Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S2056989015001152/sj5438sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S2056989015001152/sj5438Isup2.hkl |
CCDC reference: 1044324
Key indicators
- Single-crystal synchrotron study
- T = 301 K
- Mean (C-C) = 0.002 Å
- R factor = 0.028
- wR factor = 0.081
- Data-to-parameter ratio = 15.0
checkCIF/PLATON results
No syntax errors found Datablock: I
Alert level B PLAT029_ALERT_3_B _diffrn_measured_fraction_theta_full Low ....... 0.940 Note
Alert level C PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.600 35 Report PLAT913_ALERT_3_C Missing # of Very Strong Reflections in FCF .... 6 Note
Alert level G ABSMU01_ALERT_1_G Calculation of _exptl_absorpt_correction_mu not performed for this radiation type. PLAT002_ALERT_2_G Number of Distance or Angle Restraints on AtSite 2 Note PLAT042_ALERT_1_G Calc. and Reported MoietyFormula Strings Differ Please Check PLAT066_ALERT_1_G Predicted and Reported Tmin&Tmax Range Identical ? Check PLAT172_ALERT_4_G The CIF-Embedded .res File Contains DFIX Records 1 Report PLAT860_ALERT_3_G Number of Least-Squares Restraints ............. 1 Note PLAT910_ALERT_3_G Missing # of FCF Reflection(s) Below Th(Min) ... 4 Report PLAT912_ALERT_4_G Missing # of FCF Reflections Above STh/L= 0.600 12 Note PLAT952_ALERT_5_G Calculated (ThMax) and CIF-Reported Lmax Differ 4 Units PLAT958_ALERT_1_G Calculated (ThMax) and Actual (FCF) Lmax Differ 4 Units
0 ALERT level A = Most likely a serious problem - resolve or explain 1 ALERT level B = A potentially serious problem, consider carefully 2 ALERT level C = Check. Ensure it is not caused by an omission or oversight 10 ALERT level G = General information/check it is not something unexpected 4 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 5 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check
Pyridine-2,6-dicarboxylic acid (also known as dipicolinic acid and abbreviated here as H2pydc) can coordinate a metal center as a neutral molecule (H2pydc), the univalent anion (Hpydc-), or the divalent anion (pydc2-). In particular, the pyridine-2,6-dicarboxylate ligand frequently acts as a meridional tridentate ligand and sometimes also as a bidentate or bridging ligand (Park et al., 2007). The first [Cr(pydc)2]- complex was prepared as the Na+ salt according to the literature (Hoggard & Schmidtke, 1973) and its crystal structure determined using synchrotron data. Structural analysis showed the compound to be a dihydrate (Dai et al., 2006; González-Baró et al., 2008) rather than the 1.5 or 2.5 hydrates that had been suggested previously (Hoggard & Schmidtke, 1973; Fürst et al., 1979). The crystal structures of K[Cr(pydc)2] (Hakimi et al., 2012) and Rb[Cr(pydc)2] (Fürst et al., 1979) have also been reported previously but the structure of the ammonium salt is not known. Here we report the crystal structure of NH4[Cr(pydc)2] in order to clarify unambiguously the bonding mode of the two pyridine-2,6-dicarboxylato ligands and the geometrical arrangement of this ammonium salt.
Counter-ionic species play a very important role in coordination chemistry. The structure reported here is another example of a [Cr(pydc)2]- salt but with a different cation. The structural analysis shows that the two tridentate pyridine-2,6-dicarboxylate (pydc) dianions octahedrally coordinate to the CrIII metal center through one N atom and two carboxylate O atoms in a meridional arrangement. The CrIII ion is located on a crystallographic fourfold rotoinversion axis (4). An ellipsoid plot of title complex together with the atomic numbering is illustrated in Fig. 1.
The Cr—N and Cr—O bond lengths to the pydc ligands are 1.9727 (15) and 1.9889 (9) Å, respectively, and these lengths agree well with the values observed in the literature for complexes with the same [Cr(pydc)2]- anion (Fürst et al., 1979; Dai et al., 2006; González-Baró et al., 2008; Zhou et al., 2009; Hakimi et al., 2012). The coordinating pyridine N atoms are in a mutually trans arrangement. Both tridendate pydc2- ligands are nearly planar and are oriented perpendicular to one another. Bond angles about the central chromium atom are 79.10 (3) for N1—Cr1—O1, 100.90 (3) for N1—Cr1—O1i and 158.20 (5)° for O1i-–Cr1—O1ii, indicating a distorted octahedral coordination environment [symmetry codes: (i) -y+5/4, x-3/4, -z+5/4; (ii) y+3/4, -x+5/4, -z+5/4]. The C1—O1 and C1—O2 bond lengths within the carboxylate group of the pydc2- ligand are 1.2941 (15) and 1.2223 (14) Å, respectively, and can be compared with values of 1.298 (5) and 1.224 (5) Å for Rb[Cr(pydc)2] (Fürst et al., 1979). The ammonium cation, also lying on a crystallographic fourfold rotoinversion axis (4), shows a distorted tetrahedral geometry of the hydrogen atoms around the central nitrogen atom with N—H distances of 0.846 (9) Å and the H—N—H angles ranging from 105.36 (9) to 118.06 (9)°.
The pattern of hydrogen bonding around the cation is very similar to the coordination environment in the related potassium salt (Hakimi et al., 2012). The non-coordinating carbonyl O atom forms weak C—H···O hydrogen bonds that contribute to the crystal packing. The ammonium cation is also linked to the carbonyl O atoms from four neighboring pydc2- ligands through classical N—H···O hydrogen bonds (Table 1). An extensive array of these contacts generate a three-dimensional network of molecules stacked along the a-axis direction (Fig. 2). π–π interactions involving adjacent pyridine rings further link the components of the structure into a three-dimensional network. The centroid–centroid distances between the π–π stacked rings (N1/C2–C4/C3iv/C2iv)···(N1v/C2v–C4v/C3vi/C2vi) is 3.572 (2) Å [symmetry codes: (iv) 2 - x, 1/2 - y, z; (v) 1/2 + x, y, 3/2 - z; (vi) 5/2 -x, 1/2 - y, 3/2 - z].
A search of the Cambridge Structural Database (Version 5.35, May 2014 with one update; Groom & Allen, 2014) indicates a total of 16 hits for CrIII complexes with a complex anion [Cr(pydc)2]- unit. Many crystal structures of [Cr(pydc)2]- with inorganic, organic or complex counter-cations such as K+ (Hakimi et al., 2012), Na+ (Dai et al., 2006; González-Baró et al., 2008; Zhou et al., 2009), Rb+ (Fürst et al., 1979), creatH+ (creat = creatinine; Aghabozorg et al., 2008), 4,4'-bpyH+ (bpy = bipyridine; Soleimannejad et al., 2008), dmpH+ (dmp = 2,9-dimethyl-1,10-phenanthrone; Aghajani et al., 2009), 2-apymH+ (2-apym = 2-aminopyrimidine; Eshtiagh-Hosseini et al., 2010), [Cr(tpy)(pydc)]+ [tpy = 2,6-bis(2-pyridyl)pyridine; Casellato et al., 1991] and [Ag(atr)2]+ (atr = 3-amino-1H-1,2,4-triazole; Tabatabaee et al., 2011) have been determined.
Alternative coordination behaviors of the pydc ligands are found in [Cu(Hpydc)2]·3H2O, which has one neutral H2pydc and one divalent pydc2- ligand, while [Ni(Hpydc)2]·3H2O (Nathan & Mai, 2000) has two meridional univalent Hpydc- ligands. The ligands in [Ni(cyclam)(Hpydc)2]·2H2O (Park et al., 2007) and Na2[Pt(Hpydc)2]·6H2O are monodentate and bidentate, respectively, while Hpydc- is tridentate in the complexes [Cu(Hpydc)2]·3H2O and [Ni(Hpydc)2]·3H2O (Nathan & Mai, 2000).
All chemicals were reagent-grade materials and were used without further purification. The starting material, Na[Cr(pydc)2]·2H2O was prepared as described previously (Hoggard & Schmidtke, 1973). The sodium salt (0.20 g) was dissolved in 15 ml of water at 323 K and added to 3 ml of water containing 0.5 g of NH4Cl. The resulting solution was filtered and allowed to stand at room temperature for several days to give brown block-like crystals of the ammonium salt NH4[Cr(pydc)2] suitable for X-ray structural analysis.
Crystal data, data collection and structure refinement details are summarized in Table 2. All H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with C—H distances of 0.95 (ring H atoms) and with Uiso(H) = 1.2 Ueq(parent atom). The H atoms of the ammonium cation were located from difference Fourier maps and refined with restraints and a fixed N—H distance of 0.87 Å, with Uiso(H) = 1.2Ueq(N). One reflection with Fo<<<Fc was omitted from the final refinement cycles. The slightly low fraction of measured reflections results from the geometry of the 2D-SMC beamline goniostat.
Data collection: PAL ADSC Quantum-210 ADX (Arvai & Nielsen, 1983); cell refinement: HKL3000sm (Otwinowski & Minor, 1997); data reduction: HKL3000sm (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXT2014/5 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014/7 (Sheldrick, 2008, 2015b); molecular graphics: DIAMOND (Brandenburg, 2007); software used to prepare material for publication: publCIF (Westrip 2010).
(NH4)[Cr(C7H3NO4)2] | Dx = 1.855 Mg m−3 |
Mr = 400.25 | Synchrotron radiation, λ = 0.62998 Å |
Tetragonal, I41/a | Cell parameters from 20017 reflections |
a = 7.0305 (10) Å | θ = 0.4–33.6° |
c = 28.995 (6) Å | µ = 0.62 mm−1 |
V = 1433.2 (5) Å3 | T = 301 K |
Z = 4 | Block, brown |
F(000) = 812 | 0.15 × 0.10 × 0.10 mm |
ADSC Q210 CCD area detector diffractometer | 903 reflections with I > 2σ(I) |
Radiation source: PLSII 2D bending magnet | Rint = 0.052 |
ω scan | θmax = 26.0°, θmin = 4.0° |
Absorption correction: empirical (using intensity measurements) (HKL3000sm SCALEPACK; Otwinowski & Minor, 1997) | h = −9→9 |
Tmin = 0.925, Tmax = 0.940 | k = −9→9 |
6841 measured reflections | l = −36→36 |
943 independent reflections |
Refinement on F2 | 1 restraint |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.028 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.081 | w = 1/[σ2(Fo2) + (0.0461P)2 + 0.7347P] where P = (Fo2 + 2Fc2)/3 |
S = 1.21 | (Δ/σ)max = 0.001 |
943 reflections | Δρmax = 0.31 e Å−3 |
63 parameters | Δρmin = −0.86 e Å−3 |
(NH4)[Cr(C7H3NO4)2] | Z = 4 |
Mr = 400.25 | Synchrotron radiation, λ = 0.62998 Å |
Tetragonal, I41/a | µ = 0.62 mm−1 |
a = 7.0305 (10) Å | T = 301 K |
c = 28.995 (6) Å | 0.15 × 0.10 × 0.10 mm |
V = 1433.2 (5) Å3 |
ADSC Q210 CCD area detector diffractometer | 943 independent reflections |
Absorption correction: empirical (using intensity measurements) (HKL3000sm SCALEPACK; Otwinowski & Minor, 1997) | 903 reflections with I > 2σ(I) |
Tmin = 0.925, Tmax = 0.940 | Rint = 0.052 |
6841 measured reflections |
R[F2 > 2σ(F2)] = 0.028 | 1 restraint |
wR(F2) = 0.081 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.21 | Δρmax = 0.31 e Å−3 |
943 reflections | Δρmin = −0.86 e Å−3 |
63 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. |
x | y | z | Uiso*/Ueq | ||
Cr1 | 1.0000 | 0.2500 | 0.6250 | 0.01282 (14) | |
O1 | 0.88412 (13) | 0.50247 (12) | 0.63797 (3) | 0.0205 (2) | |
O2 | 0.78279 (14) | 0.69538 (13) | 0.69398 (4) | 0.0261 (2) | |
N1 | 1.0000 | 0.2500 | 0.69303 (5) | 0.0133 (3) | |
C1 | 0.86229 (15) | 0.55077 (15) | 0.68071 (4) | 0.0163 (2) | |
C2 | 0.93527 (14) | 0.40403 (15) | 0.71495 (4) | 0.0142 (2) | |
C3 | 0.93425 (15) | 0.41005 (17) | 0.76260 (4) | 0.0189 (2) | |
H3 | 0.8912 | 0.5171 | 0.7783 | 0.023* | |
C4 | 1.0000 | 0.2500 | 0.78645 (6) | 0.0201 (3) | |
H4 | 1.0000 | 0.2500 | 0.8185 | 0.024* | |
N1S | 0.5000 | 0.7500 | 0.6250 | 0.0223 (4) | |
H1S | 0.502 (3) | 0.8529 (19) | 0.6099 (7) | 0.027* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cr1 | 0.01591 (16) | 0.01591 (16) | 0.0066 (2) | 0.000 | 0.000 | 0.000 |
O1 | 0.0286 (4) | 0.0193 (4) | 0.0134 (5) | 0.0055 (3) | −0.0013 (3) | 0.0013 (3) |
O2 | 0.0304 (5) | 0.0222 (4) | 0.0258 (5) | 0.0098 (3) | −0.0009 (3) | −0.0037 (3) |
N1 | 0.0146 (5) | 0.0171 (6) | 0.0082 (7) | 0.0008 (4) | 0.000 | 0.000 |
C1 | 0.0159 (4) | 0.0170 (5) | 0.0160 (6) | 0.0004 (3) | −0.0013 (4) | −0.0005 (4) |
C2 | 0.0133 (4) | 0.0175 (4) | 0.0117 (5) | 0.0001 (3) | −0.0005 (3) | −0.0016 (3) |
C3 | 0.0171 (5) | 0.0258 (5) | 0.0137 (6) | −0.0006 (4) | 0.0005 (3) | −0.0059 (4) |
C4 | 0.0199 (7) | 0.0324 (8) | 0.0078 (8) | −0.0021 (5) | 0.000 | 0.000 |
N1S | 0.0220 (6) | 0.0220 (6) | 0.0229 (12) | 0.000 | 0.000 | 0.000 |
Cr1—N1 | 1.9727 (15) | N1—C2 | 1.3355 (12) |
Cr1—N1i | 1.9727 (15) | C1—C2 | 1.5208 (15) |
Cr1—O1 | 1.9889 (9) | C2—C3 | 1.3824 (16) |
Cr1—O1ii | 1.9889 (9) | C3—C4 | 1.3993 (15) |
Cr1—O1i | 1.9889 (9) | C3—H3 | 0.9300 |
Cr1—O1iii | 1.9889 (9) | C4—C3iii | 1.3992 (15) |
O1—C1 | 1.2941 (15) | C4—H4 | 0.9300 |
O2—C1 | 1.2223 (14) | N1S—H1S | 0.846 (9) |
N1—C2iii | 1.3354 (12) | ||
N1—Cr1—N1i | 180.0 | C2iii—N1—C2 | 123.19 (15) |
N1—Cr1—O1 | 79.10 (3) | C2iii—N1—Cr1 | 118.40 (7) |
N1i—Cr1—O1 | 100.90 (3) | C2—N1—Cr1 | 118.41 (7) |
N1—Cr1—O1ii | 100.90 (3) | O2—C1—O1 | 125.02 (11) |
N1i—Cr1—O1ii | 79.10 (3) | O2—C1—C2 | 120.87 (11) |
O1—Cr1—O1ii | 92.049 (10) | O1—C1—C2 | 114.02 (9) |
N1—Cr1—O1i | 100.90 (3) | N1—C2—C3 | 120.14 (11) |
N1i—Cr1—O1i | 79.10 (3) | N1—C2—C1 | 110.77 (10) |
O1—Cr1—O1i | 92.049 (10) | C3—C2—C1 | 129.04 (10) |
O1ii—Cr1—O1i | 158.20 (5) | C2—C3—C4 | 117.88 (11) |
N1—Cr1—O1iii | 79.10 (3) | C2—C3—H3 | 121.1 |
N1i—Cr1—O1iii | 100.90 (3) | C4—C3—H3 | 121.1 |
O1—Cr1—O1iii | 158.20 (5) | C3iii—C4—C3 | 120.77 (16) |
O1ii—Cr1—O1iii | 92.049 (10) | C3iii—C4—H4 | 119.6 |
O1i—Cr1—O1iii | 92.049 (10) | C3—C4—H4 | 119.6 |
C1—O1—Cr1 | 117.64 (7) | ||
Cr1—O1—C1—O2 | −175.18 (9) | O1—C1—C2—N1 | −2.76 (12) |
Cr1—O1—C1—C2 | 1.39 (12) | O2—C1—C2—C3 | −3.27 (17) |
C2iii—N1—C2—C3 | 0.47 (7) | O1—C1—C2—C3 | −179.99 (10) |
Cr1—N1—C2—C3 | −179.53 (7) | N1—C2—C3—C4 | −0.90 (14) |
C2iii—N1—C2—C1 | −177.04 (9) | C1—C2—C3—C4 | 176.10 (9) |
Cr1—N1—C2—C1 | 2.96 (9) | C2—C3—C4—C3iii | 0.44 (7) |
O2—C1—C2—N1 | 173.96 (9) |
Symmetry codes: (i) y+3/4, −x+5/4, −z+5/4; (ii) −y+5/4, x−3/4, −z+5/4; (iii) −x+2, −y+1/2, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···O2iv | 0.93 | 2.50 | 3.4071 (15) | 167 |
N1S—H1S···O2v | 0.85 (1) | 2.04 (1) | 2.8462 (11) | 158 (2) |
Symmetry codes: (iv) −x+3/2, −y+3/2, −z+3/2; (v) −y+5/4, x+1/4, −z+5/4. |
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···O2i | 0.93 | 2.50 | 3.4071 (15) | 166.5 |
N1S—H1S···O2ii | 0.846 (9) | 2.044 (11) | 2.8462 (11) | 158.1 (19) |
Symmetry codes: (i) −x+3/2, −y+3/2, −z+3/2; (ii) −y+5/4, x+1/4, −z+5/4. |
Experimental details
Crystal data | |
Chemical formula | (NH4)[Cr(C7H3NO4)2] |
Mr | 400.25 |
Crystal system, space group | Tetragonal, I41/a |
Temperature (K) | 301 |
a, c (Å) | 7.0305 (10), 28.995 (6) |
V (Å3) | 1433.2 (5) |
Z | 4 |
Radiation type | Synchrotron, λ = 0.62998 Å |
µ (mm−1) | 0.62 |
Crystal size (mm) | 0.15 × 0.10 × 0.10 |
Data collection | |
Diffractometer | ADSC Q210 CCD area detector diffractometer |
Absorption correction | Empirical (using intensity measurements) (HKL3000sm SCALEPACK; Otwinowski & Minor, 1997) |
Tmin, Tmax | 0.925, 0.940 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6841, 943, 903 |
Rint | 0.052 |
(sin θ/λ)max (Å−1) | 0.695 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.028, 0.081, 1.21 |
No. of reflections | 943 |
No. of parameters | 63 |
No. of restraints | 1 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.31, −0.86 |
Computer programs: PAL ADSC Quantum-210 ADX (Arvai & Nielsen, 1983), HKL3000sm (Otwinowski & Minor, 1997), SHELXT2014/5 (Sheldrick, 2015a), SHELXL2014/7 (Sheldrick, 2008, 2015b), DIAMOND (Brandenburg, 2007), publCIF (Westrip 2010).