Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807043139/ez2096sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807043139/ez2096Isup2.hkl |
CCDC reference: 663717
The title compound was bought from Shanghai Kuilin Chemical Co., Ltd. as the synthetic raw material. Crystals of (I) suitable for single-crystal X-ray analysis were grown by slow evaporation of a CH2Cl2 solution.
All H atoms were positioned geometrically and refined as riding with C—H = 0.95 and 0.98 Å. For the CH groups, Uiso(H) values are set equal to 1.2Ueq(carrier atom) and for the methyl groups they are set equal to 1.5Ueq(carrier atom). The H atoms of the methyl groups are disordered over two sites [both occupancies 0.50:0.50].
The derivatives of quinoline are of great significance as a result of their various bioactivities. For example, they can be used as antagonists, matrix metalloproteinase inhibitors and glucocorticoid mimetics (Geneste, et al. 2006; Beadle, et al., 2005; Schäfer, et al., 2003). In this paper we present the crystal structure of the title compound, 2,6-dimethylquinoline, (I).
The two methyl groups are coplanar with the quinoline ring, which is almost planar, with an r. m. s. derivation of 0.0111 (2) Å. The H atoms of the methyl groups are disordered 50:50 over two sites.
For related literature, see: Beadle et al. (2005); Geneste et al. (2006); Schäfer et al. (2003).
Data collection: CrystalClear (Molecular Structure Corporation & Rigaku, 1999); cell refinement: CrystalClear (Molecular Structure Corporation & Rigaku, 1999); data reduction: CrystalClear (Molecular Structure Corporation & Rigaku, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL (Bruker, 1997).
Fig. 1. View of a molecule of (I) showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 35% probability level. |
C11H11N | Dx = 1.224 Mg m−3 |
Mr = 157.21 | Melting point: 328 K |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71070 Å |
Hall symbol: P 2ac 2ab | Cell parameters from 2085 reflections |
a = 5.9497 (3) Å | θ = 3.0–25.0° |
b = 10.6987 (8) Å | µ = 0.07 mm−1 |
c = 13.4021 (12) Å | T = 113 K |
V = 853.10 (11) Å3 | Plate, colourless |
Z = 4 | 0.20 × 0.16 × 0.14 mm |
F(000) = 336 |
Rigaku Saturn diffractometer | 1202 independent reflections |
Radiation source: rotating anode | 1098 reflections with I > 2σ(I) |
Confocal monochromator | Rint = 0.048 |
Detector resolution: 7.31 pixels mm-1 | θmax = 27.9°, θmin = 2.4° |
ω scans | h = −7→7 |
Absorption correction: multi-scan (CrystalClear; Molecular Structure Corporation & Rigaku, 1999) | k = −14→14 |
Tmin = 0.986, Tmax = 0.990 | l = −17→17 |
10784 measured reflections |
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)] = 0.041 | H-atom parameters constrained |
wR(F2) = 0.102 | w = 1/[σ2(Fo2) + (0.0508P)2 + 0.0963P] where P = (Fo2 + 2Fc2)/3 |
S = 1.15 | (Δ/σ)max < 0.001 |
1202 reflections | Δρmax = 0.19 e Å−3 |
111 parameters | Δρmin = −0.14 e Å−3 |
0 restraints | Extinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.046 (7) |
C11H11N | V = 853.10 (11) Å3 |
Mr = 157.21 | Z = 4 |
Orthorhombic, P212121 | Mo Kα radiation |
a = 5.9497 (3) Å | µ = 0.07 mm−1 |
b = 10.6987 (8) Å | T = 113 K |
c = 13.4021 (12) Å | 0.20 × 0.16 × 0.14 mm |
Rigaku Saturn diffractometer | 1202 independent reflections |
Absorption correction: multi-scan (CrystalClear; Molecular Structure Corporation & Rigaku, 1999) | 1098 reflections with I > 2σ(I) |
Tmin = 0.986, Tmax = 0.990 | Rint = 0.048 |
10784 measured reflections |
R[F2 > 2σ(F2)] = 0.041 | 0 restraints |
wR(F2) = 0.102 | H-atom parameters constrained |
S = 1.15 | Δρmax = 0.19 e Å−3 |
1202 reflections | Δρmin = −0.14 e Å−3 |
111 parameters |
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 | Occ. (<1) | |
N1 | 1.0066 (2) | 0.52180 (13) | 0.07529 (10) | 0.0232 (4) | |
C1 | 0.9191 (3) | 0.46134 (15) | −0.00134 (13) | 0.0226 (4) | |
C2 | 0.7025 (3) | 0.48864 (16) | −0.04071 (13) | 0.0228 (4) | |
H2 | 0.6453 | 0.4420 | −0.0954 | 0.027* | |
C3 | 0.5771 (3) | 0.58242 (15) | 0.00067 (12) | 0.0216 (4) | |
H3 | 0.4325 | 0.6019 | −0.0251 | 0.026* | |
C4 | 0.6660 (3) | 0.65016 (15) | 0.08253 (12) | 0.0192 (4) | |
C5 | 0.8820 (3) | 0.61591 (15) | 0.11774 (12) | 0.0201 (4) | |
C6 | 0.9720 (3) | 0.68026 (16) | 0.20107 (13) | 0.0240 (4) | |
H6 | 1.1162 | 0.6582 | 0.2259 | 0.029* | |
C7 | 0.8528 (3) | 0.77392 (17) | 0.24591 (13) | 0.0258 (4) | |
H7 | 0.9168 | 0.8167 | 0.3011 | 0.031* | |
C8 | 0.6361 (3) | 0.80873 (15) | 0.21201 (13) | 0.0231 (4) | |
C9 | 0.5470 (3) | 0.74754 (15) | 0.13096 (12) | 0.0211 (4) | |
H9 | 0.4028 | 0.7710 | 0.1070 | 0.025* | |
C10 | 1.0594 (4) | 0.35966 (16) | −0.04720 (15) | 0.0314 (5) | |
H10A | 1.2025 | 0.3532 | −0.0113 | 0.047* | 0.50 |
H10B | 1.0884 | 0.3796 | −0.1174 | 0.047* | 0.50 |
H10C | 0.9789 | 0.2800 | −0.0428 | 0.047* | 0.50 |
H10D | 0.9774 | 0.3220 | −0.1030 | 0.047* | 0.50 |
H10E | 1.0914 | 0.2956 | 0.0031 | 0.047* | 0.50 |
H10F | 1.2010 | 0.3952 | −0.0716 | 0.047* | 0.50 |
C11 | 0.5081 (4) | 0.90984 (16) | 0.26553 (14) | 0.0306 (5) | |
H11A | 0.5989 | 0.9418 | 0.3209 | 0.046* | 0.50 |
H11B | 0.3671 | 0.8755 | 0.2915 | 0.046* | 0.50 |
H11C | 0.4749 | 0.9780 | 0.2190 | 0.046* | 0.50 |
H11D | 0.3617 | 0.9217 | 0.2334 | 0.046* | 0.50 |
H11E | 0.5935 | 0.9881 | 0.2627 | 0.046* | 0.50 |
H11F | 0.4857 | 0.8856 | 0.3353 | 0.046* | 0.50 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0235 (7) | 0.0234 (7) | 0.0227 (7) | 0.0014 (7) | 0.0019 (6) | 0.0027 (6) |
C1 | 0.0255 (9) | 0.0203 (8) | 0.0220 (8) | −0.0001 (7) | 0.0037 (7) | 0.0034 (7) |
C2 | 0.0262 (9) | 0.0208 (8) | 0.0213 (9) | −0.0043 (8) | 0.0002 (7) | 0.0000 (7) |
C3 | 0.0189 (8) | 0.0243 (8) | 0.0218 (8) | −0.0024 (7) | 0.0001 (7) | 0.0023 (7) |
C4 | 0.0199 (8) | 0.0193 (8) | 0.0185 (8) | −0.0021 (7) | 0.0019 (7) | 0.0029 (7) |
C5 | 0.0198 (8) | 0.0204 (8) | 0.0200 (8) | −0.0005 (7) | 0.0023 (7) | 0.0039 (7) |
C6 | 0.0211 (9) | 0.0305 (9) | 0.0205 (9) | −0.0022 (8) | −0.0020 (7) | 0.0027 (7) |
C7 | 0.0285 (10) | 0.0270 (9) | 0.0219 (9) | −0.0045 (8) | −0.0014 (8) | −0.0006 (7) |
C8 | 0.0278 (9) | 0.0202 (8) | 0.0213 (9) | −0.0017 (7) | 0.0048 (8) | 0.0014 (7) |
C9 | 0.0196 (8) | 0.0213 (8) | 0.0225 (8) | 0.0002 (7) | 0.0028 (7) | 0.0035 (7) |
C10 | 0.0348 (11) | 0.0266 (9) | 0.0327 (10) | 0.0047 (9) | 0.0031 (9) | −0.0022 (8) |
C11 | 0.0381 (10) | 0.0259 (9) | 0.0279 (10) | 0.0033 (9) | 0.0055 (8) | −0.0024 (7) |
N1—C1 | 1.321 (2) | C8—C9 | 1.375 (2) |
N1—C5 | 1.374 (2) | C8—C11 | 1.505 (2) |
C1—C2 | 1.423 (2) | C9—H9 | 0.9500 |
C1—C10 | 1.503 (2) | C10—H10A | 0.9800 |
C2—C3 | 1.368 (2) | C10—H10B | 0.9800 |
C2—H2 | 0.9500 | C10—H10C | 0.9800 |
C3—C4 | 1.417 (2) | C10—H10D | 0.9800 |
C3—H3 | 0.9500 | C10—H10E | 0.9800 |
C4—C9 | 1.417 (2) | C10—H10F | 0.9800 |
C4—C5 | 1.418 (2) | C11—H11A | 0.9800 |
C5—C6 | 1.417 (2) | C11—H11B | 0.9800 |
C6—C7 | 1.367 (2) | C11—H11C | 0.9800 |
C6—H6 | 0.9500 | C11—H11D | 0.9800 |
C7—C8 | 1.417 (3) | C11—H11E | 0.9800 |
C7—H7 | 0.9500 | C11—H11F | 0.9800 |
C1—N1—C5 | 117.92 (15) | H10A—C10—H10D | 141.1 |
N1—C1—C2 | 123.02 (16) | H10B—C10—H10D | 56.3 |
N1—C1—C10 | 116.98 (16) | H10C—C10—H10D | 56.3 |
C2—C1—C10 | 120.00 (17) | C1—C10—H10E | 109.5 |
C3—C2—C1 | 119.62 (17) | H10A—C10—H10E | 56.3 |
C3—C2—H2 | 120.2 | H10B—C10—H10E | 141.1 |
C1—C2—H2 | 120.2 | H10C—C10—H10E | 56.3 |
C2—C3—C4 | 119.05 (17) | H10D—C10—H10E | 109.5 |
C2—C3—H3 | 120.5 | C1—C10—H10F | 109.5 |
C4—C3—H3 | 120.5 | H10A—C10—H10F | 56.3 |
C9—C4—C3 | 122.98 (15) | H10B—C10—H10F | 56.3 |
C9—C4—C5 | 119.38 (15) | H10C—C10—H10F | 141.1 |
C3—C4—C5 | 117.63 (15) | H10D—C10—H10F | 109.5 |
N1—C5—C6 | 118.59 (16) | H10E—C10—H10F | 109.5 |
N1—C5—C4 | 122.76 (16) | C8—C11—H11A | 109.5 |
C6—C5—C4 | 118.65 (15) | C8—C11—H11B | 109.5 |
C7—C6—C5 | 120.43 (17) | H11A—C11—H11B | 109.5 |
C7—C6—H6 | 119.8 | C8—C11—H11C | 109.5 |
C5—C6—H6 | 119.8 | H11A—C11—H11C | 109.5 |
C6—C7—C8 | 121.59 (17) | H11B—C11—H11C | 109.5 |
C6—C7—H7 | 119.2 | C8—C11—H11D | 109.5 |
C8—C7—H7 | 119.2 | H11A—C11—H11D | 141.1 |
C9—C8—C7 | 118.64 (16) | H11B—C11—H11D | 56.3 |
C9—C8—C11 | 121.58 (17) | H11C—C11—H11D | 56.3 |
C7—C8—C11 | 119.77 (17) | C8—C11—H11E | 109.5 |
C8—C9—C4 | 121.29 (16) | H11A—C11—H11E | 56.3 |
C8—C9—H9 | 119.4 | H11B—C11—H11E | 141.1 |
C4—C9—H9 | 119.4 | H11C—C11—H11E | 56.3 |
C1—C10—H10A | 109.5 | H11D—C11—H11E | 109.5 |
C1—C10—H10B | 109.5 | C8—C11—H11F | 109.5 |
H10A—C10—H10B | 109.5 | H11A—C11—H11F | 56.3 |
C1—C10—H10C | 109.5 | H11B—C11—H11F | 56.3 |
H10A—C10—H10C | 109.5 | H11C—C11—H11F | 141.1 |
H10B—C10—H10C | 109.5 | H11D—C11—H11F | 109.5 |
C1—C10—H10D | 109.5 | H11E—C11—H11F | 109.5 |
C5—N1—C1—C2 | −0.6 (2) | C9—C4—C5—C6 | 0.3 (2) |
C5—N1—C1—C10 | 179.40 (14) | C3—C4—C5—C6 | −178.47 (15) |
N1—C1—C2—C3 | 0.8 (2) | N1—C5—C6—C7 | −179.55 (15) |
C10—C1—C2—C3 | −179.16 (15) | C4—C5—C6—C7 | −0.4 (2) |
C1—C2—C3—C4 | −0.3 (2) | C5—C6—C7—C8 | 0.8 (3) |
C2—C3—C4—C9 | −179.10 (15) | C6—C7—C8—C9 | −1.1 (3) |
C2—C3—C4—C5 | −0.4 (2) | C6—C7—C8—C11 | 178.20 (16) |
C1—N1—C5—C6 | 178.96 (15) | C7—C8—C9—C4 | 1.0 (2) |
C1—N1—C5—C4 | −0.2 (2) | C11—C8—C9—C4 | −178.31 (15) |
C9—C4—C5—N1 | 179.40 (14) | C3—C4—C9—C8 | 178.10 (15) |
C3—C4—C5—N1 | 0.6 (2) | C5—C4—C9—C8 | −0.6 (2) |
Experimental details
Crystal data | |
Chemical formula | C11H11N |
Mr | 157.21 |
Crystal system, space group | Orthorhombic, P212121 |
Temperature (K) | 113 |
a, b, c (Å) | 5.9497 (3), 10.6987 (8), 13.4021 (12) |
V (Å3) | 853.10 (11) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.07 |
Crystal size (mm) | 0.20 × 0.16 × 0.14 |
Data collection | |
Diffractometer | Rigaku Saturn |
Absorption correction | Multi-scan (CrystalClear; Molecular Structure Corporation & Rigaku, 1999) |
Tmin, Tmax | 0.986, 0.990 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 10784, 1202, 1098 |
Rint | 0.048 |
(sin θ/λ)max (Å−1) | 0.658 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.041, 0.102, 1.15 |
No. of reflections | 1202 |
No. of parameters | 111 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.19, −0.14 |
Computer programs: CrystalClear (Molecular Structure Corporation & Rigaku, 1999), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1997).
The derivatives of quinoline are of great significance as a result of their various bioactivities. For example, they can be used as antagonists, matrix metalloproteinase inhibitors and glucocorticoid mimetics (Geneste, et al. 2006; Beadle, et al., 2005; Schäfer, et al., 2003). In this paper we present the crystal structure of the title compound, 2,6-dimethylquinoline, (I).
The two methyl groups are coplanar with the quinoline ring, which is almost planar, with an r. m. s. derivation of 0.0111 (2) Å. The H atoms of the methyl groups are disordered 50:50 over two sites.