organic compounds
2-Phenyl-1,3-selenazole-4-carboxylic acid
aCollege of Chemistry and Life Science, Zhejiang Normal University, Jinhua 321004, Zhejiang, People's Republic of China, and bZhejiang Normal University Xingzhi College, Jinhua, Zhejiang 321004, People's Republic of China
*Correspondence e-mail: sky53@zjnu.cn
In the title compound, C10H7NO2Se, the two rings are twisted, making a dihedral angle of 12.42 (9)°. In the crystal, pairs of molecules are disposed about an inversion center, generating O—H⋯O hydrogen-bonded dimers.
Related literature
For the synthesis, see: Zhao et al. (2010). For related structures, see: Srivastava & Robins (1983); Boritzki et al. (1985); Shen et al. (2011).
Experimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2006); cell SAINT (Bruker, 2006); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S1600536811007185/ng5124sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811007185/ng5124Isup2.hkl
Reagents and solvents used were of commercially available quality and without purified before using. K2Cr2O7 (0.588 g, 2 mmol) was added to a mixed solution of acetic acid (50 ml) with 2-phenyl-4-selenazole carbinol (0.248 g, 1 mmol) under stirred conditions at room temperature. Few minutes later lots of red deposit appeared. After the deposit was filtered out, a light red solution was kept for evaporating. Some red single crystals were obtained about 19 days later.
The structure was solved by
and successive Fourier difference synthesis. The H atoms bonded to C atoms were positioned geometrically and refined using a riding model [aromatic C—H = 0.93 Å (Uiso(H) = 1.2Ueq(C))]. The H atoms bonded to O atoms were located in difference Fourier maps and refined with O—H distance restraints of 0.85 (2) and Uiso(H) = 1.5Ueq(O).Data collection: APEX2 (Bruker, 2006); cell
SAINT (Bruker, 2006); data reduction: SAINT (Bruker, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).C10H7NO2Se | F(000) = 496 |
Mr = 252.13 | Dx = 1.732 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 4000 reflections |
a = 8.0817 (3) Å | θ = 2.6–25.0° |
b = 11.5661 (4) Å | µ = 3.85 mm−1 |
c = 11.6295 (4) Å | T = 296 K |
β = 117.168 (2)° | Block, red |
V = 967.12 (6) Å3 | 0.23 × 0.22 × 0.19 mm |
Z = 4 |
Bruker APEXII area-detector diffractometer | 1705 independent reflections |
Radiation source: fine-focus sealed tube | 1487 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.022 |
Detector resolution: none pixels mm-1 | θmax = 25.0°, θmin = 2.6° |
ϕ and ω scans | h = −9→9 |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | k = −13→13 |
Tmin = 0.437, Tmax = 0.479 | l = −13→13 |
7502 measured reflections |
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)] = 0.024 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.063 | H-atom parameters constrained |
S = 1.05 | w = 1/[σ2(Fo2) + (0.0341P)2 + 0.3951P] where P = (Fo2 + 2Fc2)/3 |
1705 reflections | (Δ/σ)max = 0.001 |
127 parameters | Δρmax = 0.43 e Å−3 |
0 restraints | Δρmin = −0.19 e Å−3 |
C10H7NO2Se | V = 967.12 (6) Å3 |
Mr = 252.13 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 8.0817 (3) Å | µ = 3.85 mm−1 |
b = 11.5661 (4) Å | T = 296 K |
c = 11.6295 (4) Å | 0.23 × 0.22 × 0.19 mm |
β = 117.168 (2)° |
Bruker APEXII area-detector diffractometer | 1705 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1487 reflections with I > 2σ(I) |
Tmin = 0.437, Tmax = 0.479 | Rint = 0.022 |
7502 measured reflections |
R[F2 > 2σ(F2)] = 0.024 | 0 restraints |
wR(F2) = 0.063 | H-atom parameters constrained |
S = 1.05 | Δρmax = 0.43 e Å−3 |
1705 reflections | Δρmin = −0.19 e Å−3 |
127 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. |
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. |
x | y | z | Uiso*/Ueq | ||
Se1 | 0.26583 (4) | −0.04306 (2) | 0.60598 (2) | 0.04992 (12) | |
O1 | 0.4357 (3) | −0.41679 (16) | 0.5986 (2) | 0.0685 (6) | |
H7 | 0.4714 | −0.4799 | 0.5865 | 0.103* | |
O2 | 0.4478 (3) | −0.37486 (15) | 0.41673 (18) | 0.0661 (6) | |
N1 | 0.3215 (3) | −0.15135 (15) | 0.42195 (18) | 0.0382 (4) | |
C1 | 0.1846 (4) | 0.0295 (2) | 0.2299 (3) | 0.0543 (7) | |
H1 | 0.2010 | −0.0436 | 0.2033 | 0.065* | |
C2 | 0.1285 (4) | 0.1208 (2) | 0.1426 (3) | 0.0655 (8) | |
H2 | 0.1085 | 0.1088 | 0.0581 | 0.079* | |
C3 | 0.1028 (4) | 0.2287 (2) | 0.1809 (3) | 0.0595 (7) | |
H3 | 0.0630 | 0.2894 | 0.1220 | 0.071* | |
C4 | 0.1357 (4) | 0.2467 (2) | 0.3054 (3) | 0.0635 (8) | |
H4 | 0.1201 | 0.3201 | 0.3315 | 0.076* | |
C5 | 0.1921 (4) | 0.1566 (2) | 0.3930 (3) | 0.0538 (6) | |
H5 | 0.2141 | 0.1696 | 0.4778 | 0.065* | |
C6 | 0.2159 (3) | 0.04648 (18) | 0.3548 (2) | 0.0388 (5) | |
C7 | 0.2713 (3) | −0.05191 (17) | 0.4454 (2) | 0.0364 (5) | |
C8 | 0.3408 (3) | −0.1944 (2) | 0.6245 (2) | 0.0438 (5) | |
H8 | 0.3632 | −0.2404 | 0.6957 | 0.053* | |
C9 | 0.3587 (3) | −0.22941 (18) | 0.5206 (2) | 0.0386 (5) | |
C10 | 0.4173 (4) | −0.3472 (2) | 0.5075 (2) | 0.0455 (6) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Se1 | 0.0692 (2) | 0.04354 (17) | 0.04006 (17) | 0.01159 (11) | 0.02764 (14) | 0.00007 (10) |
O1 | 0.1212 (18) | 0.0434 (9) | 0.0619 (13) | 0.0252 (11) | 0.0600 (13) | 0.0203 (9) |
O2 | 0.1187 (17) | 0.0448 (10) | 0.0514 (12) | 0.0251 (10) | 0.0533 (12) | 0.0128 (8) |
N1 | 0.0453 (11) | 0.0337 (10) | 0.0362 (10) | 0.0043 (8) | 0.0191 (8) | 0.0046 (8) |
C1 | 0.0716 (18) | 0.0431 (14) | 0.0488 (16) | 0.0075 (12) | 0.0281 (14) | 0.0073 (11) |
C2 | 0.084 (2) | 0.0629 (18) | 0.0483 (17) | 0.0095 (15) | 0.0292 (15) | 0.0149 (14) |
C3 | 0.0576 (16) | 0.0517 (15) | 0.068 (2) | 0.0135 (12) | 0.0281 (14) | 0.0258 (14) |
C4 | 0.0721 (19) | 0.0394 (14) | 0.084 (2) | 0.0153 (13) | 0.0404 (17) | 0.0128 (13) |
C5 | 0.0674 (17) | 0.0421 (14) | 0.0571 (17) | 0.0113 (12) | 0.0331 (14) | 0.0054 (11) |
C6 | 0.0363 (12) | 0.0367 (12) | 0.0440 (13) | 0.0025 (9) | 0.0187 (10) | 0.0044 (9) |
C7 | 0.0371 (11) | 0.0357 (11) | 0.0354 (12) | 0.0012 (9) | 0.0157 (9) | 0.0013 (9) |
C8 | 0.0543 (14) | 0.0412 (12) | 0.0357 (13) | 0.0048 (11) | 0.0204 (11) | 0.0041 (10) |
C9 | 0.0438 (13) | 0.0357 (11) | 0.0360 (12) | 0.0027 (9) | 0.0179 (10) | 0.0031 (9) |
C10 | 0.0620 (15) | 0.0376 (12) | 0.0404 (13) | 0.0061 (11) | 0.0264 (12) | 0.0063 (10) |
Se1—C8 | 1.832 (2) | C2—H2 | 0.9300 |
Se1—C7 | 1.891 (2) | C3—C4 | 1.363 (4) |
O1—C10 | 1.284 (3) | C3—H3 | 0.9300 |
O1—H7 | 0.8201 | C4—C5 | 1.382 (4) |
O2—C10 | 1.230 (3) | C4—H4 | 0.9300 |
N1—C7 | 1.289 (3) | C5—C6 | 1.391 (3) |
N1—C9 | 1.381 (3) | C5—H5 | 0.9300 |
C1—C6 | 1.370 (4) | C6—C7 | 1.474 (3) |
C1—C2 | 1.390 (4) | C8—C9 | 1.344 (3) |
C1—H1 | 0.9300 | C8—H8 | 0.9300 |
C2—C3 | 1.372 (4) | C9—C10 | 1.473 (3) |
C8—Se1—C7 | 84.79 (10) | C6—C5—H5 | 119.9 |
C10—O1—H7 | 109.5 | C1—C6—C5 | 119.0 (2) |
C7—N1—C9 | 112.19 (19) | C1—C6—C7 | 119.7 (2) |
C6—C1—C2 | 120.4 (2) | C5—C6—C7 | 121.3 (2) |
C6—C1—H1 | 119.8 | N1—C7—C6 | 124.0 (2) |
C2—C1—H1 | 119.8 | N1—C7—Se1 | 114.10 (16) |
C3—C2—C1 | 120.1 (3) | C6—C7—Se1 | 121.82 (15) |
C3—C2—H2 | 120.0 | C9—C8—Se1 | 110.35 (17) |
C1—C2—H2 | 120.0 | C9—C8—H8 | 124.8 |
C4—C3—C2 | 119.9 (2) | Se1—C8—H8 | 124.8 |
C4—C3—H3 | 120.0 | C8—C9—N1 | 118.6 (2) |
C2—C3—H3 | 120.0 | C8—C9—C10 | 123.0 (2) |
C3—C4—C5 | 120.5 (3) | N1—C9—C10 | 118.48 (19) |
C3—C4—H4 | 119.8 | O2—C10—O1 | 123.5 (2) |
C5—C4—H4 | 119.8 | O2—C10—C9 | 121.9 (2) |
C4—C5—C6 | 120.1 (3) | O1—C10—C9 | 114.6 (2) |
C4—C5—H5 | 119.9 | ||
C6—C1—C2—C3 | −0.5 (5) | C5—C6—C7—Se1 | 12.7 (3) |
C1—C2—C3—C4 | 1.3 (5) | C8—Se1—C7—N1 | −0.22 (18) |
C2—C3—C4—C5 | −1.0 (4) | C8—Se1—C7—C6 | 177.7 (2) |
C3—C4—C5—C6 | 0.1 (4) | C7—Se1—C8—C9 | −0.05 (18) |
C2—C1—C6—C5 | −0.5 (4) | Se1—C8—C9—N1 | 0.3 (3) |
C2—C1—C6—C7 | 178.7 (3) | Se1—C8—C9—C10 | 179.96 (19) |
C4—C5—C6—C1 | 0.7 (4) | C7—N1—C9—C8 | −0.5 (3) |
C4—C5—C6—C7 | −178.4 (2) | C7—N1—C9—C10 | 179.8 (2) |
C9—N1—C7—C6 | −177.5 (2) | C8—C9—C10—O2 | −173.9 (3) |
C9—N1—C7—Se1 | 0.4 (2) | N1—C9—C10—O2 | 5.8 (4) |
C1—C6—C7—N1 | 11.4 (3) | C8—C9—C10—O1 | 5.3 (4) |
C5—C6—C7—N1 | −169.5 (2) | N1—C9—C10—O1 | −175.1 (2) |
C1—C6—C7—Se1 | −166.39 (19) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H7···O2i | 0.82 | 1.81 | 2.623 (2) | 171 |
Symmetry code: (i) −x+1, −y−1, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C10H7NO2Se |
Mr | 252.13 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 296 |
a, b, c (Å) | 8.0817 (3), 11.5661 (4), 11.6295 (4) |
β (°) | 117.168 (2) |
V (Å3) | 967.12 (6) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 3.85 |
Crystal size (mm) | 0.23 × 0.22 × 0.19 |
Data collection | |
Diffractometer | Bruker APEXII area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.437, 0.479 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 7502, 1705, 1487 |
Rint | 0.022 |
(sin θ/λ)max (Å−1) | 0.594 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.024, 0.063, 1.05 |
No. of reflections | 1705 |
No. of parameters | 127 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.43, −0.19 |
Computer programs: APEX2 (Bruker, 2006), SAINT (Bruker, 2006), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H7···O2i | 0.82 | 1.81 | 2.623 (2) | 171 |
Symmetry code: (i) −x+1, −y−1, −z+1. |
Acknowledgements
This project was supprted by the Natural Science of Fundation of Zhejiang (Y4080256) and the Zhejiang Students' Science and Technology Innovation Plan (Young Talent Plan) Aid.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
It has well been confirmed that the derivatives of selenazole are important in multiple fields such as chemistry and biochemistry owing to their biological activities (Srivastava et al., 1983;Boritzki et al.,1985). Interested in this field, we have been engaged in a major effort directed toward the development of syntheses of new selenazole carboxylic acid and their transition metal complexes. In a few of articles we have reported our partial research results (Zhao et al., 2010;Shen et al., 2011). Herein,we crystallize the organic ligand 2-phenyl-4-selenazole carboxylic acid.
The structure of the title, (C10H7NO2Se),suitable for X-ray, was obtained by chance. The structure of the complex is shown in Fig.1, which reveals that all atoms in each molecule are nearly coplanar in the centrosymmetric unit. The molecule is essentially planar with the dihedral angle between two neighboring rings are 12.415 (89)°. In the molecule of 2-phenyl-4-selenazole carboxylic acid,the Se—C bond length range from 1.832 (2) Å-1.891 (2)Å and the angle C—Se—C is 84.78 (10)°.
The molecules arranged in the crystal at regular intervals with O—H···O hydrogen bonds. The end to end hydrogen-bonding interactions lead to the formation a one-dimensional structure framework along the b axis, Fig 2. Between adjacent triple-helix chains there exist weak π···π interactions.