Experimental
Crystal data
C13H10O3 Mr = 214.21 Monoclinic, P 21 /n a = 8.6500 (7) Å b = 5.5077 (5) Å c = 20.9655 (18) Å β = 94.145 (3)° V = 996.22 (15) Å3 Z = 4 Mo Kα radiation μ = 0.10 mm−1 T = 293 (2) K 0.21 × 0.20 × 0.16 mm
|
Data collection
Bruker APEXII area-detector diffractometer Absorption correction: none 6310 measured reflections 1800 independent reflections 854 reflections with I > 2σ(I) Rint = 0.063
|
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A | O2—H2⋯O1i | 0.82 | 1.82 | 2.624 (3) | 168 | O3—H3A⋯O3ii | 0.82 | 2.20 | 3.0041 (18) | 168 | Symmetry codes: (i) -x+3, -y, -z; (ii) . | |
Data collection: APEX2 (Bruker, 2004
); cell refinement: APEX2; data reduction: APEX2; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008
); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008
); molecular graphics: XP in SHELXTL (Sheldrick, 2008
); software used to prepare material for publication: SHELXTL.
Supporting information
4-Hydroxyl-biphenyl-4'-carboxylic acid was dissolved in a hot ethanol-water solution (1:1; v/v) with stirring. Colorless single crystals suitable for X-ray diffraction were obtained at room temperature by slow evaporation of the solvent over a period of several days.
In the initial refinement with disorder not taken into account one of phenyl rings showed significantly elongated thermal ellipsoids indicating disorder, the dihedral angle between two phenyl rings is 5.66 (2) /%A, and the adjacent distances of C-H···C-H interactions in the biphenylene are 2.044 (1) and 2.077 (1) /%A, respectively, thus leading to a static repulsion between two phenyl rings,and the phenyl ring was thus refined as being disordered over two positions. The occupancy ratio refined to 0.57 (2) to 0.43 (2). The adps of the disordered atoms were restrained to be close to isotropic and those of equivalent atoms were set to be identical. Carbon-bound, hydroxyl and carboxylate group H atoms were placed at calculated positions and were treated as riding on their parent C or O atoms with C—H = 0.93 Å, with Uiso(H) = 1.2 Ueq(C); O—H = 0.82 Å and with Uiso(H) = 1.5 Ueq(O).
Data collection: APEX2 (Bruker, 2004); cell refinement: APEX2 (Bruker, 2004); data reduction: APEX2 (Bruker, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP in SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).
4'-Hydroxybiphenyl-4-carboxylic acid
top Crystal data top C13H10O3 | F(000) = 448 |
Mr = 214.21 | Dx = 1.428 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 1560 reflections |
a = 8.6500 (7) Å | θ = 1.4–28.0° |
b = 5.5077 (5) Å | µ = 0.10 mm−1 |
c = 20.9655 (18) Å | T = 293 K |
β = 94.145 (3)° | Plate, colorless |
V = 996.22 (15) Å3 | 0.21 × 0.20 × 0.16 mm |
Z = 4 | |
Data collection top Bruker APEXII area-detector diffractometer | 854 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.063 |
Graphite monochromator | θmax = 25.2°, θmin = 2.0° |
ϕ and ω scans | h = −10→10 |
6310 measured reflections | k = −5→6 |
1800 independent reflections | l = −24→25 |
Refinement top 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)] = 0.058 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.183 | H-atom parameters constrained |
S = 1.01 | w = 1/[σ2(Fo2) + (0.0772P)2] where P = (Fo2 + 2Fc2)/3 |
1800 reflections | (Δ/σ)max < 0.001 |
160 parameters | Δρmax = 0.18 e Å−3 |
24 restraints | Δρmin = −0.19 e Å−3 |
Crystal data top C13H10O3 | V = 996.22 (15) Å3 |
Mr = 214.21 | Z = 4 |
Monoclinic, P21/n | Mo Kα radiation |
a = 8.6500 (7) Å | µ = 0.10 mm−1 |
b = 5.5077 (5) Å | T = 293 K |
c = 20.9655 (18) Å | 0.21 × 0.20 × 0.16 mm |
β = 94.145 (3)° | |
Data collection top Bruker APEXII area-detector diffractometer | 854 reflections with I > 2σ(I) |
6310 measured reflections | Rint = 0.063 |
1800 independent reflections | |
Refinement top R[F2 > 2σ(F2)] = 0.058 | 24 restraints |
wR(F2) = 0.183 | H-atom parameters constrained |
S = 1.01 | Δρmax = 0.18 e Å−3 |
1800 reflections | Δρmin = −0.19 e Å−3 |
160 parameters | |
Special details top 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | Occ. (<1) |
C1 | 1.3074 (3) | 0.0387 (7) | 0.03781 (15) | 0.0499 (9) | |
C8 | 0.7212 (3) | 0.1508 (6) | 0.15024 (14) | 0.0448 (8) | |
C9 | 0.6208 (3) | 0.3440 (6) | 0.13452 (16) | 0.0578 (10) | |
H9 | 0.6499 | 0.4597 | 0.1054 | 0.069* | |
C10 | 0.4806 (3) | 0.3688 (7) | 0.16071 (17) | 0.0593 (10) | |
H10 | 0.4167 | 0.4999 | 0.1493 | 0.071* | |
C11 | 0.4352 (3) | 0.2019 (7) | 0.20337 (15) | 0.0525 (9) | |
C12 | 0.5302 (4) | 0.0092 (7) | 0.22074 (16) | 0.0596 (10) | |
H12 | 0.5001 | −0.1052 | 0.2500 | 0.072* | |
C13 | 0.6703 (4) | −0.0119 (6) | 0.19414 (15) | 0.0545 (9) | |
H13 | 0.7339 | −0.1424 | 0.2064 | 0.065* | |
O1 | 1.3852 (2) | −0.1522 (5) | 0.05016 (11) | 0.0704 (8) | |
O2 | 1.3483 (2) | 0.2037 (5) | 0.00069 (12) | 0.0696 (8) | |
H2 | 1.4342 | 0.1717 | −0.0112 | 0.104* | |
O3 | 0.2936 (3) | 0.2362 (5) | 0.22900 (12) | 0.0720 (8) | |
H3A | 0.2672 | 0.1099 | 0.2458 | 0.108* | |
C2 | 1.15866 (19) | 0.0702 (5) | 0.06838 (10) | 0.0480 (8) | 0.43 (2) |
C3 | 1.0867 (8) | 0.2959 (6) | 0.0682 (6) | 0.052 (3) | 0.43 (2) |
H3 | 1.1327 | 0.4288 | 0.0498 | 0.063* | 0.43 (2) |
C4 | 0.9458 (8) | 0.3228 (6) | 0.0954 (6) | 0.045 (2) | 0.43 (2) |
H4 | 0.8976 | 0.4738 | 0.0952 | 0.054* | 0.43 (2) |
C5 | 0.8770 (2) | 0.1241 (4) | 0.12279 (11) | 0.0441 (8) | 0.43 (2) |
C6 | 0.9490 (7) | −0.1015 (7) | 0.1230 (5) | 0.045 (3) | 0.43 (2) |
H6 | 0.9029 | −0.2345 | 0.1413 | 0.054* | 0.43 (2) |
C7 | 1.0898 (8) | −0.1285 (7) | 0.0958 (6) | 0.052 (3) | 0.43 (2) |
H7 | 1.1380 | −0.2795 | 0.0959 | 0.062* | 0.43 (2) |
C2' | 1.15879 (19) | 0.0709 (5) | 0.06822 (10) | 0.0480 (8) | 0.57 (2) |
C3' | 1.0571 (7) | 0.2579 (15) | 0.0469 (5) | 0.052 (2) | 0.57 (2) |
H3' | 1.0845 | 0.3647 | 0.0153 | 0.063* | 0.57 (2) |
C4' | 0.9160 (7) | 0.2818 (15) | 0.0734 (5) | 0.049 (2) | 0.57 (2) |
H4' | 0.8485 | 0.4045 | 0.0588 | 0.059* | 0.57 (2) |
C5' | 0.8725 (2) | 0.1234 (5) | 0.12205 (11) | 0.0441 (8) | 0.57 (2) |
C6' | 0.9755 (6) | −0.0581 (16) | 0.1431 (4) | 0.048 (2) | 0.57 (2) |
H6' | 0.9505 | −0.1621 | 0.1758 | 0.057* | 0.57 (2) |
C7' | 1.1161 (6) | −0.0845 (15) | 0.1155 (4) | 0.047 (2) | 0.57 (2) |
H7' | 1.1827 | −0.2097 | 0.1291 | 0.056* | 0.57 (2) |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
C1 | 0.0396 (18) | 0.061 (2) | 0.051 (2) | 0.0010 (18) | 0.0134 (16) | 0.0005 (19) |
C8 | 0.0388 (17) | 0.044 (2) | 0.0527 (18) | −0.0001 (16) | 0.0113 (15) | −0.0022 (17) |
C9 | 0.0445 (19) | 0.058 (2) | 0.073 (2) | 0.0005 (18) | 0.0159 (17) | 0.011 (2) |
C10 | 0.0418 (19) | 0.057 (2) | 0.081 (2) | 0.0079 (18) | 0.0170 (18) | 0.008 (2) |
C11 | 0.0338 (17) | 0.062 (3) | 0.064 (2) | −0.0032 (17) | 0.0160 (15) | −0.0135 (19) |
C12 | 0.049 (2) | 0.061 (3) | 0.071 (2) | 0.0015 (18) | 0.0214 (18) | 0.0075 (19) |
C13 | 0.0448 (19) | 0.051 (2) | 0.069 (2) | 0.0088 (17) | 0.0183 (17) | 0.0053 (18) |
O1 | 0.0529 (15) | 0.0705 (18) | 0.0910 (18) | 0.0171 (13) | 0.0281 (13) | 0.0188 (15) |
O2 | 0.0460 (14) | 0.083 (2) | 0.0837 (18) | 0.0127 (13) | 0.0307 (13) | 0.0194 (15) |
O3 | 0.0418 (13) | 0.090 (2) | 0.0882 (18) | 0.0033 (13) | 0.0308 (12) | −0.0057 (16) |
C2 | 0.0334 (17) | 0.062 (2) | 0.050 (2) | −0.0008 (17) | 0.0144 (15) | 0.0031 (18) |
C3 | 0.040 (5) | 0.065 (7) | 0.054 (5) | 0.002 (5) | 0.015 (4) | 0.006 (5) |
C4 | 0.046 (5) | 0.047 (6) | 0.043 (5) | 0.005 (4) | 0.012 (4) | 0.000 (4) |
C5 | 0.0367 (17) | 0.049 (2) | 0.0476 (19) | −0.0041 (16) | 0.0129 (14) | 0.0004 (17) |
C6 | 0.045 (5) | 0.052 (5) | 0.039 (5) | −0.002 (4) | 0.002 (4) | −0.008 (4) |
C7 | 0.041 (5) | 0.061 (7) | 0.052 (5) | 0.003 (4) | 0.001 (4) | −0.001 (5) |
C2' | 0.0334 (17) | 0.062 (2) | 0.050 (2) | −0.0008 (17) | 0.0144 (15) | 0.0031 (18) |
C3' | 0.044 (4) | 0.057 (5) | 0.058 (4) | 0.004 (3) | 0.014 (4) | 0.008 (4) |
C4' | 0.042 (4) | 0.049 (4) | 0.057 (4) | 0.012 (3) | 0.014 (3) | 0.000 (4) |
C5' | 0.0367 (17) | 0.049 (2) | 0.0476 (19) | −0.0041 (16) | 0.0129 (14) | 0.0004 (17) |
C6' | 0.036 (4) | 0.068 (5) | 0.039 (4) | 0.007 (3) | 0.010 (3) | 0.009 (4) |
C7' | 0.029 (3) | 0.063 (5) | 0.049 (4) | 0.011 (3) | 0.005 (3) | 0.007 (4) |
Geometric parameters (Å, º) top C1—O2 | 1.264 (4) | C3—C4 | 1.3900 |
C1—O1 | 1.265 (4) | C3—H3 | 0.9300 |
C1—C2 | 1.488 (4) | C4—C5 | 1.3900 |
C8—C13 | 1.379 (4) | C4—H4 | 0.9300 |
C8—C9 | 1.398 (4) | C5—C6 | 1.3900 |
C8—C5 | 1.510 (3) | C6—C7 | 1.3900 |
C9—C10 | 1.374 (4) | C6—H6 | 0.9300 |
C9—H9 | 0.9300 | C7—H7 | 0.9300 |
C10—C11 | 1.360 (5) | C2'—C7' | 1.3793 |
C10—H10 | 0.9300 | C2'—C3' | 1.4061 |
C11—C12 | 1.375 (4) | C3'—C4' | 1.3820 |
C11—O3 | 1.386 (4) | C3'—H3' | 0.9300 |
C12—C13 | 1.375 (4) | C4'—C5' | 1.4147 |
C12—H12 | 0.9300 | C4'—H4' | 0.9300 |
C13—H13 | 0.9300 | C5'—C6' | 1.3903 |
O2—H2 | 0.8200 | C6'—C7' | 1.3923 |
O3—H3A | 0.8200 | C6'—H6' | 0.9300 |
C2—C3 | 1.3900 | C7'—H7' | 0.9300 |
C2—C7 | 1.3900 | | |
| | | |
O2—C1—O1 | 123.7 (3) | C3—C4—C5 | 120.0 |
O2—C1—C2 | 118.1 (3) | C3—C4—H4 | 120.0 |
O1—C1—C2 | 118.2 (3) | C5—C4—H4 | 120.0 |
C13—C8—C9 | 115.4 (3) | C6—C5—C4 | 120.0 |
C13—C8—C5 | 121.9 (3) | C6—C5—C8 | 119.8 (2) |
C9—C8—C5 | 122.7 (3) | C4—C5—C8 | 120.1 (2) |
C10—C9—C8 | 122.2 (3) | C5—C6—C7 | 120.0 |
C10—C9—H9 | 118.9 | C5—C6—H6 | 120.0 |
C8—C9—H9 | 118.9 | C7—C6—H6 | 120.0 |
C11—C10—C9 | 120.1 (3) | C6—C7—C2 | 120.0 |
C11—C10—H10 | 120.0 | C6—C7—H7 | 120.0 |
C9—C10—H10 | 120.0 | C2—C7—H7 | 120.0 |
C10—C11—C12 | 120.1 (3) | C7'—C2'—C3' | 119.2 |
C10—C11—O3 | 117.9 (3) | C4'—C3'—C2' | 119.5 |
C12—C11—O3 | 122.0 (3) | C4'—C3'—H3' | 120.2 |
C11—C12—C13 | 119.0 (3) | C2'—C3'—H3' | 120.2 |
C11—C12—H12 | 120.5 | C3'—C4'—C5' | 121.3 |
C13—C12—H12 | 120.5 | C3'—C4'—H4' | 119.4 |
C12—C13—C8 | 123.3 (3) | C5'—C4'—H4' | 119.4 |
C12—C13—H13 | 118.4 | C6'—C5'—C4' | 118.4 |
C8—C13—H13 | 118.4 | C5'—C6'—C7' | 120.1 |
C3—C2—C7 | 120.0 | C5'—C6'—H6' | 120.0 |
C3—C2—C1 | 120.3 (2) | C7'—C6'—H6' | 120.0 |
C7—C2—C1 | 119.7 (2) | C2'—C7'—C6' | 121.5 |
C4—C3—C2 | 120.0 | C2'—C7'—H7' | 119.3 |
C4—C3—H3 | 120.0 | C6'—C7'—H7' | 119.3 |
C2—C3—H3 | 120.0 | | |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
O2—H2···O1i | 0.82 | 1.82 | 2.624 (3) | 168 |
O3—H3A···O3ii | 0.82 | 2.20 | 3.0041 (18) | 168 |
Symmetry codes: (i) −x+3, −y, −z; (ii) −x+1/2, y−1/2, −z+1/2. |
Experimental details
Crystal data |
Chemical formula | C13H10O3 |
Mr | 214.21 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 293 |
a, b, c (Å) | 8.6500 (7), 5.5077 (5), 20.9655 (18) |
β (°) | 94.145 (3) |
V (Å3) | 996.22 (15) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.10 |
Crystal size (mm) | 0.21 × 0.20 × 0.16 |
|
Data collection |
Diffractometer | Bruker APEXII area-detector diffractometer |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6310, 1800, 854 |
Rint | 0.063 |
(sin θ/λ)max (Å−1) | 0.599 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.058, 0.183, 1.01 |
No. of reflections | 1800 |
No. of parameters | 160 |
No. of restraints | 24 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.18, −0.19 |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
O2—H2···O1i | 0.82 | 1.82 | 2.624 (3) | 167.6 |
O3—H3A···O3ii | 0.82 | 2.20 | 3.0041 (18) | 167.6 |
Symmetry codes: (i) −x+3, −y, −z; (ii) −x+1/2, y−1/2, −z+1/2. |
Acknowledgements
The author thanks South China Normal University for supporting this study.
References
Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. 34, 1555–1573. CrossRef CAS Web of Science Google Scholar
Bruker (2004). APEX2 and SMART. Bruker AXS Inc, Madison, Wisconsin, USA. Google Scholar
Datta, A. & Pati, S. K. (2006). Chem. Soc. Rev. pp. 1305–1323. Web of Science CrossRef Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Zwier, T. S. (1996). Annu. Rev. Phys. Chem. 47, 205–241. CrossRef CAS Web of Science Google Scholar
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Hydrogen-bonding interactions between ligands are specific and directional. When present in metal complexes they usually do not rely on the properties of the metal ions, but they play an important role in the overall structures and functions of the complexes and the way in which they pack in the solid state (Zwier et al., 1996; Datta & Pati, 2006). In this context we report here the crystal structure of the title compound, (I).
The molecular structure of (I) is shown in Fig. 1. The C—O and C—C bond distances show no remarkable features. The title molecular structure acts as both a hydrogen bonding donor and acceptor, forming dimers with neighboring molecules through O—H···O hydrogen bonding with a R22(8) graph set motif (Bernstein et al., 1995). A second hydrogen bonding interaction by the hydroxyl groups forms a chain and extends the structure into a lamellar layer (Table 1, Fig. 2).