Abstract
The asymmetric unit of the title compound, 2C12H8N2·C8H10O8·2H2O, contains one 1,10-phenanthroline molecule, one half-molecule of butane-1,2,3,4-tetracarboxylic acid (H4BTC) and a water molecule, with the complete tetra-acid generated by crystallographic inversion symmetry. Intermolecular O—H⋯O hydrogen bonds and π–π stacking interactions [centroid–centroid distances = 3.672 (2) and 3.708 (2) Å form an extensive three-dimensional network, which consolidates the crystal packing.
Related literature
For the use of H4BTC as a ligand in metal–organic coordination complexes, see: Delgado et al. (2007 ▶); Liu et al. (2008 ▶); Xu et al. (2010 ▶); Zhu et al. (2011 ▶). For co-crystals involving H4BTC, see: Cheng et al. (2009 ▶); Najafpour et al. (2008 ▶). For details of the Cambridge Structural Database, see: Allen (2002 ▶).
Experimental
Crystal data
2C12H8N2·C8H10O8·2H2O
M r = 630.60
Triclinic,
a = 7.9472 (16) Å
b = 9.884 (2) Å
c = 10.628 (2) Å
α = 84.37 (3)°
β = 70.12 (3)°
γ = 72.72 (3)°
V = 749.7 (3) Å3
Z = 1
Mo Kα radiation
μ = 0.11 mm−1
T = 293 K
0.58 × 0.34 × 0.10 mm
Data collection
Rigaku R-AXIS RAPID diffractometer
Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.950, T max = 0.990
7400 measured reflections
3396 independent reflections
1960 reflections with I > 2σ(I)
R int = 0.024
Refinement
R[F 2 > 2σ(F 2)] = 0.048
wR(F 2) = 0.188
S = 1.17
3396 reflections
208 parameters
H-atom parameters constrained
Δρmax = 0.30 e Å−3
Δρmin = −0.34 e Å−3
Data collection: RAPID-AUTO (Rigaku, 1998 ▶); cell refinement: RAPID-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2004 ▶); 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.
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811021398/sj5157sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021398/sj5157Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| O1—H1A⋯O5iii | 0.87 | 1.70 | 2.565 (3) | 172 |
| O4—H4A⋯N2 | 0.86 | 1.90 | 2.723 (3) | 159 |
| O5—H5B⋯O2iv | 0.88 | 1.98 | 2.817 (3) | 160 |
| O5—H5C⋯N1 | 0.85 | 2.09 | 2.858 (3) | 149 |
Symmetry codes: (iii)
; (iv)
.
Acknowledgments
This project was supported by the K. C. Wong Magna Fund of Ningbo University.
supplementary crystallographic information
Comment
Systems with butane-1,2,3,4-tetracarboxylic acid (H4BTC) as a ligand have been widely studied (Delgado et al., 2007; Liu et al., 2008; Xu et al., 2010; Zhu et al., 2011). A search of the Cambridge structural database (version 5.32, May 2011) (Allen, 2002) showed that most of the literature dealing with butane-1,2,3,4-tetracarboxylic acid concentrated on metal-organic coordination complexes. In contrast, utilization of the butane-1,2,3,4-tetracarboxylic acid seems relatively limited in the construction of co-crystals (Cheng et al., 2009; Najafpour et al., 2008). In this paper, we report the structure of the title cocrystal.
The asymmetric unit of the title cocrystal consists of one 1,10-phenanthroline, unit one half molecule of butane-1,2,3,4-tetracarboxylic acid and a water molecule as depicted in Figure 1. The present 1,10-phenanthroline molecule preserves a nearly perfect coplanarity with a maximum deviation from the best fit meanplane 0.123 (1) Å. The carboxylato group with C1 and C4 atoms is gauche with the C1–C2–C3–C4 torsion angle being 63.35 (2)°. These values agree well with reported structures (Cheng et al., 2009; Najafpour et al., 2008;). The butane-1,2,3,4-tetracarboxylic acid molecules and water molecules are interlinked via O–H···O hydrogen bonds to generate a 1-dimensional supramolecular chain (Figure 2), which is further interconnected by interchain O–H···N hydrogen bonds to construct a 2-dimensional layer parallel to the (001) plane (Figure 3). The resulting layers are arranged in such a way that the 1,10-phenanthroline ligands are each sandwiched between two antiparallel phen neighbors from different adjacent layers, and the mean interplanar distances between the neighboring phen ligands are 3.67 Å and 3.71 Å, suggesting significant intermolecular face-to-face π–π stacking interactions. Such interlayer interactions are regarded as the driving forces to assemble the layers into a three-dimensional supramolecular architecture as shown in Figure 4.
Experimental
All chemicals were obtained from commerical sources and were used as obtained. 1,10-phenanthroline (0.1983 g, 1.00 mmol) was added to a stirred mixture solution of butane-1,2,3,4-tetracarboxylic acid (0.1173 g, 0.50 mmol) in 10 ml H2O and 10 ml me thanol, and the resulting mixture was stirred for 30 min. Colorless crystals were obtained from the solution after standing at room temperature for two months.
Refinement
H atoms bonded to C atoms were placed in geometrically calculated positions and were refined using a riding model, with Uiso(H) = 1.2 Ueq(C). H atoms attached to O atoms were found in a difference Fourier synthesis and were refined using a riding model, with the O–H distances fixed as initially found and with Uiso(H) values set at 1.2 Ueq(O).
Figures
Fig. 1.
The content of asymmetric unit showing the atomic numbering and 45% probability displacement ellipsoids [Symmetry codes: (i) -x, -y + 1, -z + 1].
Fig. 2.
Supramolecular assembly of a one-dimensional chain via O–H···O hydrogen bonds.
Fig. 3.
Supramolecular assembly of a two-dimensional layer via O–H···N hydrogen bonds.
Fig. 4.
Supramolecular assembly of three-dimensional architecture through π–π stacking interactions.
Crystal data
| 2C12H8N2·C8H10O8·2H2O | Z = 1 |
| Mr = 630.60 | F(000) = 330 |
| Triclinic, P1 | Dx = 1.397 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 7.9472 (16) Å | Cell parameters from 4546 reflections |
| b = 9.884 (2) Å | θ = 3.1–27.5° |
| c = 10.628 (2) Å | µ = 0.11 mm−1 |
| α = 84.37 (3)° | T = 293 K |
| β = 70.12 (3)° | Block, colorless |
| γ = 72.72 (3)° | 0.58 × 0.34 × 0.10 mm |
| V = 749.7 (3) Å3 |
Data collection
| Rigaku R-AXIS RAPID diffractometer | 3396 independent reflections |
| Radiation source: fine-focus sealed tube | 1960 reflections with I > 2σ(I) |
| graphite | Rint = 0.024 |
| ω scans | θmax = 27.5°, θmin = 3.1° |
| Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | h = −10→10 |
| Tmin = 0.950, Tmax = 0.990 | k = −12→12 |
| 7400 measured reflections | l = −13→13 |
Refinement
| 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)] = 0.048 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.188 | H-atom parameters constrained |
| S = 1.17 | w = 1/[σ2(Fo2) + (0.0607P)2 + 0.4694P] where P = (Fo2 + 2Fc2)/3 |
| 3396 reflections | (Δ/σ)max < 0.001 |
| 208 parameters | Δρmax = 0.30 e Å−3 |
| 0 restraints | Δρmin = −0.34 e Å−3 |
Special details
| 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)
| x | y | z | Uiso*/Ueq | ||
| O1 | −0.5184 (3) | 0.7050 (2) | 0.4404 (3) | 0.0745 (7) | |
| H1A | −0.5899 | 0.7919 | 0.4447 | 0.089* | |
| O2 | −0.3498 (3) | 0.8187 (2) | 0.4902 (3) | 0.0734 (7) | |
| C1 | −0.3757 (4) | 0.7102 (3) | 0.4718 (3) | 0.0434 (6) | |
| C2 | −0.2475 (4) | 0.5669 (3) | 0.4825 (3) | 0.0484 (6) | |
| H2A | −0.2240 | 0.5103 | 0.4055 | 0.058* | |
| H2B | −0.3086 | 0.5200 | 0.5619 | 0.058* | |
| C3 | −0.0619 (3) | 0.5737 (2) | 0.4898 (2) | 0.0389 (5) | |
| H3A | −0.0862 | 0.6351 | 0.5647 | 0.047* | |
| C4 | 0.0425 (4) | 0.6356 (2) | 0.3614 (2) | 0.0408 (5) | |
| O3 | 0.0605 (3) | 0.5952 (2) | 0.25216 (19) | 0.0652 (6) | |
| O4 | 0.1121 (3) | 0.73303 (19) | 0.37990 (18) | 0.0532 (5) | |
| H4A | 0.1639 | 0.7706 | 0.3054 | 0.064* | |
| N1 | 0.0963 (3) | 1.0528 (2) | 0.2323 (2) | 0.0514 (6) | |
| C5 | −0.0353 (5) | 1.1744 (3) | 0.2717 (3) | 0.0613 (8) | |
| H5A | −0.0890 | 1.1934 | 0.3629 | 0.074* | |
| C6 | −0.0969 (5) | 1.2746 (3) | 0.1844 (4) | 0.0705 (9) | |
| H6A | −0.1915 | 1.3571 | 0.2170 | 0.085* | |
| C7 | −0.0175 (5) | 1.2505 (3) | 0.0505 (3) | 0.0677 (9) | |
| H7A | −0.0565 | 1.3168 | −0.0096 | 0.081* | |
| C8 | 0.1230 (4) | 1.1255 (3) | 0.0040 (3) | 0.0546 (7) | |
| C9 | 0.2172 (5) | 1.0959 (4) | −0.1356 (3) | 0.0696 (9) | |
| H9A | 0.1810 | 1.1599 | −0.1982 | 0.084* | |
| C10 | 0.3561 (6) | 0.9781 (4) | −0.1774 (3) | 0.0734 (10) | |
| H10A | 0.4185 | 0.9633 | −0.2687 | 0.088* | |
| C11 | 0.4106 (4) | 0.8744 (3) | −0.0853 (3) | 0.0571 (7) | |
| C12 | 0.5552 (5) | 0.7492 (4) | −0.1252 (4) | 0.0746 (10) | |
| H12A | 0.6236 | 0.7328 | −0.2154 | 0.089* | |
| C13 | 0.5961 (5) | 0.6515 (4) | −0.0328 (4) | 0.0777 (10) | |
| H13A | 0.6935 | 0.5690 | −0.0586 | 0.093* | |
| C14 | 0.4888 (5) | 0.6777 (3) | 0.1014 (4) | 0.0709 (9) | |
| H14A | 0.5149 | 0.6093 | 0.1639 | 0.085* | |
| C15 | 0.3153 (4) | 0.8952 (3) | 0.0537 (3) | 0.0466 (6) | |
| C16 | 0.1741 (4) | 1.0267 (3) | 0.0985 (2) | 0.0449 (6) | |
| N2 | 0.3519 (3) | 0.7946 (2) | 0.1444 (2) | 0.0552 (6) | |
| O5 | 0.2570 (3) | 0.9523 (2) | 0.4390 (2) | 0.0597 (6) | |
| H5B | 0.2932 | 1.0275 | 0.4404 | 0.072* | |
| H5C | 0.1736 | 0.9754 | 0.4011 | 0.072* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0631 (13) | 0.0483 (11) | 0.131 (2) | −0.0092 (10) | −0.0622 (14) | 0.0059 (12) |
| O2 | 0.0697 (14) | 0.0409 (11) | 0.124 (2) | −0.0077 (10) | −0.0544 (14) | −0.0078 (11) |
| C1 | 0.0420 (13) | 0.0434 (13) | 0.0460 (14) | −0.0107 (11) | −0.0188 (11) | 0.0070 (11) |
| C2 | 0.0450 (14) | 0.0369 (12) | 0.0677 (17) | −0.0104 (11) | −0.0269 (13) | 0.0080 (12) |
| C3 | 0.0394 (12) | 0.0340 (11) | 0.0442 (13) | −0.0094 (10) | −0.0166 (10) | 0.0046 (10) |
| C4 | 0.0475 (14) | 0.0363 (12) | 0.0392 (13) | −0.0102 (10) | −0.0178 (11) | 0.0053 (10) |
| O3 | 0.0941 (17) | 0.0659 (13) | 0.0441 (11) | −0.0352 (12) | −0.0239 (11) | 0.0055 (9) |
| O4 | 0.0683 (13) | 0.0509 (11) | 0.0502 (11) | −0.0332 (10) | −0.0205 (9) | 0.0110 (8) |
| N1 | 0.0597 (14) | 0.0524 (13) | 0.0431 (12) | −0.0176 (11) | −0.0171 (11) | 0.0022 (10) |
| C5 | 0.068 (2) | 0.0575 (17) | 0.0536 (17) | −0.0092 (15) | −0.0186 (15) | −0.0078 (14) |
| C6 | 0.077 (2) | 0.0546 (17) | 0.080 (2) | −0.0035 (16) | −0.0384 (19) | −0.0002 (16) |
| C7 | 0.082 (2) | 0.0611 (19) | 0.070 (2) | −0.0191 (17) | −0.0424 (19) | 0.0141 (16) |
| C8 | 0.0687 (18) | 0.0576 (16) | 0.0503 (16) | −0.0299 (15) | −0.0282 (14) | 0.0125 (13) |
| C9 | 0.093 (3) | 0.083 (2) | 0.0443 (16) | −0.041 (2) | −0.0266 (17) | 0.0164 (16) |
| C10 | 0.091 (3) | 0.096 (3) | 0.0380 (15) | −0.048 (2) | −0.0102 (16) | 0.0071 (17) |
| C11 | 0.0575 (17) | 0.0677 (18) | 0.0488 (16) | −0.0326 (15) | −0.0060 (13) | −0.0067 (14) |
| C12 | 0.066 (2) | 0.086 (2) | 0.066 (2) | −0.0365 (19) | 0.0029 (17) | −0.0179 (19) |
| C13 | 0.058 (2) | 0.064 (2) | 0.098 (3) | −0.0149 (16) | −0.0048 (19) | −0.025 (2) |
| C14 | 0.068 (2) | 0.0519 (17) | 0.082 (2) | −0.0128 (15) | −0.0131 (18) | −0.0047 (16) |
| C15 | 0.0533 (15) | 0.0488 (14) | 0.0434 (14) | −0.0281 (12) | −0.0121 (12) | 0.0034 (11) |
| C16 | 0.0548 (15) | 0.0496 (14) | 0.0382 (13) | −0.0246 (12) | −0.0179 (11) | 0.0054 (11) |
| N2 | 0.0594 (15) | 0.0461 (12) | 0.0576 (14) | −0.0170 (11) | −0.0144 (12) | 0.0017 (11) |
| O5 | 0.0634 (13) | 0.0495 (11) | 0.0780 (14) | −0.0128 (9) | −0.0418 (11) | 0.0047 (10) |
Geometric parameters (Å, °)
| O1—C1 | 1.302 (3) | C7—H7A | 0.9300 |
| O1—H1A | 0.8734 | C8—C16 | 1.406 (4) |
| O2—C1 | 1.196 (3) | C8—C9 | 1.431 (4) |
| C1—C2 | 1.499 (3) | C9—C10 | 1.333 (5) |
| C2—C3 | 1.525 (3) | C9—H9A | 0.9300 |
| C2—H2A | 0.9700 | C10—C11 | 1.423 (5) |
| C2—H2B | 0.9700 | C10—H10A | 0.9300 |
| C3—C4 | 1.514 (3) | C11—C12 | 1.399 (5) |
| C3—C3i | 1.540 (4) | C11—C15 | 1.416 (4) |
| C3—H3A | 0.9800 | C12—C13 | 1.359 (5) |
| C4—O3 | 1.214 (3) | C12—H12A | 0.9300 |
| C4—O4 | 1.303 (3) | C13—C14 | 1.393 (5) |
| O4—H4A | 0.8635 | C13—H13A | 0.9300 |
| N1—C5 | 1.330 (4) | C14—N2 | 1.321 (4) |
| N1—C16 | 1.361 (3) | C14—H14A | 0.9300 |
| C5—C6 | 1.387 (4) | C15—N2 | 1.354 (4) |
| C5—H5A | 0.9300 | C15—C16 | 1.438 (4) |
| C6—C7 | 1.359 (5) | O5—H5B | 0.8756 |
| C6—H6A | 0.9300 | O5—H5C | 0.8533 |
| C7—C8 | 1.393 (4) | ||
| Cg1···Cg3ii | 3.672 (2) | Cg2···Cg3iii | 3.708 (2) |
| C1—O1—H1A | 106.5 | C7—C8—C16 | 118.4 (3) |
| O2—C1—O1 | 123.2 (2) | C7—C8—C9 | 122.2 (3) |
| O2—C1—C2 | 123.5 (2) | C16—C8—C9 | 119.4 (3) |
| O1—C1—C2 | 113.4 (2) | C10—C9—C8 | 121.1 (3) |
| C1—C2—C3 | 112.9 (2) | C10—C9—H9A | 119.5 |
| C1—C2—H2A | 109.0 | C8—C9—H9A | 119.5 |
| C3—C2—H2A | 109.0 | C9—C10—C11 | 121.3 (3) |
| C1—C2—H2B | 109.0 | C9—C10—H10A | 119.4 |
| C3—C2—H2B | 109.0 | C11—C10—H10A | 119.4 |
| H2A—C2—H2B | 107.8 | C12—C11—C15 | 117.1 (3) |
| C4—C3—C2 | 109.7 (2) | C12—C11—C10 | 123.0 (3) |
| C4—C3—C3i | 108.5 (2) | C15—C11—C10 | 119.8 (3) |
| C2—C3—C3i | 112.0 (2) | C13—C12—C11 | 120.3 (3) |
| C4—C3—H3A | 108.9 | C13—C12—H12A | 119.8 |
| C2—C3—H3A | 108.9 | C11—C12—H12A | 119.8 |
| C3i—C3—H3A | 108.9 | C12—C13—C14 | 118.6 (3) |
| O3—C4—O4 | 124.0 (2) | C12—C13—H13A | 120.7 |
| O3—C4—C3 | 122.1 (2) | C14—C13—H13A | 120.7 |
| O4—C4—C3 | 113.9 (2) | N2—C14—C13 | 123.5 (4) |
| C4—O4—H4A | 111.9 | N2—C14—H14A | 118.2 |
| C5—N1—C16 | 117.5 (2) | C13—C14—H14A | 118.2 |
| N1—C5—C6 | 123.7 (3) | N2—C15—C11 | 122.0 (3) |
| N1—C5—H5A | 118.1 | N2—C15—C16 | 119.6 (2) |
| C6—C5—H5A | 118.1 | C11—C15—C16 | 118.5 (3) |
| C7—C6—C5 | 119.1 (3) | N1—C16—C8 | 121.9 (3) |
| C7—C6—H6A | 120.4 | N1—C16—C15 | 118.4 (2) |
| C5—C6—H6A | 120.4 | C8—C16—C15 | 119.7 (2) |
| C6—C7—C8 | 119.4 (3) | C14—N2—C15 | 118.3 (3) |
| C6—C7—H7A | 120.3 | H5B—O5—H5C | 107.6 |
| C8—C7—H7A | 120.3 |
Symmetry codes: (i) −x, −y+1, −z+1; (ii) −x, −y+2, −z; (iii) −x+1, −y+2, −z.
Hydrogen-bond geometry (Å, °)
| Cg1, Cg2 and Cg3 are the centroids of the N1/C5-C8/C16/, N2/C14-C11/C15, and C8-C11/C15/C16, rings respectively. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1—H1A···O5iv | 0.87 | 1.70 | 2.565 (3) | 172 |
| O4—H4A···N2 | 0.86 | 1.90 | 2.723 (3) | 159 |
| O5—H5B···O2v | 0.88 | 1.98 | 2.817 (3) | 160 |
| O5—H5C···N1 | 0.85 | 2.09 | 2.858 (3) | 149 |
Symmetry codes: (iv) x−1, y, z; (v) −x, −y+2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SJ5157).
References
- Allen, F. H. (2002). Acta Cryst. B58, 380–388. [DOI] [PubMed]
- Cheng, Y., Wu, J., Zhu, H.-L. & Lin, J. (2009). Acta Cryst. E65, o835. [DOI] [PMC free article] [PubMed]
- Delgado, L. C., Fabelo, O., Pasàn, J., Delgado, F. S., Lloret, F., Julve, M. & Ruiz-Pérez, C. (2007). Inorg. Chem. 46, 7458–7465. [DOI] [PubMed]
- Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
- Liu, Y. Y., Ma, J. F., Yang, J., Ma, J. C. & Su, Z. M. (2008). CrystEngComm, 10, 894–904.
- Najafpour, M. M., Hołyńska, M. & Lis, T. (2008). Acta Cryst. E64, o985. [DOI] [PMC free article] [PubMed]
- Rigaku (1998). RAPID-AUTO Rigaku Corporation, Tokyo, Japan.
- Rigaku/MSC (2004). CrystalStructure Rigaku/MSC Inc., The Woodlands, Texas, USA.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Xu, Y.-Y., Xing, Y.-Y., Duan, X.-Y., Li, Y.-Z., Zhu, H.-Z. & Meng, Q.-J. (2010). CrystEngComm, 12, 567–572.
- Zhu, H.-L., Xu, W., Lin, J.-L., Cheng, Y. & Zheng, Y.-Q. (2011). Inorg. Chim. Acta, 366, 27–38.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811021398/sj5157sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021398/sj5157Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report




