metal-organic compounds
5,6-Dihydro-1,10-phenanthroline-1,10-diium μ-oxido-bis[pentafluoridotantalate(V)]
aCollege of Chemistry and Pharmacy Engineering, Nanyang Normal University, Nanyang 473061, People's Republic of China
*Correspondence e-mail: nysymzh@126.com
In the title compound, (C12H12N2)[Ta2F10O], the doubly protonated 5,6-dihydro-1,10-phenantroline-1,10-diium cation is located on a twofold rotation axis, whereas the isolated [Ta2OF10]2− dianion has -1 symmetry. In the so far unknown dianion, the symmetry-related TaV atoms are octahedrally coordinated by five F atoms and a bridging O atom, the latter being located on an inversion centre. The two pyridine rings in the cation make a dihedral angle of 22.8 (4)°. The cations and dianions are arranged in layers parallel to (100) and are connected through N—H⋯F and C—H⋯F hydrogen-bonding interactions into a three-dimensional structure.
Related literature
For structure–property relations of metal oxyfluorides, see: Hagerman & Poeppelmeier (1995); Halasyamani & Poeppelmeier (1998); Welk et al. (2002).
Experimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2008); cell SAINT (Bruker, 2008); 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/S1600536812014742/wm2602sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812014742/wm2602Isup2.hkl
All chemicals were of reagent grade quality obtained from commercial sources and were used without further purification. The title compound was obtained by using a two-step hydrothermal method in a 50 mL Teflon-lined autoclave. Firstly, 0.66 g Ta2O5 (1.5 mmol) was dissolved in 1.11 g HF (40wt%) (7.4 mmol) and heated to 453 K for 4 hours. After it was cooled, the solution was added into 0.90 mL H3PO4 (85wt%), 0.24 g 2,2'-bipyridine (1.5 mmol), 2.0 mL ethylene glycol and 1.0 mL H2O. Then the mixture was stirred for half an hour, and transferred into a Teflon-lined stainless steel autoclave (50 mL) and treated at 453 K for 7 days. After the mixture was slowly cooled to room temperature, yellow block-like crystals suitable for X-ray
were obtained. It worth noting that the reaction of 2,2'-bipyridine and ethylene glycol produced the 5,6-dihydro-1,10-phenantroline ligand. The chemical composition of the title compound was confirmed by EDS and elemental analysis. The results of EDS indicate the presence of the elements Ta, F, O, C and N. The Ta composition was quantified by ICP-OES: Anal./Calcd (%): Ta: 48.59/48.12. C, H, and N analysis was performed on a PerkinElmer 2400II elemental analyzer. Anal./Calcd (%): C, 19.16; H, 1.61; N,3.72 %. Found: C, 19.63; H, 1.94; N, 3.17 %. IR (KBr, cm-1) (Fig. 3): 3110, 3057, 2920, 2861, 1621,1584,1494, 1457, 1431, 1367, 1330, 1282, 1234, 1181, 1149, 1033, 869, 784, 715, 593 and 535.The H atoms bonded to C and N were positioned geometrically and refined using a riding model, with C—H = 0.93 Å for H atoms bound to sp2 C atoms, and 0.97 Å for H atoms bound to sp3 C atoms, and with N—H = 0.86 Å, and with Uiso(H) = 1.2 (1.5) times Ueq(C), and Uiso(H) = 1.2 times Ueq(N), respectively. The highest and lowest remaining electron density was located 0.84 Å and 0.72 Å from atom Ta1.
Data collection: APEX2 (Bruker, 2008); cell
SAINT (Bruker, 2008); data reduction: SAINT (Bruker, 2008); 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).(C12H12N2)[Ta2F10O] | F(000) = 1368 |
Mr = 752.14 | Dx = 2.831 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -C 2yc | Cell parameters from 3156 reflections |
a = 13.536 (2) Å | θ = 2.4–28.3° |
b = 11.3031 (17) Å | µ = 12.50 mm−1 |
c = 11.5316 (17) Å | T = 296 K |
β = 90.093 (2)° | Block, yellow |
V = 1764.4 (5) Å3 | 0.21 × 0.20 × 0.17 mm |
Z = 4 |
Bruker APEXII CCD diffractometer | 1725 independent reflections |
Radiation source: fine-focus sealed tube | 1573 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.029 |
ϕ and ω scans | θmax = 26.0°, θmin = 2.9° |
Absorption correction: multi-scan (SADABS; Bruker, 2008) | h = −13→16 |
Tmin = 0.179, Tmax = 0.225 | k = −13→13 |
4738 measured reflections | l = −14→12 |
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)] = 0.028 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.072 | H-atom parameters constrained |
S = 1.05 | w = 1/[σ2(Fo2) + (0.0278P)2 + 20.5568P] where P = (Fo2 + 2Fc2)/3 |
1725 reflections | (Δ/σ)max < 0.001 |
124 parameters | Δρmax = 1.96 e Å−3 |
0 restraints | Δρmin = −1.14 e Å−3 |
(C12H12N2)[Ta2F10O] | V = 1764.4 (5) Å3 |
Mr = 752.14 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 13.536 (2) Å | µ = 12.50 mm−1 |
b = 11.3031 (17) Å | T = 296 K |
c = 11.5316 (17) Å | 0.21 × 0.20 × 0.17 mm |
β = 90.093 (2)° |
Bruker APEXII CCD diffractometer | 1725 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2008) | 1573 reflections with I > 2σ(I) |
Tmin = 0.179, Tmax = 0.225 | Rint = 0.029 |
4738 measured reflections |
R[F2 > 2σ(F2)] = 0.028 | 0 restraints |
wR(F2) = 0.072 | H-atom parameters constrained |
S = 1.05 | w = 1/[σ2(Fo2) + (0.0278P)2 + 20.5568P] where P = (Fo2 + 2Fc2)/3 |
1725 reflections | Δρmax = 1.96 e Å−3 |
124 parameters | Δρmin = −1.14 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 | ||
Ta1 | 0.193168 (19) | 0.18732 (2) | 0.13666 (2) | 0.03630 (12) | |
C2 | 0.9169 (6) | 0.2166 (8) | 0.9660 (7) | 0.0499 (19) | |
H2A | 0.9123 | 0.1448 | 1.0050 | 0.060* | |
C1 | 0.9649 (4) | 0.2220 (5) | 0.8646 (5) | 0.0210 (10) | |
C5 | 0.9738 (5) | 0.3254 (5) | 0.8051 (5) | 0.0332 (13) | |
N1 | 0.9318 (6) | 0.4270 (7) | 0.8502 (7) | 0.069 (2) | |
H1A | 0.9361 | 0.4931 | 0.8136 | 0.083* | |
C4 | 0.8832 (7) | 0.4207 (9) | 0.9546 (7) | 0.062 (2) | |
H4A | 0.8558 | 0.4890 | 0.9858 | 0.075* | |
C3 | 0.8742 (7) | 0.3164 (9) | 1.0135 (7) | 0.060 (2) | |
H3A | 0.8403 | 0.3127 | 1.0834 | 0.072* | |
F1 | 0.2944 (5) | 0.0732 (6) | 0.1479 (5) | 0.093 (2) | |
F2 | 0.1355 (4) | 0.1192 (5) | 0.2716 (4) | 0.0684 (14) | |
F3 | 0.1159 (4) | 0.0811 (4) | 0.0475 (4) | 0.0692 (15) | |
F4 | 0.0908 (5) | 0.2992 (5) | 0.1343 (7) | 0.0867 (19) | |
F5 | 0.2665 (4) | 0.2877 (5) | 0.2351 (5) | 0.0720 (15) | |
O1 | 0.2500 | 0.2500 | 0.0000 | 0.082 (3) | |
C6 | 1.0104 (5) | 0.1139 (6) | 0.8134 (6) | 0.0408 (15) | |
H6A | 0.9827 | 0.0436 | 0.8490 | 0.049* | |
H6B | 1.0811 | 0.1141 | 0.8270 | 0.049* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ta1 | 0.03744 (18) | 0.03940 (18) | 0.03206 (18) | −0.00695 (11) | 0.00427 (11) | −0.00056 (11) |
C2 | 0.047 (4) | 0.069 (5) | 0.033 (4) | −0.008 (4) | 0.001 (3) | 0.012 (4) |
C1 | 0.023 (3) | 0.023 (2) | 0.016 (2) | −0.001 (2) | 0.004 (2) | 0.002 (2) |
C5 | 0.039 (3) | 0.032 (3) | 0.028 (3) | 0.000 (3) | 0.001 (3) | −0.004 (2) |
N1 | 0.087 (5) | 0.062 (5) | 0.059 (4) | 0.015 (4) | 0.000 (4) | −0.007 (4) |
C4 | 0.069 (6) | 0.076 (6) | 0.042 (4) | 0.016 (5) | 0.015 (4) | −0.022 (4) |
C3 | 0.056 (5) | 0.099 (7) | 0.025 (4) | 0.003 (4) | 0.013 (3) | −0.012 (4) |
F1 | 0.094 (4) | 0.117 (5) | 0.066 (3) | 0.058 (4) | −0.006 (3) | −0.024 (3) |
F2 | 0.097 (4) | 0.066 (3) | 0.042 (3) | −0.019 (3) | 0.024 (3) | 0.005 (2) |
F3 | 0.095 (4) | 0.065 (3) | 0.048 (3) | −0.038 (3) | −0.010 (3) | 0.002 (2) |
F4 | 0.070 (4) | 0.061 (3) | 0.128 (6) | 0.017 (3) | −0.009 (4) | 0.007 (3) |
F5 | 0.071 (3) | 0.082 (4) | 0.063 (3) | −0.031 (3) | 0.001 (3) | −0.023 (3) |
O1 | 0.106 (8) | 0.095 (7) | 0.045 (5) | −0.054 (6) | 0.018 (5) | 0.008 (5) |
C6 | 0.043 (4) | 0.031 (3) | 0.048 (4) | 0.002 (3) | 0.005 (3) | 0.004 (3) |
Ta1—F4 | 1.877 (5) | C5—N1 | 1.384 (9) |
Ta1—F5 | 1.886 (5) | C5—C5i | 1.455 (13) |
Ta1—F1 | 1.886 (5) | N1—C4 | 1.374 (11) |
Ta1—O1 | 1.8924 (3) | N1—H1A | 0.8600 |
Ta1—F3 | 1.895 (4) | C4—C3 | 1.366 (13) |
Ta1—F2 | 1.905 (4) | C4—H4A | 0.9300 |
C2—C1 | 1.340 (9) | C3—H3A | 0.9300 |
C2—C3 | 1.381 (12) | O1—Ta1ii | 1.8924 (3) |
C2—H2A | 0.9300 | C6—C6i | 1.488 (14) |
C1—C5 | 1.361 (8) | C6—H6A | 0.9700 |
C1—C6 | 1.490 (8) | C6—H6B | 0.9700 |
F4—Ta1—F5 | 89.5 (3) | C5—C1—C6 | 117.8 (5) |
F4—Ta1—F1 | 176.8 (3) | C1—C5—N1 | 119.1 (6) |
F5—Ta1—F1 | 89.3 (3) | C1—C5—C5i | 119.0 (4) |
F4—Ta1—O1 | 92.1 (2) | N1—C5—C5i | 122.0 (5) |
F5—Ta1—O1 | 93.55 (17) | C4—N1—C5 | 118.9 (8) |
F1—Ta1—O1 | 91.0 (2) | C4—N1—H1A | 120.5 |
F4—Ta1—F3 | 90.7 (3) | C5—N1—H1A | 120.5 |
F5—Ta1—F3 | 175.8 (2) | C3—C4—N1 | 121.6 (8) |
F1—Ta1—F3 | 90.2 (3) | C3—C4—H4A | 119.2 |
O1—Ta1—F3 | 90.60 (15) | N1—C4—H4A | 119.2 |
F4—Ta1—F2 | 88.9 (3) | C4—C3—C2 | 118.1 (7) |
F5—Ta1—F2 | 88.1 (2) | C4—C3—H3A | 121.0 |
F1—Ta1—F2 | 88.1 (3) | C2—C3—H3A | 121.0 |
O1—Ta1—F2 | 178.07 (15) | Ta1ii—O1—Ta1 | 180.00 (2) |
F3—Ta1—F2 | 87.7 (2) | C1—C6—C6i | 108.2 (5) |
C1—C2—C3 | 120.8 (7) | C1—C6—H6A | 110.1 |
C1—C2—H2A | 119.6 | C6i—C6—H6A | 110.1 |
C3—C2—H2A | 119.6 | C1—C6—H6B | 110.1 |
C2—C1—C5 | 121.5 (6) | C6i—C6—H6B | 110.1 |
C2—C1—C6 | 120.7 (6) | H6A—C6—H6B | 108.4 |
C3—C2—C1—C5 | 0.4 (11) | C5i—C5—N1—C4 | 179.8 (8) |
C3—C2—C1—C6 | −179.6 (7) | C5—N1—C4—C3 | −1.0 (13) |
C2—C1—C5—N1 | −0.4 (10) | N1—C4—C3—C2 | 1.0 (14) |
C6—C1—C5—N1 | 179.6 (6) | C1—C2—C3—C4 | −0.7 (13) |
C2—C1—C5—C5i | −179.6 (8) | C2—C1—C6—C6i | 138.0 (7) |
C6—C1—C5—C5i | 0.4 (10) | C5—C1—C6—C6i | −42.0 (9) |
C1—C5—N1—C4 | 0.7 (11) |
Symmetry codes: (i) −x+2, y, −z+3/2; (ii) −x+1/2, −y+1/2, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···F4iii | 0.86 | 2.45 | 3.114 (10) | 135 |
C4—H4A···F1iv | 0.93 | 2.26 | 3.066 (9) | 145 |
C6—H6A···F3v | 0.97 | 2.28 | 3.219 (8) | 163 |
C6—H6B···F5vi | 0.97 | 2.45 | 3.268 (9) | 142 |
Symmetry codes: (iii) −x+1, −y+1, −z+1; (iv) x+1/2, y+1/2, z+1; (v) −x+1, −y, −z+1; (vi) −x+3/2, −y+1/2, −z+1. |
Experimental details
Crystal data | |
Chemical formula | (C12H12N2)[Ta2F10O] |
Mr | 752.14 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 296 |
a, b, c (Å) | 13.536 (2), 11.3031 (17), 11.5316 (17) |
β (°) | 90.093 (2) |
V (Å3) | 1764.4 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 12.50 |
Crystal size (mm) | 0.21 × 0.20 × 0.17 |
Data collection | |
Diffractometer | Bruker APEXII CCD diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2008) |
Tmin, Tmax | 0.179, 0.225 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4738, 1725, 1573 |
Rint | 0.029 |
(sin θ/λ)max (Å−1) | 0.617 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.028, 0.072, 1.05 |
No. of reflections | 1725 |
No. of parameters | 124 |
H-atom treatment | H-atom parameters constrained |
w = 1/[σ2(Fo2) + (0.0278P)2 + 20.5568P] where P = (Fo2 + 2Fc2)/3 | |
Δρmax, Δρmin (e Å−3) | 1.96, −1.14 |
Computer programs: APEX2 (Bruker, 2008), SAINT (Bruker, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
Ta1—F4 | 1.877 (5) | Ta1—O1 | 1.8924 (3) |
Ta1—F5 | 1.886 (5) | Ta1—F3 | 1.895 (4) |
Ta1—F1 | 1.886 (5) | Ta1—F2 | 1.905 (4) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···F4i | 0.86 | 2.45 | 3.114 (10) | 134.5 |
C4—H4A···F1ii | 0.93 | 2.26 | 3.066 (9) | 145.0 |
C6—H6A···F3iii | 0.97 | 2.28 | 3.219 (8) | 162.8 |
C6—H6B···F5iv | 0.97 | 2.45 | 3.268 (9) | 141.7 |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) x+1/2, y+1/2, z+1; (iii) −x+1, −y, −z+1; (iv) −x+3/2, −y+1/2, −z+1. |
References
Bruker (2008). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Hagerman, M. E. & Poeppelmeier, K. R. (1995). Chem. Mater. 7, 602–621. CrossRef CAS Web of Science Google Scholar
Halasyamani, P. S. & Poeppelmeier, K. R. (1998). Chem. Mater. 10, 2753–2769. Web of Science CrossRef CAS Google Scholar
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Welk, M. E., Norquist, A. J., Arnold, F. P., Stern, C. L. & Poeppelmeier, K. R. (2002). Inorg. Chem. 41, 5119–5125. Web of Science CSD CrossRef PubMed CAS Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Metal oxyfluorides have received considerable attention in recent years due to their structure-related properties such as ferroelectricity, piezoelectricity and second-order nonlinear optical activity (Hagerman & Poeppelmeier, 1995; Halasyamani & Poeppelmeier, 1998; Welk et al., 2002). In this article, we report on a new oxidofluoridotantalate with composition [C12H12N2][Ta2OF10] that was obtained by means of a two-step hydrothermal method.
The title compound (Fig. 1) contains one diprotonated 5,6-dihydro-1,10-phenantroline-1,10-diium cation (symmetry 2) and one [Ta2OF10]2- dianion (symmetry 1). In the latter, the TaV ion is coordinated by five fluorine atoms and one oxygen atom, forming an octahedral coordination geometry. It is noteworthy that the title compound features the first oxidofluoridotantalate with composition [Ta2OF10]2-. The cation is not flat, as can be expected from the 5,6-dihydro bridging sp3 carbon atoms, with a dihedral angle of of 22.8 (4)° between the two pyridine rings. The cations and dianions are arranged in layers parallel to (100) and are connected through N—H···F and C—H···F hydrogen bonding interactions into a three-dimensional structure (Fig. 2).
It should be noted that the hydrothermal conditions make it possible that parts of the fluorine atoms are replaced by OH- ions. To exclude the presence of the latter, additional characterisation methods were employed (see details in the experimental part). Moreover, IR spectroscopy revealed no inclusion of OH- in the compound (Fig. 3).