supplementary materials


Acta Cryst. (2009). E65, o2104    [ doi:10.1107/S1600536809030542 ]

(E)-3-Dimethylamino-1-(4-pyridyl)prop-2-en-1-one

L. Ni, G.-W. Zhu and H. Wei

Abstract top

The title compound, C10H12N2O, is approximately planar, the r.m.s. deviation of the non-H atoms from the mean plane being 0.099 Å.

Comment top

As part of our ongoing studies of heteroaromatic compounds (Ni et al., 2009), we now report the synthesis and structure of the title compound, (I).

As shown in Fig. 1, non-hydrogen atoms including the pyridine ring, N,N-Dimethylamino, and prop-2-en-1-one are coplanar with the r.m.s deviation of the fitted atoms being 0.099 Å.

Related literature top

For an isomer of the title compound with the same space group and similar unit-cell parameters, see: Ni et al. (2009).

Experimental top

A mixture of 4-acetylpyridine(10 mmol) and N,N-dimethylformamide-dimethyl acetal(40 ml) was refluxed for four hours. After concentration invacuo, recrystallization of the orange residue from ethanol afforded yellow blocks of (I). Anal. Calc. for C10H12N2O: C 68.10, H 6.81, N 15.89%; Found: C 68.05, H 6.69, N 15.81%.

Refinement top

All H atoms were geometrically positioned (C—H = 0.93–0.97Å) and refined as riding with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C).

Computing details top

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT-Plus (Bruker, 2004); data reduction: SAINT-Plus (Bruker, 2004); 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: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), drawn with 30% probability displacement ellipsoids for the non-hydrogen atoms.
(E)-3-Dimethylamino-1-(4-pyridyl)prop-2-en-1-one top
Crystal data top
C10H12N2OF(000) = 376
Mr = 176.22Dx = 1.217 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 1784 reflections
a = 5.6300 (11) Åθ = 1.8–25.5°
b = 22.850 (5) ŵ = 0.08 mm1
c = 7.8400 (16) ÅT = 294 K
β = 107.57 (3)°Block, yellow
V = 961.5 (3) Å30.12 × 0.10 × 0.08 mm
Z = 4
Data collection top
Bruker APEXII CCD
diffractometer
1784 independent reflections
Radiation source: fine-focus sealed tube1503 reflections with I > 2σ(I)
graphiteRint = 0.022
φ and ω scansθmax = 25.5°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Bruker, 2004)
h = 66
Tmin = 0.990, Tmax = 0.994k = 2726
5177 measured reflectionsl = 79
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)] = 0.040H-atom parameters not refined
wR(F2) = 0.137 w = 1/[σ2(Fo2) + (0.092P)2 + 0.1151P]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max = 0.001
1784 reflectionsΔρmax = 0.20 e Å3
121 parametersΔρmin = 0.12 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.016 (6)
Crystal data top
C10H12N2OV = 961.5 (3) Å3
Mr = 176.22Z = 4
Monoclinic, P21/nMo Kα radiation
a = 5.6300 (11) ŵ = 0.08 mm1
b = 22.850 (5) ÅT = 294 K
c = 7.8400 (16) Å0.12 × 0.10 × 0.08 mm
β = 107.57 (3)°
Data collection top
Bruker APEXII CCD
diffractometer
1784 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2004)
1503 reflections with I > 2σ(I)
Tmin = 0.990, Tmax = 0.994Rint = 0.022
5177 measured reflectionsθmax = 25.5°
Refinement top
R[F2 > 2σ(F2)] = 0.040H-atom parameters not refined
wR(F2) = 0.137Δρmax = 0.20 e Å3
S = 1.00Δρmin = 0.12 e Å3
1784 reflectionsAbsolute structure: ?
121 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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
C10.8254 (2)0.15312 (5)0.68372 (16)0.0403 (3)
C20.6652 (3)0.20055 (6)0.65592 (17)0.0451 (4)
H20.54900.20360.71830.054*
C30.6795 (3)0.24329 (7)0.5346 (2)0.0541 (4)
H30.56980.27470.51800.065*
C40.9907 (3)0.19670 (8)0.4672 (2)0.0634 (5)
H41.10400.19470.40220.076*
C50.9919 (3)0.15168 (7)0.5851 (2)0.0533 (4)
H51.10340.12080.59800.064*
C60.8303 (2)0.10391 (6)0.81421 (18)0.0441 (4)
C70.6972 (2)0.11110 (6)0.94016 (18)0.0452 (4)
H70.60120.14440.93770.054*
C80.7118 (3)0.06832 (6)1.06560 (18)0.0453 (4)
H80.81470.03671.06320.054*
C90.4227 (3)0.11224 (8)1.2011 (2)0.0668 (5)
H9A0.50850.14901.22710.100*
H9B0.35190.10281.29480.100*
H9C0.29240.11501.08940.100*
C100.6374 (3)0.01980 (7)1.3199 (2)0.0641 (5)
H10A0.75050.00831.29660.096*
H10B0.48150.00111.31120.096*
H10C0.70690.03551.43800.096*
N10.8397 (3)0.24245 (6)0.44017 (18)0.0617 (4)
N20.5966 (2)0.06690 (5)1.18924 (16)0.0494 (4)
O10.9520 (2)0.05981 (5)0.80351 (16)0.0677 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0414 (7)0.0407 (7)0.0388 (7)0.0052 (5)0.0120 (5)0.0024 (5)
C20.0477 (7)0.0453 (8)0.0433 (7)0.0010 (6)0.0153 (6)0.0018 (6)
C30.0581 (9)0.0476 (8)0.0541 (9)0.0035 (6)0.0131 (7)0.0068 (6)
C40.0583 (9)0.0715 (11)0.0699 (10)0.0001 (8)0.0337 (8)0.0178 (8)
C50.0500 (8)0.0541 (9)0.0623 (9)0.0035 (6)0.0268 (7)0.0092 (7)
C60.0480 (7)0.0410 (7)0.0460 (7)0.0005 (5)0.0184 (6)0.0004 (6)
C70.0498 (7)0.0429 (7)0.0467 (7)0.0020 (6)0.0202 (6)0.0009 (5)
C80.0499 (8)0.0442 (8)0.0460 (8)0.0016 (6)0.0210 (6)0.0037 (6)
C90.0651 (10)0.0810 (12)0.0631 (10)0.0146 (8)0.0326 (8)0.0008 (8)
C100.0914 (12)0.0553 (9)0.0583 (9)0.0050 (8)0.0415 (9)0.0036 (7)
N10.0633 (8)0.0598 (8)0.0646 (8)0.0018 (6)0.0232 (7)0.0176 (6)
N20.0576 (7)0.0507 (7)0.0476 (7)0.0002 (5)0.0274 (6)0.0012 (5)
O10.0928 (9)0.0519 (7)0.0772 (8)0.0237 (6)0.0538 (7)0.0171 (5)
Geometric parameters (Å, °) top
C1—C21.3846 (18)C7—C81.3713 (19)
C1—C51.3842 (19)C7—H70.9300
C1—C61.5148 (18)C8—N21.3193 (17)
C2—C31.382 (2)C8—H80.9300
C2—H20.9300C9—N21.4476 (19)
C3—N11.329 (2)C9—H9A0.9600
C3—H30.9300C9—H9B0.9600
C4—N11.323 (2)C9—H9C0.9600
C4—C51.382 (2)C10—N21.4555 (19)
C4—H40.9300C10—H10A0.9600
C5—H50.9300C10—H10B0.9600
C6—O11.2357 (16)C10—H10C0.9600
C6—C71.4180 (18)
C2—C1—C5116.72 (12)C6—C7—H7120.4
C2—C1—C6124.44 (12)N2—C8—C7127.45 (13)
C5—C1—C6118.84 (12)N2—C8—H8116.3
C1—C2—C3119.39 (13)C7—C8—H8116.3
C1—C2—H2120.3N2—C9—H9A109.5
C3—C2—H2120.3N2—C9—H9B109.5
N1—C3—C2124.31 (14)H9A—C9—H9B109.5
N1—C3—H3117.8N2—C9—H9C109.5
C2—C3—H3117.8H9A—C9—H9C109.5
N1—C4—C5124.67 (14)H9B—C9—H9C109.5
N1—C4—H4117.7N2—C10—H10A109.5
C5—C4—H4117.7N2—C10—H10B109.5
C4—C5—C1119.24 (14)H10A—C10—H10B109.5
C4—C5—H5120.4N2—C10—H10C109.5
C1—C5—H5120.4H10A—C10—H10C109.5
O1—C6—C7124.21 (12)H10B—C10—H10C109.5
O1—C6—C1117.19 (12)C4—N1—C3115.67 (13)
C7—C6—C1118.60 (11)C8—N2—C9121.45 (12)
C8—C7—C6119.15 (12)C8—N2—C10121.81 (13)
C8—C7—H7120.4C9—N2—C10116.74 (12)
Acknowledgements top

The authors acknowledge financial support from the Science Foundation of Beihua University.

references
References top

Bruker (2004). APEX2, SAINT-Plus and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.

Ni, L., Zhao, J.-L. & Wei, H. (2009). Acta Cryst. E65, o0000. [HB5023]

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.