Abstract
In the title compound, C14H15N3O2, one of the methyl C atoms of the tert-butyl group lies almost in the plane of the chromene ring system [deviation = −0.097 (2) Å], one lies above and one lies below [deviations = 1.460 (3) and 1.006 (3) Å, respectively]. The C—C—N—N torsion angle is 142.33 (17)°. In the crystal, moelcules are linked by weak C—H⋯O hydrogen bonds to generate C(6) chains propagating in the [010] direction.
Keywords: crystal structure, chromene, coumarin, hydrogen bonding
Related literature
For background to the biological properties of coumarins, see: Basanagouda et al. (2009 ▸); Liu et al. (2008 ▸); Mustafa et al. (2011 ▸); Ronad et al. (2008 ▸); Tian et al. (2000 ▸); Puttaraju et al. (2013 ▸). For a related structure, see: Chandra et al. (2014 ▸).
Experimental
Crystal data
C14H15N3O2
M r = 257.29
Monoclinic,
a = 10.6816 (7) Å
b = 11.1416 (8) Å
c = 11.5409 (8) Å
β = 100.674 (4)°
V = 1349.72 (16) Å3
Z = 4
Cu Kα radiation
μ = 0.71 mm−1
T = 293 K
0.30 × 0.25 × 0.20 mm
Data collection
Bruker X8 Proteum diffractometer
5911 measured reflections
2165 independent reflections
1949 reflections with I > 2σ(I)
R int = 0.037
Refinement
R[F 2 > 2σ(F 2)] = 0.045
wR(F 2) = 0.132
S = 1.04
2165 reflections
175 parameters
H-atom parameters constrained
Δρmax = 0.13 e Å−3
Δρmin = −0.17 e Å−3
Data collection: APEX2 (Bruker, 2009 ▸); cell refinement: SAINT (Bruker, 2009 ▸); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▸); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▸); molecular graphics: PLATON (Spek, 2009 ▸); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S205698901500290X/hb7363sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S205698901500290X/hb7363Isup2.hkl
Supporting information file. DOI: 10.1107/S205698901500290X/hb7363Isup3.cml
. DOI: 10.1107/S205698901500290X/hb7363fig1.tif
Perspective diagram of the molecule with 50% probability displacement ellipsoids.
b . DOI: 10.1107/S205698901500290X/hb7363fig2.tif
Packing diagram of the molecule viewed parallel to the b axis.
CCDC reference: 1048730
Additional supporting information: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (, ).
| DHA | DH | HA | D A | DHA |
|---|---|---|---|---|
| C14H14AO2i | 0.97 | 2.55 | 3.311(2) | 135 |
Symmetry code: (i)
.
Acknowledgments
MM would like to thank UGC, New Delhi, Government of India, for the award of a project under the head F. No. 41–920/2012(SR) (dated: 25-07-2012). In addition, SD is thankful to the Council of Scientific and Industrial Research, New Delhi, India, for financial assistance [grant No. 02 (0172)/13/EMR-II].
supplementary crystallographic information
S1. Comment
Coumarin and its substituents are of well known heterocyclic compounds, which have a variety of biologically activities; such as anti-tumour (Mustafa et al., 2011), anti-bacterial (Basanagouda et al., 2009; Liu et al., 2008) and analgesic (Ronad et al., 2008) agents. In addition, coumarin derivatives have been found to be very useful in many applications; such as nonlinear optical materials and as intermediates for the drug synthesis (Tian et al., 2000). In our previous work (Puttaraju et al., 2013), we have reported the synthesis, in vitro antimicrobial and anticancer activities of new coumarin derivatives substituted dihydrobenzo[4,5]imidazo[1,2-a]pyrimidin-4-ones. In continuation to this, we have synthesized the title compound to study its molecular and crystal structure.
In the molecular structure of the title compound (Fig. 1), the chromene moiety is almost planar, with the maximum deviation from the mean plane being 0.093 (2) Å for atom C10, respectively. The azidomethyl group is in anti-periplanar conformation with respect to the chromene moiety, as indicated by the torsion angle value of 172.35 (14)° (C3–C4–C14–N1). The bond lengths and angles are within normal ranges and are comparable to related structure (Chandra et al., 2014). The crystal structure features C—H···O hydrogen bonds, which link the molecules into [010] chains, as shown in Fig. 2.
S2. Experimental
6-tert-Butyl-4-bromomethylcoumarins (0.001 mmol. 0.5 g) were taken in 15 ml acetone in a round bottomed flask and stirred. To this, sodium azide (0.002 mol, 0.13 g) in 5 ml of water was added drop wise with stirring, which was continued for 3 hrs (reaction was monitored by TLC). The reaction mixture was poured in to ice cold water, separated solid was filtered and recrystallized from ethyl alcohol to get pale yelllow blocks of the title compound.
S3. Refinement
The H atoms were positioned geometrically and allowed to ride on their parent atom, with C–H distance in the range of 0.93 to 0.97 Å; Uiso(H) = 1.2–1.5Ueq (carrier atom) for all H atoms.
Figures
Fig. 1.

Perspective diagram of the molecule with 50% probability displacement ellipsoids.
Fig. 2.

Packing diagram of the molecule viewed parallel to the b axis.
Crystal data
| C14H15N3O2 | F(000) = 544 |
| Mr = 257.29 | Dx = 1.266 Mg m−3 |
| Monoclinic, P21/c | Cu Kα radiation, λ = 1.54178 Å |
| Hall symbol: -P 2ybc | Cell parameters from 2165 reflections |
| a = 10.6816 (7) Å | θ = 5.6–64.5° |
| b = 11.1416 (8) Å | µ = 0.71 mm−1 |
| c = 11.5409 (8) Å | T = 293 K |
| β = 100.674 (4)° | Block, pale yellow |
| V = 1349.72 (16) Å3 | 0.30 × 0.25 × 0.20 mm |
| Z = 4 |
Data collection
| Bruker X8 Proteum diffractometer | 1949 reflections with I > 2σ(I) |
| Radiation source: Bruker MicroStar microfocus rotating anode | Rint = 0.037 |
| Helios multilayer optics monochromator | θmax = 64.5°, θmin = 5.6° |
| Detector resolution: 10.7 pixels mm-1 | h = −12→12 |
| φ and ω scans | k = −12→12 |
| 5911 measured reflections | l = −13→13 |
| 2165 independent reflections |
Refinement
| Refinement on F2 | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.132 | H-atom parameters constrained |
| S = 1.04 | w = 1/[σ2(Fo2) + (0.0667P)2 + 0.2532P] where P = (Fo2 + 2Fc2)/3 |
| 2165 reflections | (Δ/σ)max < 0.001 |
| 175 parameters | Δρmax = 0.13 e Å−3 |
| 0 restraints | Δρmin = −0.17 e Å−3 |
Special details
| Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles |
| Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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)
| x | y | z | Uiso*/Ueq | ||
| O1 | 0.59056 (12) | 0.02266 (11) | 0.31873 (10) | 0.0633 (4) | |
| O2 | 0.43714 (15) | 0.00517 (14) | 0.16423 (12) | 0.0886 (6) | |
| N1 | 0.32064 (15) | −0.31631 (13) | 0.42079 (19) | 0.0852 (7) | |
| N2 | 0.29968 (12) | −0.42384 (13) | 0.41655 (12) | 0.0581 (5) | |
| N3 | 0.26741 (17) | −0.51960 (15) | 0.40562 (16) | 0.0784 (7) | |
| C1 | 0.79791 (14) | −0.09815 (13) | 0.63907 (13) | 0.0464 (5) | |
| C2 | 0.68585 (13) | −0.15469 (12) | 0.58820 (12) | 0.0441 (4) | |
| C3 | 0.61248 (13) | −0.11775 (12) | 0.48071 (12) | 0.0429 (4) | |
| C4 | 0.49582 (14) | −0.17576 (13) | 0.42299 (13) | 0.0478 (5) | |
| C5 | 0.43662 (16) | −0.13424 (15) | 0.31759 (14) | 0.0585 (6) | |
| C6 | 0.48347 (19) | −0.03397 (17) | 0.26019 (15) | 0.0642 (6) | |
| C7 | 0.65570 (15) | −0.01975 (13) | 0.42495 (13) | 0.0493 (5) | |
| C8 | 0.76681 (17) | 0.03930 (15) | 0.47367 (16) | 0.0593 (6) | |
| C9 | 0.83629 (16) | −0.00013 (14) | 0.57861 (16) | 0.0566 (5) | |
| C10 | 0.88114 (15) | −0.14115 (14) | 0.75389 (14) | 0.0553 (5) | |
| C11 | 0.9105 (3) | −0.0370 (2) | 0.8404 (2) | 0.0925 (9) | |
| C12 | 1.0051 (2) | −0.1916 (3) | 0.7259 (2) | 0.0969 (10) | |
| C13 | 0.8160 (2) | −0.2375 (2) | 0.81437 (18) | 0.0840 (8) | |
| C14 | 0.44697 (15) | −0.27965 (14) | 0.48332 (16) | 0.0581 (5) | |
| H2 | 0.65810 | −0.21990 | 0.62690 | 0.0530* | |
| H5 | 0.36230 | −0.17200 | 0.28040 | 0.0700* | |
| H8 | 0.79420 | 0.10520 | 0.43560 | 0.0710* | |
| H9 | 0.91130 | 0.03960 | 0.61060 | 0.0680* | |
| H11A | 0.83230 | −0.00230 | 0.85410 | 0.1390* | |
| H11B | 0.95900 | 0.02280 | 0.80810 | 0.1390* | |
| H11C | 0.95890 | −0.06580 | 0.91360 | 0.1390* | |
| H12A | 1.05700 | −0.22160 | 0.79690 | 0.1450* | |
| H12B | 1.05020 | −0.12930 | 0.69340 | 0.1450* | |
| H12C | 0.98610 | −0.25570 | 0.66980 | 0.1450* | |
| H13A | 0.73560 | −0.20790 | 0.82820 | 0.1260* | |
| H13B | 0.86890 | −0.25830 | 0.88820 | 0.1260* | |
| H13C | 0.80210 | −0.30740 | 0.76490 | 0.1260* | |
| H14A | 0.50560 | −0.34650 | 0.48640 | 0.0700* | |
| H14B | 0.44200 | −0.25750 | 0.56360 | 0.0700* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0776 (8) | 0.0686 (8) | 0.0471 (7) | 0.0085 (6) | 0.0204 (6) | 0.0127 (5) |
| O2 | 0.1016 (11) | 0.1144 (12) | 0.0476 (8) | 0.0252 (9) | 0.0082 (7) | 0.0190 (7) |
| N1 | 0.0611 (9) | 0.0489 (9) | 0.1292 (15) | −0.0037 (7) | −0.0249 (9) | −0.0015 (8) |
| N2 | 0.0521 (8) | 0.0577 (9) | 0.0598 (9) | −0.0068 (6) | −0.0019 (6) | −0.0048 (6) |
| N3 | 0.0802 (11) | 0.0653 (11) | 0.0841 (12) | −0.0237 (8) | 0.0010 (9) | −0.0092 (8) |
| C1 | 0.0489 (8) | 0.0428 (8) | 0.0493 (8) | −0.0053 (6) | 0.0141 (6) | −0.0055 (6) |
| C2 | 0.0509 (8) | 0.0375 (7) | 0.0453 (8) | −0.0036 (6) | 0.0128 (6) | −0.0017 (6) |
| C3 | 0.0502 (8) | 0.0387 (7) | 0.0419 (8) | 0.0032 (6) | 0.0143 (6) | −0.0056 (6) |
| C4 | 0.0539 (8) | 0.0422 (8) | 0.0467 (8) | 0.0079 (6) | 0.0080 (6) | −0.0100 (6) |
| C5 | 0.0616 (10) | 0.0630 (10) | 0.0482 (9) | 0.0110 (8) | 0.0030 (7) | −0.0106 (7) |
| C6 | 0.0770 (12) | 0.0753 (11) | 0.0424 (9) | 0.0209 (9) | 0.0166 (8) | 0.0016 (8) |
| C7 | 0.0617 (9) | 0.0488 (8) | 0.0422 (8) | 0.0082 (7) | 0.0223 (7) | 0.0029 (6) |
| C8 | 0.0679 (10) | 0.0516 (9) | 0.0653 (11) | −0.0080 (8) | 0.0307 (8) | 0.0070 (7) |
| C9 | 0.0556 (9) | 0.0527 (9) | 0.0644 (10) | −0.0122 (7) | 0.0189 (8) | −0.0018 (7) |
| C10 | 0.0535 (9) | 0.0556 (9) | 0.0541 (9) | −0.0116 (7) | 0.0027 (7) | −0.0021 (7) |
| C11 | 0.1146 (18) | 0.0844 (14) | 0.0685 (13) | −0.0236 (13) | −0.0093 (12) | −0.0150 (11) |
| C12 | 0.0754 (13) | 0.1139 (19) | 0.0993 (17) | 0.0241 (12) | 0.0111 (12) | 0.0184 (14) |
| C13 | 0.0873 (13) | 0.0933 (15) | 0.0614 (11) | −0.0298 (11) | −0.0126 (10) | 0.0242 (10) |
| C14 | 0.0529 (9) | 0.0432 (8) | 0.0715 (10) | −0.0048 (7) | −0.0059 (7) | −0.0042 (7) |
Geometric parameters (Å, º)
| O1—C6 | 1.370 (2) | C10—C12 | 1.527 (3) |
| O1—C7 | 1.3763 (19) | C10—C13 | 1.518 (3) |
| O2—C6 | 1.208 (2) | C2—H2 | 0.9300 |
| N1—N2 | 1.218 (2) | C5—H5 | 0.9300 |
| N1—C14 | 1.466 (2) | C8—H8 | 0.9300 |
| N2—N3 | 1.121 (2) | C9—H9 | 0.9300 |
| C1—C2 | 1.384 (2) | C11—H11A | 0.9600 |
| C1—C9 | 1.398 (2) | C11—H11B | 0.9600 |
| C1—C10 | 1.530 (2) | C11—H11C | 0.9600 |
| C2—C3 | 1.4008 (19) | C12—H12A | 0.9600 |
| C3—C4 | 1.452 (2) | C12—H12B | 0.9600 |
| C3—C7 | 1.389 (2) | C12—H12C | 0.9600 |
| C4—C5 | 1.345 (2) | C13—H13A | 0.9600 |
| C4—C14 | 1.494 (2) | C13—H13B | 0.9600 |
| C5—C6 | 1.435 (3) | C13—H13C | 0.9600 |
| C7—C8 | 1.382 (2) | C14—H14A | 0.9700 |
| C8—C9 | 1.370 (3) | C14—H14B | 0.9700 |
| C10—C11 | 1.525 (3) | ||
| C6—O1—C7 | 121.29 (13) | C3—C2—H2 | 119.00 |
| N2—N1—C14 | 116.07 (15) | C4—C5—H5 | 119.00 |
| N1—N2—N3 | 172.26 (18) | C6—C5—H5 | 119.00 |
| C2—C1—C9 | 117.04 (14) | C7—C8—H8 | 120.00 |
| C2—C1—C10 | 122.92 (13) | C9—C8—H8 | 120.00 |
| C9—C1—C10 | 120.01 (14) | C1—C9—H9 | 119.00 |
| C1—C2—C3 | 122.70 (13) | C8—C9—H9 | 119.00 |
| C2—C3—C4 | 124.58 (13) | C10—C11—H11A | 110.00 |
| C2—C3—C7 | 117.50 (13) | C10—C11—H11B | 110.00 |
| C4—C3—C7 | 117.91 (13) | C10—C11—H11C | 109.00 |
| C3—C4—C5 | 118.81 (14) | H11A—C11—H11B | 109.00 |
| C3—C4—C14 | 118.39 (13) | H11A—C11—H11C | 109.00 |
| C5—C4—C14 | 122.81 (15) | H11B—C11—H11C | 109.00 |
| C4—C5—C6 | 122.65 (16) | C10—C12—H12A | 109.00 |
| O1—C6—O2 | 116.67 (17) | C10—C12—H12B | 110.00 |
| O1—C6—C5 | 117.49 (15) | C10—C12—H12C | 109.00 |
| O2—C6—C5 | 125.85 (18) | H12A—C12—H12B | 109.00 |
| O1—C7—C3 | 121.73 (14) | H12A—C12—H12C | 109.00 |
| O1—C7—C8 | 116.95 (14) | H12B—C12—H12C | 109.00 |
| C3—C7—C8 | 121.31 (14) | C10—C13—H13A | 109.00 |
| C7—C8—C9 | 119.38 (15) | C10—C13—H13B | 110.00 |
| C1—C9—C8 | 122.06 (16) | C10—C13—H13C | 109.00 |
| C1—C10—C11 | 110.18 (14) | H13A—C13—H13B | 109.00 |
| C1—C10—C12 | 108.64 (14) | H13A—C13—H13C | 109.00 |
| C1—C10—C13 | 112.18 (14) | H13B—C13—H13C | 109.00 |
| C11—C10—C12 | 109.72 (19) | N1—C14—H14A | 109.00 |
| C11—C10—C13 | 107.06 (16) | N1—C14—H14B | 109.00 |
| C12—C10—C13 | 109.04 (17) | C4—C14—H14A | 109.00 |
| N1—C14—C4 | 110.84 (14) | C4—C14—H14B | 109.00 |
| C1—C2—H2 | 119.00 | H14A—C14—H14B | 108.00 |
| C7—O1—C6—O2 | −175.54 (16) | C2—C3—C4—C5 | −177.54 (15) |
| C7—O1—C6—C5 | 4.2 (2) | C2—C3—C4—C14 | 2.2 (2) |
| C6—O1—C7—C3 | −3.5 (2) | C7—C3—C4—C14 | −178.75 (14) |
| C6—O1—C7—C8 | 176.23 (16) | C2—C3—C7—O1 | 179.59 (13) |
| N2—N1—C14—C4 | 142.33 (17) | C2—C3—C7—C8 | −0.1 (2) |
| C10—C1—C2—C3 | −177.49 (14) | C4—C3—C7—O1 | 0.5 (2) |
| C2—C1—C9—C8 | 0.1 (2) | C4—C3—C7—C8 | −179.21 (15) |
| C10—C1—C9—C8 | 177.99 (15) | C7—C3—C4—C5 | 1.5 (2) |
| C2—C1—C10—C11 | −128.80 (18) | C3—C4—C5—C6 | −0.6 (2) |
| C2—C1—C10—C12 | 110.99 (19) | C14—C4—C5—C6 | 179.65 (16) |
| C2—C1—C10—C13 | −9.6 (2) | C5—C4—C14—N1 | −7.9 (2) |
| C9—C1—C2—C3 | 0.3 (2) | C3—C4—C14—N1 | 172.35 (14) |
| C9—C1—C10—C12 | −66.8 (2) | C4—C5—C6—O1 | −2.2 (3) |
| C9—C1—C10—C13 | 172.62 (15) | C4—C5—C6—O2 | 177.53 (19) |
| C9—C1—C10—C11 | 53.5 (2) | C3—C7—C8—C9 | 0.5 (2) |
| C1—C2—C3—C4 | 178.72 (14) | O1—C7—C8—C9 | −179.18 (15) |
| C1—C2—C3—C7 | −0.3 (2) | C7—C8—C9—C1 | −0.5 (3) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C14—H14A···O2i | 0.97 | 2.55 | 3.311 (2) | 135 |
Symmetry code: (i) −x+1, y−1/2, −z+1/2.
Footnotes
Supporting information for this paper is available from the IUCr electronic archives (Reference: HB7363).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S205698901500290X/hb7363sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S205698901500290X/hb7363Isup2.hkl
Supporting information file. DOI: 10.1107/S205698901500290X/hb7363Isup3.cml
. DOI: 10.1107/S205698901500290X/hb7363fig1.tif
Perspective diagram of the molecule with 50% probability displacement ellipsoids.
b . DOI: 10.1107/S205698901500290X/hb7363fig2.tif
Packing diagram of the molecule viewed parallel to the b axis.
CCDC reference: 1048730
Additional supporting information: crystallographic information; 3D view; checkCIF report
