Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807033910/sg2182sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807033910/sg2182Isup2.hkl |
CCDC reference: 667135
A mixture of 2,2-bipyridyl-N,N'-dioxide (0.182 g, 0.001 mol), TbCl36H2O (0.374 g, 0.1 mol) was added to 30 ml me thanol, The mixture was heated at 350 K or so for 5 h under reflux with stirring.The resulting solution was then filtered off. Single crystals suitable for X-ray diffraction analysis formed after a week by slow evaporation of the solvent.
The H atoms were positioned geometrically and treated as riding on their parent atoms, with C—H distances of 0.93 Å (pyridine ring), 0.86 Å (amine group) and 0.96 Å (methyl), and with Uiso(H) 1.2Ueq(C).
Lanthanide complexes have been investigated intensively because of their potential application in various optical devices [Ropp et al., 2004; McGehee et al., 1999; Tsaryuk et al., 2003]. As shown in Fig.1, in the title compound the TbIII ion are coordinated to three Cl atoms and four O atoms which belong to a 2,2-bipyridyl-N,N'-dioxide molecule and two methanol molecules, respectively in a distorted pentagonal bipyramid geometry, with atom O2 O2A O1 O1A and Cl2 locating at equatorial positions. The crystal structure of (I) contains extensive hydrogen bonding. Neighbouring molecules are connected to each other mainly via O(2)—H(7)···Cl(2)(i) hydrogen bonds [symmetry code: (i) is -x + 2,-y,z + 1/2], the sum of the angles and bond length of d(D···A) about O(2)—H(7)···Cl(2)(i) are 128 (10)/% and 3.179 (8) A/%,respectively.
For related literature, see: McGehee et al. (1999); Ropp (2004); Tsaryuk et al. (2003).
Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Siemens, 1996); software used to prepare material for publication: SHELXTL.
Fig. 1. The molecular structure of (I), showing 30% probability displacement ellipsoids. | |
Fig. 2. The packing diagram of (I), viewed along the z axis; hydrogen bonds are shown as dashed lines. |
[TbCl3(C10H12N2O2)(CH4O)2] | Z = 4 |
Mr = 517.54 | F(000) = 1000 |
Orthorhombic, C2221 | Dx = 2.047 Mg m−3 |
Hall symbol: C 2c 2 | Mo Kα radiation, λ = 0.71073 Å |
a = 13.985 (4) Å | µ = 4.71 mm−1 |
b = 15.054 (4) Å | T = 298 K |
c = 7.976 (2) Å | Block, yellow |
V = 1679.2 (8) Å3 | 0.20 × 0.13 × 0.12 mm |
Bruker APEXII CCD area-detector diffractometer | 1480 independent reflections |
Radiation source: fine-focus sealed tube | 1156 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.070 |
φ and ω scans | θmax = 25.3°, θmin = 2.7° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −16→16 |
Tmin = 0.453, Tmax = 0.595 | k = −18→18 |
4917 measured reflections | l = −9→9 |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H atoms treated by a mixture of independent and constrained refinement |
R[F2 > 2σ(F2)] = 0.039 | w = 1/[σ2(Fo2) + (0.018P)2 + 0.004P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.073 | (Δ/σ)max = 0.002 |
S = 0.98 | Δρmax = 0.94 e Å−3 |
1480 reflections | Δρmin = −1.22 e Å−3 |
95 parameters | Extinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
76 restraints | Extinction coefficient: 0.00061 (16) |
Primary atom site location: structure-invariant direct methods | Absolute structure: Flack (1983), with how many Friedel pairs? |
Secondary atom site location: difference Fourier map | Absolute structure parameter: −0.06 (3) |
[TbCl3(C10H12N2O2)(CH4O)2] | V = 1679.2 (8) Å3 |
Mr = 517.54 | Z = 4 |
Orthorhombic, C2221 | Mo Kα radiation |
a = 13.985 (4) Å | µ = 4.71 mm−1 |
b = 15.054 (4) Å | T = 298 K |
c = 7.976 (2) Å | 0.20 × 0.13 × 0.12 mm |
Bruker APEXII CCD area-detector diffractometer | 1480 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1156 reflections with I > 2σ(I) |
Tmin = 0.453, Tmax = 0.595 | Rint = 0.070 |
4917 measured reflections |
R[F2 > 2σ(F2)] = 0.039 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.073 | Δρmax = 0.94 e Å−3 |
S = 0.98 | Δρmin = −1.22 e Å−3 |
1480 reflections | Absolute structure: Flack (1983), with how many Friedel pairs? |
95 parameters | Absolute structure parameter: −0.06 (3) |
76 restraints |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
x | y | z | Uiso*/Ueq | ||
Cl1 | 0.7799 (2) | 0.15435 (17) | −0.1542 (4) | 0.0439 (7) | |
N3 | 0.5828 (3) | 0.0943 (3) | 0.0755 (7) | 0.0290 (10) | |
C5 | 0.5081 (4) | 0.0484 (3) | −0.0001 (9) | 0.0292 (11) | |
C4 | 0.4313 (3) | 0.0947 (4) | −0.0678 (8) | 0.0308 (12) | |
H4 | 0.3814 | 0.0640 | −0.1184 | 0.037* | |
C3 | 0.4292 (3) | 0.1869 (4) | −0.0600 (8) | 0.0320 (12) | |
H3 | 0.3778 | 0.2179 | −0.1053 | 0.038* | |
C2 | 0.5039 (4) | 0.2328 (3) | 0.0156 (9) | 0.0315 (12) | |
H2 | 0.5025 | 0.2945 | 0.0208 | 0.038* | |
C1 | 0.5807 (3) | 0.1865 (3) | 0.0834 (8) | 0.0302 (11) | |
H1 | 0.6307 | 0.2172 | 0.1339 | 0.036* | |
O1 | 0.6523 (4) | 0.0482 (4) | 0.1438 (8) | 0.0287 (11) | |
Tb1 | 0.78927 (4) | 0.0000 | 0.0000 | 0.0237 (2) | |
O2 | 0.8425 (6) | 0.0574 (6) | 0.2615 (10) | 0.0487 (19) | |
C7 | 0.8075 (8) | 0.1191 (8) | 0.3768 (13) | 0.052 (2) | |
H7A | 0.8356 | 0.1082 | 0.4847 | 0.077* | |
H7B | 0.7393 | 0.1136 | 0.3847 | 0.077* | |
H7C | 0.8236 | 0.1781 | 0.3404 | 0.077* | |
Cl2 | 0.9862 (2) | 0.0000 | 0.0000 | 0.0493 (9) | |
H7 | 0.860 (8) | 0.013 (11) | 0.320 (13) | 0.08 (5)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0432 (16) | 0.0358 (14) | 0.0528 (18) | −0.0030 (15) | 0.0040 (16) | 0.0116 (12) |
N3 | 0.0264 (18) | 0.027 (2) | 0.033 (2) | 0.0045 (17) | 0.0051 (18) | −0.0006 (19) |
C5 | 0.027 (2) | 0.028 (2) | 0.033 (3) | 0.0028 (18) | 0.005 (2) | 0.000 (2) |
C4 | 0.029 (2) | 0.030 (2) | 0.034 (3) | 0.004 (2) | 0.004 (2) | 0.001 (2) |
C3 | 0.030 (2) | 0.030 (2) | 0.035 (3) | 0.005 (2) | 0.005 (2) | 0.001 (2) |
C2 | 0.031 (2) | 0.028 (2) | 0.036 (3) | 0.0040 (19) | 0.006 (2) | 0.001 (2) |
C1 | 0.028 (2) | 0.027 (2) | 0.035 (3) | 0.0028 (19) | 0.006 (2) | −0.001 (2) |
O1 | 0.0264 (19) | 0.027 (2) | 0.033 (3) | 0.0063 (18) | 0.0041 (17) | −0.002 (2) |
Tb1 | 0.0189 (3) | 0.0285 (3) | 0.0238 (3) | 0.000 | 0.000 | −0.0023 (7) |
O2 | 0.041 (3) | 0.069 (5) | 0.036 (3) | 0.024 (4) | −0.013 (3) | −0.025 (3) |
C7 | 0.043 (4) | 0.070 (6) | 0.041 (4) | 0.024 (4) | −0.013 (4) | −0.027 (3) |
Cl2 | 0.0222 (12) | 0.083 (3) | 0.042 (2) | 0.000 | 0.000 | 0.000 (5) |
Cl1—Tb1 | 2.632 (3) | C1—H1 | 0.9300 |
N3—O1 | 1.312 (7) | O1—Tb1 | 2.347 (6) |
N3—C5 | 1.3900 | Tb1—O1i | 2.347 (6) |
N3—C1 | 1.3900 | Tb1—O2 | 2.377 (7) |
C5—C4 | 1.3900 | Tb1—O2i | 2.377 (7) |
C5—C5i | 1.4572 | Tb1—Cl1i | 2.632 (3) |
C4—C3 | 1.3900 | Tb1—Cl2 | 2.754 (3) |
C4—H4 | 0.9300 | O2—C7 | 1.396 (12) |
C3—C2 | 1.3900 | O2—H7 | 0.85 (14) |
C3—H3 | 0.9300 | C7—H7A | 0.9600 |
C2—C1 | 1.3900 | C7—H7B | 0.9600 |
C2—H2 | 0.9300 | C7—H7C | 0.9600 |
O1—N3—C5 | 118.3 (5) | O1i—Tb1—Cl1 | 90.21 (17) |
O1—N3—C1 | 121.7 (5) | O1—Tb1—Cl1 | 85.13 (17) |
C5—N3—C1 | 120.0 | O2—Tb1—Cl1 | 96.0 (2) |
N3—C5—C4 | 120.0 | O2i—Tb1—Cl1 | 85.8 (2) |
N3—C5—C5i | 119.8 (5) | O1i—Tb1—Cl1i | 85.13 (17) |
C4—C5—C5i | 120.1 (5) | O1—Tb1—Cl1i | 90.21 (17) |
C3—C4—C5 | 120.0 | O2—Tb1—Cl1i | 85.8 (2) |
C3—C4—H4 | 120.0 | O2i—Tb1—Cl1i | 96.0 (2) |
C5—C4—H4 | 120.0 | Cl1—Tb1—Cl1i | 174.30 (14) |
C4—C3—C2 | 120.0 | O1i—Tb1—Cl2 | 144.69 (16) |
C4—C3—H3 | 120.0 | O1—Tb1—Cl2 | 144.69 (16) |
C2—C3—H3 | 120.0 | O2—Tb1—Cl2 | 71.7 (2) |
C1—C2—C3 | 120.0 | O2i—Tb1—Cl2 | 71.7 (2) |
C1—C2—H2 | 120.0 | Cl1—Tb1—Cl2 | 92.85 (7) |
C3—C2—H2 | 120.0 | Cl1i—Tb1—Cl2 | 92.85 (7) |
C2—C1—N3 | 120.0 | C7—O2—Tb1 | 135.3 (7) |
C2—C1—H1 | 120.0 | C7—O2—H7 | 105 (9) |
N3—C1—H1 | 120.0 | Tb1—O2—H7 | 107 (10) |
N3—O1—Tb1 | 124.4 (5) | O2—C7—H7A | 109.5 |
O1i—Tb1—O1 | 70.6 (3) | O2—C7—H7B | 109.5 |
O1i—Tb1—O2 | 142.8 (3) | H7A—C7—H7B | 109.5 |
O1—Tb1—O2 | 73.4 (3) | O2—C7—H7C | 109.5 |
O1i—Tb1—O2i | 73.4 (3) | H7A—C7—H7C | 109.5 |
O1—Tb1—O2i | 142.8 (3) | H7B—C7—H7C | 109.5 |
O2—Tb1—O2i | 143.5 (4) |
Symmetry code: (i) x, −y, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H7···Cl2ii | 0.85 (9) | 2.59 (9) | 3.179 (8) | 128 (10) |
Symmetry code: (ii) −x+2, −y, z+1/2. |
Experimental details
Crystal data | |
Chemical formula | [TbCl3(C10H12N2O2)(CH4O)2] |
Mr | 517.54 |
Crystal system, space group | Orthorhombic, C2221 |
Temperature (K) | 298 |
a, b, c (Å) | 13.985 (4), 15.054 (4), 7.976 (2) |
V (Å3) | 1679.2 (8) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 4.71 |
Crystal size (mm) | 0.20 × 0.13 × 0.12 |
Data collection | |
Diffractometer | Bruker APEXII CCD area-detector |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.453, 0.595 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4917, 1480, 1156 |
Rint | 0.070 |
(sin θ/λ)max (Å−1) | 0.600 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.039, 0.073, 0.98 |
No. of reflections | 1480 |
No. of parameters | 95 |
No. of restraints | 76 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.94, −1.22 |
Absolute structure | Flack (1983), with how many Friedel pairs? |
Absolute structure parameter | −0.06 (3) |
Computer programs: APEX2 (Bruker, 2005), SAINT (Siemens, 1996), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Siemens, 1996), SHELXTL.
Cl1—Tb1 | 2.632 (3) | Tb1—O2 | 2.377 (7) |
O1—Tb1 | 2.347 (6) | Tb1—Cl2 | 2.754 (3) |
O1i—Tb1—O2 | 142.8 (3) | O1—Tb1—Cl1i | 90.21 (17) |
O1—Tb1—O2 | 73.4 (3) | O2—Tb1—Cl1i | 85.8 (2) |
O1i—Tb1—O2i | 73.4 (3) | Cl1—Tb1—Cl1i | 174.30 (14) |
O1—Tb1—Cl1 | 85.13 (17) | O1—Tb1—Cl2 | 144.69 (16) |
O2—Tb1—Cl1 | 96.0 (2) | O2—Tb1—Cl2 | 71.7 (2) |
Symmetry code: (i) x, −y, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H7···Cl2ii | 0.85 (9) | 2.59 (9) | 3.179 (8) | 128 (10) |
Symmetry code: (ii) −x+2, −y, z+1/2. |
Lanthanide complexes have been investigated intensively because of their potential application in various optical devices [Ropp et al., 2004; McGehee et al., 1999; Tsaryuk et al., 2003]. As shown in Fig.1, in the title compound the TbIII ion are coordinated to three Cl atoms and four O atoms which belong to a 2,2-bipyridyl-N,N'-dioxide molecule and two methanol molecules, respectively in a distorted pentagonal bipyramid geometry, with atom O2 O2A O1 O1A and Cl2 locating at equatorial positions. The crystal structure of (I) contains extensive hydrogen bonding. Neighbouring molecules are connected to each other mainly via O(2)—H(7)···Cl(2)(i) hydrogen bonds [symmetry code: (i) is -x + 2,-y,z + 1/2], the sum of the angles and bond length of d(D···A) about O(2)—H(7)···Cl(2)(i) are 128 (10)/% and 3.179 (8) A/%,respectively.