organic compounds
4-Oxo-N-phenyl-1,4-dihydropyridine-3-carboxamide
aSchool of Chemical Engineering and Pharmacy, Wuhan Institute of Technology, Wuhan, Hubei 430205, People's Republic of China
*Correspondence e-mail: sihuilong@wit.edu.cn
The title compound, C12H10N2O2, shows a nearly planar conformation. The is sustained by hydrogen bonds between the NH and the carbonyl O function of the 4-oxo-1,4-dihydropyridine ring of the molecules, forming infinite chains along the b-axis direction.
Keywords: crystal structure; hydrogen bonding.
CCDC reference: 2280191
Structure description
The title compound (Fig. 1) is a derivative of N-phenylnicotinamide, which is an efficient molluscicide (Dunlop et al., 1980). In addition, the compound can be used as a raw material for many chemical reactions. We were interested in its solid-state behavior since it is a structural isomer of N-phenyl-2-hydroxynicotinanilide, which has interesting structural properties (Zhoujin et al., 2021). In our study, the compound was synthesized by an amide condensation reaction (Narajan et al., 2016), and single crystals were obtained by slow evaporation of an acetone solution of the compound. The compound has a nearly planar conformation as evidenced by the dihedral angle between the 4-oxo-1,4-dihydropyridine and benzene rings of 6.80 (8)°. An intramolecular hydrogen bond is formed between the NH of the amide and the carbonyl O atom on the 4-oxo-1,4-dihydropyridine ring. In the crystal, the molecules form chains along the b-axis direction through hydrogen bonds between the NH group and the carbonyl O atom of the 4-oxo-1,4-dihydropyridine ring (Fig. 2, Table 1).
Synthesis and crystallization
4-Hydroxynicotinic acid (0.51 g, 3.67 mmol), 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide hydrochloride (EDC, 1.06 g, 5.51 mmol) and hydroxybenzotriazole (HOBT, 0.60 g, 4.40 mmol) were dissolved in 6 ml of DMF and stirred at 0°C for 1 h. Then diisopropylethylamine (DIPEA, 0.95 g, 7.34 mmol) and aniline (0.28 ml, 3.67 mmol) were added and the reaction was completed under continuous stirring at 50°C for 12 h. Then 20 ml of deionized water were added to the reaction mixture, which was placed into a refrigerator at 5°C overnight. The resulting precipitate was collected by filtration and washed with deionized water to obtain 0.306 g (39% based on 4-hydroxynicotinic acid) of the title compound (Fig. 3). The obtained compound was fully dissolved in acetone under ultrasound until a clear solution was obtained, which was then filtered into a transparent glass bottle. The bottle was placed in a fume hood for slow evaporation of the solvent. Colorless rod-shaped crystals (Fig. 4) were obtained in a few days.
Refinement
Crystal data, data collection and structure .
details are summarized in Table 2Structural data
CCDC reference: 2280191
https://doi.org/10.1107/S2414314623006016/im4020sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314623006016/im4020Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314623006016/im4020Isup3.cml
Data collection: CrysAlis PRO 1.171.41.113a (Rigaku OD, 2021); cell
CrysAlis PRO 1.171.41.113a (Rigaku OD, 2021); data reduction: CrysAlis PRO 1.171.41.113a (Rigaku OD, 2021); program(s) used to solve structure: SHELXT (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2018/3 (Sheldrick, 2015b); molecular graphics: Olex2 1.5 (Dolomanov et al., 2009), Mercury (Macrae et al., 2020); software used to prepare material for publication: Olex2 1.5 (Dolomanov et al., 2009).C12H10N2O2 | Dx = 1.371 Mg m−3 |
Mr = 214.22 | Cu Kα radiation, λ = 1.54184 Å |
Orthorhombic, P212121 | Cell parameters from 5537 reflections |
a = 6.68228 (10) Å | θ = 3.3–77.1° |
b = 11.79159 (18) Å | µ = 0.79 mm−1 |
c = 13.1717 (2) Å | T = 276 K |
V = 1037.86 (3) Å3 | Block, clear light colourless |
Z = 4 | 0.1 × 0.07 × 0.05 mm |
F(000) = 448 |
Rigaku Oxford Diffraction, Synergy Custom system, HyPix diffractometer | 2075 independent reflections |
Radiation source: Rotating-anode X-ray tube, Rigaku (Cu) X-ray Source | 2003 reflections with I > 2σ(I) |
Mirror monochromator | Rint = 0.019 |
Detector resolution: 10.0000 pixels mm-1 | θmax = 77.2°, θmin = 5.0° |
ω scans | h = −8→8 |
Absorption correction: multi-scan (CrysAlisPro; Rigaku OD, 2021) | k = −13→14 |
Tmin = 0.864, Tmax = 1.000 | l = −14→16 |
6101 measured reflections |
Refinement on F2 | H atoms treated by a mixture of independent and constrained refinement |
Least-squares matrix: full | w = 1/[σ2(Fo2) + (0.0478P)2 + 0.0929P] where P = (Fo2 + 2Fc2)/3 |
R[F2 > 2σ(F2)] = 0.030 | (Δ/σ)max < 0.001 |
wR(F2) = 0.083 | Δρmax = 0.21 e Å−3 |
S = 1.06 | Δρmin = −0.14 e Å−3 |
2075 reflections | Extinction correction: SHELXL-2018/3 (Sheldrick 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
154 parameters | Extinction coefficient: 0.027 (3) |
0 restraints | Absolute structure: Flack x determined using 788 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013) |
Primary atom site location: dual | Absolute structure parameter: 0.11 (8) |
Hydrogen site location: mixed |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
Refinement. The positions of H atoms at N1 and N2 were obtained from the difference Fourier map and were refined freely. Other H atoms were positioned geometrically with C—H = 0.93 Å and constrained to ride on their parent atoms, with Uiso(H) = 1.2 Ueq(C) (Table 2). |
x | y | z | Uiso*/Ueq | ||
O1 | 0.25139 (19) | 0.41568 (10) | 0.25242 (11) | 0.0504 (4) | |
O2 | 0.4568 (3) | 0.68655 (14) | 0.4334 (2) | 0.0985 (8) | |
N1 | −0.0559 (2) | 0.71242 (14) | 0.26837 (14) | 0.0522 (4) | |
H1 | −0.122 (4) | 0.780 (2) | 0.2688 (18) | 0.060 (6)* | |
N2 | 0.5233 (2) | 0.50907 (12) | 0.37556 (12) | 0.0418 (3) | |
C1 | 0.1596 (3) | 0.50951 (14) | 0.25749 (13) | 0.0415 (4) | |
C2 | 0.2281 (3) | 0.60428 (14) | 0.31705 (14) | 0.0417 (4) | |
C3 | 0.1157 (3) | 0.70093 (15) | 0.32024 (16) | 0.0497 (4) | |
H3 | 0.159842 | 0.761165 | 0.359932 | 0.060* | |
C4 | −0.1229 (3) | 0.62714 (18) | 0.20986 (16) | 0.0553 (5) | |
H4 | −0.240686 | 0.636483 | 0.173182 | 0.066* | |
C5 | −0.0226 (3) | 0.52847 (17) | 0.20341 (15) | 0.0534 (5) | |
H5 | −0.073310 | 0.470945 | 0.162547 | 0.064* | |
C6 | 0.4136 (3) | 0.60500 (15) | 0.38116 (17) | 0.0485 (5) | |
C7 | 0.7012 (2) | 0.48310 (14) | 0.42740 (12) | 0.0372 (4) | |
C8 | 0.8102 (3) | 0.56149 (14) | 0.48339 (13) | 0.0414 (4) | |
H8 | 0.766564 | 0.636194 | 0.488177 | 0.050* | |
C9 | 0.9846 (3) | 0.52788 (17) | 0.53218 (15) | 0.0489 (4) | |
H9 | 1.056878 | 0.580418 | 0.569958 | 0.059* | |
C10 | 1.0519 (3) | 0.41749 (18) | 0.52534 (16) | 0.0534 (5) | |
H10 | 1.168367 | 0.395585 | 0.558657 | 0.064* | |
C11 | 0.9447 (3) | 0.33961 (16) | 0.46848 (15) | 0.0512 (5) | |
H11 | 0.989888 | 0.265248 | 0.463118 | 0.061* | |
C12 | 0.7708 (3) | 0.37210 (15) | 0.41965 (14) | 0.0447 (4) | |
H12 | 0.699818 | 0.319469 | 0.381348 | 0.054* | |
H2 | 0.471 (3) | 0.455 (2) | 0.3385 (19) | 0.061 (7)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0506 (7) | 0.0403 (6) | 0.0602 (8) | −0.0014 (5) | −0.0053 (6) | −0.0110 (5) |
O2 | 0.0752 (11) | 0.0582 (10) | 0.162 (2) | 0.0273 (8) | −0.0592 (12) | −0.0567 (11) |
N1 | 0.0498 (8) | 0.0454 (8) | 0.0614 (10) | 0.0053 (7) | −0.0058 (7) | 0.0124 (7) |
N2 | 0.0383 (7) | 0.0354 (7) | 0.0518 (8) | −0.0002 (6) | −0.0030 (6) | −0.0095 (6) |
C1 | 0.0434 (8) | 0.0399 (8) | 0.0411 (8) | −0.0060 (7) | 0.0023 (7) | 0.0022 (7) |
C2 | 0.0404 (8) | 0.0369 (8) | 0.0478 (9) | −0.0013 (6) | 0.0012 (7) | 0.0006 (7) |
C3 | 0.0482 (9) | 0.0395 (9) | 0.0613 (11) | 0.0018 (7) | −0.0056 (8) | 0.0019 (8) |
C4 | 0.0516 (10) | 0.0588 (11) | 0.0555 (11) | −0.0042 (9) | −0.0138 (9) | 0.0172 (9) |
C5 | 0.0586 (11) | 0.0510 (10) | 0.0506 (10) | −0.0091 (9) | −0.0146 (9) | 0.0035 (8) |
C6 | 0.0429 (9) | 0.0349 (8) | 0.0677 (12) | 0.0013 (7) | −0.0071 (8) | −0.0117 (8) |
C7 | 0.0363 (7) | 0.0371 (8) | 0.0383 (7) | −0.0004 (6) | 0.0048 (6) | −0.0016 (6) |
C8 | 0.0422 (8) | 0.0374 (8) | 0.0445 (9) | −0.0024 (6) | 0.0020 (7) | −0.0028 (7) |
C9 | 0.0469 (9) | 0.0532 (10) | 0.0465 (9) | −0.0069 (8) | −0.0044 (8) | −0.0033 (8) |
C10 | 0.0470 (9) | 0.0621 (11) | 0.0510 (10) | 0.0061 (8) | −0.0060 (8) | 0.0042 (9) |
C11 | 0.0550 (10) | 0.0451 (9) | 0.0536 (11) | 0.0116 (8) | 0.0016 (9) | −0.0004 (8) |
C12 | 0.0483 (9) | 0.0376 (8) | 0.0482 (9) | 0.0002 (7) | −0.0003 (8) | −0.0051 (7) |
O1—C1 | 1.267 (2) | C4—C5 | 1.346 (3) |
O2—C6 | 1.217 (2) | C5—H5 | 0.9300 |
N1—H1 | 0.91 (2) | C7—C8 | 1.389 (2) |
N1—C3 | 1.341 (3) | C7—C12 | 1.393 (2) |
N1—C4 | 1.344 (3) | C8—H8 | 0.9300 |
N2—C6 | 1.350 (2) | C8—C9 | 1.388 (2) |
N2—C7 | 1.405 (2) | C9—H9 | 0.9300 |
N2—H2 | 0.88 (3) | C9—C10 | 1.380 (3) |
C1—C2 | 1.440 (2) | C10—H10 | 0.9300 |
C1—C5 | 1.428 (2) | C10—C11 | 1.384 (3) |
C2—C3 | 1.365 (2) | C11—H11 | 0.9300 |
C2—C6 | 1.500 (2) | C11—C12 | 1.382 (3) |
C3—H3 | 0.9300 | C12—H12 | 0.9300 |
C4—H4 | 0.9300 | ||
C3—N1—H1 | 120.0 (15) | O2—C6—N2 | 124.36 (17) |
C3—N1—C4 | 120.09 (17) | O2—C6—C2 | 121.23 (16) |
C4—N1—H1 | 119.8 (15) | N2—C6—C2 | 114.41 (15) |
C6—N2—C7 | 128.00 (15) | C8—C7—N2 | 123.83 (15) |
C6—N2—H2 | 115.0 (16) | C8—C7—C12 | 119.29 (15) |
C7—N2—H2 | 116.8 (16) | C12—C7—N2 | 116.87 (15) |
O1—C1—C2 | 123.54 (16) | C7—C8—H8 | 120.1 |
O1—C1—C5 | 121.55 (16) | C9—C8—C7 | 119.73 (16) |
C5—C1—C2 | 114.91 (16) | C9—C8—H8 | 120.1 |
C1—C2—C6 | 125.01 (15) | C8—C9—H9 | 119.6 |
C3—C2—C1 | 119.31 (16) | C10—C9—C8 | 120.84 (17) |
C3—C2—C6 | 115.63 (15) | C10—C9—H9 | 119.6 |
N1—C3—C2 | 122.60 (17) | C9—C10—H10 | 120.3 |
N1—C3—H3 | 118.7 | C9—C10—C11 | 119.48 (17) |
C2—C3—H3 | 118.7 | C11—C10—H10 | 120.3 |
N1—C4—H4 | 119.4 | C10—C11—H11 | 119.9 |
N1—C4—C5 | 121.13 (17) | C12—C11—C10 | 120.18 (18) |
C5—C4—H4 | 119.4 | C12—C11—H11 | 119.9 |
C1—C5—H5 | 119.0 | C7—C12—H12 | 119.8 |
C4—C5—C1 | 121.92 (17) | C11—C12—C7 | 120.47 (17) |
C4—C5—H5 | 119.0 | C11—C12—H12 | 119.8 |
O1—C1—C2—C3 | −178.02 (16) | C5—C1—C2—C3 | 1.9 (3) |
O1—C1—C2—C6 | −0.6 (3) | C5—C1—C2—C6 | 179.37 (17) |
O1—C1—C5—C4 | 178.76 (18) | C6—N2—C7—C8 | −9.9 (3) |
N1—C4—C5—C1 | −0.4 (3) | C6—N2—C7—C12 | 171.15 (18) |
N2—C7—C8—C9 | 179.95 (16) | C6—C2—C3—N1 | −178.90 (18) |
N2—C7—C12—C11 | −179.93 (16) | C7—N2—C6—O2 | 0.9 (4) |
C1—C2—C3—N1 | −1.2 (3) | C7—N2—C6—C2 | −178.75 (16) |
C1—C2—C6—O2 | −176.4 (2) | C7—C8—C9—C10 | 0.4 (3) |
C1—C2—C6—N2 | 3.3 (3) | C8—C7—C12—C11 | 1.1 (3) |
C2—C1—C5—C4 | −1.2 (3) | C8—C9—C10—C11 | 0.4 (3) |
C3—N1—C4—C5 | 1.2 (3) | C9—C10—C11—C12 | −0.5 (3) |
C3—C2—C6—O2 | 1.2 (3) | C10—C11—C12—C7 | −0.3 (3) |
C3—C2—C6—N2 | −179.15 (17) | C12—C7—C8—C9 | −1.1 (2) |
C4—N1—C3—C2 | −0.4 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 0.91 (2) | 1.84 (3) | 2.744 (2) | 171 (2) |
C8—H8···O2 | 0.93 | 2.27 | 2.861 (2) | 121 |
N2—H2···O1 | 0.88 (3) | 1.91 (2) | 2.6731 (18) | 144 (2) |
Symmetry code: (i) −x, y+1/2, −z+1/2. |
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