metal-organic compounds
Bis[dihydrobis(pyrazol-1-yl-κN2)borato]bis(methanol-κO)iron(II)
aInstitut für Anorganische Chemie, Christian-Albrechts-Universität Kiel, Max-Eyth-Strasse 2, 24118 Kiel, Germany
*Correspondence e-mail: sossinger@ac.uni-kiel.de
The II bis(pyrazolyl)borate complexes. The of the title compound, [Fe(H2B(pz)2)2(CH3OH)2] [H2B(pz)2 = dihydrobis(pyrazol-1-yl)borate, C6H8BN4], consists of one FeII cation that is located on a centre of inversion, as well as one methanol molecule and one H2B(pz)2 dianion that occupy general positions. In the crystal, the FeII cations are coordinated by two methanol molecules and four N atoms of two H2B(pz)2 anions within a slightly distorted octahedron. Bond lengths and angles between the FeII atom and the H2B(pz)2 anion are comparable to those in related FeII complexes.
was undertaken as part of a project on the synthesis of new spin-crossover compounds based on octahedral FeCCDC reference: 1497420
Structure description
Concerning the background of this project, see Naggert et al. (2015). For related crystal structures of discrete octahedral FeII bis(pyrazolyl)borate complexes with N-donor ligands, see: Real et al. (1997); Thompson et al. (2004); Milek et al. (2013); Nihei et al. (2013); Kulmaczewski et al. (2014); Naggert et al. (2015). The title compound is illustrated in Fig. 1. Despite the presence of a hydroxy group, classical hydrogen-bonding interactions are not evident in the crystal structure.
Synthesis and crystallization
Iron(II) perchlorate hydrate and solvents were purchased by Sigma–Aldrich. All reactions were carried out using dry solvents and under an inert atmosphere. Potassium dihydrobis(pyrazolyl)borate K[H2B(pz)2] and [Fe(H2B(pz)2)2(CH3OH)2] were prepared according to literature methods (Trofimenko, 1967; Real et al., 1997).
A solution of K[H2B(pz)2] (283 mg, 1.52 mmol) in methanol (3 ml) was added dropwise to a solution of Fe(ClO4)2·6H2O (276 mg, 0.76 mmol) in methanol (1 ml). The yellow Fe[H2B(pz)2]2 solution was stirred for 10 min at room temperature. The resulting KClO4 precipitate was removed by filtration and washed with methanol (6 ml). After further stirring for one h the solution was stored at 245 K. After four days colorless crystals of [Fe(H2B(pz)2)2(CH3OH)2] were collected by suction filtration. They decompose in air within a few days.
Refinement
Crystal data, data collection and structure .
details are summarized in Table 1Structural data
CCDC reference: 1497420
10.1107/S2414314616012529/bt4021sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S2414314616012529/bt4021Isup2.hkl
Data collection: X-AREA (Stoe & Cie, 2008); cell
X-AREA (Stoe & Cie, 2008); data reduction: X-AREA (Stoe & Cie, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: XP in SHELXTL (Sheldrick, 2008); software used to prepare material for publication: publCIF (Westrip, 2010).[Fe(C6H8B2N4)2(CH4O)2] | F(000) = 432 |
Mr = 413.88 | Dx = 1.424 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 9.7430 (5) Å | Cell parameters from 11751 reflections |
b = 8.6535 (3) Å | θ = 2.3–27.0° |
c = 12.3173 (6) Å | µ = 0.81 mm−1 |
β = 111.670 (4)° | T = 170 K |
V = 965.09 (8) Å3 | Block, colorless |
Z = 2 | 0.20 × 0.12 × 0.06 mm |
Stoe IPDS-2 diffractometer | 1898 reflections with I > 2σ(I) |
ω scans | Rint = 0.026 |
Absorption correction: numerical (X-RED and X-SHAPE; Stoe & Cie, 2008) | θmax = 27.0°, θmin = 2.3° |
Tmin = 0.781, Tmax = 0.898 | h = −12→12 |
11312 measured reflections | k = −11→11 |
2103 independent reflections | l = −15→15 |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.034 | H-atom parameters constrained |
wR(F2) = 0.089 | w = 1/[σ2(Fo2) + (0.0485P)2 + 0.3892P] where P = (Fo2 + 2Fc2)/3 |
S = 1.07 | (Δ/σ)max < 0.001 |
2103 reflections | Δρmax = 0.25 e Å−3 |
125 parameters | Δρmin = −0.45 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 | ||
Fe1 | 0.0000 | 0.5000 | 0.5000 | 0.02887 (12) | |
N1 | 0.20696 (15) | 0.55724 (18) | 0.64018 (12) | 0.0315 (3) | |
N2 | 0.31387 (15) | 0.64416 (17) | 0.62205 (13) | 0.0306 (3) | |
N3 | 0.09829 (15) | 0.55320 (19) | 0.37541 (13) | 0.0314 (3) | |
N4 | 0.22449 (15) | 0.63870 (17) | 0.40243 (13) | 0.0310 (3) | |
B1 | 0.2792 (2) | 0.7456 (2) | 0.51128 (18) | 0.0339 (4) | |
H1A | 0.3691 | 0.8017 | 0.5143 | 0.041* | |
H1B | 0.2021 | 0.8225 | 0.5069 | 0.041* | |
C1 | 0.44303 (18) | 0.6245 (2) | 0.71101 (16) | 0.0344 (4) | |
H1 | 0.5336 | 0.6730 | 0.7186 | 0.041* | |
C2 | 0.4231 (2) | 0.5218 (2) | 0.79007 (16) | 0.0365 (4) | |
H2 | 0.4947 | 0.4860 | 0.8614 | 0.044* | |
C3 | 0.2736 (2) | 0.4828 (2) | 0.74114 (16) | 0.0350 (4) | |
H3 | 0.2258 | 0.4128 | 0.7750 | 0.042* | |
C4 | 0.2818 (2) | 0.6172 (2) | 0.32000 (17) | 0.0361 (4) | |
H4 | 0.3698 | 0.6636 | 0.3193 | 0.043* | |
C5 | 0.1932 (2) | 0.5174 (2) | 0.23664 (17) | 0.0383 (4) | |
H5 | 0.2059 | 0.4823 | 0.1679 | 0.046* | |
C6 | 0.0806 (2) | 0.4795 (2) | 0.27593 (16) | 0.0353 (4) | |
H6 | 0.0019 | 0.4105 | 0.2372 | 0.042* | |
O1 | 0.09492 (14) | 0.26492 (15) | 0.51071 (11) | 0.0370 (3) | |
H1O1 | 0.0844 | 0.2074 | 0.5620 | 0.056* | |
C11 | 0.2429 (2) | 0.2333 (2) | 0.51817 (19) | 0.0433 (4) | |
H11A | 0.2564 | 0.2732 | 0.4483 | 0.065* | |
H11B | 0.2599 | 0.1214 | 0.5236 | 0.065* | |
H11C | 0.3133 | 0.2836 | 0.5877 | 0.065* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Fe1 | 0.02591 (19) | 0.0335 (2) | 0.02633 (19) | −0.00137 (13) | 0.00856 (13) | −0.00076 (13) |
N1 | 0.0277 (7) | 0.0358 (8) | 0.0289 (7) | −0.0039 (6) | 0.0082 (6) | −0.0006 (6) |
N2 | 0.0269 (7) | 0.0315 (7) | 0.0317 (7) | −0.0026 (5) | 0.0090 (6) | −0.0022 (6) |
N3 | 0.0286 (7) | 0.0362 (7) | 0.0296 (7) | −0.0034 (6) | 0.0111 (6) | −0.0008 (6) |
N4 | 0.0287 (7) | 0.0330 (7) | 0.0320 (7) | −0.0015 (6) | 0.0121 (6) | 0.0018 (6) |
B1 | 0.0330 (9) | 0.0320 (10) | 0.0357 (10) | −0.0018 (8) | 0.0115 (8) | 0.0011 (8) |
C1 | 0.0267 (8) | 0.0381 (9) | 0.0350 (9) | −0.0009 (7) | 0.0072 (7) | −0.0035 (7) |
C2 | 0.0331 (9) | 0.0401 (10) | 0.0310 (8) | 0.0034 (7) | 0.0055 (7) | −0.0008 (7) |
C3 | 0.0366 (9) | 0.0369 (9) | 0.0299 (8) | −0.0016 (7) | 0.0105 (7) | 0.0010 (7) |
C4 | 0.0350 (9) | 0.0369 (9) | 0.0406 (9) | 0.0015 (7) | 0.0190 (7) | 0.0038 (7) |
C5 | 0.0440 (10) | 0.0388 (10) | 0.0367 (9) | 0.0022 (8) | 0.0203 (8) | −0.0005 (7) |
C6 | 0.0365 (9) | 0.0363 (9) | 0.0325 (9) | −0.0010 (7) | 0.0122 (7) | −0.0033 (7) |
O1 | 0.0362 (6) | 0.0355 (7) | 0.0398 (7) | −0.0003 (5) | 0.0144 (5) | 0.0009 (5) |
C11 | 0.0380 (10) | 0.0438 (11) | 0.0480 (11) | 0.0066 (8) | 0.0157 (9) | −0.0003 (9) |
Fe1—N3i | 2.1376 (14) | C1—C2 | 1.384 (3) |
Fe1—N3 | 2.1376 (14) | C1—H1 | 0.9500 |
Fe1—N1i | 2.1728 (14) | C2—C3 | 1.396 (3) |
Fe1—N1 | 2.1729 (14) | C2—H2 | 0.9500 |
Fe1—O1 | 2.2183 (13) | C3—H3 | 0.9500 |
Fe1—O1i | 2.2183 (13) | C4—C5 | 1.375 (3) |
N1—C3 | 1.337 (2) | C4—H4 | 0.9500 |
N1—N2 | 1.368 (2) | C5—C6 | 1.392 (3) |
N2—C1 | 1.340 (2) | C5—H5 | 0.9500 |
N2—B1 | 1.551 (2) | C6—H6 | 0.9500 |
N3—C6 | 1.335 (2) | O1—C11 | 1.437 (2) |
N3—N4 | 1.367 (2) | O1—H1O1 | 0.8400 |
N4—C4 | 1.340 (2) | C11—H11A | 0.9800 |
N4—B1 | 1.552 (2) | C11—H11B | 0.9800 |
B1—H1A | 0.9900 | C11—H11C | 0.9800 |
B1—H1B | 0.9900 | ||
N3i—Fe1—N3 | 180.0 | N2—B1—H1B | 110.0 |
N3i—Fe1—N1i | 89.49 (5) | N4—B1—H1B | 110.0 |
N3—Fe1—N1i | 90.51 (5) | H1A—B1—H1B | 108.4 |
N3i—Fe1—N1 | 90.51 (5) | N2—C1—C2 | 108.88 (16) |
N3—Fe1—N1 | 89.49 (5) | N2—C1—H1 | 125.6 |
N1i—Fe1—N1 | 180.0 | C2—C1—H1 | 125.6 |
N3i—Fe1—O1 | 92.71 (5) | C1—C2—C3 | 104.27 (16) |
N3—Fe1—O1 | 87.29 (5) | C1—C2—H2 | 127.9 |
N1i—Fe1—O1 | 94.73 (5) | C3—C2—H2 | 127.9 |
N1—Fe1—O1 | 85.27 (5) | N1—C3—C2 | 110.88 (16) |
N3i—Fe1—O1i | 87.29 (5) | N1—C3—H3 | 124.6 |
N3—Fe1—O1i | 92.71 (5) | C2—C3—H3 | 124.6 |
N1i—Fe1—O1i | 85.27 (5) | N4—C4—C5 | 109.31 (16) |
N1—Fe1—O1i | 94.73 (5) | N4—C4—H4 | 125.3 |
O1—Fe1—O1i | 180.0 | C5—C4—H4 | 125.3 |
C3—N1—N2 | 106.20 (14) | C4—C5—C6 | 104.27 (17) |
C3—N1—Fe1 | 128.24 (12) | C4—C5—H5 | 127.9 |
N2—N1—Fe1 | 122.32 (11) | C6—C5—H5 | 127.9 |
C1—N2—N1 | 109.77 (14) | N3—C6—C5 | 110.81 (17) |
C1—N2—B1 | 128.69 (15) | N3—C6—H6 | 124.6 |
N1—N2—B1 | 121.54 (13) | C5—C6—H6 | 124.6 |
C6—N3—N4 | 106.37 (14) | C11—O1—Fe1 | 124.41 (12) |
C6—N3—Fe1 | 128.01 (13) | C11—O1—H1O1 | 103.7 |
N4—N3—Fe1 | 122.89 (11) | Fe1—O1—H1O1 | 115.1 |
C4—N4—N3 | 109.23 (15) | O1—C11—H11A | 109.5 |
C4—N4—B1 | 129.11 (15) | O1—C11—H11B | 109.5 |
N3—N4—B1 | 121.61 (13) | H11A—C11—H11B | 109.5 |
N2—B1—N4 | 108.45 (15) | O1—C11—H11C | 109.5 |
N2—B1—H1A | 110.0 | H11A—C11—H11C | 109.5 |
N4—B1—H1A | 110.0 | H11B—C11—H11C | 109.5 |
Symmetry code: (i) −x, −y+1, −z+1. |
Acknowledgements
This work was supported by the DFG (SFB 677 Function by Switching). We gratefully acknowledge financial support by the State of Schleswig–Holstein.
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