organic compounds
Butyl 2-[(azidocarbonyl)amino]benzoate
aLaboratoire de Chimie Organique et Analytique, University Sultan Moulay Slimane, Faculty of Science and Technology, BP 523, Beni-Mellal, Morocco, bUniv. Lille, CNRS, Centrale Lille, ENSCL, Univ. Artois, UMR 8181 - UCCS - Unite, de Catalyse et Chimie du Solide, F-59000 Lille, France, and cLaboratoire de Spectro-Chimie Applique et Environnement, University Sultan, Moulay Slimane, Faculty of Science and Technology, BP 523, Beni-Mellal, Morocco
*Correspondence e-mail: hasna.yassine@yahoo.com
The title compound, C12H14N4O3, is planar with an r.m.s deviation of 0.025 Å from the plane through all 19 non-hydrogen atoms. An intramolecular N—H⋯O interaction closes an S(6) ring. In the crystal, molecules are linked by C—H⋯π and weak offset π–π stacking interactions [inter-centroid distance = 3.614 (2) Å], forming undulating sheets parallel to (001).
Keywords: crystal structure; azides; π–π interactions.
CCDC reference: 1504127
Structure description
As part of our ongoing studies of azide derivatives, we now describe the title compound, C12H14N4O3, with the molecular structure shown in Fig. 1. All non-hydrogen atoms are almost co-planar, with an r.m.s deviation of 0.025 Å from the plane through all 19 non-hydrogen atoms. Bond lengths and angles in the azide group are normal, with the N2—N3 bond [1.246 (3) Å] longer than the terminal N1—N2 distance [1.114 (3) Å] which has more triple-bond character. The azide angle is slightly bent [N1—N2—N3 = 175.2 (2)°]. An intramolecular N—H⋯O interaction closes an S(6) ring (Table 1; Fig. 1). A closely similar structure, ethyl 2-[(azidocarbonyl)amino]benzoate was reported recently (Yassine et al., 2016).
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In the crystal, molecules are linked by C—H⋯π and weak offset π–π stacking interactions [Cg1⋯Cg1i = 3.614 (2) Å, where Cg1 is the centroid of the C2–C7 ring; symmetry code: (i) −x, y, − z], forming sheets parallel to (001) (Table 1 and Fig. 2).
Synthesis and crystallization
A solution of 2-(butoxycarbonyl)benzoic acid (100 mg, 0.45 mmol), DPPA (0.194 ml, 0.90 mmol) and Et3N (0.127 ml, 0.90 mmol) in toluene (5 ml) was refluxed for 4 h. After cooling to room temperature, the reaction mixture was concentrated. The residue was recrystallized from EtOAc–hexane (1:9 v/v) to give blue block-shaped crystals in a yield of 63%, m.p. = 317 K.
1H NMR (300 MHz, CDCl3, δ p.p.m.): 10.87 (1H, NH), 8.48 (1H, H6), 8.03 (1H, H3), 7.55 (1H, H4), 7.11 (1H, H5), 4.32 (2H, H9), 1.76 (2H, H10), 1.48 (2H, H11), 0.98 (3H, H12). 13C NMR (75 MHz, CDCl3, δ p.p.m.): 168.00(C8), 154.40(C1), 140.58(C2), 134.59(C4), 130.89(C6), 122.85(C5), 119.50(C3), 115.54(C7), 65.44(C9), 30.53(C10), 19.22(C11), 13.70(C12).
Refinement
Crystal data, data collection and structure . The reflection (0 6 12) affected by the beam-stop was removed during refinement.
details are summarized in Table 2Structural data
CCDC reference: 1504127
10.1107/S2414314616014541/sj4055sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S2414314616014541/sj4055Isup2.hkl
Supporting information file. DOI: 10.1107/S2414314616014541/sj4055Isup3.cml
Data collection: APEX2 (Bruker, 2009); cell
SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXS2014 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012) and Mercury (Macrae et al., 2008); software used to prepare material for publication: PLATON (Spek, 2009) and publCIF (Westrip, 2010).C12H14N4O3 | F(000) = 1104 |
Mr = 262.27 | Dx = 1.324 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.780 (3) Å | Cell parameters from 2318 reflections |
b = 17.698 (5) Å | θ = 2.3–25.0° |
c = 15.819 (4) Å | µ = 0.10 mm−1 |
β = 105.985 (16)° | T = 299 K |
V = 2632.2 (12) Å3 | Block, purple |
Z = 8 | 0.30 × 0.22 × 0.15 mm |
Bruker DUO APEXII CCD diffractometer | 1370 reflections with I > 2σ(I) |
φ and ω scans | Rint = 0.064 |
Absorption correction: multi-scan (SADABS; Bruker,2009) | θmax = 25.0°, θmin = 2.3° |
Tmin = 0.662, Tmax = 0.746 | h = −11→11 |
28366 measured reflections | k = −20→20 |
2318 independent reflections | l = −18→18 |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.045 | w = 1/[σ2(Fo2) + (0.0486P)2 + 1.1042P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.117 | (Δ/σ)max < 0.001 |
S = 0.98 | Δρmax = 0.18 e Å−3 |
2318 reflections | Δρmin = −0.14 e Å−3 |
173 parameters | Extinction correction: SHELXL-2014/7 (Sheldrick 2015), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.00046 (17) |
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. |
x | y | z | Uiso*/Ueq | ||
O1 | 0.82291 (15) | −0.05566 (8) | 0.54241 (9) | 0.0619 (4) | |
O2 | 0.78779 (17) | 0.06864 (9) | 0.53246 (10) | 0.0711 (5) | |
O3 | 1.13563 (18) | 0.25170 (9) | 0.69941 (11) | 0.0749 (5) | |
N1 | 0.9649 (2) | 0.40575 (13) | 0.63239 (15) | 0.0870 (7) | |
N2 | 0.9465 (2) | 0.34416 (13) | 0.61991 (13) | 0.0656 (5) | |
N3 | 0.9168 (2) | 0.27669 (11) | 0.60087 (12) | 0.0664 (6) | |
C1 | 1.0288 (2) | 0.22860 (13) | 0.64945 (14) | 0.0555 (6) | |
C2 | 1.0654 (2) | 0.09038 (12) | 0.66053 (13) | 0.0514 (5) | |
C7 | 1.0039 (2) | 0.02017 (12) | 0.62878 (13) | 0.0522 (5) | |
C8 | 0.8622 (2) | 0.01555 (13) | 0.56352 (14) | 0.0555 (6) | |
N4 | 0.99075 (19) | 0.15649 (9) | 0.62810 (11) | 0.0581 (5) | |
H4N | 0.9102 | 0.1502 | 0.5896 | 0.070* | |
C3 | 1.1961 (2) | 0.09132 (13) | 0.72320 (14) | 0.0604 (6) | |
H3 | 1.2379 | 0.1372 | 0.7446 | 0.072* | |
C4 | 1.2644 (2) | 0.02473 (14) | 0.75398 (15) | 0.0645 (6) | |
H4 | 1.3521 | 0.0263 | 0.7961 | 0.077* | |
C5 | 1.2056 (2) | −0.04399 (14) | 0.72361 (15) | 0.0668 (7) | |
H5 | 1.2529 | −0.0886 | 0.7449 | 0.080* | |
C6 | 1.0765 (2) | −0.04600 (13) | 0.66150 (15) | 0.0621 (6) | |
H6 | 1.0365 | −0.0924 | 0.6408 | 0.075* | |
C9 | 0.6860 (2) | −0.06591 (12) | 0.47901 (15) | 0.0600 (6) | |
H9A | 0.6846 | −0.0407 | 0.4243 | 0.072* | |
H9B | 0.6115 | −0.0444 | 0.5013 | 0.072* | |
C10 | 0.6622 (2) | −0.14899 (11) | 0.46373 (14) | 0.0567 (6) | |
H10A | 0.6634 | −0.1734 | 0.5188 | 0.068* | |
H10B | 0.7390 | −0.1700 | 0.4434 | 0.068* | |
C11 | 0.5212 (2) | −0.16541 (12) | 0.39631 (15) | 0.0673 (7) | |
H11A | 0.4447 | −0.1445 | 0.4170 | 0.081* | |
H11B | 0.5199 | −0.1403 | 0.3416 | 0.081* | |
C12 | 0.4946 (3) | −0.24873 (13) | 0.37882 (17) | 0.0868 (9) | |
H12A | 0.4046 | −0.2557 | 0.3360 | 0.130* | |
H12B | 0.5688 | −0.2697 | 0.3570 | 0.130* | |
H12C | 0.4935 | −0.2738 | 0.4324 | 0.130* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0566 (10) | 0.0519 (9) | 0.0651 (10) | 0.0001 (7) | −0.0033 (8) | −0.0033 (7) |
O2 | 0.0679 (11) | 0.0531 (10) | 0.0743 (11) | 0.0064 (8) | −0.0106 (8) | −0.0025 (8) |
O3 | 0.0629 (11) | 0.0601 (10) | 0.0861 (12) | −0.0046 (8) | −0.0058 (9) | −0.0045 (9) |
N1 | 0.0811 (16) | 0.0590 (15) | 0.1032 (18) | 0.0072 (12) | −0.0046 (13) | −0.0056 (13) |
N2 | 0.0610 (13) | 0.0582 (15) | 0.0685 (13) | 0.0045 (11) | 0.0025 (10) | −0.0006 (11) |
N3 | 0.0684 (13) | 0.0497 (12) | 0.0701 (13) | −0.0028 (10) | 0.0006 (10) | −0.0021 (10) |
C1 | 0.0562 (15) | 0.0542 (14) | 0.0525 (13) | −0.0018 (12) | 0.0088 (12) | −0.0007 (11) |
C2 | 0.0491 (13) | 0.0511 (13) | 0.0523 (13) | 0.0007 (11) | 0.0111 (11) | 0.0007 (10) |
C7 | 0.0501 (13) | 0.0535 (13) | 0.0506 (12) | 0.0011 (11) | 0.0096 (10) | −0.0008 (10) |
C8 | 0.0591 (15) | 0.0519 (14) | 0.0536 (13) | 0.0016 (12) | 0.0122 (11) | −0.0030 (11) |
N4 | 0.0552 (11) | 0.0491 (12) | 0.0602 (11) | −0.0004 (9) | −0.0005 (9) | −0.0003 (9) |
C3 | 0.0557 (14) | 0.0585 (15) | 0.0614 (14) | −0.0027 (12) | 0.0069 (11) | −0.0013 (11) |
C4 | 0.0523 (14) | 0.0653 (16) | 0.0675 (15) | 0.0023 (12) | 0.0021 (11) | 0.0035 (13) |
C5 | 0.0604 (16) | 0.0602 (15) | 0.0726 (16) | 0.0092 (12) | 0.0064 (13) | 0.0057 (13) |
C6 | 0.0599 (15) | 0.0534 (14) | 0.0674 (15) | 0.0004 (11) | 0.0080 (12) | −0.0012 (12) |
C9 | 0.0562 (14) | 0.0536 (14) | 0.0617 (14) | 0.0035 (11) | 0.0022 (11) | −0.0019 (11) |
C10 | 0.0543 (13) | 0.0528 (13) | 0.0567 (14) | 0.0018 (10) | 0.0047 (11) | 0.0003 (10) |
C11 | 0.0585 (15) | 0.0610 (16) | 0.0707 (15) | −0.0001 (12) | −0.0021 (12) | −0.0023 (12) |
C12 | 0.083 (2) | 0.0685 (18) | 0.090 (2) | −0.0093 (15) | −0.0069 (15) | −0.0108 (14) |
O1—C8 | 1.333 (2) | C4—H4 | 0.9300 |
O1—C9 | 1.446 (2) | C5—C6 | 1.371 (3) |
O2—C8 | 1.207 (2) | C5—H5 | 0.9300 |
O3—C1 | 1.195 (2) | C6—H6 | 0.9300 |
N1—N2 | 1.114 (2) | C9—C10 | 1.498 (3) |
N2—N3 | 1.246 (3) | C9—H9A | 0.9700 |
N3—C1 | 1.433 (3) | C9—H9B | 0.9700 |
C1—N4 | 1.346 (3) | C10—C11 | 1.521 (3) |
C2—C3 | 1.385 (3) | C10—H10A | 0.9700 |
C2—N4 | 1.400 (2) | C10—H10B | 0.9700 |
C2—C7 | 1.411 (3) | C11—C12 | 1.510 (3) |
C7—C6 | 1.393 (3) | C11—H11A | 0.9700 |
C7—C8 | 1.485 (3) | C11—H11B | 0.9700 |
N4—H4N | 0.8600 | C12—H12A | 0.9600 |
C3—C4 | 1.376 (3) | C12—H12B | 0.9600 |
C3—H3 | 0.9300 | C12—H12C | 0.9600 |
C4—C5 | 1.374 (3) | ||
C8—O1—C9 | 116.14 (16) | C5—C6—C7 | 121.3 (2) |
N1—N2—N3 | 175.2 (2) | C5—C6—H6 | 119.4 |
N2—N3—C1 | 110.28 (19) | C7—C6—H6 | 119.4 |
O3—C1—N4 | 128.4 (2) | O1—C9—C10 | 107.97 (17) |
O3—C1—N3 | 123.5 (2) | O1—C9—H9A | 110.1 |
N4—C1—N3 | 108.10 (19) | C10—C9—H9A | 110.1 |
C3—C2—N4 | 122.53 (19) | O1—C9—H9B | 110.1 |
C3—C2—C7 | 119.0 (2) | C10—C9—H9B | 110.1 |
N4—C2—C7 | 118.50 (19) | H9A—C9—H9B | 108.4 |
C6—C7—C2 | 119.0 (2) | C9—C10—C11 | 111.82 (17) |
C6—C7—C8 | 119.6 (2) | C9—C10—H10A | 109.3 |
C2—C7—C8 | 121.38 (19) | C11—C10—H10A | 109.3 |
O2—C8—O1 | 122.3 (2) | C9—C10—H10B | 109.3 |
O2—C8—C7 | 125.7 (2) | C11—C10—H10B | 109.3 |
O1—C8—C7 | 112.08 (19) | H10A—C10—H10B | 107.9 |
C1—N4—C2 | 128.32 (19) | C12—C11—C10 | 113.11 (19) |
C1—N4—H4N | 115.8 | C12—C11—H11A | 109.0 |
C2—N4—H4N | 115.8 | C10—C11—H11A | 109.0 |
C4—C3—C2 | 120.4 (2) | C12—C11—H11B | 109.0 |
C4—C3—H3 | 119.8 | C10—C11—H11B | 109.0 |
C2—C3—H3 | 119.8 | H11A—C11—H11B | 107.8 |
C5—C4—C3 | 121.2 (2) | C11—C12—H12A | 109.5 |
C5—C4—H4 | 119.4 | C11—C12—H12B | 109.5 |
C3—C4—H4 | 119.4 | H12A—C12—H12B | 109.5 |
C6—C5—C4 | 119.2 (2) | C11—C12—H12C | 109.5 |
C6—C5—H5 | 120.4 | H12A—C12—H12C | 109.5 |
C4—C5—H5 | 120.4 | H12B—C12—H12C | 109.5 |
Cg1 is the centroid of the C2–C7 ring |
D—H···A | D—H | H···A | D···A | D—H···A |
N4—H4N···O2 | 0.86 | 1.93 | 2.644 (2) | 139 |
C9—H9A···Cg1i | 0.97 | 2.89 | 3.681 (3) | 139 |
Symmetry code: (i) x+1/2, y+1/2, z+1. |
Acknowledgements
The X-rays diffractometer is funded by Région NPDC, FEDER, CNRS and MESR.
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