organic compounds
4-(4-Pyridyl)pyridinium 3′,4,4′-tricarboxybiphenyl-3-carboxylate dihydrate
aSchool of Chemistry and Environment, South China Normal University, Guangzhou 510006, People's Republic of China, and bSchool of Chemistry and Environment, South China Normal University, Guangzhou 510006, People's Republic of China, and, South China Normal University, Key Laboratory of Technology of Electrochemical Energy Storage and Power Generation in Guangdong Universities, Guangzhou 510006, People's Republic of China
*Correspondence e-mail: luoyf2004@yahoo.com.cn
In the title compound, C10H9N2+·C16H9O8−·2H2O, both the cation and anion possess crystallographically imposed centres of symmetry, causing the nitrogen-bound H atom in the 4-(4-pyridyl)pyridinium cation and the acidic H atom of the carboxylate groups at the 3 and 3′ positions in the anion to be disordered over two positions with equal occupancies. In the crystal packing, the cations, anions and water molecules are connected by O—H⋯O, C—H⋯O and N—H⋯N hydrogen bonds, forming layers parallel to (20). These layer are further connected into a three-dimensional supramolecular network by O—H⋯O hydrogen bonds involving the water molecules as H-atom donors and by weak π–π stacking interactions between neighbouring benzene and pyridine rings, with centroid–centroid distances of 3.756 (5) Å.
Experimental
Crystal data
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Data collection
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Refinement
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Data collection: APEX2 (Bruker, 2005); cell 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: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.
Supporting information
10.1107/S1600536809050831/rz2388sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536809050831/rz2388Isup2.hkl
A mixture of 4,4'-bipyridine (0.078 g, 0.5 mmol), 4-4'-dicarboxybiphenyl-3-3'dicarboxylic acid (0.165 g; 0.5 mmol), water (10 mL) was stirred vigorously for 30 min and then sealed in a Teflon-lined stainless-steel autoclave (25 mL capacity). The autoclave was heated and maintained at 433K for 3 days, and then cooled to room temperature at 5Kh-1 to obtain colourless block crystals suitable for X-ray analysis.
Water H atoms were located in a difference Fourier map and refined with the O–H distance restrained to 0.84 Å and with Uiso(H) = 1.5 Ueq(O). The H atom bound to the N1 nitrogen atom in the cation and the carboxylic H atoms were refined with distance restraints of N–H = 0.90 Å and O–H = 0.90 Å, respectively. The H1A and H2A hydrogen atoms are disordered over two centrosymmetrically related positions and were therefore refined with site occupancies of 0.5. All other H atoms were placed at calculated positions and treated as riding on the parent atoms, with C–H = 0.93Å, and with Uiso(H) = 1.2 Ueq(C).
Data collection: APEX2 (Bruker, 2005); cell
SAINT (Bruker, 2005); data reduction: SAINT (Bruker, 2005); 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: SHELXTL (Sheldrick, 2008).Fig. 1. The molecular structure of the title compound showing the atomic-numbering scheme and 50% probability ellipsoids. Only one position of the disordered H atoms in the cation and anion is shown. Symmetry codes: (i) 1-x, 2-y, -z; (ii) 2-x, -y, 1-z; (iii) -x, 1-y, -z. | |
Fig. 2. Partial packing diagram of the title compound showing the layered network formed by intermolecular O—H···O, C—H···O and N—H···N hydrogen bonds (dashed lines). Both positions of the disordered H atoms in the cation and anions are shown. |
C10H9N2+·C16H9O8−·2H2O | Z = 1 |
Mr = 522.46 | F(000) = 272 |
Triclinic, P1 | Dx = 1.498 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.1955 (8) Å | Cell parameters from 2061 reflections |
b = 8.935 (1) Å | θ = 2.4–28.2° |
c = 9.8847 (11) Å | µ = 0.12 mm−1 |
α = 90.7920 (11)° | T = 296 K |
β = 106.4850 (13)° | Block, colourless |
γ = 107.1180 (15)° | 0.23 × 0.21 × 0.19 mm |
V = 579.09 (11) Å3 |
Bruker APEXII area-detector diffractometer | 1818 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.014 |
Graphite monochromator | θmax = 25.2°, θmin = 2.2° |
ϕ and ω scan | h = −7→8 |
2990 measured reflections | k = −10→9 |
2050 independent reflections | l = −11→11 |
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)] = 0.039 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.112 | w = 1/[σ2(Fo2) + (0.0562P)2 + 0.2257P] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max < 0.001 |
2050 reflections | Δρmax = 0.32 e Å−3 |
180 parameters | Δρmin = −0.25 e Å−3 |
3 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.071 (9) |
C10H9N2+·C16H9O8−·2H2O | γ = 107.1180 (15)° |
Mr = 522.46 | V = 579.09 (11) Å3 |
Triclinic, P1 | Z = 1 |
a = 7.1955 (8) Å | Mo Kα radiation |
b = 8.935 (1) Å | µ = 0.12 mm−1 |
c = 9.8847 (11) Å | T = 296 K |
α = 90.7920 (11)° | 0.23 × 0.21 × 0.19 mm |
β = 106.4850 (13)° |
Bruker APEXII area-detector diffractometer | 1818 reflections with I > 2σ(I) |
2990 measured reflections | Rint = 0.014 |
2050 independent reflections |
R[F2 > 2σ(F2)] = 0.039 | 3 restraints |
wR(F2) = 0.112 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.03 | Δρmax = 0.32 e Å−3 |
2050 reflections | Δρmin = −0.25 e Å−3 |
180 parameters |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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 | Occ. (<1) | |
C1 | 0.4881 (3) | 1.01415 (19) | 0.18864 (18) | 0.0405 (4) | |
H1 | 0.5318 | 1.1230 | 0.2095 | 0.049* | |
C2 | 0.4740 (2) | 0.94960 (17) | 0.05542 (16) | 0.0321 (4) | |
C3 | 0.4103 (3) | 0.78512 (18) | 0.03012 (17) | 0.0361 (4) | |
H3 | 0.4008 | 0.7393 | −0.0576 | 0.043* | |
C4 | 0.3611 (2) | 0.68843 (17) | 0.13133 (17) | 0.0333 (4) | |
C5 | 0.3102 (3) | 0.51258 (19) | 0.09704 (18) | 0.0397 (4) | |
C6 | 0.3725 (2) | 0.75584 (18) | 0.26291 (16) | 0.0344 (4) | |
C7 | 0.3003 (3) | 0.65386 (19) | 0.36673 (18) | 0.0389 (4) | |
C8 | 0.4384 (3) | 0.91911 (19) | 0.28990 (18) | 0.0407 (4) | |
H8 | 0.4490 | 0.9650 | 0.3779 | 0.049* | |
C9 | 0.9236 (3) | −0.1318 (2) | 0.19327 (19) | 0.0447 (4) | |
H9 | 0.8726 | −0.2254 | 0.1336 | 0.054* | |
C10 | 0.9232 (3) | −0.13691 (19) | 0.33220 (18) | 0.0412 (4) | |
H10 | 0.8722 | −0.2331 | 0.3647 | 0.049* | |
C11 | 0.9987 (2) | 0.00096 (18) | 0.42445 (17) | 0.0351 (4) | |
C12 | 1.0714 (3) | 0.1400 (2) | 0.3674 (2) | 0.0490 (5) | |
H12 | 1.1234 | 0.2355 | 0.4243 | 0.059* | |
C13 | 1.0666 (3) | 0.1367 (2) | 0.2273 (2) | 0.0524 (5) | |
H13 | 1.1151 | 0.2311 | 0.1914 | 0.063* | |
N1 | 0.9947 (2) | 0.00297 (17) | 0.14119 (15) | 0.0428 (4) | |
H1A | 0.997 (7) | 0.004 (5) | 0.049 (2) | 0.051* | 0.50 |
O1 | 0.4404 (2) | 0.44851 (15) | 0.14281 (16) | 0.0572 (4) | |
O3 | 0.1949 (2) | 0.51807 (15) | 0.33352 (14) | 0.0596 (4) | |
O4 | 0.3524 (3) | 0.72538 (16) | 0.49433 (14) | 0.0647 (5) | |
H4A | 0.3092 | 0.6627 | 0.5465 | 0.097* | |
O1W | 0.2145 (3) | 0.5413 (2) | 0.66452 (17) | 0.0799 (6) | |
H1W | 0.3004 | 0.5290 | 0.7356 | 0.120* | |
H2W | 0.1031 | 0.5241 | 0.6817 | 0.120* | |
O2 | 0.1336 (2) | 0.43770 (14) | 0.01377 (15) | 0.0520 (4) | |
H2A | 0.040 (8) | 0.490 (8) | 0.001 (8) | 0.078* | 0.50 |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0520 (10) | 0.0255 (8) | 0.0388 (9) | 0.0025 (7) | 0.0159 (8) | −0.0015 (7) |
C2 | 0.0325 (8) | 0.0276 (8) | 0.0339 (8) | 0.0060 (6) | 0.0100 (6) | 0.0017 (6) |
C3 | 0.0467 (9) | 0.0279 (8) | 0.0327 (8) | 0.0081 (7) | 0.0141 (7) | −0.0006 (6) |
C4 | 0.0346 (8) | 0.0277 (8) | 0.0352 (8) | 0.0066 (6) | 0.0102 (6) | 0.0025 (6) |
C5 | 0.0549 (10) | 0.0293 (8) | 0.0396 (9) | 0.0115 (8) | 0.0231 (8) | 0.0057 (7) |
C6 | 0.0353 (8) | 0.0308 (8) | 0.0339 (8) | 0.0054 (6) | 0.0104 (7) | 0.0027 (6) |
C7 | 0.0447 (9) | 0.0324 (8) | 0.0376 (9) | 0.0063 (7) | 0.0152 (7) | 0.0023 (7) |
C8 | 0.0526 (10) | 0.0325 (8) | 0.0323 (9) | 0.0041 (7) | 0.0153 (7) | −0.0022 (7) |
C9 | 0.0530 (11) | 0.0371 (9) | 0.0421 (10) | 0.0122 (8) | 0.0135 (8) | −0.0016 (7) |
C10 | 0.0513 (10) | 0.0285 (8) | 0.0431 (10) | 0.0093 (7) | 0.0163 (8) | 0.0035 (7) |
C11 | 0.0373 (8) | 0.0286 (8) | 0.0391 (9) | 0.0092 (6) | 0.0119 (7) | 0.0039 (6) |
C12 | 0.0691 (13) | 0.0293 (9) | 0.0425 (10) | 0.0041 (8) | 0.0190 (9) | 0.0022 (7) |
C13 | 0.0714 (13) | 0.0379 (10) | 0.0451 (10) | 0.0079 (9) | 0.0226 (9) | 0.0093 (8) |
N1 | 0.0516 (9) | 0.0454 (8) | 0.0332 (8) | 0.0152 (7) | 0.0151 (7) | 0.0064 (6) |
O1 | 0.0725 (10) | 0.0442 (7) | 0.0666 (9) | 0.0307 (7) | 0.0254 (7) | 0.0142 (6) |
O3 | 0.0830 (10) | 0.0355 (7) | 0.0522 (8) | −0.0054 (7) | 0.0330 (7) | 0.0011 (6) |
O4 | 0.0976 (11) | 0.0443 (8) | 0.0368 (7) | −0.0065 (7) | 0.0266 (7) | 0.0019 (6) |
O1W | 0.0693 (10) | 0.0986 (13) | 0.0630 (10) | 0.0071 (9) | 0.0252 (8) | 0.0340 (9) |
O2 | 0.0599 (9) | 0.0273 (6) | 0.0601 (8) | 0.0046 (6) | 0.0146 (7) | −0.0086 (6) |
C1—C8 | 1.378 (2) | C9—N1 | 1.334 (2) |
C1—C2 | 1.395 (2) | C9—C10 | 1.375 (3) |
C1—H1 | 0.9300 | C9—H9 | 0.9300 |
C2—C3 | 1.400 (2) | C10—C11 | 1.392 (2) |
C2—C2i | 1.488 (3) | C10—H10 | 0.9300 |
C3—C4 | 1.385 (2) | C11—C12 | 1.392 (2) |
C3—H3 | 0.9300 | C11—C11ii | 1.489 (3) |
C4—C6 | 1.397 (2) | C12—C13 | 1.375 (3) |
C4—C5 | 1.514 (2) | C12—H12 | 0.9300 |
C5—O1 | 1.222 (2) | C13—N1 | 1.334 (2) |
C5—O2 | 1.277 (2) | C13—H13 | 0.9300 |
C6—C8 | 1.391 (2) | N1—H1A | 0.921 (18) |
C6—C7 | 1.484 (2) | O4—H4A | 0.8200 |
C7—O3 | 1.209 (2) | O1W—H1W | 0.8263 |
C7—O4 | 1.307 (2) | O1W—H2W | 0.8370 |
C8—H8 | 0.9300 | O2—H2A | 0.911 (19) |
C8—C1—C2 | 121.02 (15) | C6—C8—H8 | 119.4 |
C8—C1—H1 | 119.5 | N1—C9—C10 | 122.24 (16) |
C2—C1—H1 | 119.5 | N1—C9—H9 | 118.9 |
C1—C2—C3 | 117.26 (15) | C10—C9—H9 | 118.9 |
C1—C2—C2i | 121.74 (17) | C9—C10—C11 | 120.39 (16) |
C3—C2—C2i | 121.00 (17) | C9—C10—H10 | 119.8 |
C4—C3—C2 | 122.24 (15) | C11—C10—H10 | 119.8 |
C4—C3—H3 | 118.9 | C10—C11—C12 | 116.23 (16) |
C2—C3—H3 | 118.9 | C10—C11—C11ii | 121.63 (18) |
C3—C4—C6 | 119.43 (14) | C12—C11—C11ii | 122.14 (18) |
C3—C4—C5 | 117.83 (14) | C13—C12—C11 | 120.36 (16) |
C6—C4—C5 | 122.62 (14) | C13—C12—H12 | 119.8 |
O1—C5—O2 | 122.14 (16) | C11—C12—H12 | 119.8 |
O1—C5—C4 | 119.75 (16) | N1—C13—C12 | 122.31 (17) |
O2—C5—C4 | 117.99 (15) | N1—C13—H13 | 118.8 |
C8—C6—C4 | 118.80 (15) | C12—C13—H13 | 118.8 |
C8—C6—C7 | 121.15 (14) | C13—N1—C9 | 118.47 (15) |
C4—C6—C7 | 119.90 (14) | C13—N1—H1A | 120 (3) |
O3—C7—O4 | 123.27 (16) | C9—N1—H1A | 121 (3) |
O3—C7—C6 | 122.33 (15) | C7—O4—H4A | 109.5 |
O4—C7—C6 | 114.33 (14) | H1W—O1W—H2W | 109.1 |
C1—C8—C6 | 121.24 (15) | C5—O2—H2A | 115 (5) |
C1—C8—H8 | 119.4 |
Symmetry codes: (i) −x+1, −y+2, −z; (ii) −x+2, −y, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···N1iii | 0.92 (2) | 1.89 (2) | 2.814 (3) | 177 (4) |
O4—H4A···O1W | 0.82 | 1.75 | 2.5657 (19) | 176 |
O1W—H1W···O1iv | 0.83 | 1.86 | 2.642 (2) | 157 |
O1W—H2W···O3v | 0.84 | 2.03 | 2.841 (2) | 165 |
O2—H2A···O2vi | 0.91 (2) | 1.54 (2) | 2.446 (3) | 173 (7) |
C3—H3···O1vii | 0.93 | 2.54 | 3.270 (2) | 135 |
C13—H13···O2viii | 0.93 | 2.57 | 3.448 (2) | 159 |
C9—H9···O2ix | 0.93 | 2.36 | 3.246 (2) | 160 |
Symmetry codes: (iii) −x+2, −y, −z; (iv) −x+1, −y+1, −z+1; (v) −x, −y+1, −z+1; (vi) −x, −y+1, −z; (vii) −x+1, −y+1, −z; (viii) x+1, y, z; (ix) −x+1, −y, −z. |
Experimental details
Crystal data | |
Chemical formula | C10H9N2+·C16H9O8−·2H2O |
Mr | 522.46 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 296 |
a, b, c (Å) | 7.1955 (8), 8.935 (1), 9.8847 (11) |
α, β, γ (°) | 90.7920 (11), 106.4850 (13), 107.1180 (15) |
V (Å3) | 579.09 (11) |
Z | 1 |
Radiation type | Mo Kα |
µ (mm−1) | 0.12 |
Crystal size (mm) | 0.23 × 0.21 × 0.19 |
Data collection | |
Diffractometer | Bruker APEXII area-detector diffractometer |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 2990, 2050, 1818 |
Rint | 0.014 |
(sin θ/λ)max (Å−1) | 0.599 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.039, 0.112, 1.03 |
No. of reflections | 2050 |
No. of parameters | 180 |
No. of restraints | 3 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.32, −0.25 |
Computer programs: APEX2 (Bruker, 2005), SAINT (Bruker, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···N1i | 0.921 (18) | 1.894 (19) | 2.814 (3) | 177 (4) |
O4—H4A···O1W | 0.82 | 1.75 | 2.5657 (19) | 175.5 |
O1W—H1W···O1ii | 0.83 | 1.86 | 2.642 (2) | 157.0 |
O1W—H2W···O3iii | 0.84 | 2.03 | 2.841 (2) | 164.7 |
O2—H2A···O2iv | 0.911 (19) | 1.54 (2) | 2.446 (3) | 173 (7) |
C3—H3···O1v | 0.93 | 2.54 | 3.270 (2) | 135.4 |
C13—H13···O2vi | 0.93 | 2.57 | 3.448 (2) | 158.6 |
C9—H9···O2vii | 0.93 | 2.36 | 3.246 (2) | 159.6 |
Symmetry codes: (i) −x+2, −y, −z; (ii) −x+1, −y+1, −z+1; (iii) −x, −y+1, −z+1; (iv) −x, −y+1, −z; (v) −x+1, −y+1, −z; (vi) x+1, y, z; (vii) −x+1, −y, −z. |
Acknowledgements
The authors acknowledge the Chan Xue Yan Cooperative Special Project of Guangdong Province, the Ministry of Science and Technology (project No. 2007A090302046), the Project of Science and Technology of Guangdong Province (project No. 2007A020200002-4) and the Natural Science Foundation of Guangdong Province (No. 9151063101000037) for supporting this work.
References
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In recent years, research on coordination polymers has made considerable progress in the fields of supramolecular chemistry and crystal engineering, because of their intriguing structural motifs and functional properties, such as molecular adsorption, magnetism, and luminescence. In general, hydrogen bonding interactions between ligands are specific and directional. In this context, biphenyl-3,3',4,4'-tetracarboxylic acid and 4,4'-bipyridine are excellent candidates for the construction of three-dimensional network motifs (Wang et al., 2006; Wang et al., 2007; Yang et al., 2007). Recently, we obtained the title compound under hydrothermal conditions and report its crystal structure here.
The asymmetric unit of the title compound contains one half of a monoprotic 4-4'-bipyridinium cation, one half of a 3-3'-4-tricarboxybiphenyl-4'-carboxylato anion and a water molecule, with both cation and anion possessing crystallographically imposed centre of symmetry (Fig. 1). As a result, the H1A nitrogen-bound hydrogen atom in the cation and acidic H2A hydrogen atom in the anion are disordered over two positions with site occupancies of 0.5. Bond lengths and angles are unexceptional. In the crystal packing (Fig. 2), cations, anions and lattice water molecules are linked by intermolecular O—H···O, C—H···O and N—H···N hydrogen bonds (Table 1) into layers parallel to (2 1 0). The layers are further connected into a three-dimensional network by O—H···O hydrogen bonds involving the water molecules as H-donors and by weak π–π stacking interactions involving neighbouring benzene and pyridine rings, with centroid-to-centroid distances of 3.756 (5) Å.