organic compounds
of phenyl(pyridin-2-yl)methanol
aDepartment of Chemistry, Chungnam National University, Daejeon 305-764, Republic of Korea
*Correspondence e-mail: skkang@cnu.ac.kr
In the title compound, C12H11NO, the pyridine and phenyl rings are inclined to each other by 71.42 (10)°. In the crystal, O—H⋯N hydrogen bonds link the molecules into helical chains extending along the c-axis direction.
CCDC reference: 1015307
1. Related literature
For the synthesis of the title compound and some derivatives, see: Frassoldati et al. (2013); Tao et al. (2012). For its use in synthesis, see: Miyamura et al. (2008); Lucchesi et al. (2008); Lash et al. (2007); Szajna et al. (2004).
2. Experimental
2.1. Crystal data
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2.2. Data collection
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2.3. Refinement
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Data collection: SMART (Bruker, 2002); cell SAINT (Bruker, 2002); data reduction: SAINT; program(s) used to solve structure: SHELXS2013 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: WinGX (Farrugia, 2012).
Supporting information
CCDC reference: 1015307
10.1107/S1600536814016857/su2760sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536814016857/su2760Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536814016857/su2760Isup3.cml
To a solution of 2-benzoylpyridine (5.0 g, 0.027 mol) in EtOH (60 ml) was added NaBH4 (3.13 g, 0.083 mol) slowly at room temperature. The solution was stirred gently for 1 h. After adding 60 ml H2O, this solution was heated at 363 K for 15 min. After cooling, the product was extracted with AcOEt (50 ml). The solvent was evaporated under reduced pressure to leave a pale green oil. Colourless crystals of the title compound were obtained by slow evaporation of a solution in EtOH at room temperature.
Atom H8 of the OH group was located in a difference Fourier map and freely refined. C-bound H atoms were positioned geometrically and refined using a riding model: C—H = 0.93 - 0.98 Å with Uiso(H) = 1.2Ueq(C).
Data collection: SMART (Bruker, 2002); cell
SAINT (Bruker, 2002); data reduction: SAINT (Bruker, 2002); program(s) used to solve structure: SHELXS2013 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: WinGX (Farrugia, 2012).C12H11NO | F(000) = 392 |
Mr = 185.22 | Dx = 1.25 Mg m−3 |
Orthorhombic, Pna21 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2c -2n | Cell parameters from 973 reflections |
a = 7.4385 (8) Å | θ = 2.6–19.7° |
b = 14.3429 (16) Å | µ = 0.08 mm−1 |
c = 9.2255 (10) Å | T = 296 K |
V = 984.27 (19) Å3 | Block, colourless |
Z = 4 | 0.3 × 0.26 × 0.18 mm |
Bruker SMART CCD area-detector diffractometer | Rint = 0.055 |
Radiation source: fine-focus sealed tube | θmax = 27.5°, θmin = 2.6° |
ϕ and ω scans | h = −7→9 |
7290 measured reflections | k = −18→18 |
2245 independent reflections | l = −11→11 |
1190 reflections with I > 2σ(I) |
Refinement on F2 | 1 restraint |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.039 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.084 | w = 1/[σ2(Fo2) + (0.0303P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.81 | (Δ/σ)max < 0.001 |
2245 reflections | Δρmax = 0.09 e Å−3 |
131 parameters | Δρmin = −0.12 e Å−3 |
C12H11NO | V = 984.27 (19) Å3 |
Mr = 185.22 | Z = 4 |
Orthorhombic, Pna21 | Mo Kα radiation |
a = 7.4385 (8) Å | µ = 0.08 mm−1 |
b = 14.3429 (16) Å | T = 296 K |
c = 9.2255 (10) Å | 0.3 × 0.26 × 0.18 mm |
Bruker SMART CCD area-detector diffractometer | 1190 reflections with I > 2σ(I) |
7290 measured reflections | Rint = 0.055 |
2245 independent reflections |
R[F2 > 2σ(F2)] = 0.039 | 1 restraint |
wR(F2) = 0.084 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.81 | Δρmax = 0.09 e Å−3 |
2245 reflections | Δρmin = −0.12 e Å−3 |
131 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
N1 | 0.4374 (3) | 0.37463 (19) | 0.8538 (3) | 0.0544 (7) | |
C2 | 0.4309 (5) | 0.2902 (3) | 0.9150 (5) | 0.0738 (12) | |
H2 | 0.4616 | 0.2851 | 1.0124 | 0.089* | |
C3 | 0.3819 (5) | 0.2112 (3) | 0.8433 (6) | 0.0773 (12) | |
H3 | 0.3794 | 0.154 | 0.8907 | 0.093* | |
C4 | 0.3365 (4) | 0.2177 (2) | 0.7004 (5) | 0.0733 (12) | |
H4 | 0.302 | 0.1651 | 0.6485 | 0.088* | |
C5 | 0.3426 (4) | 0.3039 (2) | 0.6344 (4) | 0.0582 (9) | |
H5 | 0.3119 | 0.3104 | 0.5372 | 0.07* | |
C6 | 0.3949 (4) | 0.3804 (2) | 0.7141 (3) | 0.0434 (7) | |
C7 | 0.4046 (4) | 0.4769 (2) | 0.6482 (3) | 0.0501 (8) | |
H7 | 0.5021 | 0.5116 | 0.6949 | 0.06* | |
O8 | 0.4471 (3) | 0.46457 (19) | 0.5006 (3) | 0.0700 (7) | |
H8 | 0.474 (5) | 0.526 (3) | 0.460 (5) | 0.111 (16)* | |
C9 | 0.2299 (3) | 0.52994 (18) | 0.6693 (3) | 0.0409 (7) | |
C10 | 0.0771 (4) | 0.5047 (2) | 0.5952 (4) | 0.0587 (9) | |
H10 | 0.0817 | 0.4549 | 0.5307 | 0.07* | |
C11 | −0.0819 (4) | 0.5515 (3) | 0.6146 (4) | 0.0715 (11) | |
H11 | −0.1837 | 0.5334 | 0.5633 | 0.086* | |
C12 | −0.0908 (5) | 0.6244 (3) | 0.7087 (4) | 0.0679 (10) | |
H12 | −0.1989 | 0.6557 | 0.7224 | 0.081* | |
C13 | 0.0579 (5) | 0.6514 (2) | 0.7824 (4) | 0.0697 (10) | |
H13 | 0.0515 | 0.7017 | 0.8459 | 0.084* | |
C14 | 0.2204 (4) | 0.6043 (2) | 0.7639 (4) | 0.0570 (8) | |
H14 | 0.3219 | 0.623 | 0.8151 | 0.068* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0530 (17) | 0.061 (2) | 0.0488 (19) | 0.0047 (13) | 0.0014 (14) | 0.0027 (15) |
C2 | 0.066 (3) | 0.084 (3) | 0.071 (3) | 0.019 (2) | 0.008 (2) | 0.024 (2) |
C3 | 0.059 (2) | 0.059 (3) | 0.114 (4) | 0.006 (2) | 0.015 (2) | 0.029 (3) |
C4 | 0.059 (2) | 0.049 (2) | 0.112 (4) | 0.0045 (17) | 0.006 (3) | −0.008 (2) |
C5 | 0.056 (2) | 0.057 (2) | 0.062 (2) | 0.0079 (16) | 0.0005 (17) | −0.0047 (19) |
C6 | 0.0362 (15) | 0.0463 (19) | 0.0476 (19) | 0.0058 (13) | 0.0045 (15) | −0.0004 (15) |
C7 | 0.0500 (18) | 0.0578 (19) | 0.0426 (19) | −0.0030 (15) | 0.0052 (15) | −0.0001 (16) |
O8 | 0.0827 (17) | 0.0741 (18) | 0.0530 (15) | 0.0020 (14) | 0.0260 (13) | 0.0028 (13) |
C9 | 0.0452 (16) | 0.0391 (15) | 0.0383 (15) | −0.0036 (14) | 0.0017 (14) | 0.0062 (14) |
C10 | 0.059 (2) | 0.047 (2) | 0.069 (2) | −0.0019 (17) | −0.0103 (18) | −0.0040 (17) |
C11 | 0.052 (2) | 0.072 (2) | 0.090 (3) | 0.0003 (19) | −0.009 (2) | 0.010 (2) |
C12 | 0.061 (2) | 0.071 (2) | 0.072 (3) | 0.016 (2) | 0.011 (2) | 0.014 (2) |
C13 | 0.091 (3) | 0.057 (2) | 0.061 (2) | 0.018 (2) | 0.004 (2) | −0.005 (2) |
C14 | 0.066 (2) | 0.0535 (18) | 0.0512 (19) | −0.0022 (16) | −0.0088 (18) | −0.0012 (17) |
N1—C6 | 1.329 (4) | C7—H7 | 0.98 |
N1—C2 | 1.338 (4) | O8—H8 | 0.98 (5) |
C2—C3 | 1.362 (5) | C9—C10 | 1.374 (4) |
C2—H2 | 0.93 | C9—C14 | 1.380 (4) |
C3—C4 | 1.364 (5) | C10—C11 | 1.372 (4) |
C3—H3 | 0.93 | C10—H10 | 0.93 |
C4—C5 | 1.379 (5) | C11—C12 | 1.361 (5) |
C4—H4 | 0.93 | C11—H11 | 0.93 |
C5—C6 | 1.376 (4) | C12—C13 | 1.354 (5) |
C5—H5 | 0.93 | C12—H12 | 0.93 |
C6—C7 | 1.514 (4) | C13—C14 | 1.395 (4) |
C7—O8 | 1.408 (4) | C13—H13 | 0.93 |
C7—C9 | 1.518 (4) | C14—H14 | 0.93 |
C6—N1—C2 | 117.2 (3) | C9—C7—H7 | 108.8 |
N1—C2—C3 | 123.9 (4) | C7—O8—H8 | 108 (3) |
N1—C2—H2 | 118.1 | C10—C9—C14 | 118.4 (3) |
C3—C2—H2 | 118.1 | C10—C9—C7 | 120.8 (3) |
C2—C3—C4 | 118.6 (4) | C14—C9—C7 | 120.8 (3) |
C2—C3—H3 | 120.7 | C11—C10—C9 | 121.3 (3) |
C4—C3—H3 | 120.7 | C11—C10—H10 | 119.4 |
C3—C4—C5 | 118.7 (4) | C9—C10—H10 | 119.4 |
C3—C4—H4 | 120.7 | C12—C11—C10 | 120.1 (4) |
C5—C4—H4 | 120.7 | C12—C11—H11 | 120 |
C6—C5—C4 | 119.2 (3) | C10—C11—H11 | 120 |
C6—C5—H5 | 120.4 | C13—C12—C11 | 120.0 (3) |
C4—C5—H5 | 120.4 | C13—C12—H12 | 120 |
N1—C6—C5 | 122.4 (3) | C11—C12—H12 | 120 |
N1—C6—C7 | 115.8 (3) | C12—C13—C14 | 120.5 (3) |
C5—C6—C7 | 121.8 (3) | C12—C13—H13 | 119.8 |
O8—C7—C6 | 106.5 (3) | C14—C13—H13 | 119.8 |
O8—C7—C9 | 112.3 (2) | C9—C14—C13 | 119.8 (3) |
C6—C7—C9 | 111.4 (2) | C9—C14—H14 | 120.1 |
O8—C7—H7 | 108.8 | C13—C14—H14 | 120.1 |
C6—C7—H7 | 108.8 |
D—H···A | D—H | H···A | D···A | D—H···A |
O8—H8···N1i | 0.98 (5) | 1.85 (5) | 2.809 (4) | 166 (4) |
Symmetry code: (i) −x+1, −y+1, z−1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O8—H8···N1i | 0.98 (5) | 1.85 (5) | 2.809 (4) | 166 (4) |
Symmetry code: (i) −x+1, −y+1, z−1/2. |
Acknowledgements
This work was supported by research funding of Chungnam National University.
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