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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2007 Dec 6;64(Pt 1):o61. doi: 10.1107/S1600536807061685

2-(2-Methoxy­phen­yl)-4,4-dimethyl-4,5-dihydro-1,3-oxazole

A Thiruvalluvar a,*, Ray J Butcher b, Prakash Karegoudar c, B Shivarama Holla d
PMCID: PMC2915019  PMID: 21200938

Abstract

In the title mol­ecule, C12H15NO2, the oxazole ring adopts an envelope conformation. Overall, the mol­ecule is approximately planar, the dihedral angle between the mean plane through all but the methyl­ene C atom of the five-membered ring and the aromatic ring being 8.6 (1)°. A weak C—H⋯O inter­action contributes to the stabilization of the crystal structure.

Related literature

For related crystal structures, see: Swaleh & Ziemer (2001); Rybakov et al. (2006).graphic file with name e-64-00o61-scheme1.jpg

Experimental

Crystal data

  • C12H15NO2

  • M r = 205.25

  • Monoclinic, Inline graphic

  • a = 8.1495 (2) Å

  • b = 10.9369 (3) Å

  • c = 12.0864 (3) Å

  • β = 91.305 (3)°

  • V = 1076.99 (5) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 200 (2) K

  • 0.39 × 0.31 × 0.24 mm

Data collection

  • Oxford Diffraction Gemini diffractometer

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2007) T min = 0.717, T max = 1.000 (expected range = 0.702–0.980)

  • 34412 measured reflections

  • 3740 independent reflections

  • 2596 reflections with I > 2σ(I)

  • R int = 0.027

Refinement

  • R[F 2 > 2σ(F 2)] = 0.048

  • wR(F 2) = 0.163

  • S = 1.13

  • 3740 reflections

  • 139 parameters

  • H-atom parameters constrained

  • Δρmax = 0.43 e Å−3

  • Δρmin = −0.20 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2007); cell refinement: CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: PLATON (Spek, 2003).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536807061685/tk2221sup1.cif

e-64-00o61-sup1.cif (18.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807061685/tk2221Isup2.hkl

e-64-00o61-Isup2.hkl (179.7KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C26—H26⋯O1 0.93 2.35 2.7136 (12) 103

Acknowledgments

RJB acknowledges the NSF–MRI program for funding to purchase the X-ray CCD diffractometer.

supplementary crystallographic information

Comment

Swaleh and Ziemer (2001) reported the crystal structure of 2-[(2-phenyl-1,3-oxazol-4-yl)methyl]-2H-1,2,3-benzotriazole, wherein the phenyl and oxazole rings are essentially co-planar. Rybakov et al. (2006) reported the crystal structure of 5-(4-bromophenyl)-1,3-oxazol-2-amine, wherein the oxazole and the aromatic rings form a dihedral angle of 9.68 (7)°. In the title molecule, C12H15NO2 (I), Fig. 1, the oxazole ring is in an envelope conformation. The dihedral angle between the mean plane through the O1/C2/N3/C5 atoms and that through the aromatic ring is 8.6 (1)°. A weak C—H···O interaction contributes to the stabilization of the crystal structure (Table 1).

Experimental

To a solution of 2-methoxy benzyl chloride (15.8 g, 0.1 mol) in dichloromethane (50 ml), 2-amino-2-methyl-1-propanol (8.3 g, 0.11 mol) in dichloromethane (50 ml) was added at 298–303 K over 30 min. After stirring for 1 h, dichloromethane was distilled off under reduced pressure. The obtained product was recrystallized using ethyl acetate as the solvent to yield 10 g of (I) (86.5%).

Refinement

The H atoms were positioned geometrically and allowed to ride on their parent atoms with C—H = 0.93–0.97 Å, and with Uiso = 1.2–1.5 times Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) showing the atomic numbering and 50% probability displacement ellipsoids.

Crystal data

C12H15NO2 F000 = 440
Mr = 205.25 Dx = 1.266 Mg m3
Monoclinic, P21/n Melting point: 410(1) K
Hall symbol: -P 2yn Mo Kα radiation λ = 0.71073 Å
a = 8.1495 (2) Å Cell parameters from 14583 reflections
b = 10.9369 (3) Å θ = 4.6–32.5º
c = 12.0864 (3) Å µ = 0.09 mm1
β = 91.305 (3)º T = 200 (2) K
V = 1076.99 (5) Å3 Prism, colourless
Z = 4 0.39 × 0.31 × 0.24 mm

Data collection

Oxford Diffraction Gemini diffractometer 3740 independent reflections
Radiation source: fine-focus sealed tube 2596 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.027
Detector resolution: 10.5081 pixels mm-1 θmax = 32.6º
T = 200(2) K θmin = 4.6º
φ and ω scans h = −12→12
Absorption correction: multi-scan(CrysAlis RED; Oxford Diffraction, 2007) k = −16→16
Tmin = 0.717, Tmax = 1.000 l = −18→18
34412 measured reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.048 H-atom parameters constrained
wR(F2) = 0.163   w = 1/[σ2(Fo2) + (0.099P)2] where P = (Fo2 + 2Fc2)/3
S = 1.13 (Δ/σ)max < 0.001
3740 reflections Δρmax = 0.43 e Å3
139 parameters Δρmin = −0.20 e Å3
Primary atom site location: structure-invariant direct methods Extinction correction: none

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 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)

x y z Uiso*/Ueq
O1 0.61501 (9) 0.49026 (7) 0.33582 (5) 0.0357 (2)
O2 0.40996 (9) 0.22987 (6) 0.11696 (6) 0.0332 (2)
N3 0.65111 (10) 0.39575 (8) 0.17107 (7) 0.0325 (2)
C2 0.56870 (11) 0.40277 (7) 0.25852 (7) 0.0230 (2)
C4 0.78858 (13) 0.48460 (9) 0.18188 (8) 0.0310 (3)
C5 0.74394 (15) 0.55882 (10) 0.28508 (10) 0.0409 (3)
C12 0.33176 (17) 0.14486 (11) 0.04469 (10) 0.0445 (4)
C14 0.79827 (15) 0.56238 (11) 0.07847 (10) 0.0442 (4)
C15 0.94665 (14) 0.41267 (10) 0.20004 (11) 0.0428 (4)
C21 0.42972 (11) 0.32650 (8) 0.29281 (7) 0.0235 (2)
C22 0.35474 (11) 0.23841 (8) 0.22165 (7) 0.0254 (2)
C23 0.22969 (13) 0.16468 (9) 0.26164 (9) 0.0333 (3)
C24 0.18045 (13) 0.17635 (10) 0.37044 (10) 0.0389 (3)
C25 0.25034 (13) 0.26249 (11) 0.44046 (9) 0.0385 (3)
C26 0.37380 (12) 0.33708 (9) 0.40107 (8) 0.0300 (3)
H5A 0.83805 0.56661 0.33518 0.0491*
H5B 0.70600 0.63992 0.26448 0.0491*
H12A 0.38149 0.14833 −0.02649 0.0668*
H12B 0.21733 0.16474 0.03700 0.0668*
H12C 0.34348 0.06393 0.07459 0.0668*
H14A 0.82155 0.51117 0.01626 0.0662*
H14B 0.88401 0.62191 0.08799 0.0662*
H14C 0.69541 0.60335 0.06566 0.0662*
H15A 0.96128 0.35762 0.13920 0.0641*
H15B 0.94063 0.36683 0.26757 0.0641*
H15C 1.03780 0.46817 0.20484 0.0641*
H23 0.17905 0.10747 0.21531 0.0399*
H24 0.09887 0.12517 0.39659 0.0466*
H25 0.21528 0.27039 0.51280 0.0463*
H26 0.42061 0.39563 0.44781 0.0360*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0389 (4) 0.0352 (4) 0.0334 (4) −0.0092 (3) 0.0072 (3) −0.0128 (3)
O2 0.0348 (4) 0.0360 (4) 0.0288 (3) −0.0099 (3) 0.0026 (3) −0.0042 (3)
N3 0.0315 (4) 0.0313 (4) 0.0352 (4) −0.0108 (3) 0.0101 (3) −0.0042 (3)
C2 0.0250 (4) 0.0206 (4) 0.0234 (4) 0.0013 (3) 0.0010 (3) −0.0022 (3)
C4 0.0303 (5) 0.0276 (5) 0.0352 (5) −0.0080 (4) 0.0051 (4) −0.0003 (4)
C5 0.0431 (6) 0.0303 (5) 0.0496 (7) −0.0132 (5) 0.0087 (5) −0.0089 (4)
C12 0.0492 (7) 0.0448 (6) 0.0394 (6) −0.0134 (5) −0.0026 (5) −0.0095 (5)
C14 0.0402 (6) 0.0441 (6) 0.0483 (7) −0.0097 (5) 0.0044 (5) 0.0124 (5)
C15 0.0354 (6) 0.0412 (6) 0.0519 (7) −0.0010 (5) 0.0043 (5) 0.0036 (5)
C21 0.0220 (4) 0.0220 (4) 0.0266 (4) 0.0038 (3) 0.0031 (3) 0.0006 (3)
C22 0.0219 (4) 0.0258 (4) 0.0284 (4) 0.0018 (3) 0.0015 (3) 0.0011 (3)
C23 0.0246 (5) 0.0310 (5) 0.0443 (6) −0.0041 (4) 0.0024 (4) 0.0026 (4)
C24 0.0267 (5) 0.0404 (6) 0.0500 (6) −0.0010 (4) 0.0123 (4) 0.0112 (5)
C25 0.0335 (5) 0.0466 (6) 0.0361 (5) 0.0082 (5) 0.0135 (4) 0.0088 (4)
C26 0.0300 (5) 0.0328 (5) 0.0274 (4) 0.0066 (4) 0.0058 (4) 0.0037 (3)

Geometric parameters (Å, °)

O1—C2 1.3838 (11) C5—H5A 0.9700
O1—C5 1.4393 (14) C5—H5B 0.9700
O2—C12 1.4171 (14) C12—H12A 0.9600
O2—C22 1.3558 (11) C12—H12B 0.9600
N3—C2 1.2675 (12) C12—H12C 0.9600
N3—C4 1.4865 (13) C14—H14A 0.9600
C2—C21 1.4737 (12) C14—H14B 0.9600
C4—C5 1.5387 (15) C14—H14C 0.9600
C4—C14 1.5154 (16) C15—H15A 0.9600
C4—C15 1.5211 (15) C15—H15B 0.9600
C21—C22 1.4203 (12) C15—H15C 0.9600
C21—C26 1.4001 (13) C23—H23 0.9300
C22—C23 1.3946 (14) C24—H24 0.9300
C23—C24 1.3895 (16) C25—H25 0.9300
C24—C25 1.3807 (16) C26—H26 0.9300
C25—C26 1.3879 (15)
O1···C12i 3.3873 (14) H12B···H23 2.2700
O2···N3 2.7428 (11) H12C···C23 2.7000
O1···H26ii 2.9200 H12C···H23 2.2400
O1···H26 2.3500 H12C···C26xi 3.0700
O1···H23iii 2.7800 H14A···H15A 2.5000
O2···H5Aiv 2.7700 H14A···C24v 2.9200
O2···H25v 2.8100 H14B···H15C 2.5100
N3···O2 2.7428 (11) H14B···C21x 3.0500
N3···C25v 3.3942 (14) H14B···C26x 3.0700
N3···H25v 2.7000 H14C···H5B 2.4400
C12···O1vi 3.3873 (14) H14C···H24iii 2.4600
C25···N3vii 3.3942 (14) H14C···C12viii 3.0700
C2···H23iii 3.0400 H15A···H14A 2.5000
C2···H15B 3.0600 H15B···C2 3.0600
C5···H25ii 3.0900 H15B···C24xii 3.1000
C12···H14Cviii 3.0700 H15B···H5A 2.4800
C12···H23 2.4700 H15B···H12Ai 2.5500
C21···H14Biv 3.0500 H15C···H5A 2.5300
C23···H12B 2.7100 H15C···H14B 2.5100
C23···H12C 2.7000 H15C···C23x 2.8900
C23···H15Civ 2.8900 H23···C12 2.4700
C24···H15Bix 3.1000 H23···H12B 2.2700
C24···H14Avii 2.9200 H23···H12C 2.2400
C26···H12Ciii 3.0700 H23···O1xi 2.7800
C26···H14Biv 3.0700 H23···C2xi 3.0400
H5A···H15B 2.4800 H24···H14Cxi 2.4600
H5A···H15C 2.5300 H25···C5ii 3.0900
H5A···O2x 2.7700 H25···O2vii 2.8100
H5B···H14C 2.4400 H25···N3vii 2.7000
H12A···H15Bvi 2.5500 H26···O1 2.3500
H12B···C23 2.7100 H26···O1ii 2.9200
C2—O1—C5 105.25 (7) H5A—C5—H5B 109.00
C12—O2—C22 117.79 (8) O2—C12—H12A 109.00
C2—N3—C4 107.44 (8) O2—C12—H12B 109.00
O1—C2—N3 117.61 (8) O2—C12—H12C 109.00
O1—C2—C21 113.65 (7) H12A—C12—H12B 109.00
N3—C2—C21 128.72 (8) H12A—C12—H12C 109.00
N3—C4—C5 102.97 (8) H12B—C12—H12C 109.00
N3—C4—C14 110.35 (8) C4—C14—H14A 109.00
N3—C4—C15 107.98 (8) C4—C14—H14B 109.00
C5—C4—C14 112.96 (9) C4—C14—H14C 109.00
C5—C4—C15 111.78 (9) H14A—C14—H14B 109.00
C14—C4—C15 110.46 (9) H14A—C14—H14C 109.00
O1—C5—C4 105.01 (8) H14B—C14—H14C 109.00
C2—C21—C22 122.44 (8) C4—C15—H15A 109.00
C2—C21—C26 118.99 (8) C4—C15—H15B 109.00
C22—C21—C26 118.51 (8) C4—C15—H15C 109.00
O2—C22—C21 117.68 (8) H15A—C15—H15B 109.00
O2—C22—C23 122.98 (8) H15A—C15—H15C 109.00
C21—C22—C23 119.34 (8) H15B—C15—H15C 109.00
C22—C23—C24 120.26 (9) C22—C23—H23 120.00
C23—C24—C25 121.25 (10) C24—C23—H23 120.00
C24—C25—C26 118.88 (10) C23—C24—H24 119.00
C21—C26—C25 121.73 (9) C25—C24—H24 119.00
O1—C5—H5A 111.00 C24—C25—H25 121.00
O1—C5—H5B 111.00 C26—C25—H25 121.00
C4—C5—H5A 111.00 C21—C26—H26 119.00
C4—C5—H5B 111.00 C25—C26—H26 119.00
C5—O1—C2—N3 5.16 (11) N3—C4—C5—O1 12.97 (10)
C5—O1—C2—C21 −176.76 (8) C14—C4—C5—O1 132.00 (9)
C2—O1—C5—C4 −11.14 (10) C15—C4—C5—O1 −102.69 (10)
C12—O2—C22—C21 −177.98 (9) C2—C21—C22—O2 −3.21 (13)
C12—O2—C22—C23 2.38 (13) C2—C21—C22—C23 176.46 (8)
C4—N3—C2—O1 3.72 (11) C26—C21—C22—O2 179.69 (8)
C4—N3—C2—C21 −174.03 (9) C26—C21—C22—C23 −0.65 (13)
C2—N3—C4—C5 −10.28 (10) C2—C21—C26—C25 −175.91 (9)
C2—N3—C4—C14 −131.11 (9) C22—C21—C26—C25 1.29 (14)
C2—N3—C4—C15 108.08 (9) O2—C22—C23—C24 178.86 (9)
O1—C2—C21—C22 174.63 (8) C21—C22—C23—C24 −0.79 (14)
O1—C2—C21—C26 −8.28 (12) C22—C23—C24—C25 1.65 (16)
N3—C2—C21—C22 −7.55 (15) C23—C24—C25—C26 −1.01 (16)
N3—C2—C21—C26 169.54 (9) C24—C25—C26—C21 −0.48 (16)

Symmetry codes: (i) x+1/2, −y+1/2, z+1/2; (ii) −x+1, −y+1, −z+1; (iii) −x+1/2, y+1/2, −z+1/2; (iv) −x+3/2, y−1/2, −z+1/2; (v) x+1/2, −y+1/2, z−1/2; (vi) x−1/2, −y+1/2, z−1/2; (vii) x−1/2, −y+1/2, z+1/2; (viii) −x+1, −y+1, −z; (ix) x−1, y, z; (x) −x+3/2, y+1/2, −z+1/2; (xi) −x+1/2, y−1/2, −z+1/2; (xii) x+1, y, z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C26—H26···O1 0.93 2.35 2.7136 (12) 103

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: TK2221).

References

  1. Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
  2. Oxford Diffraction (2007). CrysAlis CCD and CrysAlis RED Versions 1.171.32. Oxford Diffraction Ltd, Abingdon, Oxfordshire, England.
  3. Rybakov, V. B., Alifanov, V. L. & Babaev, E. V. (2006). Acta Cryst. E62, o4746–o4747.
  4. Sheldrick, G. M. (1990). Acta Cryst. A46, 467–473.
  5. Sheldrick, G. M. (1997). SHELXL97 University of Göttingen, Germany.
  6. Spek, A. L. (2003). J. Appl. Cryst.36, 7–13.
  7. Swaleh, S. & Ziemer, B. (2001). Acta Cryst. E57, o35–o36.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536807061685/tk2221sup1.cif

e-64-00o61-sup1.cif (18.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807061685/tk2221Isup2.hkl

e-64-00o61-Isup2.hkl (179.7KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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