metal-organic compounds
(2,2′-Bipyridine-κ2N,N′)tetrabromidoplatinum(IV)
aSchool of Applied Chemical Engineering, The Research Institute of Catalysis, Chonnam National University, Gwangju 500-757, Republic of Korea
*Correspondence e-mail: hakwang@chonnam.ac.kr
In the title complex, [PtBr4(C10H8N2)], the PtIV ion has a slightly distorted octahedral coordination defined by two N atoms of the chelating 2,2′-bipyridine ligand and four bromide ions. As a result of the different trans effects of the N and Br atoms, the Pt—Br bonds trans to the N atom are slightly shorter than those to mutually trans Br atoms. In the the molecules are arranged in a V-shaped packing pattern along the b axis and stacked in columns along the a axis. In the columns, several intermolecular π–π interactions between the pyridine rings are present. The shortest ring centroid–centroid distance is 3.921 (6) Å, with a dihedral angle of 1.6 (5)° between the ring planes. The complexes are connected by C—H⋯Br hydrogen bonds, forming chains along the b axis.
Experimental
Crystal data
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Data collection: SMART (Bruker, 2000); cell SAINT (Bruker, 2000); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and PLATON (Spek, 2009); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S1600536810034793/fj2332sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536810034793/fj2332Isup2.hkl
To a solution of K2PtBr6 (0.1003 g, 0.133 mmol) in H2O (10 ml) was added 2,2'-bipyridine (0.0210 g, 0.134 mmol), and the mixture was refluxed for 3 h. The formed precipitate was separated by filtration, washed with water, and dried at 50 °C, to give an orange-yellow powder (0.0705 g). Crystals suitable for X-ray analysis were obtained by slow evaporation from an N,N-dimethylformamide solution at 50 °C.
H atoms were positioned geometrically and allowed to ride on their respective parent atoms [C—H = 0.95 Å and Uiso(H) = 1.2Ueq(C)]. The highest peak (1.69 e Å-3) and the deepest hole (-1.66 e Å-3) in the difference Fourier map are located 0.96 and 0.96 Å from the Pt1 atom, respectively.
Data collection: SMART (Bruker, 2000); cell
SAINT (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and PLATON (Spek, 2009); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).[PtBr4(C10H8N2)] | F(000) = 600 |
Mr = 670.91 | Dx = 3.165 Mg m−3 |
Monoclinic, Pn | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P -2yac | Cell parameters from 3381 reflections |
a = 8.3146 (7) Å | θ = 2.7–27.0° |
b = 6.9010 (5) Å | µ = 21.30 mm−1 |
c = 12.5873 (10) Å | T = 200 K |
β = 102.940 (2)° | Block, orange |
V = 703.91 (10) Å3 | 0.25 × 0.12 × 0.08 mm |
Z = 2 |
Bruker SMART 1000 CCD diffractometer | 2257 independent reflections |
Radiation source: fine-focus sealed tube | 2128 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.033 |
ϕ and ω scans | θmax = 27.0°, θmin = 3.0° |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | h = −8→10 |
Tmin = 0.462, Tmax = 1.000 | k = −8→8 |
4282 measured reflections | l = −16→15 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.027 | H-atom parameters constrained |
wR(F2) = 0.053 | w = 1/[σ2(Fo2) + (0.0057P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.98 | (Δ/σ)max < 0.001 |
2257 reflections | Δρmax = 1.69 e Å−3 |
154 parameters | Δρmin = −1.66 e Å−3 |
2 restraints | Absolute structure: Flack (1983), 714 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: −0.004 (14) |
[PtBr4(C10H8N2)] | V = 703.91 (10) Å3 |
Mr = 670.91 | Z = 2 |
Monoclinic, Pn | Mo Kα radiation |
a = 8.3146 (7) Å | µ = 21.30 mm−1 |
b = 6.9010 (5) Å | T = 200 K |
c = 12.5873 (10) Å | 0.25 × 0.12 × 0.08 mm |
β = 102.940 (2)° |
Bruker SMART 1000 CCD diffractometer | 2257 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | 2128 reflections with I > 2σ(I) |
Tmin = 0.462, Tmax = 1.000 | Rint = 0.033 |
4282 measured reflections |
R[F2 > 2σ(F2)] = 0.027 | H-atom parameters constrained |
wR(F2) = 0.053 | Δρmax = 1.69 e Å−3 |
S = 0.98 | Δρmin = −1.66 e Å−3 |
2257 reflections | Absolute structure: Flack (1983), 714 Friedel pairs |
154 parameters | Absolute structure parameter: −0.004 (14) |
2 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 | ||
Pt1 | 0.05995 (4) | 0.30254 (5) | 0.15692 (3) | 0.01371 (9) | |
Br1 | −0.17951 (12) | 0.09180 (15) | 0.14380 (8) | 0.0242 (2) | |
Br2 | −0.05252 (13) | 0.51205 (15) | 0.27909 (8) | 0.0237 (2) | |
Br3 | 0.21931 (13) | 0.12002 (14) | 0.31519 (8) | 0.0232 (2) | |
Br4 | −0.08910 (13) | 0.48563 (15) | −0.00258 (8) | 0.0239 (2) | |
N1 | 0.2650 (9) | 0.4685 (11) | 0.1594 (6) | 0.0155 (18) | |
N2 | 0.1677 (10) | 0.1400 (11) | 0.0559 (6) | 0.0159 (18) | |
C1 | 0.3042 (12) | 0.6354 (13) | 0.2127 (8) | 0.018 (2) | |
H1 | 0.2326 | 0.6863 | 0.2550 | 0.021* | |
C2 | 0.4468 (14) | 0.7363 (14) | 0.2081 (9) | 0.028 (3) | |
H2 | 0.4746 | 0.8531 | 0.2479 | 0.034* | |
C3 | 0.5471 (16) | 0.6627 (13) | 0.1441 (11) | 0.024 (2) | |
H3 | 0.6445 | 0.7304 | 0.1389 | 0.029* | |
C4 | 0.5072 (13) | 0.4909 (15) | 0.0873 (9) | 0.024 (2) | |
H4 | 0.5768 | 0.4401 | 0.0436 | 0.029* | |
C5 | 0.3659 (11) | 0.3954 (14) | 0.0951 (8) | 0.018 (2) | |
C6 | 0.3148 (12) | 0.2147 (15) | 0.0401 (8) | 0.019 (2) | |
C7 | 0.4026 (14) | 0.1139 (14) | −0.0252 (8) | 0.024 (2) | |
H7 | 0.5045 | 0.1630 | −0.0360 | 0.029* | |
C8 | 0.3388 (13) | −0.0589 (14) | −0.0740 (8) | 0.023 (2) | |
H8 | 0.3975 | −0.1291 | −0.1182 | 0.027* | |
C9 | 0.1902 (13) | −0.1282 (15) | −0.0583 (8) | 0.027 (2) | |
H9 | 0.1453 | −0.2448 | −0.0928 | 0.032* | |
C10 | 0.1068 (12) | −0.0280 (13) | 0.0075 (8) | 0.021 (2) | |
H10 | 0.0055 | −0.0774 | 0.0190 | 0.025* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Pt1 | 0.01098 (16) | 0.01521 (16) | 0.01523 (16) | −0.00154 (17) | 0.00355 (13) | −0.00061 (16) |
Br1 | 0.0181 (6) | 0.0250 (5) | 0.0309 (6) | −0.0078 (5) | 0.0086 (5) | −0.0009 (5) |
Br2 | 0.0231 (6) | 0.0243 (5) | 0.0258 (5) | 0.0033 (5) | 0.0100 (5) | −0.0038 (5) |
Br3 | 0.0224 (6) | 0.0243 (5) | 0.0216 (5) | 0.0040 (5) | 0.0022 (5) | 0.0029 (4) |
Br4 | 0.0193 (5) | 0.0292 (5) | 0.0224 (5) | −0.0006 (5) | 0.0028 (5) | 0.0071 (5) |
N1 | 0.007 (4) | 0.015 (4) | 0.022 (4) | −0.002 (3) | −0.004 (4) | 0.001 (3) |
N2 | 0.016 (5) | 0.017 (4) | 0.018 (4) | −0.003 (3) | 0.011 (4) | −0.004 (3) |
C1 | 0.015 (5) | 0.018 (5) | 0.021 (5) | 0.000 (4) | 0.006 (5) | −0.002 (4) |
C2 | 0.024 (6) | 0.018 (5) | 0.039 (7) | −0.009 (5) | −0.001 (6) | 0.001 (5) |
C3 | 0.010 (5) | 0.021 (5) | 0.037 (7) | −0.005 (5) | −0.005 (5) | 0.002 (6) |
C4 | 0.017 (6) | 0.019 (5) | 0.041 (7) | −0.002 (4) | 0.014 (5) | 0.002 (5) |
C5 | 0.010 (5) | 0.020 (5) | 0.022 (5) | 0.000 (4) | 0.001 (4) | −0.006 (4) |
C6 | 0.014 (5) | 0.025 (6) | 0.019 (5) | 0.005 (4) | 0.004 (5) | 0.006 (4) |
C7 | 0.022 (6) | 0.027 (6) | 0.025 (6) | 0.002 (5) | 0.010 (5) | 0.002 (4) |
C8 | 0.027 (6) | 0.025 (5) | 0.017 (5) | 0.010 (5) | 0.007 (5) | −0.003 (4) |
C9 | 0.030 (6) | 0.028 (6) | 0.025 (6) | −0.004 (5) | 0.012 (5) | −0.009 (5) |
C10 | 0.018 (6) | 0.018 (5) | 0.025 (5) | −0.009 (4) | 0.001 (5) | −0.010 (4) |
Pt1—N2 | 2.046 (7) | C3—C4 | 1.386 (14) |
Pt1—N1 | 2.048 (7) | C3—H3 | 0.9500 |
Pt1—Br1 | 2.4412 (10) | C4—C5 | 1.370 (13) |
Pt1—Br2 | 2.4442 (10) | C4—H4 | 0.9500 |
Pt1—Br4 | 2.4595 (11) | C5—C6 | 1.443 (14) |
Pt1—Br3 | 2.4756 (11) | C6—C7 | 1.401 (13) |
N1—C1 | 1.336 (11) | C7—C8 | 1.391 (14) |
N1—C5 | 1.385 (11) | C7—H7 | 0.9500 |
N2—C10 | 1.354 (11) | C8—C9 | 1.380 (14) |
N2—C6 | 1.382 (12) | C8—H8 | 0.9500 |
C1—C2 | 1.387 (14) | C9—C10 | 1.379 (13) |
C1—H1 | 0.9500 | C9—H9 | 0.9500 |
C2—C3 | 1.380 (17) | C10—H10 | 0.9500 |
C2—H2 | 0.9500 | ||
N2—Pt1—N1 | 80.6 (3) | C1—C2—H2 | 120.9 |
N2—Pt1—Br1 | 95.5 (2) | C2—C3—C4 | 120.7 (11) |
N1—Pt1—Br1 | 176.0 (2) | C2—C3—H3 | 119.7 |
N2—Pt1—Br2 | 176.0 (2) | C4—C3—H3 | 119.7 |
N1—Pt1—Br2 | 95.4 (2) | C5—C4—C3 | 119.0 (10) |
Br1—Pt1—Br2 | 88.50 (4) | C5—C4—H4 | 120.5 |
N2—Pt1—Br4 | 89.1 (2) | C3—C4—H4 | 120.5 |
N1—Pt1—Br4 | 89.5 (2) | C4—C5—N1 | 120.6 (9) |
Br1—Pt1—Br4 | 89.80 (4) | C4—C5—C6 | 123.1 (9) |
Br2—Pt1—Br4 | 90.91 (4) | N1—C5—C6 | 116.3 (8) |
N2—Pt1—Br3 | 89.5 (2) | N2—C6—C7 | 119.6 (9) |
N1—Pt1—Br3 | 88.8 (2) | N2—C6—C5 | 115.4 (8) |
Br1—Pt1—Br3 | 91.88 (4) | C7—C6—C5 | 125.0 (9) |
Br2—Pt1—Br3 | 90.34 (4) | C8—C7—C6 | 119.2 (10) |
Br4—Pt1—Br3 | 177.93 (4) | C8—C7—H7 | 120.4 |
C1—N1—C5 | 119.7 (8) | C6—C7—H7 | 120.4 |
C1—N1—Pt1 | 126.7 (6) | C9—C8—C7 | 119.9 (9) |
C5—N1—Pt1 | 113.5 (6) | C9—C8—H8 | 120.0 |
C10—N2—C6 | 120.5 (8) | C7—C8—H8 | 120.0 |
C10—N2—Pt1 | 125.3 (6) | C10—C9—C8 | 119.9 (9) |
C6—N2—Pt1 | 114.2 (6) | C10—C9—H9 | 120.0 |
N1—C1—C2 | 121.7 (9) | C8—C9—H9 | 120.0 |
N1—C1—H1 | 119.1 | N2—C10—C9 | 120.8 (9) |
C2—C1—H1 | 119.1 | N2—C10—H10 | 119.6 |
C3—C2—C1 | 118.3 (10) | C9—C10—H10 | 119.6 |
C3—C2—H2 | 120.9 | ||
N2—Pt1—N1—C1 | 178.8 (8) | C3—C4—C5—N1 | −0.4 (16) |
Br2—Pt1—N1—C1 | −1.2 (8) | C3—C4—C5—C6 | −179.3 (10) |
Br4—Pt1—N1—C1 | 89.6 (8) | C1—N1—C5—C4 | 1.1 (14) |
Br3—Pt1—N1—C1 | −91.5 (8) | Pt1—N1—C5—C4 | 179.3 (8) |
N2—Pt1—N1—C5 | 0.8 (6) | C1—N1—C5—C6 | −179.9 (9) |
Br2—Pt1—N1—C5 | −179.3 (6) | Pt1—N1—C5—C6 | −1.7 (11) |
Br4—Pt1—N1—C5 | −88.4 (6) | C10—N2—C6—C7 | −0.9 (14) |
Br3—Pt1—N1—C5 | 90.5 (6) | Pt1—N2—C6—C7 | 178.4 (7) |
N1—Pt1—N2—C10 | 179.6 (9) | C10—N2—C6—C5 | 179.4 (9) |
Br1—Pt1—N2—C10 | −1.1 (9) | Pt1—N2—C6—C5 | −1.3 (11) |
Br4—Pt1—N2—C10 | −90.8 (8) | C4—C5—C6—N2 | −179.1 (9) |
Br3—Pt1—N2—C10 | 90.7 (8) | N1—C5—C6—N2 | 2.0 (13) |
N1—Pt1—N2—C6 | 0.3 (6) | C4—C5—C6—C7 | 1.3 (16) |
Br1—Pt1—N2—C6 | 179.6 (6) | N1—C5—C6—C7 | −177.6 (9) |
Br4—Pt1—N2—C6 | 89.9 (6) | N2—C6—C7—C8 | 0.7 (14) |
Br3—Pt1—N2—C6 | −88.6 (6) | C5—C6—C7—C8 | −179.7 (10) |
C5—N1—C1—C2 | −1.8 (14) | C6—C7—C8—C9 | 0.4 (15) |
Pt1—N1—C1—C2 | −179.7 (7) | C7—C8—C9—C10 | −1.3 (16) |
N1—C1—C2—C3 | 1.6 (16) | C6—N2—C10—C9 | 0.1 (15) |
C1—C2—C3—C4 | −0.9 (17) | Pt1—N2—C10—C9 | −179.2 (8) |
C2—C3—C4—C5 | 0.3 (17) | C8—C9—C10—N2 | 1.0 (16) |
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1···Br2 | 0.95 | 2.73 | 3.366 (9) | 125 |
C3—H3···Br1i | 0.95 | 2.89 | 3.734 (10) | 149 |
C10—H10···Br1 | 0.95 | 2.70 | 3.335 (9) | 125 |
Symmetry code: (i) x+1, y+1, z. |
Experimental details
Crystal data | |
Chemical formula | [PtBr4(C10H8N2)] |
Mr | 670.91 |
Crystal system, space group | Monoclinic, Pn |
Temperature (K) | 200 |
a, b, c (Å) | 8.3146 (7), 6.9010 (5), 12.5873 (10) |
β (°) | 102.940 (2) |
V (Å3) | 703.91 (10) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 21.30 |
Crystal size (mm) | 0.25 × 0.12 × 0.08 |
Data collection | |
Diffractometer | Bruker SMART 1000 CCD diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2000) |
Tmin, Tmax | 0.462, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4282, 2257, 2128 |
Rint | 0.033 |
(sin θ/λ)max (Å−1) | 0.638 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.027, 0.053, 0.98 |
No. of reflections | 2257 |
No. of parameters | 154 |
No. of restraints | 2 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 1.69, −1.66 |
Absolute structure | Flack (1983), 714 Friedel pairs |
Absolute structure parameter | −0.004 (14) |
Computer programs: SMART (Bruker, 2000), SAINT (Bruker, 2000), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997) and PLATON (Spek, 2009).
Pt1—N2 | 2.046 (7) | Pt1—Br2 | 2.4442 (10) |
Pt1—N1 | 2.048 (7) | Pt1—Br4 | 2.4595 (11) |
Pt1—Br1 | 2.4412 (10) | Pt1—Br3 | 2.4756 (11) |
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1···Br2 | 0.95 | 2.73 | 3.366 (9) | 125 |
C3—H3···Br1i | 0.95 | 2.89 | 3.734 (10) | 149 |
C10—H10···Br1 | 0.95 | 2.70 | 3.335 (9) | 125 |
Symmetry code: (i) x+1, y+1, z. |
Acknowledgements
This work was supported by Priority Research Centers Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology (2009–0094056).
References
Bruker (2000). SADABS, SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565. CrossRef IUCr Journals Google Scholar
Flack, H. D. (1983). Acta Cryst. A39, 876–881. CrossRef CAS Web of Science IUCr Journals Google Scholar
Hambley, T. W. (1986). Acta Cryst. C42, 49–51. CSD CrossRef CAS Web of Science IUCr Journals Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Spek, A. L. (2009). Acta Cryst. D65, 148–155. Web of Science CrossRef CAS IUCr Journals Google Scholar
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The title complex, [PtBr4(bipy)], is isomorphous with the chloro analogue [PtCl4(bipy)] (Hambley, 1986). The central Pt(IV) ion has a slightly distorted octahedral coordination defined by two N atoms of the chelating 2,2'-bipyridine ligand and four bromide ions (Fig. 1). The main contribution to the distortion of octahedron is the tight N1—Pt1—N2 chelate angle (80.6 (3)°), which results in non-linear trans axes (<Br1—Pt1—N1 = 176.0 (2)°, <Br2—Pt1—N2 = 176.0 (2)° and <Br3—Pt1—Br4 = 177.93 (4)°). As a result of the different trans effects of the N and Br atoms, the Pt—Br bonds trans to the N atom (2.4412 (10) Å and 2.4442 (10) Å) are slightly shorter than bond lengths to mutually trans Br atoms (2.4595 (11) Å and 2.4756 (11) Å) (Table 1). In the crystal structure, the complex molecules are arranged in a V-shaped packing pattern along the b axis and stacked in columns along the a axis (Fig. 2). In the columns, several intermolecular π-π interactions between the pyridine rings are present, with a shortest ring centroid-centroid distance of 3.921 (6) Å, and the dihedral angle between the ring planes is 1.6 (5)°. Moreover, there are intra- and intermolecular hydrogen bonds between the C and Br atoms with d(C···Br) = 3.335 (9) Å–3.734 (10) Å (Table 2). The complexes are connected by the C—H···Br hydrogen bonds, forming one-dimensional chains along the b axis.