research communications
Crystal structures of two isostructural bivalent metal N-benzoylglycinates
aSchool of Chemical Sciences, Goa University PO, Goa 403206, India
*Correspondence e-mail: srini@unigoa.ac.in
The crystal structures of two coordination compounds of N-benzoylglycine, viz. catena-poly[[[diaquabis(N-benzoylglycinato)cobalt(II)]-μ-aqua] dihydrate], {[Co(C9H8NO3)2(H2O)3]·2H2O}n, 1, and catena-poly[[[diaquabis(N-benzoylglycinato)nickel(II)]-μ-aqua] dihydrate], {[Ni(C9H8NO3)2(H2O)3]·2H2O}n, 2, are described. The structures of 1 and 2 were reported previously [Morelock et al. (1979). J. Am. Chem. Soc. 101, 4858–4866] and redetermined in this work to determine the H-atom coordinates. In the isostructural compounds, the central metal is located on an inversion centre and exhibits a distorted octahedral geometry. A pair of terminal aqua ligands disposed trans to each other and a pair of monodentate N-benzoylglycinate ligands form the square base and account for four of the six vertices of the octahedron. A μ2-bridging aqua ligand links the bivalent metals into one-dimensional chains extending along the c-axis direction. The one-dimensional chains stabilized by O—H⋯O hydrogen bonds are interlinked by N—H⋯O and C—H⋯O hydrogen-bonding interactions.
1. Chemical context
Hippuric acid known by other names such as N-benzoylglycine or benzoylaminoethanoic acid or N-(benzenecarbonyl)glycine is a derivative of glycine and is produced in metabolic processes (Pero, 2010). Hence the benzoyl-substituted glycine, namely N-benzoylglycine and its compounds, have been the subject of several investigations. The crystal structures of N-benzoylglycine and many of its derivatives are archived in the Cambridge Structural Database (CSD, version 5.40, update of September 2019; Groom et al., 2016). Unlike N-benzoylglycine, which crystallizes in the non-centrosymmetric Sohncke P212121, a majority of its derivatives are centrosymmetric solids. In most of these compounds, N-benzoylglycine functions as a charge-balancing (N-benzoylglycinate) anion. In addition, the anion can also coordinate to a metal as observed in the title compounds. The N-benzoylglycinates of CoII 1 and NiII 2 are some of the first examples of a series of α-amino acid compounds of the first-row transition-metal ions that exhibit low-dimensional magnetic properties (Morelock et al., 1979). Based on a study of the visible spectra and the magnetic properties, compound 1 was shown to be a metamagnet and 2 an antiferromagnet.
In the previous report, the title compounds 1 and 2 were prepared in an aqueous ethanolic medium by the reaction of the sodium salt of hippuric acid with the corresponding bivalent metal perchlorate (Morelock et al. 1979). The polymeric structure of 1 and 2 due to aqua bridging was described, but the hydrogen-atom coordinates were not reported. N-Benzoylglycinates with a different stoichiometry represented by the formula M(C9H8NO3)2·6H2O (M = Co or Ni) are also known in the literature (Marcotrigiano & Pellacani, 1975). However, these were not structurally characterized. In the present work we have synthesized the title compounds by a direct acid–base reaction of cobalt carbonate (or nickel carbonate) with N-benzoylglycine (hippuric acid) to obtain [Co(H2O)3(C9H8NO3)2]·2H2O, 1, and [Ni(H2O)3(C9H8NO3)2]·2H2O, 2, respectively. The infrared spectra of both compounds are nearly identical, indicating similar structures. A comparison of the spectra of 1 and 2 with that of the free ligand (N-benzoylglycine) reveals notable changes in the profile of the spectra in the 3700–2750 cm−1 region. This can be explained by the presence of water molecules in 1 and 2, unlike in the free acid. N-Benzoylglycine exhibits a strong signal at ∼1743 cm−1 assignable for the –COOH vibration, which is shifted to lower energies in 1 and 2 due to deprotonation (Fig. 1). Despite a slightly different synthetic methodology, the product obtained by us is the same as evidenced by the structural details of 1 and 2, which are in good agreement with the earlier work (Morelock et al. 1979) as shown below.
2. Structural commentary
The molecular structure of the isostructural compounds [M(H2O)3(C9H8NO3)2]·2H2O (M = Co 1, M = Ni 2) is illustrated in Fig. 2. Compounds 1 and 2 crystallize in the centrosymmetric monoclinic C2/c with the central cobalt (or nickel) ion located on an inversion centre. All of the atoms in both structures have been labelled so as to maintain parity for the ligand oxygen atoms and donor hydrogen and acceptor oxygen atoms in the hydrogen-bonding scheme. Other than the central metal, the structure consists of a unique terminal water (O1W), a unique monodentate N-benzoylglycinate (O2), a bridging aqua ligand (O2W) with the oxygen situated on a twofold axis and a non-ligated water (O3W), which constitute half of the formula unit of 1 or 2. In view of the special position of the central metal, the other half is generated by the application of inversion symmetry. The geometric parameters of the N-benzoylglycinates are in the normal ranges and are in agreement with reported data (Natarajan et al., 2007). The metal–oxygen bond distances (Tables 1 and 2) scatter in a very narrow range [2.0563 (15) to 2.1899 (9) Å in 1; 2.029 (2) to 2.1450 (12) Å in 2]. In both compounds, the carboxylate oxygen (O2) of the N-benzoylglycinate makes the shortest M—O bond length while the longest M—O bond distance is observed for the bridging aqua ligand (O2W). Both compounds exhibit ideal values for the trans O—M—O bond angles while the cis O—M—O angles show a slight deviation [87.41 (6) to 92.59 (6)° in 1; 87.27 (8) to 92.73 (8)° in 2] indicating a slight distortion of the {MO6} octahedron (Tables 1 and 2). The difference Δ between the longest and the shortest M—O bonds can be considered as a measure of the distortion from ideal geometry and is 0.1336 (0.18) and 0.114 (0.12) Å for compounds 1 and 2, respectively. The values in brackets are the difference Δ calculated from the reported bond distances of the earlier study. It is interesting to note that the same trend is observed with {CoO6} octahedron being slightly more distorted. The central metal exhibits hexa coordination and is bonded to two terminal aqua ligands (O1W, O1Wi) [symmetry code: (i) −x + 1, −y + 1, −z + 1] disposed trans to each other and two monodentate N-benzoylglycinate (O2, O2i) ligands accounting for the square base of the octahedron. The μ2-bridging binding mode of the aqua ligand (O2W) makes two axial bonds trans to each other completing the octahedral geometry around the central metal. The bridging binding mode results in the formation of a one-dimensional chain structure extending along the c-axis direction (Fig. 3). In the infinite chain, the observed M⋯M separations of 4.0015 (2) Å or 3.9492 (8) Å in 1 or 2, respectively, are in very good agreement with the earlier work (Morelock et al. 1979). The M—O2W—Mii bond angle θ for 1 [symmetry code: (ii) −x + 1, y, −z + ] and 2 [symmetry code: (ii) −x + 1, y, −z + ] are 132.03 (11) and 134.02 (15)° for 1 and 2, respectively, which follow the earlier trend with the reported θ values being 128.3 and 137.2° (Morelock et al. 1979). The Θ value is marginally higher for 2 and is accompanied by a shorter Ni1—O2W bond distance of 2.1450 (12) Å. The decreasing bond distance is attributed to increasing orbital overlap, explaining the larger superexchange in 2 leading to spin-pairing.
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3. Supramolecular features
The isostructural compounds 1 and 2 exhibit several non-covalent interactions, namely O—H⋯O, N—H⋯O and C—H⋯O hydrogen bonds (Tables 3 and 4) in their supramolecular structures. All of the hydrogen atoms attached to the water molecules, the hydrogen atom bonded to nitrogen N1 and a hydrogen atom attached to the methylene carbon C9 function as hydrogen donors and four of the six oxygen atoms, namely O1, O2, O3 and O3W, function as hydrogen acceptors. All of the O—H⋯O hydrogen bonds are intrachain interactions (Fig. 3). The non-ligated water O3W interlinks adjacent chains with the aid of a single short N1—H1⋯O3W interaction at H⋯A distances of 2.13 (3) and 2.04 (5) Å in 1 and 2, respectively, accompanied by D—H⋯A angles of 149 (2) and 151 (4)° (Fig. 4). A short C9—H9B⋯O3iv interaction at a H⋯A distance 2.51 Å in 1 (2.50 Å in 2) accompanied by D—H⋯A angle of 177.9° in 1, (176.4° in 2) links the H9B atom of a methylene group of N-benzoylglycinate in one chain with the O3 atom of a symmetry-related N-benzoylglycinate in a neighboring chain functioning as a hydrogen acceptor (Fig. 5). These interchain hydrogen-bonding interactions serve to hold the chains together along the b axis, forming a layer of chains in the bc plane. Thus, the findings of our present study once again support the original findings, namely compounds 1 and 2 are unique examples of psuedo one-dimensional (1D) magnetic materials in which three-dimensional magnetic ordering was predicted not to occur until T → 0 K. In addition to the hydrogen-bonding interactions, 1 and 2 exhibit π–π stacking interactions (Hunter & Sanders, 1990). For the analysis of short ring interactions, the program PLATON (Spek, 2020) was used. The ring centroid–centroid distances (Cg⋯Cg) between the adjacent benzene rings in 1 and 2 are found to be 4.0435 (2) and 3.9807 (5) Å, respectively. It has been reported that stacking interactions can exist at very long Cg⋯Cg distances of up to 7 Å (Ninković et al., 2011). Hence, the observed Cg⋯Cg distances can be attributed to the π–π stacking of the benzene rings.
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4. Database survey
The Cambridge Structural Database (CSD, version 5.40, update of September 2019; Groom et al., 2016) lists several structurally characterized organic and metal–organic compounds of N-benzoylglycine. Since the first report on the of N-benzoylglycine (Ringertz, 1971), several compounds of N-benzoylglycine have been structurally characterized. Excepting an example of a 1:1 of N-benzoylglycine, namely glibenclamide hippuric acid (Goyal et al., 2017), the structures of thirty two compounds containing the monoanionic N-benzoylglycinate were retrieved from the CSD (Groom et al., 2016). Three of these do not contain any metal and are charge-balanced by organic cations (Görbitz & Sagstuen, 2004; Chadha et al., 2016; John et al., 2018). Of the twenty nine examples of N-benzoylglycinates with metal–organic cations, eight contain bivalent metal (Table 5) and aqua ligands. In this work, a comparative study of bivalent metal N-benzoylglycinates containing only aqua ligands has been undertaken. It is interesting to note that all of these compounds contain coordinated water molecules. In this list of compounds, excepting the N-benzoylglycinate of ZnII (Grewe et al., 1982), the rest are all centrosymmetric. In all eight compounds, the N-benzoylglycinate coordinates to the metal only through the carboxylate oxygen atoms. In five of these, including the title compounds, N-benzoylglycinate functions as a monodentate ligand. The bridging binding mode in the N-benzoylglycinates of CaII (Jisha et al., 2010), BaII (Natarajan et al. 2007), CuII (Brown & Trefonas, 1973) and PbII (Battistuzzi et al., 1996) can explain the polymeric nature of these compounds, excepting the CuII which is a dimer. The structure of the dimeric copper compound (Refcode CUHIPT; Brown & Trefonas, 1973) contains both a monodentate as well as a monoatomic bridging N-benzoylglycinate. It is interesting to note that the dinuclear CuII compound of N-benzoylglycine does not adopt the paddle-wheel structure. The N-benzoylglycinate of FeII (Morelock et al., 1982) is also isostructural with the title compounds and is a 1D polymer. It is interesting to note that in the three isostructural N-benzoylglycinates of 3d metals, an aqua ligand functions as a bridging ligand to extend the structure, and not the N-benzoylglycinate.
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5. Synthesis and crystallization
For the synthesis of 1, N-benzoylglycine (1.792 g, 10 mmol) taken in distilled water (50 mL) was heated with stirring to obtain a clear solution. Into this, CoCO3 (0.595 g, 5 mmol) was added in small portions. Brisk effervescence was observed accompanied by the dissolution of the insoluble carbonate, resulting in a pink-coloured solution. When most of the carbonate had dissolved, a small amount (∼25 mg) of the carbonate was added and the heating continued for a further hour. The hot reaction mixture was filtered and the clear pink filtrate was left undisturbed for crystallization. The crystals obtained after a few days were isolated by filtration and dried in air, yield = 90%. A similar procedure was employed for 2 using nickel carbonate instead of cobalt carbonate and the filtrate obtained was light green. Crystals were isolated as before, yield = 80%.
6. Refinement
Crystal data, data collection and structure . O- and N-bound H atoms were freely refined. C-bound hydrogen atoms were placed at calculated positions C—H = 0.93–0.97 Å) and refined isotropically [Uiso(H) = 1.2Ueq(C). using a riding-atom model.
details are summarized in Table 6
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Supporting information
https://doi.org/10.1107/S2056989020009287/ex2034sup1.cif
contains datablocks 1, 2. DOI:Structure factors: contains datablock 1. DOI: https://doi.org/10.1107/S2056989020009287/ex20341sup2.hkl
Structure factors: contains datablock 2. DOI: https://doi.org/10.1107/S2056989020009287/ex20342sup3.hkl
For both structures, data collection: APEX3 (Bruker, 2019); cell
SAINT (Bruker, 2019); data reduction: SAINT (Bruker, 2019); program(s) used to solve structure: SHELXT2014/5 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2018/3 (Sheldrick, 2015b); molecular graphics: OLEX2 (Dolomanov et al., 2009), shelXle (Hübschle et al., 2011); software used to prepare material for publication: publCIF (Westrip, 2010).[Co(C9H8NO3)2(H2O)3]·2H2O | F(000) = 1052 |
Mr = 505.34 | Dx = 1.487 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
a = 40.843 (2) Å | Cell parameters from 4616 reflections |
b = 6.9072 (4) Å | θ = 3.0–28.0° |
c = 8.0031 (4) Å | µ = 0.82 mm−1 |
β = 91.891 (2)° | T = 293 K |
V = 2256.6 (2) Å3 | Plate, pink |
Z = 4 | 0.35 × 0.27 × 0.04 mm |
Bruker D8 Quest Eco diffractometer | 2070 reflections with I > 2σ(I) |
Radiation source: Sealed Tube | Rint = 0.046 |
φ and ω scans | θmax = 28.3°, θmin = 3.0° |
Absorption correction: numerical (SADABS; Krause et al., 2015) | h = −54→54 |
Tmin = 0.610, Tmax = 0.746 | k = −9→9 |
15061 measured reflections | l = −10→10 |
2799 independent reflections |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.037 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.086 | w = 1/[σ2(Fo2) + (0.0214P)2 + 3.6234P] where P = (Fo2 + 2Fc2)/3 |
S = 1.08 | (Δ/σ)max < 0.001 |
2799 reflections | Δρmax = 0.39 e Å−3 |
171 parameters | Δρmin = −0.42 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. |
Refinement. Suitable single crystals were selected under a polarizing microscope in HR2-643 parabar 10312 oil from Hampton Research. The crystal was mounted on a 20 micron 0.4–0.5 mm HR4-953 Mounted Cryoloops loop from Hampton Research and transferred to the Bruker D8 Quest Eco diffractometer. Reflections harvested from two sets of 12, 0.5ο φ scans were used to determine unit-cell parameters and was used to determine the data-collection strategy. Unit-cell parameters were refined using reflections harvested from the data collection. The frames were integrated with the Bruker SAINT software package using a narrow-frame algorithm. The integration of the data using a monoclinic unit cell yielded a total of 15061 reflections to a maximum θ angle of 28.26° (0.75 Å resolution) for 1 and 17095 reflections to a maximum θ angle of 30.52° (0.70 Å resolution) for 2. All data were corrected for Lorentz and polarization effects and subsequently scaled. A numerical absorption correction was performed by SADABS (Krause et al., 2015). The space group was determined and the structures were solved using the intrinsic phasing method (Bruker, 2019; Sheldrick, 2008). The structures were refined in APEX3 v2019.1-0 by SHELXL (Sheldrick, 2015). |
x | y | z | Uiso*/Ueq | ||
Co1 | 0.500000 | 0.500000 | 0.500000 | 0.02504 (12) | |
O1W | 0.53443 (4) | 0.6984 (3) | 0.5847 (2) | 0.0359 (4) | |
H1WA | 0.5349 (7) | 0.699 (4) | 0.682 (4) | 0.058 (10)* | |
H1WB | 0.5538 (7) | 0.690 (4) | 0.550 (3) | 0.050 (9)* | |
O2W | 0.500000 | 0.3711 (3) | 0.750000 | 0.0274 (5) | |
H2W | 0.4817 (7) | 0.305 (4) | 0.761 (4) | 0.072 (10)* | |
O2 | 0.46352 (4) | 0.6817 (2) | 0.57632 (18) | 0.0327 (4) | |
O3 | 0.44216 (4) | 0.7725 (3) | 0.32901 (18) | 0.0397 (4) | |
C8 | 0.44162 (5) | 0.7613 (3) | 0.4833 (3) | 0.0283 (5) | |
C9 | 0.41364 (5) | 0.8469 (4) | 0.5790 (3) | 0.0334 (5) | |
H9A | 0.405396 | 0.748241 | 0.652987 | 0.040* | |
H9B | 0.422184 | 0.951677 | 0.648337 | 0.040* | |
N1 | 0.38658 (5) | 0.9200 (3) | 0.4767 (3) | 0.0349 (5) | |
H1 | 0.3849 (6) | 1.039 (4) | 0.469 (3) | 0.037 (8)* | |
O1 | 0.36670 (5) | 0.6242 (3) | 0.4197 (3) | 0.0629 (6) | |
C1 | 0.36437 (6) | 0.8018 (4) | 0.4068 (3) | 0.0388 (6) | |
C2 | 0.33558 (6) | 0.8888 (4) | 0.3134 (3) | 0.0385 (6) | |
C3 | 0.31275 (8) | 0.7639 (5) | 0.2456 (4) | 0.0642 (9) | |
H3 | 0.316051 | 0.631037 | 0.255105 | 0.077* | |
C4 | 0.28480 (8) | 0.8330 (6) | 0.1628 (4) | 0.0752 (11) | |
H4 | 0.269374 | 0.746529 | 0.118400 | 0.090* | |
C5 | 0.27986 (7) | 1.0263 (6) | 0.1465 (4) | 0.0667 (10) | |
H5 | 0.261079 | 1.073072 | 0.091414 | 0.080* | |
C6 | 0.30260 (7) | 1.1508 (5) | 0.2113 (4) | 0.0647 (9) | |
H6 | 0.299329 | 1.283351 | 0.198759 | 0.078* | |
C7 | 0.33062 (7) | 1.0849 (4) | 0.2959 (4) | 0.0499 (7) | |
H7 | 0.345894 | 1.172283 | 0.340250 | 0.060* | |
O3W | 0.40263 (5) | 0.3206 (3) | 0.5364 (2) | 0.0412 (4) | |
H3WA | 0.3916 (8) | 0.420 (6) | 0.520 (4) | 0.081 (13)* | |
H3WB | 0.4083 (8) | 0.319 (5) | 0.639 (4) | 0.074 (11)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Co1 | 0.0247 (2) | 0.0338 (2) | 0.01649 (18) | 0.0018 (2) | −0.00142 (13) | 0.00037 (17) |
O1W | 0.0350 (10) | 0.0495 (11) | 0.0230 (9) | −0.0071 (8) | −0.0003 (7) | −0.0027 (8) |
O2W | 0.0294 (12) | 0.0368 (13) | 0.0159 (10) | 0.000 | 0.0003 (8) | 0.000 |
O2 | 0.0315 (8) | 0.0446 (10) | 0.0216 (7) | 0.0107 (7) | −0.0029 (6) | −0.0006 (7) |
O3 | 0.0398 (9) | 0.0569 (11) | 0.0222 (8) | 0.0138 (9) | −0.0022 (7) | 0.0012 (7) |
C8 | 0.0303 (11) | 0.0301 (12) | 0.0241 (10) | 0.0036 (10) | −0.0026 (8) | −0.0016 (9) |
C9 | 0.0319 (12) | 0.0397 (13) | 0.0283 (11) | 0.0086 (10) | −0.0033 (9) | −0.0052 (10) |
N1 | 0.0309 (11) | 0.0339 (12) | 0.0396 (12) | 0.0079 (9) | −0.0028 (8) | −0.0026 (9) |
O1 | 0.0679 (14) | 0.0367 (11) | 0.0820 (16) | 0.0057 (10) | −0.0293 (11) | −0.0015 (10) |
C1 | 0.0371 (13) | 0.0404 (14) | 0.0385 (13) | 0.0039 (12) | −0.0032 (10) | −0.0024 (11) |
C2 | 0.0320 (13) | 0.0474 (15) | 0.0359 (13) | 0.0030 (12) | −0.0002 (10) | 0.0014 (11) |
C3 | 0.0579 (19) | 0.060 (2) | 0.072 (2) | −0.0079 (16) | −0.0251 (16) | 0.0049 (16) |
C4 | 0.0534 (19) | 0.097 (3) | 0.073 (2) | −0.014 (2) | −0.0290 (17) | 0.007 (2) |
C5 | 0.0393 (15) | 0.105 (3) | 0.0552 (19) | 0.0147 (19) | −0.0096 (13) | 0.0112 (19) |
C6 | 0.0544 (19) | 0.070 (2) | 0.069 (2) | 0.0216 (17) | −0.0092 (16) | 0.0097 (17) |
C7 | 0.0415 (15) | 0.0540 (17) | 0.0539 (17) | 0.0074 (14) | −0.0037 (12) | 0.0005 (14) |
O3W | 0.0454 (11) | 0.0412 (11) | 0.0368 (11) | 0.0000 (9) | −0.0036 (8) | 0.0005 (8) |
Co1—O2 | 2.0563 (15) | N1—H1 | 0.83 (3) |
Co1—O2i | 2.0563 (15) | O1—C1 | 1.235 (3) |
Co1—O1W | 2.0622 (17) | C1—C2 | 1.498 (3) |
Co1—O1Wi | 2.0622 (17) | C2—C3 | 1.370 (4) |
Co1—O2Wi | 2.1899 (9) | C2—C7 | 1.376 (4) |
Co1—O2W | 2.1899 (9) | C3—C4 | 1.386 (4) |
O1W—H1WA | 0.78 (3) | C3—H3 | 0.9300 |
O1W—H1WB | 0.85 (3) | C4—C5 | 1.357 (5) |
O2W—H2W | 0.88 (3) | C4—H4 | 0.9300 |
O2W—H2Wii | 0.88 (3) | C5—C6 | 1.356 (5) |
O2—C8 | 1.270 (2) | C5—H5 | 0.9300 |
O3—C8 | 1.238 (2) | C6—C7 | 1.387 (4) |
C8—C9 | 1.517 (3) | C6—H6 | 0.9300 |
C9—N1 | 1.445 (3) | C7—H7 | 0.9300 |
C9—H9A | 0.9700 | O3W—H3WA | 0.83 (4) |
C9—H9B | 0.9700 | O3W—H3WB | 0.84 (3) |
N1—C1 | 1.330 (3) | ||
O2—Co1—O2i | 180.0 | C8—C9—H9A | 108.5 |
O2—Co1—O1W | 89.40 (7) | N1—C9—H9B | 108.5 |
O2i—Co1—O1W | 90.60 (7) | C8—C9—H9B | 108.5 |
O2—Co1—O1Wi | 90.60 (7) | H9A—C9—H9B | 107.5 |
O2i—Co1—O1Wi | 89.40 (7) | C1—N1—C9 | 121.5 (2) |
O1W—Co1—O1Wi | 180.0 | C1—N1—H1 | 121.7 (18) |
O2—Co1—O2Wi | 92.59 (6) | C9—N1—H1 | 116.7 (18) |
O2i—Co1—O2Wi | 87.41 (6) | O1—C1—N1 | 121.7 (2) |
O1W—Co1—O2Wi | 90.55 (7) | O1—C1—C2 | 119.8 (2) |
O1Wi—Co1—O2Wi | 89.45 (7) | N1—C1—C2 | 118.5 (2) |
O2—Co1—O2W | 87.41 (6) | C3—C2—C7 | 118.9 (3) |
O2i—Co1—O2W | 92.59 (6) | C3—C2—C1 | 117.3 (2) |
O1W—Co1—O2W | 89.45 (7) | C7—C2—C1 | 123.8 (2) |
O1Wi—Co1—O2W | 90.55 (7) | C2—C3—C4 | 120.8 (3) |
O2Wi—Co1—O2W | 180.0 | C2—C3—H3 | 119.6 |
Co1—O1W—H1WA | 109 (2) | C4—C3—H3 | 119.6 |
Co1—O1W—H1WB | 118.5 (19) | C5—C4—C3 | 120.2 (3) |
H1WA—O1W—H1WB | 110 (3) | C5—C4—H4 | 119.9 |
Co1ii—O2W—Co1 | 132.03 (11) | C3—C4—H4 | 119.9 |
Co1ii—O2W—H2W | 95 (2) | C6—C5—C4 | 119.3 (3) |
Co1—O2W—H2W | 109 (2) | C6—C5—H5 | 120.3 |
Co1ii—O2W—H2Wii | 109 (2) | C4—C5—H5 | 120.3 |
Co1—O2W—H2Wii | 95 (2) | C5—C6—C7 | 121.5 (3) |
H2W—O2W—H2Wii | 118 (4) | C5—C6—H6 | 119.3 |
C8—O2—Co1 | 126.39 (14) | C7—C6—H6 | 119.3 |
O3—C8—O2 | 125.2 (2) | C2—C7—C6 | 119.3 (3) |
O3—C8—C9 | 121.20 (19) | C2—C7—H7 | 120.4 |
O2—C8—C9 | 113.61 (18) | C6—C7—H7 | 120.4 |
N1—C9—C8 | 115.14 (18) | H3WA—O3W—H3WB | 108 (3) |
N1—C9—H9A | 108.5 | ||
Co1—O2—C8—O3 | −14.5 (3) | N1—C1—C2—C7 | −0.2 (4) |
Co1—O2—C8—C9 | 166.03 (14) | C7—C2—C3—C4 | −1.1 (5) |
O3—C8—C9—N1 | 6.9 (3) | C1—C2—C3—C4 | 177.5 (3) |
O2—C8—C9—N1 | −173.6 (2) | C2—C3—C4—C5 | 0.7 (6) |
C8—C9—N1—C1 | 78.1 (3) | C3—C4—C5—C6 | 0.3 (6) |
C9—N1—C1—O1 | −3.4 (4) | C4—C5—C6—C7 | −0.8 (5) |
C9—N1—C1—C2 | 175.3 (2) | C3—C2—C7—C6 | 0.5 (4) |
O1—C1—C2—C3 | 0.0 (4) | C1—C2—C7—C6 | −178.0 (3) |
N1—C1—C2—C3 | −178.7 (3) | C5—C6—C7—C2 | 0.5 (5) |
O1—C1—C2—C7 | 178.5 (3) |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1, y, −z+3/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1WA···O2ii | 0.78 (3) | 1.93 (3) | 2.714 (2) | 176 (3) |
O1W—H1WB···O3Wi | 0.85 (3) | 1.93 (3) | 2.780 (3) | 178 (3) |
O2W—H2W···O3iii | 0.88 (3) | 1.80 (3) | 2.6576 (18) | 163 (3) |
C9—H9B···O3iv | 0.97 | 2.51 | 3.481 (3) | 178 |
N1—H1···O3Wv | 0.83 (3) | 2.13 (3) | 2.880 (3) | 149 (2) |
O3W—H3WA···O1 | 0.83 (4) | 1.90 (4) | 2.708 (3) | 164 (3) |
O3W—H3WB···O3iii | 0.84 (3) | 2.12 (3) | 2.873 (3) | 149 (3) |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1, y, −z+3/2; (iii) x, −y+1, z+1/2; (iv) x, −y+2, z+1/2; (v) x, y+1, z. |
[Ni(C9H8NO3)2(H2O)3]·2H2O | F(000) = 1056 |
Mr = 505.12 | Dx = 1.497 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
a = 40.884 (4) Å | Cell parameters from 8047 reflections |
b = 6.9438 (8) Å | θ = 3.0–30.5° |
c = 7.8983 (8) Å | µ = 0.93 mm−1 |
β = 91.900 (2)° | T = 293 K |
V = 2241.0 (4) Å3 | Plate, green |
Z = 4 | 0.29 × 0.24 × 0.05 mm |
Bruker D8 Quest Eco diffractometer | 2995 reflections with I > 2σ(I) |
Radiation source: Sealed Tube | Rint = 0.036 |
φ and ω scans | θmax = 30.5°, θmin = 3.0° |
Absorption correction: numerical (SADABS; Krause et al., 2015) | h = −58→58 |
Tmin = 0.608, Tmax = 0.746 | k = −9→9 |
17095 measured reflections | l = −11→11 |
3392 independent reflections |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.056 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.151 | w = 1/[σ2(Fo2) + (0.0534P)2 + 10.915P] where P = (Fo2 + 2Fc2)/3 |
S = 1.15 | (Δ/σ)max < 0.001 |
3392 reflections | Δρmax = 1.24 e Å−3 |
174 parameters | Δρmin = −0.75 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 | ||
Ni1 | 0.500000 | 0.500000 | 0.500000 | 0.01759 (14) | |
O1W | 0.46631 (6) | 0.6995 (4) | 0.4192 (3) | 0.0285 (4) | |
H1WA | 0.4671 (12) | 0.696 (8) | 0.305 (7) | 0.058 (14)* | |
H1WB | 0.4475 (12) | 0.690 (7) | 0.447 (6) | 0.043 (12)* | |
O2W | 0.500000 | 0.3793 (4) | 0.250000 | 0.0202 (5) | |
H2W | 0.4841 (9) | 0.322 (6) | 0.263 (5) | 0.034 (11)* | |
O2 | 0.53585 (5) | 0.6801 (3) | 0.4257 (2) | 0.0268 (4) | |
O3 | 0.55711 (6) | 0.7689 (4) | 0.6765 (3) | 0.0351 (5) | |
C8 | 0.55754 (7) | 0.7599 (4) | 0.5190 (3) | 0.0226 (5) | |
C9 | 0.58529 (8) | 0.8493 (5) | 0.4233 (4) | 0.0300 (6) | |
H9A | 0.593708 | 0.753037 | 0.347050 | 0.036* | |
H9B | 0.576431 | 0.953631 | 0.354201 | 0.036* | |
N1 | 0.61229 (6) | 0.9234 (4) | 0.5260 (4) | 0.0309 (5) | |
H1 | 0.6146 (12) | 1.056 (8) | 0.526 (6) | 0.049 (13)* | |
O1 | 0.63274 (9) | 0.6289 (4) | 0.5816 (5) | 0.0642 (10) | |
C1 | 0.63502 (8) | 0.8063 (5) | 0.5955 (4) | 0.0353 (7) | |
C2 | 0.66370 (8) | 0.8938 (6) | 0.6870 (5) | 0.0379 (7) | |
C3 | 0.68705 (12) | 0.7700 (8) | 0.7561 (6) | 0.0591 (12) | |
H3 | 0.683771 | 0.637691 | 0.748942 | 0.071* | |
C4 | 0.71526 (13) | 0.8407 (11) | 0.8360 (7) | 0.0746 (17) | |
H4 | 0.731124 | 0.755654 | 0.877935 | 0.090* | |
C5 | 0.71989 (12) | 1.0344 (10) | 0.8535 (7) | 0.0687 (16) | |
H5 | 0.738643 | 1.081793 | 0.908817 | 0.082* | |
C6 | 0.69707 (12) | 1.1556 (8) | 0.7899 (6) | 0.0602 (12) | |
H6 | 0.700203 | 1.287520 | 0.802593 | 0.072* | |
C7 | 0.66879 (10) | 1.0893 (7) | 0.7054 (6) | 0.0501 (10) | |
H7 | 0.653429 | 1.176328 | 0.661677 | 0.060* | |
O3W | 0.59732 (7) | 0.3249 (4) | 0.4678 (4) | 0.0389 (6) | |
H3WB | 0.5916 (14) | 0.323 (9) | 0.362 (8) | 0.076 (19)* | |
H3WA | 0.611 (2) | 0.407 (13) | 0.485 (11) | 0.12 (3)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ni1 | 0.0173 (2) | 0.0246 (2) | 0.01079 (19) | −0.00141 (17) | −0.00075 (14) | −0.00031 (17) |
O1W | 0.0269 (10) | 0.0380 (12) | 0.0204 (9) | 0.0067 (9) | −0.0004 (8) | 0.0033 (8) |
O2W | 0.0212 (13) | 0.0262 (13) | 0.0132 (11) | 0.000 | −0.0013 (9) | 0.000 |
O2 | 0.0246 (9) | 0.0393 (12) | 0.0164 (8) | −0.0116 (8) | −0.0010 (7) | 0.0008 (8) |
O3 | 0.0328 (11) | 0.0521 (15) | 0.0204 (9) | −0.0160 (10) | −0.0010 (8) | −0.0017 (9) |
C8 | 0.0221 (12) | 0.0246 (12) | 0.0211 (11) | −0.0038 (9) | −0.0002 (9) | 0.0029 (10) |
C9 | 0.0283 (14) | 0.0373 (16) | 0.0242 (12) | −0.0099 (12) | −0.0006 (10) | 0.0052 (12) |
N1 | 0.0246 (12) | 0.0318 (13) | 0.0360 (13) | −0.0082 (10) | −0.0012 (10) | 0.0031 (11) |
O1 | 0.067 (2) | 0.0349 (15) | 0.089 (3) | −0.0063 (14) | −0.0317 (18) | 0.0038 (15) |
C1 | 0.0331 (16) | 0.0359 (17) | 0.0367 (16) | −0.0054 (13) | −0.0027 (13) | 0.0024 (13) |
C2 | 0.0294 (15) | 0.049 (2) | 0.0352 (16) | −0.0032 (14) | −0.0019 (12) | −0.0030 (15) |
C3 | 0.055 (3) | 0.057 (3) | 0.064 (3) | 0.008 (2) | −0.020 (2) | −0.005 (2) |
C4 | 0.047 (3) | 0.104 (5) | 0.071 (3) | 0.018 (3) | −0.025 (2) | −0.006 (3) |
C5 | 0.039 (2) | 0.108 (5) | 0.058 (3) | −0.020 (3) | −0.010 (2) | −0.014 (3) |
C6 | 0.053 (3) | 0.065 (3) | 0.062 (3) | −0.024 (2) | −0.009 (2) | −0.004 (2) |
C7 | 0.0386 (19) | 0.054 (2) | 0.057 (2) | −0.0104 (18) | −0.0091 (17) | −0.002 (2) |
O3W | 0.0391 (13) | 0.0405 (14) | 0.0367 (13) | −0.0001 (11) | −0.0027 (10) | −0.0007 (11) |
Ni1—O2i | 2.029 (2) | N1—H1 | 0.93 (5) |
Ni1—O2 | 2.029 (2) | O1—C1 | 1.240 (5) |
Ni1—O1Wi | 2.041 (2) | C1—C2 | 1.487 (5) |
Ni1—O1W | 2.041 (2) | C2—C7 | 1.380 (6) |
Ni1—O2Wi | 2.1450 (12) | C2—C3 | 1.384 (6) |
Ni1—O2W | 2.1450 (12) | C3—C4 | 1.386 (7) |
O1W—H1WA | 0.90 (5) | C3—H3 | 0.9300 |
O1W—H1WB | 0.81 (5) | C4—C5 | 1.364 (9) |
O2W—H2W | 0.77 (4) | C4—H4 | 0.9300 |
O2W—H2Wii | 0.77 (4) | C5—C6 | 1.342 (8) |
O2—C8 | 1.262 (3) | C5—H5 | 0.9300 |
O3—C8 | 1.246 (3) | C6—C7 | 1.394 (6) |
C8—C9 | 1.517 (4) | C6—H6 | 0.9300 |
C9—N1 | 1.443 (4) | C7—H7 | 0.9300 |
C9—H9A | 0.9700 | O3W—H3WB | 0.86 (6) |
C9—H9B | 0.9700 | O3W—H3WA | 0.81 (9) |
N1—C1 | 1.338 (5) | ||
O2i—Ni1—O2 | 180.00 (12) | C8—C9—H9A | 108.3 |
O2i—Ni1—O1Wi | 88.72 (10) | N1—C9—H9B | 108.3 |
O2—Ni1—O1Wi | 91.28 (10) | C8—C9—H9B | 108.3 |
O2i—Ni1—O1W | 91.28 (10) | H9A—C9—H9B | 107.4 |
O2—Ni1—O1W | 88.72 (10) | C1—N1—C9 | 121.4 (3) |
O1Wi—Ni1—O1W | 180.0 | C1—N1—H1 | 122 (3) |
O2i—Ni1—O2Wi | 87.27 (8) | C9—N1—H1 | 116 (3) |
O2—Ni1—O2Wi | 92.73 (8) | O1—C1—N1 | 121.2 (3) |
O1Wi—Ni1—O2Wi | 89.87 (8) | O1—C1—C2 | 120.3 (3) |
O1W—Ni1—O2Wi | 90.13 (8) | N1—C1—C2 | 118.5 (3) |
O2i—Ni1—O2W | 92.73 (8) | C7—C2—C3 | 118.0 (4) |
O2—Ni1—O2W | 87.27 (8) | C7—C2—C1 | 124.6 (4) |
O1Wi—Ni1—O2W | 90.13 (8) | C3—C2—C1 | 117.4 (4) |
O1W—Ni1—O2W | 89.87 (8) | C2—C3—C4 | 120.8 (5) |
O2Wi—Ni1—O2W | 180.0 | C2—C3—H3 | 119.6 |
Ni1—O1W—H1WA | 104 (3) | C4—C3—H3 | 119.6 |
Ni1—O1W—H1WB | 120 (3) | C5—C4—C3 | 120.4 (5) |
H1WA—O1W—H1WB | 109 (4) | C5—C4—H4 | 119.8 |
Ni1—O2W—Ni1ii | 134.02 (15) | C3—C4—H4 | 119.8 |
Ni1—O2W—H2W | 93 (3) | C6—C5—C4 | 119.2 (4) |
Ni1ii—O2W—H2W | 111 (3) | C6—C5—H5 | 120.4 |
Ni1—O2W—H2Wii | 111 (3) | C4—C5—H5 | 120.4 |
Ni1ii—O2W—H2Wii | 93 (3) | C5—C6—C7 | 121.8 (5) |
H2W—O2W—H2Wii | 118 (6) | C5—C6—H6 | 119.1 |
C8—O2—Ni1 | 127.02 (18) | C7—C6—H6 | 119.1 |
O3—C8—O2 | 124.9 (3) | C2—C7—C6 | 119.7 (4) |
O3—C8—C9 | 120.8 (2) | C2—C7—H7 | 120.2 |
O2—C8—C9 | 114.3 (2) | C6—C7—H7 | 120.2 |
N1—C9—C8 | 115.9 (2) | H3WB—O3W—H3WA | 110 (7) |
N1—C9—H9A | 108.3 | ||
Ni1—O2—C8—O3 | −13.6 (5) | N1—C1—C2—C3 | −179.3 (4) |
Ni1—O2—C8—C9 | 166.8 (2) | C7—C2—C3—C4 | −2.3 (8) |
O3—C8—C9—N1 | 6.8 (5) | C1—C2—C3—C4 | 176.8 (5) |
O2—C8—C9—N1 | −173.5 (3) | C2—C3—C4—C5 | 2.5 (9) |
C8—C9—N1—C1 | 78.0 (4) | C3—C4—C5—C6 | −1.1 (9) |
C9—N1—C1—O1 | −3.9 (6) | C4—C5—C6—C7 | −0.4 (9) |
C9—N1—C1—C2 | 174.6 (3) | C3—C2—C7—C6 | 0.8 (7) |
O1—C1—C2—C7 | 178.3 (4) | C1—C2—C7—C6 | −178.2 (4) |
N1—C1—C2—C7 | −0.2 (6) | C5—C6—C7—C2 | 0.5 (8) |
O1—C1—C2—C3 | −0.7 (6) |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1, y, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1WA···O2ii | 0.90 (5) | 1.82 (5) | 2.726 (3) | 174 (5) |
O1W—H1WB···O3Wi | 0.81 (5) | 1.97 (5) | 2.783 (4) | 176 (5) |
O2W—H2W···O3i | 0.77 (4) | 1.88 (4) | 2.634 (3) | 167 (4) |
C9—H9B···O3iii | 0.97 | 2.50 | 3.465 (4) | 176 |
N1—H1···O3Wiv | 0.93 (5) | 2.04 (5) | 2.888 (4) | 151 (4) |
O3W—H3WB···O3v | 0.86 (6) | 2.10 (6) | 2.858 (4) | 147 (5) |
O3W—H3WA···O1 | 0.81 (9) | 1.92 (9) | 2.697 (4) | 159 (8) |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1, y, −z+1/2; (iii) x, −y+2, z−1/2; (iv) x, y+1, z; (v) x, −y+1, z−1/2. |
CN = coordination number of metal, C9H9NO3 = N-benzoylglycine, C9H8NO3 = N-benzoylglycinate. |
Compound | Space group | CN | Binding mode | Dimensionality | Refcode |
C9H9NO3 | P212121 | - | - | monomer | HIPPAC |
[Ca(H2O)2(C9H8NO3)2]·H2O | P21/c | 8 | µ2-tridentate | 1D | ANEDON |
[Ba2(H2O)3(C9H8NO3)4] | P1 | 9, 10 | µ3-tridentate, µ3-tetradentate | 2D | HIFFIM |
[Fe(H2O)3(C9H8NO3)2]·2H2O | C2/c | 6 | monodentate | 1D | BITDAJ |
[Co(H2O)3(C9H8NO3)2]·2H2O | C2/c | 6 | monodentate | 1D | COHIPP10, this work |
[Ni(H2O)3(C9H8NO3)2]·2H2O | C2/c | 6 | monodentate | 1D | ANIHIP, this work |
[Cu2(H2O)4(C9H8NO3)4]·2H2O | P21/c | 5, 5 | monodentate, µ2-monoatomic | dimer | CUHIPT |
[Zn(H2O)3(C9H8NO3)2]·2H2O | P1 | 5 | monodentate | monomer | BIZFUL |
[Pb(H2O)2(C9H8NO3)2]·2H2O | C2/c | 8 | µ2-tridentate | 1D | TEZMOA |
References: HIPPAC: Ringertz (1971); ANEDON: Jisha et al. (2010); HIFFIM: Natarajan et al. (2007); BITDAJ: Morelock et al. (1982); COHIPP10: Morelock et al. (1979); CUHIPT: Brown & Trefonas (1973); BIZFUL: Grewe et al. (1982); TEZMOA: Battistuzzi et al. (1996). |
Funding information
KUN acknowledges the University Grants Commission (UGC), New Delhi, for the sanction of a UGC Basic Scientific Research Fellowship. BRS acknowledges the Department of Science & Technology (DST), New Delhi, for the sanction of a Bruker D8 Quest Eco single crystal X-ray diffractometerunder the DST–FIST program.
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