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The title compound, C16H15N3, shows a hindrance effect between adjacent amino and methyl groups that leads to a structural distortion, which is reflected in the non-planarity of the quinoline entity and in the bond angles and distances. The crystal packing consists of chains along the b axis sustained by an inter­molecular hydrogen bond between the amino group and the N atom of the pyridyl ring.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270107006221/gd3088sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270107006221/gd3088Isup2.hkl
Contains datablock I

CCDC reference: 645574

Computing details top

Data collection: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1993); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: TEXSAN (Molecular Structure Corporation, 1999); program(s) used to solve structure: SHELXTL-Plus (Bruker, 1999); program(s) used to refine structure: SHELXTL-Plus; molecular graphics: MaterialStudio (Accelrys, 2002); software used to prepare material for publication: SHELXTL-Plus.

4,6-Dimethyl-2-(3-pyridyl)quinolin-5-amine top
Crystal data top
C16H15N3F(000) = 528
Mr = 249.31Dx = 1.300 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 21 reflections
a = 9.397 (3) Åθ = 20–26°
b = 18.314 (2) ŵ = 0.08 mm1
c = 7.399 (4) ÅT = 298 K
V = 1273.4 (8) Å3Irregular block, colourless
Z = 40.54 × 0.48 × 0.40 mm
Data collection top
Rigaku AFC-7S
diffractometer
1138 reflections with I > 2σ(I)
Radiation source: normal-focus sealed tubeRint = 0.041
Graphite monochromatorθmax = 25.0°, θmin = 2.2°
ω–2θ scansh = 111
Absorption correction: ψ scan
(North et al., 1968)
k = 121
Tmin = 0.949, Tmax = 0.972l = 08
1447 measured reflections3 standard reflections every 150 reflections
1309 independent reflections intensity decay: none
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.038H-atom parameters constrained
wR(F2) = 0.103 w = 1/[σ2(Fo2) + (0.0607P)2 + 0.1555P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max < 0.001
1309 reflectionsΔρmax = 0.15 e Å3
173 parametersΔρmin = 0.15 e Å3
0 restraintsExtinction correction: SHELXTL-Plus, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.025 (4)
Special details top

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) top
xyzUiso*/Ueq
N10.9153 (2)0.42667 (11)0.0123 (3)0.0399 (5)
N21.1038 (3)0.67413 (12)0.1028 (4)0.0644 (8)
H2A1.17610.70270.09420.077*
H2B1.02740.68900.15520.077*
N30.6600 (3)0.25546 (12)0.1636 (4)0.0592 (7)
C10.7888 (3)0.44510 (13)0.0762 (3)0.0398 (6)
C20.7521 (3)0.51823 (13)0.1114 (4)0.0435 (6)
H2C0.65970.52930.14700.052*
C30.8495 (3)0.57342 (13)0.0944 (3)0.0419 (6)
C40.9910 (3)0.55483 (13)0.0414 (3)0.0374 (6)
C51.1104 (3)0.60344 (13)0.0317 (4)0.0436 (6)
C61.2355 (3)0.58178 (14)0.0514 (4)0.0459 (7)
C71.2492 (3)0.50951 (15)0.1124 (4)0.0489 (7)
H71.33230.49550.17110.059*
C81.1442 (3)0.45955 (13)0.0880 (4)0.0452 (7)
H81.15850.41140.12320.054*
C91.0140 (3)0.48030 (13)0.0097 (3)0.0380 (6)
C111.3600 (3)0.63368 (16)0.0729 (5)0.0677 (9)
H11B1.33010.67570.14050.102*
H11C1.39150.64990.04390.102*
H11A1.43860.61170.13540.102*
C100.7974 (3)0.65075 (13)0.1239 (4)0.0534 (7)
H10A0.80210.66350.24960.080*
H10B0.85610.68420.05730.080*
H10C0.70090.65360.08190.080*
C120.6869 (3)0.38412 (13)0.1032 (3)0.0410 (6)
C130.7389 (3)0.31504 (14)0.1437 (4)0.0477 (7)
H130.83680.31010.15800.057*
C140.5195 (3)0.26343 (17)0.1370 (5)0.0599 (8)
H140.46190.22220.14430.072*
C150.4568 (3)0.32930 (17)0.0997 (5)0.0574 (8)
H150.35870.33260.08510.069*
C160.5405 (3)0.39026 (16)0.0842 (4)0.0530 (7)
H160.49940.43550.06100.064*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0417 (11)0.0367 (10)0.0412 (11)0.0014 (10)0.0007 (10)0.0008 (9)
N20.0633 (15)0.0413 (12)0.088 (2)0.0072 (12)0.0088 (17)0.0187 (13)
N30.0554 (15)0.0513 (13)0.0710 (18)0.0064 (13)0.0036 (14)0.0093 (13)
C10.0413 (14)0.0429 (13)0.0352 (13)0.0033 (12)0.0002 (12)0.0004 (11)
C20.0434 (13)0.0439 (14)0.0433 (14)0.0083 (13)0.0049 (13)0.0004 (12)
C30.0533 (15)0.0385 (12)0.0340 (13)0.0103 (12)0.0013 (13)0.0006 (11)
C40.0419 (13)0.0374 (12)0.0329 (11)0.0046 (11)0.0024 (11)0.0002 (10)
C50.0513 (15)0.0385 (13)0.0409 (14)0.0007 (13)0.0043 (13)0.0009 (11)
C60.0452 (14)0.0484 (15)0.0442 (14)0.0051 (13)0.0030 (13)0.0018 (12)
C70.0454 (13)0.0540 (16)0.0473 (15)0.0029 (13)0.0108 (14)0.0032 (14)
C80.0443 (14)0.0417 (14)0.0497 (16)0.0037 (12)0.0058 (14)0.0050 (12)
C90.0435 (14)0.0369 (12)0.0337 (12)0.0051 (11)0.0010 (11)0.0005 (11)
C110.0627 (18)0.0664 (19)0.074 (2)0.0154 (17)0.0111 (19)0.0096 (18)
C100.0583 (17)0.0433 (14)0.0587 (17)0.0113 (13)0.0038 (16)0.0032 (13)
C120.0422 (13)0.0440 (14)0.0366 (13)0.0002 (12)0.0007 (13)0.0006 (12)
C130.0436 (14)0.0455 (15)0.0540 (16)0.0002 (13)0.0009 (14)0.0060 (13)
C140.0526 (18)0.0601 (18)0.067 (2)0.0143 (16)0.0022 (17)0.0069 (16)
C150.0369 (14)0.0679 (19)0.0675 (19)0.0047 (14)0.0022 (15)0.0064 (17)
C160.0468 (15)0.0540 (16)0.0582 (17)0.0075 (14)0.0012 (15)0.0022 (15)
Geometric parameters (Å, º) top
N1—C11.323 (3)C2—H2C0.9300
C1—C21.407 (3)C6—C111.516 (4)
C2—C31.369 (4)C7—H70.9300
C3—C41.427 (4)C8—H80.9300
C4—C51.434 (4)C11—H11B0.9600
C5—C61.385 (4)C11—H11C0.9600
C6—C71.404 (4)C11—H11A0.9600
C7—C81.357 (4)C10—H10A0.9600
C8—C91.406 (3)C10—H10B0.9600
C9—N11.361 (3)C10—H10C0.9600
C4—C91.433 (3)C12—C161.387 (4)
C1—C121.485 (3)C12—C131.389 (3)
C3—C101.514 (3)C13—H130.9300
C5—N21.399 (3)C14—C151.371 (4)
N2—H2A0.8600C14—H140.9300
N2—H2B0.8600C15—C161.371 (4)
N3—C131.327 (3)C15—H150.9300
N3—C141.343 (4)C16—H160.9300
C1—N1—C9118.1 (2)N1—C9—C4123.6 (2)
C5—N2—H2A120.0C8—C9—C4119.8 (2)
C5—N2—H2B120.0C6—C11—H11B109.4
H2A—N2—H2B120.0C6—C11—H11C109.7
C13—N3—C14116.3 (3)H11B—C11—H11C108.2
N1—C1—C2121.9 (2)C6—C11—H11A112.4
N1—C1—C12115.8 (2)H11B—C11—H11A108.1
C2—C1—C12122.2 (2)H11C—C11—H11A109.1
C3—C2—C1121.4 (2)C3—C10—H10A110.6
C3—C2—H2C119.3C3—C10—H10B109.7
C1—C2—H2C119.3H10A—C10—H10B108.4
C2—C3—C4118.2 (2)C3—C10—H10C108.0
C2—C3—C10117.4 (2)H10A—C10—H10C110.1
C4—C3—C10124.3 (2)H10B—C10—H10C110.1
C3—C4—C9116.1 (2)C16—C12—C13116.4 (3)
C3—C4—C5126.5 (2)C16—C12—C1124.4 (2)
C9—C4—C5117.4 (2)C13—C12—C1119.2 (2)
C6—C5—N2118.0 (2)N3—C13—C12125.2 (3)
C6—C5—C4120.6 (2)N3—C13—H13117.4
N2—C5—C4121.4 (2)C12—C13—H13117.4
C5—C6—C7119.3 (2)N3—C14—C15123.2 (3)
C5—C6—C11121.5 (2)N3—C14—H14118.4
C7—C6—C11119.1 (2)C15—C14—H14118.4
C8—C7—C6121.8 (3)C14—C15—C16119.1 (3)
C8—C7—H7119.1C14—C15—H15120.4
C6—C7—H7119.1C16—C15—H15120.4
C7—C8—C9120.3 (2)C15—C16—C12119.6 (3)
C7—C8—H8119.8C15—C16—H16120.2
C9—C8—H8119.8C12—C16—H16120.2
N1—C9—C8116.6 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C10—H10B···N20.962.362.915 (4)116
N2—H2A···N3i0.862.553.183 (4)131
C7—H7···CgAii0.932.743.405 (4)129
C10—H10A···CgBiii0.962.913.838 (4)162
Symmetry codes: (i) x+2, y+1/2, z1/2; (ii) x+5/2, y+1, z+1/2; (iii) x+3/2, y+1, z1/2.
 

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