Literature DB >> 21578313

5-Methyl-3-[1-(2-pyridylmeth-yl)-1H-benzimidazol-2-ylmeth-yl]isoxazole.

Mohamadou Lamine Doumbia, Rachid Bouhfid, El Mokhtar Essassi, Lahcen El Ammari.   

Abstract

The title compound, C(18)H(16)N(4)O, is built up from fused six- and five-membered rings linked to a five-membered isoxazole ring and to a six-membered pyridine ring through a CH(2) group. The fused-ring system is essentially planar, with a maximum deviation of 0.019 (1) Å. It forms inter-planar angles of 70.03 (7)° with the isoxazole ring and 81.68 (7)° with the pyridine ring; the two latter rings are also planar, the maximum deviations from the mean planes being 0.0028 (15) and 0.0047 (12) Å, respectively. In the crystal, weak inter-molecular non-classical C-H⋯N hydrogen bonds link the mol-ecules, forming a zigzag-like chain parallel to the b axis. A weak intra-molecular C-H⋯N hydrogen bond may help to define the conformation of the mol-ecule.

Entities:  

Year:  2009        PMID: 21578313      PMCID: PMC2971225          DOI: 10.1107/S1600536809040100

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

Isoxazoles and their derivatives are key inter­mediates for the preparation of products which mimics natural compounds, see: Baraldi et al. (1987 ▶). For their biological activity, see: Boros et al. (2006 ▶); Desai & Desai (2006 ▶); Eddington et al. (2002 ▶); Kang et al. (2000 ▶); Ko et al. (1998 ▶); Lee & Kim (2002 ▶); Sbai et al. (2003 ▶).

Experimental

Crystal data

C18H16N4O M = 304.35 Monoclinic, a = 11.0761 (2) Å b = 8.6535 (1) Å c = 16.5920 (3) Å β = 103.136 (1)° V = 1548.68 (4) Å3 Z = 4 Mo Kα radiation μ = 0.09 mm−1 T = 298 K 0.28 × 0.16 × 0.06 mm

Data collection

Bruker X8 Kappa APEX II diffractometer Absorption correction: none 29777 measured reflections 3567 independent reflections 2460 reflections with I > 2σ(I) R int = 0.047

Refinement

R[F 2 > 2σ(F 2)] = 0.040 wR(F 2) = 0.105 S = 1.01 3567 reflections 214 parameters H-atom parameters constrained Δρmax = 0.15 e Å−3 Δρmin = −0.14 e Å−3 Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: SAINT (Bruker, 2005 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶) and PLATON (Spek, 2009 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809040100/dn2494sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809040100/dn2494Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C18H16N4OF(000) = 640
Mr = 304.35Dx = 1.305 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 3567 reflections
a = 11.0761 (2) Åθ = 2.5–27.5°
b = 8.6535 (1) ŵ = 0.09 mm1
c = 16.5920 (3) ÅT = 298 K
β = 103.136 (1)°Block, white
V = 1548.68 (4) Å30.28 × 0.16 × 0.06 mm
Z = 4
Bruker X8 APEX Diffractometer2460 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.047
graphiteθmax = 27.5°, θmin = 2.5°
φ and ω scansh = −14→14
29777 measured reflectionsk = −11→11
3567 independent reflectionsl = −21→17
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 constrained
wR(F2) = 0.105w = 1/[σ2(Fo2) + (0.0445P)2 + 0.2578P] where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max < 0.001
3567 reflectionsΔρmax = 0.15 e Å3
214 parametersΔρmin = −0.14 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: 0.0099 (13)
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.
xyzUiso*/Ueq
O10.35108 (10)−0.03671 (13)0.02360 (6)0.0584 (3)
N10.28238 (12)0.07631 (17)0.05503 (8)0.0587 (4)
N20.14275 (11)0.00694 (14)0.28340 (7)0.0462 (3)
N30.02122 (11)0.07134 (13)0.16088 (7)0.0421 (3)
N4−0.03858 (11)0.38647 (14)0.14258 (7)0.0472 (3)
C10.41164 (13)−0.12534 (17)0.08719 (9)0.0461 (4)
C20.38459 (14)−0.07581 (17)0.15741 (9)0.0467 (4)
H20.4130−0.11630.21020.056*
C30.30411 (13)0.05044 (16)0.13448 (9)0.0438 (3)
C40.24511 (14)0.15139 (17)0.18861 (9)0.0519 (4)
H4B0.30670.17740.23840.061 (5)*
H4A0.21780.24690.15950.067 (5)*
C50.13705 (13)0.07608 (15)0.21254 (8)0.0414 (3)
C60.02351 (13)−0.04756 (15)0.27876 (8)0.0428 (3)
C7−0.02328 (16)−0.13135 (18)0.33632 (10)0.0559 (4)
H70.0275−0.16080.38660.067*
C8−0.14703 (17)−0.1693 (2)0.31653 (11)0.0655 (5)
H8−0.1803−0.22490.35430.079*
C9−0.22337 (16)−0.1265 (2)0.24140 (11)0.0657 (5)
H9−0.3067−0.15380.23020.079*
C10−0.17938 (14)−0.04485 (19)0.18304 (10)0.0553 (4)
H10−0.2307−0.01650.13270.066*
C11−0.05416 (13)−0.00683 (15)0.20323 (8)0.0416 (3)
C12−0.01820 (15)0.13746 (17)0.07846 (8)0.0469 (4)
H12A−0.08120.07080.04580.052 (4)*
H12B0.05210.13750.05260.056 (4)*
C13−0.06934 (12)0.29955 (15)0.07513 (7)0.0380 (3)
C14−0.08168 (16)0.53187 (18)0.13659 (10)0.0568 (4)
H14−0.06190.59400.18350.068*
C15−0.15277 (16)0.5944 (2)0.06597 (11)0.0610 (4)
H15−0.18010.69610.06500.073*
C16−0.18271 (15)0.5037 (2)−0.00321 (10)0.0600 (4)
H16−0.23050.5428−0.05240.072*
C17−0.14106 (13)0.35385 (18)0.00120 (9)0.0496 (4)
H17−0.16080.2897−0.04490.060*
C180.48944 (16)−0.2503 (2)0.06534 (11)0.0633 (4)
H18A0.4381−0.32180.02860.095*
H18B0.5309−0.30330.11470.095*
H18C0.5499−0.20680.03860.095*
U11U22U33U12U13U23
O10.0632 (7)0.0749 (8)0.0368 (6)0.0062 (6)0.0106 (5)0.0119 (5)
N10.0609 (8)0.0670 (9)0.0474 (8)0.0091 (7)0.0107 (6)0.0143 (6)
N20.0487 (7)0.0438 (7)0.0433 (7)0.0026 (5)0.0050 (5)0.0042 (5)
N30.0491 (7)0.0372 (6)0.0381 (6)0.0050 (5)0.0062 (5)0.0019 (5)
N40.0572 (7)0.0463 (7)0.0355 (6)0.0096 (6)0.0050 (5)−0.0026 (5)
C10.0454 (8)0.0521 (9)0.0390 (8)−0.0074 (7)0.0056 (6)0.0096 (6)
C20.0527 (8)0.0491 (8)0.0355 (7)−0.0054 (7)0.0040 (6)0.0085 (6)
C30.0440 (8)0.0443 (8)0.0414 (8)−0.0110 (6)0.0059 (6)0.0065 (6)
C40.0578 (9)0.0440 (8)0.0526 (9)−0.0097 (7)0.0100 (7)−0.0012 (7)
C50.0484 (8)0.0321 (7)0.0420 (8)0.0014 (6)0.0068 (6)−0.0029 (6)
C60.0475 (8)0.0373 (7)0.0432 (8)0.0054 (6)0.0096 (6)−0.0002 (6)
C70.0647 (10)0.0542 (9)0.0504 (9)0.0019 (8)0.0161 (8)0.0061 (7)
C80.0718 (12)0.0661 (11)0.0664 (11)−0.0091 (9)0.0321 (9)−0.0011 (9)
C90.0516 (10)0.0804 (12)0.0689 (11)−0.0106 (9)0.0216 (9)−0.0147 (10)
C100.0481 (9)0.0634 (10)0.0520 (9)0.0048 (7)0.0063 (7)−0.0097 (8)
C110.0475 (8)0.0354 (7)0.0419 (8)0.0058 (6)0.0100 (6)−0.0044 (6)
C120.0575 (9)0.0478 (8)0.0337 (7)0.0062 (7)0.0068 (6)−0.0024 (6)
C130.0392 (7)0.0435 (8)0.0306 (7)0.0010 (6)0.0067 (5)0.0019 (6)
C140.0714 (11)0.0463 (9)0.0523 (9)0.0088 (8)0.0136 (8)−0.0049 (7)
C150.0641 (10)0.0475 (9)0.0717 (12)0.0137 (8)0.0164 (9)0.0134 (8)
C160.0548 (9)0.0641 (10)0.0551 (10)0.0061 (8)0.0001 (7)0.0237 (8)
C170.0514 (9)0.0563 (9)0.0365 (8)−0.0040 (7)0.0004 (6)0.0035 (7)
C180.0676 (11)0.0635 (10)0.0621 (10)0.0020 (8)0.0216 (9)0.0026 (8)
O1—C11.3526 (17)C7—H70.9300
O1—N11.4100 (17)C8—C91.388 (2)
N1—C31.3044 (17)C8—H80.9300
N2—C51.3079 (17)C9—C101.374 (2)
N2—C61.3880 (18)C9—H90.9300
N3—C51.3720 (17)C10—C111.390 (2)
N3—C111.3840 (18)C10—H100.9300
N3—C121.4548 (16)C12—C131.5090 (19)
N4—C131.3270 (16)C12—H12A0.9700
N4—C141.3414 (19)C12—H12B0.9700
C1—C21.338 (2)C13—C171.3833 (18)
C1—C181.478 (2)C14—C151.366 (2)
C2—C31.407 (2)C14—H140.9300
C2—H20.9300C15—C161.368 (2)
C3—C41.504 (2)C15—H150.9300
C4—C51.494 (2)C16—C171.372 (2)
C4—H4B0.9700C16—H160.9300
C4—H4A0.9700C17—H170.9300
C6—C71.390 (2)C18—H18A0.9600
C6—C111.3945 (19)C18—H18B0.9600
C7—C81.375 (2)C18—H18C0.9600
C1—O1—N1108.57 (11)C10—C9—H9119.0
C3—N1—O1105.28 (11)C8—C9—H9119.0
C5—N2—C6104.75 (11)C9—C10—C11116.48 (15)
C5—N3—C11106.49 (11)C9—C10—H10121.8
C5—N3—C12127.86 (12)C11—C10—H10121.8
C11—N3—C12125.63 (12)N3—C11—C10132.63 (13)
C13—N4—C14116.77 (12)N3—C11—C6105.05 (12)
C2—C1—O1109.15 (13)C10—C11—C6122.32 (14)
C2—C1—C18134.95 (14)N3—C12—C13115.46 (11)
O1—C1—C18115.90 (13)N3—C12—H12A108.4
C1—C2—C3105.48 (12)C13—C12—H12A108.4
C1—C2—H2127.3N3—C12—H12B108.4
C3—C2—H2127.3C13—C12—H12B108.4
N1—C3—C2111.51 (13)H12A—C12—H12B107.5
N1—C3—C4119.88 (13)N4—C13—C17122.74 (13)
C2—C3—C4128.61 (13)N4—C13—C12118.28 (11)
C5—C4—C3112.85 (12)C17—C13—C12118.90 (12)
C5—C4—H4B109.0N4—C14—C15124.12 (15)
C3—C4—H4B109.0N4—C14—H14117.9
C5—C4—H4A109.0C15—C14—H14117.9
C3—C4—H4A109.0C14—C15—C16118.38 (15)
H4B—C4—H4A107.8C14—C15—H15120.8
N2—C5—N3113.28 (12)C16—C15—H15120.8
N2—C5—C4124.10 (13)C15—C16—C17118.87 (14)
N3—C5—C4122.62 (12)C15—C16—H16120.6
N2—C6—C7129.63 (13)C17—C16—H16120.6
N2—C6—C11110.42 (12)C16—C17—C13119.12 (14)
C7—C6—C11119.95 (14)C16—C17—H17120.4
C8—C7—C6117.89 (15)C13—C17—H17120.4
C8—C7—H7121.1C1—C18—H18A109.5
C6—C7—H7121.1C1—C18—H18B109.5
C7—C8—C9121.43 (16)H18A—C18—H18B109.5
C7—C8—H8119.3C1—C18—H18C109.5
C9—C8—H8119.3H18A—C18—H18C109.5
C10—C9—C8121.93 (16)H18B—C18—H18C109.5
D—H···AD—HH···AD···AD—H···A
C2—H2···N4i0.932.523.385 (2)155
C12—H12B···N10.972.603.479 (2)151
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C2—H2⋯N4i0.932.523.385 (2)155
C12—H12B⋯N10.972.603.479 (2)151

Symmetry code: (i) .

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