research communications
Synthesis, κN1)cobalt(II) fumarate
and Hirshfeld surface analysis of tetraaquabis(isonicotinamide-aOndokuz Mayıs University, Faculty of Arts and Sciences, Department of Physics, 55139, Samsun, Turkey, and bKing Saud University, Faculty of Science, Department of Chemistry, Riyadh, Saudi Arabia
*Correspondence e-mail: sevgi.koroglu@omu.edu.tr
The reaction of cobalt(II) with fumaric acid (H2fum) and isonicotinamide in a basic solution produces the title salt, [Co(C6H6N2O)2(H2O)4](C4H2O4). In the complex cation, the CoII atom, located on an inversion centre, is coordinated by two isonicotinamide and four water molecules in a distorted N2O4 octahedral geometry. The fumarate anion is located on another inversion centre and is linked to neighbouring complex cations via O—H⋯O and N—H⋯O hydrogen bonds and weak C—H⋯O hydrogen bonds. In the crystal, the complex cations are further linked by O—H⋯O, N—H⋯O and weak C—H⋯O hydrogen bonds, forming a three-dimensional supramolecular architectecture. Hirshfeld surface analyses (dnorm surfaces and two-dimensional fingerprint plots) for the title compound are presented and discussed.
Keywords: crystal structure; fumaric acid; isonicotinamide; cobalt(II); Hirshfeld surfaces.
CCDC reference: 1561543
1. Chemical context
Metal carboxylates have attracted intense attention because of their interesting framework topologies (Rao et al., 2004). Among metal carboxylates, fumarate dianions (fum) have good conformational freedom and they possess some desirable features such as being versatile ligands because of the four electron-donor oxygen atoms they carry, and their ability to link inorganic moieties (Zheng et al., 2003). Moreover, metal fumarates exhibit interesting structural varieties.
Dicarboxylic acids such as fumaric acid and et al., 2003; Aakeröy et al., 2002). Dicarboxylic acid ligands are utilized in the synthesis of a wide variety of metal carboxylates. For this reason they have been investigated extensively, both experimentally and computationally. We describe herein the synthesis, structural features and Hirshfeld surface analysis of the title salt.
have been particularly useful in creating many supramolecular structures involving isonicotinamide and a variety of carboxylic acid molecules (Vishweshwar2. Structural commentary
The molecular structure of the title compound is illustrated in Fig. 1. The CoII cation and midpoint of the C=C bond of the fumarate anion are each located on an inversion centre. In the complex cation, the CoII atom is coordinated to two isonicotinamide ligands and four water molecules in a distorted N2O4 octahedral geometry. The fumarate anion interacts with neighboring complex cations via O—H⋯O and N—H⋯O hydrogen bonds and weak C—H⋯O hydrogen bonds (Table 1).
3. Supramolecular features
In the crystal, the fumarate anions and complex cations are linked by O—H⋯O, N—H⋯O and C—H⋯O hydrogen bonds; the complex cations also interact with each other through O—H⋯O, N—H⋯O and C—H⋯O hydrogen bonds, forming a three-dimensional supramolecular architecture (Table 1, Fig. 2).
4. Hirshfeld surface analysis
Crystal Explorer 17.5 (Turner et al., 2017) was used to analyse the interactions in the crystal and fingerprint plots mapped over dnorm (Figs. 3 and 4) were generated. The contact distances to the closest atom inside (di) and outside (de) of the Hirshfeld surface are used to analyse the intermolecular interactions via the mapping of dnorm. The molecular Hirshfeld surfaces were obtained using a standard (high) surface resolution with the three-dimensional dnorm surfaces mapped over a fixed colour scale of −1.227 (red) to 1.279 (blue). Many studies on Hirshfeld surfaces can be found in the literature (see, for example, Şen et al., 2018; Yaman et al., 2018).
In a dnorm surface, any intermolecular interactions will appear as red spots. The red spots indicate the regions of donor–acceptor interactions. There are many red spots in the dnorm surface (Fig. 3), which are usually on the O-acceptor atoms involved in the interactions listed in Table 1. Strong hydrogen-bond interactions, such as O—H⋯O, are seen as a bright-red areas on the Hirshfeld surfaces (Şen et al., 2017).
The fingerprint plot for the title complex is presented in Fig. 5. The H⋯H interactions appear in the middle of the scattered points in the two-dimensional fingerprint plots with an overall contribution to the Hirshfeld surface of 35.5% (Fig. 6b). The contribution from the O⋯H/H⋯O contacts, corresponding to C—H⋯O, N—H⋯O and O—H⋯O interactions, is represented by a pair of sharp spikes characteristic of a strong hydrogen-bond interaction (35.9%) (Fig. 6a). The C⋯C/C⋯C contacts have a sharp spike between the O⋯H and H⋯O spikes (5.7%) (Fig. 6d). The contribution of the other intermolecular contacts to the Hirshfeld surfaces is C⋯H/H⋯C (10.3%) (Fig. 6c).
5. Database survey
A search of the Cambridge Structural Database for fumaric acid and isonicotinamide revealed the presence of seven structures: isonicotinohyrazide nicotinamide fumaric acid (Aitipamula et al., 2013), catena-poly[[aquabis[N-(pyridin-3-yl)isonicotinamide-κN1)copper(II)]-(μ2-fumarato-κO,O′)-(Qiblawi & LaDuca, 2012), bis(isonicotinamide) fumaric acid (Aakeröy et al., 2002), catena-[bis(μ2-fumarato)bis(μ2-3-pyridylisonicotinamide)dizinctrihydrate] (Uebler et al., 2013) and catena-[bis(μ-but-2-enedioato)bis(μ-pyridine-4-carbohydrazide)dizinc(II)] (Naskar et al., 2017). In these compounds, the C—H⋯O hydrogen bonds have H⋯O distances ranging from 2.56 to 3.59 Å and C⋯O distances ranging from 3.27 to 3.96 Å. The N—H⋯O hydrogen bonds have H⋯O distances ranging from 1.86 to 2.33 Å and N⋯O distances ranging from 2.82 to 3.15 Å.
6. Synthesis and crystallization
An aqueous solution of fumaric acid (26 mmol, 3 g) in water was added to a solution of NaOH (52 mmol, 2.07 g) while stirring. A solution of CoCl2·6H2O (25 mmol, 6.19 g) in water was added. The reaction mixture was stirred for an hour at room temperature. The pink mixture was filtered and left to dry. The pink crystals (0.88 mmol, 0.20 g) were dissolved in water and added to an aqueous solution of isonicotinamide (1.75 mmol, 0.21 g). The resulting suspension was filtered and allowed to crystallize for five weeks at room temperature yielding orange block-shaped crystals suitable for X-ray diffraction analysis.
7. Refinement
Crystal data, data collection and structure . The N-bound and C-bound hydrogen atoms were positioned geometrically and treated as riding: N—H = 0.86 Å and C—H = 0.93 Å with Uiso(H) = 1.2Ueq(C,N). Water H atoms were found in a difference-Fourier map, restrained with O—H = 0.85 Å and refined with Uiso(H) = 1.5Ueq(O).
details are summarized in Table 2
|
Supporting information
CCDC reference: 1561543
https://doi.org/10.1107/S205698901800107X/xu5915sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S205698901800107X/xu5915Isup2.hkl
Data collection: APEX2 (Bruker, 2007); cell
SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXT2014 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2016 (Sheldrick, 2015b); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: WinGX (Farrugia, 2012) and PLATON (Spek, 2009).[Co(C6H6N2O)2(H2O)4](C4H2O4) | F(000) = 506 |
Mr = 489.30 | Dx = 1.604 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.6914 (10) Å | Cell parameters from 9553 reflections |
b = 10.0106 (11) Å | θ = 3.1–28.3° |
c = 11.3811 (12) Å | µ = 0.91 mm−1 |
β = 113.416 (3)° | T = 296 K |
V = 1013.22 (19) Å3 | Block, orange |
Z = 2 | 0.25 × 0.19 × 0.16 mm |
Bruker APEXII CCD diffractometer | 1830 reflections with I > 2σ(I) |
φ and ω scans | Rint = 0.032 |
Absorption correction: analytical (X-RED32; Stoe & Cie, 2002) | θmax = 26.0°, θmin = 3.1° |
Tmin = 0.394, Tmax = 0.746 | h = −11→11 |
19963 measured reflections | k = −12→12 |
1962 independent reflections | l = −14→13 |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.032 | H-atom parameters constrained |
wR(F2) = 0.077 | w = 1/[σ2(Fo2) + (0.0211P)2 + 1.1735P] where P = (Fo2 + 2Fc2)/3 |
S = 1.14 | (Δ/σ)max < 0.001 |
1962 reflections | Δρmax = 0.35 e Å−3 |
144 parameters | Δρmin = −0.35 e Å−3 |
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. |
x | y | z | Uiso*/Ueq | ||
Co1 | 0.500000 | 0.500000 | 0.500000 | 0.01658 (12) | |
O3 | 0.60307 (15) | 0.65750 (13) | 0.62150 (13) | 0.0237 (3) | |
H3A | 0.696404 | 0.660264 | 0.635017 | 0.035* | |
H3B | 0.594575 | 0.646860 | 0.692916 | 0.035* | |
O2 | 0.39661 (15) | 0.64187 (13) | 0.35319 (13) | 0.0240 (3) | |
H2A | 0.368923 | 0.604165 | 0.279836 | 0.036* | |
H2B | 0.458953 | 0.704445 | 0.358200 | 0.036* | |
O4 | 0.55105 (17) | 0.63859 (14) | 0.83392 (14) | 0.0283 (3) | |
O1 | −0.09235 (17) | 0.70328 (16) | 0.68073 (17) | 0.0365 (4) | |
O5 | 0.72605 (18) | 0.48025 (16) | 0.88934 (16) | 0.0356 (4) | |
N1 | 0.31337 (18) | 0.52596 (16) | 0.55744 (16) | 0.0208 (3) | |
C7 | 0.6189 (2) | 0.54056 (19) | 0.90123 (18) | 0.0221 (4) | |
C3 | 0.1007 (2) | 0.5713 (2) | 0.66124 (18) | 0.0216 (4) | |
C8 | 0.5656 (2) | 0.48648 (19) | 0.99864 (19) | 0.0239 (4) | |
H8 | 0.629871 | 0.429951 | 1.061428 | 0.029* | |
N2 | −0.0347 (3) | 0.5112 (2) | 0.7922 (2) | 0.0491 (6) | |
H2C | −0.102155 | 0.523521 | 0.822413 | 0.059* | |
H2D | 0.020826 | 0.440936 | 0.812861 | 0.059* | |
C4 | 0.1453 (2) | 0.6727 (2) | 0.6015 (2) | 0.0268 (4) | |
H4 | 0.103978 | 0.757665 | 0.594549 | 0.032* | |
C2 | 0.1627 (2) | 0.4464 (2) | 0.6655 (2) | 0.0297 (5) | |
H2 | 0.134441 | 0.375248 | 0.703564 | 0.036* | |
C6 | −0.0163 (2) | 0.6003 (2) | 0.7141 (2) | 0.0279 (4) | |
C5 | 0.2516 (2) | 0.64642 (19) | 0.5523 (2) | 0.0263 (4) | |
H5 | 0.281757 | 0.715892 | 0.513627 | 0.032* | |
C1 | 0.2671 (2) | 0.4283 (2) | 0.6126 (2) | 0.0275 (4) | |
H1 | 0.307396 | 0.343382 | 0.615691 | 0.033* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Co1 | 0.01724 (19) | 0.01624 (19) | 0.0214 (2) | −0.00028 (12) | 0.01310 (14) | 0.00056 (13) |
O3 | 0.0239 (7) | 0.0251 (7) | 0.0276 (7) | −0.0036 (6) | 0.0162 (6) | −0.0033 (6) |
O2 | 0.0259 (7) | 0.0220 (7) | 0.0258 (7) | −0.0015 (5) | 0.0121 (6) | 0.0031 (5) |
O4 | 0.0421 (8) | 0.0219 (7) | 0.0319 (7) | 0.0059 (6) | 0.0264 (7) | 0.0046 (6) |
O1 | 0.0332 (8) | 0.0303 (8) | 0.0602 (11) | −0.0001 (7) | 0.0334 (8) | −0.0075 (7) |
O5 | 0.0354 (8) | 0.0430 (9) | 0.0409 (9) | 0.0129 (7) | 0.0284 (7) | 0.0091 (7) |
N1 | 0.0207 (8) | 0.0199 (8) | 0.0274 (8) | −0.0003 (6) | 0.0154 (7) | −0.0003 (6) |
C7 | 0.0262 (9) | 0.0217 (9) | 0.0234 (9) | −0.0018 (8) | 0.0151 (8) | −0.0023 (8) |
C3 | 0.0178 (9) | 0.0268 (10) | 0.0247 (9) | −0.0017 (7) | 0.0134 (7) | −0.0023 (8) |
C8 | 0.0282 (10) | 0.0240 (10) | 0.0243 (10) | 0.0033 (8) | 0.0155 (8) | 0.0037 (7) |
N2 | 0.0411 (12) | 0.0675 (15) | 0.0591 (14) | 0.0163 (11) | 0.0416 (11) | 0.0225 (11) |
C4 | 0.0285 (10) | 0.0182 (9) | 0.0425 (12) | 0.0012 (8) | 0.0234 (9) | −0.0016 (8) |
C2 | 0.0303 (10) | 0.0270 (10) | 0.0428 (12) | 0.0024 (9) | 0.0261 (10) | 0.0110 (9) |
C6 | 0.0208 (9) | 0.0359 (12) | 0.0330 (11) | −0.0056 (9) | 0.0170 (8) | −0.0089 (9) |
C5 | 0.0300 (10) | 0.0191 (9) | 0.0397 (11) | −0.0005 (8) | 0.0245 (9) | 0.0032 (8) |
C1 | 0.0274 (10) | 0.0204 (10) | 0.0432 (12) | 0.0039 (8) | 0.0229 (9) | 0.0058 (8) |
Co1—O3i | 2.0731 (13) | C7—C8 | 1.498 (3) |
Co1—O3 | 2.0731 (13) | C3—C2 | 1.380 (3) |
Co1—O2i | 2.1171 (13) | C3—C4 | 1.383 (3) |
Co1—O2 | 2.1171 (13) | C3—C6 | 1.509 (3) |
Co1—N1 | 2.1694 (16) | C8—C8ii | 1.313 (4) |
Co1—N1i | 2.1694 (16) | C8—H8 | 0.9300 |
O3—H3A | 0.8556 | N2—C6 | 1.320 (3) |
O3—H3B | 0.8555 | N2—H2C | 0.8600 |
O2—H2A | 0.8564 | N2—H2D | 0.8600 |
O2—H2B | 0.8564 | C4—C5 | 1.380 (3) |
O4—C7 | 1.258 (2) | C4—H4 | 0.9300 |
O1—C6 | 1.236 (3) | C2—C1 | 1.379 (3) |
O5—C7 | 1.254 (2) | C2—H2 | 0.9300 |
N1—C1 | 1.332 (3) | C5—H5 | 0.9300 |
N1—C5 | 1.337 (2) | C1—H1 | 0.9300 |
O3i—Co1—O3 | 180.0 | O4—C7—C8 | 118.86 (17) |
O3i—Co1—O2i | 88.15 (6) | C2—C3—C4 | 117.75 (17) |
O3—Co1—O2i | 91.85 (6) | C2—C3—C6 | 123.14 (18) |
O3i—Co1—O2 | 91.85 (6) | C4—C3—C6 | 119.07 (18) |
O3—Co1—O2 | 88.15 (6) | C8ii—C8—C7 | 124.4 (2) |
O2i—Co1—O2 | 180.0 | C8ii—C8—H8 | 117.8 |
O3i—Co1—N1 | 93.08 (6) | C7—C8—H8 | 117.8 |
O3—Co1—N1 | 86.92 (6) | C6—N2—H2C | 120.0 |
O2i—Co1—N1 | 91.85 (6) | C6—N2—H2D | 120.0 |
O2—Co1—N1 | 88.15 (6) | H2C—N2—H2D | 120.0 |
O3i—Co1—N1i | 86.92 (6) | C5—C4—C3 | 119.29 (18) |
O3—Co1—N1i | 93.08 (6) | C5—C4—H4 | 120.4 |
O2i—Co1—N1i | 88.14 (6) | C3—C4—H4 | 120.4 |
O2—Co1—N1i | 91.85 (6) | C1—C2—C3 | 119.26 (18) |
N1—Co1—N1i | 180.0 | C1—C2—H2 | 120.4 |
Co1—O3—H3A | 109.8 | C3—C2—H2 | 120.4 |
Co1—O3—H3B | 109.6 | O1—C6—N2 | 123.2 (2) |
H3A—O3—H3B | 109.1 | O1—C6—C3 | 119.28 (19) |
Co1—O2—H2A | 109.9 | N2—C6—C3 | 117.5 (2) |
Co1—O2—H2B | 109.8 | N1—C5—C4 | 123.21 (18) |
H2A—O2—H2B | 109.1 | N1—C5—H5 | 118.4 |
C1—N1—C5 | 117.00 (16) | C4—C5—H5 | 118.4 |
C1—N1—Co1 | 122.07 (13) | N1—C1—C2 | 123.47 (19) |
C5—N1—Co1 | 120.48 (13) | N1—C1—H1 | 118.3 |
O5—C7—O4 | 124.37 (18) | C2—C1—H1 | 118.3 |
O5—C7—C8 | 116.71 (18) | ||
O5—C7—C8—C8ii | −161.6 (3) | C2—C3—C6—N2 | 15.6 (3) |
O4—C7—C8—C8ii | 15.7 (4) | C4—C3—C6—N2 | −166.7 (2) |
C2—C3—C4—C5 | −1.8 (3) | C1—N1—C5—C4 | 0.4 (3) |
C6—C3—C4—C5 | −179.59 (19) | Co1—N1—C5—C4 | −172.01 (17) |
C4—C3—C2—C1 | 1.1 (3) | C3—C4—C5—N1 | 1.1 (3) |
C6—C3—C2—C1 | 178.8 (2) | C5—N1—C1—C2 | −1.2 (3) |
C2—C3—C6—O1 | −162.7 (2) | Co1—N1—C1—C2 | 171.10 (17) |
C4—C3—C6—O1 | 14.9 (3) | C3—C2—C1—N1 | 0.5 (4) |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1, −y+1, −z+2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H2A···O5i | 0.86 | 1.96 | 2.814 (2) | 171 |
O2—H2B···O4iii | 0.86 | 1.88 | 2.7165 (19) | 165 |
O3—H3A···O1iv | 0.86 | 1.95 | 2.792 (2) | 168 |
O3—H3B···O4 | 0.86 | 1.82 | 2.6652 (19) | 172 |
N2—H2C···O5v | 0.86 | 2.13 | 2.955 (2) | 160 |
N2—H2D···O1vi | 0.86 | 2.47 | 3.288 (3) | 159 |
C1—H1···O4vii | 0.93 | 2.41 | 3.322 (2) | 168 |
C2—H2···O1vi | 0.93 | 2.30 | 3.225 (3) | 173 |
Symmetry codes: (i) −x+1, −y+1, −z+1; (iii) x, −y+3/2, z−1/2; (iv) x+1, y, z; (v) x−1, y, z; (vi) −x, y−1/2, −z+3/2; (vii) −x+1, y−1/2, −z+3/2. |
Funding information
This research project was supported by a grant from the `Research Center of the Female Scientific and Medical Colleges', Deanship of Scientific Research, King Saud University.
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