 9.0230 (18) Å | θ = 2.1–25.6° |
c = 13.942 (3) Å | µ = 0.32 mm−1 |
V = 1099.6 (4) Å3 | T = 293 K |
Z = 4 | Block, yellow |
F(000) = 464 | 0.20 × 0.20 × 0.20 mm |
Siemens P4 diffractometer | 2340 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.030 |
Graphite monochromator | θmax = 27.0°, θmin = 2.7° |
2θ/ω scans | h = −11→11 |
Absorption correction: multi-scan (XPREP in SHELXTL; Sheldrick, 2008) | k = −11→11 |
Tmin = 0.939, Tmax = 0.969 | l = −17→17 |
3398 measured reflections | 3 standard reflections every 97 reflections |
2398 independent reflections | intensity decay: 2.1% |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.062 | H-atom parameters constrained |
wR(F2) = 0.108 | w = 1/[σ2(Fo2) + (0.0513P)2 + 0.585P] where P = (Fo2 + 2Fc2)/3 |
S = 0.99 | (Δ/σ)max = 0.001 |
2398 reflections | Δρmax = 0.18 e Å−3 |
136 parameters | Δρmin = −0.28 e Å−3 |
0 restraints | Absolute structure: Flack (1983), 500 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.02 (10) |
C10H11N4+·Cl− | V = 1099.6 (4) Å3 |
Mr = 222.68 | Z = 4 |
Orthorhombic, P212121 | Mo Kα radiation |
a = 8.7410 (17) Å | µ = 0.32 mm−1 |
b = 9.0230 (18) Å | T = 293 K |
c = 13.942 (3) Å | 0.20 × 0.20 × 0.20 mm |
Siemens P4 diffractometer | 2340 reflections with I > 2σ(I) |
Absorption correction: multi-scan (XPREP in SHELXTL; Sheldrick, 2008) | Rint = 0.030 |
Tmin = 0.939, Tmax = 0.969 | 3 standard reflections every 97 reflections |
3398 measured reflections | intensity decay: 2.1% |
2398 independent reflections |
R[F2 > 2σ(F2)] = 0.062 | H-atom parameters constrained |
wR(F2) = 0.108 | Δρmax = 0.18 e Å−3 |
S = 0.99 | Δρmin = −0.28 e Å−3 |
2398 reflections | Absolute structure: Flack (1983), 500 Friedel pairs |
136 parameters | Absolute structure parameter: 0.02 (10) |
0 restraints |
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. |
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) |
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) |
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) |
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. |
Experimental details
Crystal data | |
Chemical formula | C10H11N4+·Cl− |
Mr | 222.68 |
Crystal system, space group | Orthorhombic, P212121 |
Temperature (K) | 293 |
a, b, c (Å) | 8.7410 (17), 9.0230 (18), 13.942 (3) |
V (Å3) | 1099.6 (4) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.32 |
Crystal size (mm) | 0.20 × 0.20 × 0.20 |
Data collection | |
Diffractometer | Siemens P4 diffractometer |
Absorption correction | Multi-scan (XPREP in SHELXTL; Sheldrick, 2008) |
Tmin, Tmax | 0.939, 0.969 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3398, 2398, 2340 |
Rint | 0.030 |
(sin θ/λ)max (Å−1) | 0.639 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.062, 0.108, 0.99 |
No. of reflections | 2398 |
No. of parameters | 136 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.18, −0.28 |
Absolute structure | Flack (1983), 500 Friedel pairs |
Absolute structure parameter | 0.02 (10) |
Computer programs: XSCANS (Bruker, 2000), SHELXTL (Sheldrick, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008).
N1—C10 | 1.324 (4) | C2—C3 | 1.410 (4) |
N1—C8 | 1.411 (4) | C3—C7 | 1.411 (4) |
N2—C10 | 1.263 (4) | C3—C4 | 1.420 (4) |
N3—C10 | 1.337 (4) | C4—C5 | 1.361 (4) |
N4—C6 | 1.293 (4) | C5—C6 | 1.406 (4) |
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) | ||
C10—N1—C8 | 125.4 (3) | 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) |
C1—C2—C3 | 121.1 (3) | C9—C8—N1 | 121.9 (3) |
C2—C3—C7 | 119.5 (3) | C9—C8—C7 | 119.7 (3) |
C2—C3—C4 | 123.1 (3) | N1—C8—C7 | 118.3 (3) |
C7—C3—C4 | 117.3 (3) | C8—C9—C1 | 122.0 (3) |
C5—C4—C3 | 118.7 (3) | N2—C10—N1 | 118.8 (3) |
C4—C5—C6 | 119.5 (3) | N2—C10—N3 | 119.5 (3) |
N4—C6—C5 | 120.6 (3) | N1—C10—N3 | 121.6 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···Cl1i | 0.86 | 2.34 | 3.171 (3) | 161.5 |
N2—H2A···Cl1i | 0.86 | 2.65 | 3.401 (3) | 146.3 |
N2—H2B···Cl1ii | 0.86 | 2.64 | 3.405 (3) | 148.6 |
N3—H3A···Cl1ii | 0.86 | 2.39 | 3.198 (3) | 157.6 |
N3—H3B···Cl1 | 0.86 | 2.46 | 3.269 (3) | 156.4 |
Symmetry codes: (i) −x+3/2, −y+2, z+1/2; (ii) −x+2, y+1/2, −z+3/2. |
Acknowledgements
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.
References
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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).