Download citation
Download citation
link to html
The title complex, [Pd(C5H5N)4](BF4)2, contains tetra­pyridine­palladium(II) cations residing on crystallographic inversion centres. These are linked by weak C—H...F inter­actions (involving disordered BF4 anions) [range 2.988 (12)–3.431 (10) Å], together with C—H...π(pyridine) inter­actions. The F atoms are disordered equally over two positions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807034411/gg2027sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807034411/gg2027Isup2.hkl
Contains datablock I

CCDC reference: 657593

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.011 Å
  • Disorder in solvent or counterion
  • R factor = 0.046
  • wR factor = 0.154
  • Data-to-parameter ratio = 16.2

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT153_ALERT_1_C The su's on the Cell Axes are Equal (x 100000) 700 Ang. PLAT164_ALERT_4_C Nr. of Refined C-H H-Atoms in Heavy-At Struct... 7 PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C4 PLAT243_ALERT_4_C High 'Solvent' Ueq as Compared to Neighbors for F1' PLAT243_ALERT_4_C High 'Solvent' Ueq as Compared to Neighbors for F2' PLAT243_ALERT_4_C High 'Solvent' Ueq as Compared to Neighbors for F3' PLAT243_ALERT_4_C High 'Solvent' Ueq as Compared to Neighbors for F4' PLAT244_ALERT_4_C Low 'Solvent' Ueq as Compared to Neighbors for F2 PLAT244_ALERT_4_C Low 'Solvent' Ueq as Compared to Neighbors for F3 PLAT244_ALERT_4_C Low 'Solvent' Ueq as Compared to Neighbors for F4 PLAT244_ALERT_4_C Low 'Solvent' Ueq as Compared to Neighbors for B PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.07 PLAT302_ALERT_4_C Anion/Solvent Disorder ......................... 44.00 Perc. PLAT342_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 11
Alert level G PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 20
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 14 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 10 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

The design of supramolecular coordination compounds by self-assembly is a developing research area (Lehn, 1995, Braga et al., 1998). Four-coordinate PdII complexes with square-planar geometry and four pyridine ligands, in particular, is a potentially useful building block for producing an array of interesting molecular architectures by means of C—H···π-ring interactions, thanks to the mobility of pyridine planes. It is for that reason that we have tried to prepare the title compound (I) to be able to compare the results with the structure of the same compound with acetone solvate (Lutz et al., 2000).

Normally, the tetrakis(pyridine-N)palladium(II) ion has a square-planar coordination, with the anion occupying the apical positions of an octahedron. Pd···X lengths are 4.299 (5) Å in (I) (X = B); 4.028 (7) Å (X = B, Lutz et al., 2000); 4.4759 (11) Å in the orthorhombic phase and 4.100 (2) Å in the triclinic phase (X = I, Tebbe et al., 1996); 3.112 (2) Å (X = O, Liqing et al. 2005) and 3.079 (4) or 3.031 (3) Å (X = F, Holzbock et al., 2000). The packing will come defined by the solvate presence and the size of the anion which will alter, in addition, the dihedral angle between the pyridine planes. This angle is equal to 89.53 (19)° in (I), 89.62° in the Liqing structure, a range of 85.73 to 81.13° in the Holzbock structure, 85.33° in orthorhombic phase and 83.37° in triclinic phase of the Tebbe structure and 78.25 to 58.13° in the Lutz structure. The C—H···π-(ring) interaction only takes place in (I) and the triclinic phase of the Tebbe structure producing a one-dimensional-structure. The data for C4—H4···N2 (pyridine ring) (symmetry = 1/2 + x, 1/2 - y, 1/2 + z) are H-centroid distance 2.97 Å, γ = 20.28°. This fact suggests that the solvate absence and a dihedral angle between the pyridine planes next to 90° facilitate this interaction.

Related literature top

For related literature, see: Braga et al. (1998); Holzbock et al. (2000); Lehn (1995); Liqing et al. (2005); Lutz et al. (2000); Ma et al. (2005); Tebbe et al. (1996).

Experimental top

A solution of 0.070 g (0.308 mmol) [PdCl2(CH3CN)2] was dissolved in a mixture of CH2Cl2 (10 ml) and methanol (10 ml). About 0.1230 g, (0.625 mmol) of pyridine was added to a solution. Then, a solution of 0.070 g, (0.625 mmol) of NaBF4 in methanol (2 ml) was added dropwise with vigorous stirring. After 2 h, stirring was stopped, and the product precipitated as yellow solid, was filtered, washed with diethylether, and dried under vacuum. Crystals were obtained by evaporation of acetonitrile solution. Yield: 0.15 g, (81%) - C20H20B2F8N4Pd (596.42). (%): C, 40.27; H, 3.38; N, 9.39; found: C, 40.26; H, 3.37; N, 9.39. Conductivity (Ω-1 cm2 mol-1, 1.03 x 10-3 M in acetonitrile): 279. IR(KBr, cm-1): ν(C=C)py; ν(C=N)py 1603, δ(C=C)py; δ(C=N)py 1448, ν(B—F) 1068, δ(C—H)oop 769, 695. IR (polyethylene, cm-1): ν(Pd—N)as(py) 472. 1H NMR (250 MHz, [D3]-acetonitrile solution) δ = 7.58–7.43 (m, 8H, py), 8.85–8.72 (m, 8H, py), 8.04–7.90 (m, 4H, py). 13C NMR (63 MHz, [D3]-acetonitrile solution) δ = 128–126(py), 142–140(py), 154–152(py).

Structure description top

The design of supramolecular coordination compounds by self-assembly is a developing research area (Lehn, 1995, Braga et al., 1998). Four-coordinate PdII complexes with square-planar geometry and four pyridine ligands, in particular, is a potentially useful building block for producing an array of interesting molecular architectures by means of C—H···π-ring interactions, thanks to the mobility of pyridine planes. It is for that reason that we have tried to prepare the title compound (I) to be able to compare the results with the structure of the same compound with acetone solvate (Lutz et al., 2000).

Normally, the tetrakis(pyridine-N)palladium(II) ion has a square-planar coordination, with the anion occupying the apical positions of an octahedron. Pd···X lengths are 4.299 (5) Å in (I) (X = B); 4.028 (7) Å (X = B, Lutz et al., 2000); 4.4759 (11) Å in the orthorhombic phase and 4.100 (2) Å in the triclinic phase (X = I, Tebbe et al., 1996); 3.112 (2) Å (X = O, Liqing et al. 2005) and 3.079 (4) or 3.031 (3) Å (X = F, Holzbock et al., 2000). The packing will come defined by the solvate presence and the size of the anion which will alter, in addition, the dihedral angle between the pyridine planes. This angle is equal to 89.53 (19)° in (I), 89.62° in the Liqing structure, a range of 85.73 to 81.13° in the Holzbock structure, 85.33° in orthorhombic phase and 83.37° in triclinic phase of the Tebbe structure and 78.25 to 58.13° in the Lutz structure. The C—H···π-(ring) interaction only takes place in (I) and the triclinic phase of the Tebbe structure producing a one-dimensional-structure. The data for C4—H4···N2 (pyridine ring) (symmetry = 1/2 + x, 1/2 - y, 1/2 + z) are H-centroid distance 2.97 Å, γ = 20.28°. This fact suggests that the solvate absence and a dihedral angle between the pyridine planes next to 90° facilitate this interaction.

For related literature, see: Braga et al. (1998); Holzbock et al. (2000); Lehn (1995); Liqing et al. (2005); Lutz et al. (2000); Ma et al. (2005); Tebbe et al. (1996).

Computing details top

Data collection: CAD-4-PC (Kretschmar, 1996); cell refinement: CAD-4-PC; data reduction: WinGX-PC (Farrugia, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP (Brueggemann & Schmid, 1990); software used to prepare material for publication: PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The asymmetric unit of (I), showing the atomic numbering scheme. Displacement ellipsoids are drawn at the 50% probability level. A position of the disorder of the BF4 has only been drawn for greater clarity of the figure.
Tetrakis(pyridine-κN)palladium(II) bis(tetrafluoridoborate) top
Crystal data top
[Pd(C5H5N)4](BF4)2F(000) = 1184
Mr = 596.42Dx = 1.643 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 25 reflections
a = 15.640 (7) Åθ = 9–18°
b = 10.886 (7) ŵ = 0.85 mm1
c = 15.711 (7) ÅT = 295 K
β = 115.63 (3)°Prism, yellow
V = 2412 (2) Å30.18 × 0.15 × 0.11 mm
Z = 4
Data collection top
Enraf–Nonius CAD-4
diffractometer
Rint = 0.064
Radiation source: fine-focus sealed tubeθmax = 30.0°, θmin = 2.4°
Graphite monochromatorh = 2121
ω/2θ' scansk = 1415
6864 measured reflectionsl = 2212
3521 independent reflections3 standard reflections every 120 min
1872 reflections with I > 2σ(I) intensity decay: none
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.046Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.154H atoms treated by a mixture of independent and constrained refinement
S = 0.97 w = 1/[σ2(Fo2) + (0.0885P)2]
where P = (Fo2 + 2Fc2)/3
3521 reflections(Δ/σ)max = 0.001
217 parametersΔρmax = 0.96 e Å3
20 restraintsΔρmin = 0.52 e Å3
Crystal data top
[Pd(C5H5N)4](BF4)2V = 2412 (2) Å3
Mr = 596.42Z = 4
Monoclinic, C2/cMo Kα radiation
a = 15.640 (7) ŵ = 0.85 mm1
b = 10.886 (7) ÅT = 295 K
c = 15.711 (7) Å0.18 × 0.15 × 0.11 mm
β = 115.63 (3)°
Data collection top
Enraf–Nonius CAD-4
diffractometer
Rint = 0.064
6864 measured reflections3 standard reflections every 120 min
3521 independent reflections intensity decay: none
1872 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.04620 restraints
wR(F2) = 0.154H atoms treated by a mixture of independent and constrained refinement
S = 0.97Δρmax = 0.96 e Å3
3521 reflectionsΔρmin = 0.52 e Å3
217 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Pd0.25000.25000.50000.04425 (17)
N10.3643 (3)0.3627 (3)0.5562 (3)0.0524 (10)
N20.2482 (3)0.2718 (3)0.3707 (3)0.0515 (10)
C10.3518 (4)0.4830 (5)0.5591 (5)0.0706 (16)
H10.281 (4)0.507 (6)0.540 (4)0.085*
C20.4256 (5)0.5640 (5)0.5942 (5)0.090 (2)
H20.41450.64790.59390.107*
C30.5147 (5)0.5201 (7)0.6291 (6)0.107 (3)
H30.56620.57300.65600.128*
C40.5284 (5)0.3985 (8)0.6246 (7)0.119 (3)
H40.58970.36780.64600.142*
C50.4529 (4)0.3202 (5)0.5888 (5)0.081 (2)
H50.466 (6)0.234 (5)0.602 (5)0.097*
C60.3069 (5)0.2063 (5)0.3457 (4)0.0618 (14)
H60.339 (4)0.159 (5)0.392 (4)0.074*
C70.3078 (5)0.2172 (6)0.2601 (5)0.0747 (19)
H70.359 (4)0.175 (6)0.251 (4)0.090*
C80.2451 (5)0.2970 (7)0.1942 (5)0.0736 (17)
H80.246 (5)0.302 (6)0.139 (5)0.088*
C90.1841 (5)0.3641 (5)0.2183 (4)0.0753 (17)
H90.130 (4)0.420 (6)0.181 (4)0.090*
C100.1872 (5)0.3496 (5)0.3071 (5)0.0682 (15)
H100.139 (4)0.375 (5)0.328 (4)0.082*
B0.4188 (3)0.0789 (4)0.0683 (3)0.0520 (13)
F10.3608 (6)0.1363 (7)0.1009 (6)0.087 (4)0.50
F1'0.3416 (6)0.1358 (9)0.0789 (9)0.126 (6)0.50
F20.4665 (5)0.1591 (5)0.0370 (5)0.074 (2)0.50
F2'0.4267 (10)0.1392 (11)0.0085 (7)0.209 (9)0.50
F30.3647 (5)0.0047 (5)0.0055 (5)0.078 (2)0.50
F3'0.3989 (8)0.0435 (5)0.0473 (11)0.171 (8)0.50
F40.4867 (5)0.0047 (7)0.1429 (4)0.095 (3)0.50
F4'0.5011 (6)0.0967 (14)0.1496 (6)0.206 (8)0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pd0.0444 (3)0.0326 (2)0.0633 (3)0.0010 (3)0.0304 (2)0.0053 (3)
N10.047 (2)0.0369 (19)0.075 (3)0.0015 (16)0.028 (2)0.0004 (18)
N20.056 (2)0.037 (2)0.069 (2)0.0016 (15)0.034 (2)0.0049 (16)
C10.064 (3)0.037 (2)0.107 (5)0.000 (2)0.033 (3)0.002 (3)
C20.089 (5)0.036 (3)0.135 (6)0.014 (3)0.041 (5)0.014 (4)
C30.070 (4)0.070 (4)0.149 (7)0.031 (4)0.018 (4)0.019 (5)
C40.046 (3)0.093 (6)0.184 (9)0.002 (4)0.020 (4)0.028 (6)
C50.053 (3)0.049 (3)0.131 (6)0.001 (2)0.032 (4)0.011 (3)
C60.073 (4)0.048 (2)0.082 (4)0.001 (2)0.050 (3)0.002 (3)
C70.087 (4)0.068 (4)0.094 (5)0.013 (3)0.063 (4)0.018 (3)
C80.091 (5)0.069 (3)0.071 (4)0.018 (3)0.044 (4)0.011 (3)
C90.094 (4)0.055 (3)0.069 (4)0.002 (3)0.027 (3)0.001 (3)
C100.084 (4)0.045 (3)0.084 (4)0.005 (3)0.044 (3)0.001 (3)
B0.057 (3)0.050 (3)0.053 (3)0.009 (3)0.027 (3)0.000 (2)
F10.106 (7)0.068 (7)0.130 (8)0.010 (6)0.092 (7)0.010 (6)
F1'0.087 (7)0.124 (12)0.189 (13)0.034 (7)0.079 (8)0.083 (10)
F20.083 (5)0.050 (4)0.123 (7)0.013 (3)0.076 (5)0.007 (4)
F2'0.31 (2)0.232 (19)0.121 (11)0.107 (17)0.131 (13)0.071 (11)
F30.075 (5)0.051 (4)0.096 (5)0.010 (4)0.026 (4)0.032 (4)
F3'0.166 (12)0.038 (4)0.39 (2)0.003 (6)0.201 (15)0.006 (9)
F40.097 (6)0.101 (7)0.062 (5)0.015 (5)0.013 (4)0.020 (5)
F4'0.139 (11)0.25 (2)0.138 (11)0.006 (13)0.023 (8)0.043 (12)
Geometric parameters (Å, º) top
Pd—N1i2.028 (4)C6—C71.357 (9)
Pd—N12.028 (4)C6—H60.85 (6)
Pd—N2i2.033 (5)C7—C81.382 (11)
Pd—N22.033 (5)C7—H70.99 (6)
N1—C11.328 (6)C8—C91.379 (9)
N1—C51.335 (7)C8—H80.88 (7)
N2—C101.342 (7)C9—C101.384 (9)
N2—C61.348 (7)C9—H91.00 (6)
C1—C21.365 (8)C10—H100.99 (6)
C1—H11.05 (6)B—F11.370 (6)
C2—C31.344 (10)B—F21.371 (5)
C2—H20.9300B—F3'1.375 (6)
C3—C41.348 (11)B—F4'1.380 (7)
C3—H30.9300B—F2'1.425 (7)
C4—C51.365 (9)B—F31.428 (6)
C4—H40.9300B—F1'1.430 (7)
C5—H50.96 (6)B—F41.441 (6)
N1i—Pd—N1180.00 (17)N2—C6—C7122.9 (6)
N1i—Pd—N2i89.63 (17)N2—C6—H6108 (4)
N1—Pd—N2i90.37 (17)C7—C6—H6129 (4)
N1i—Pd—N290.37 (17)C6—C7—C8119.3 (6)
N1—Pd—N289.63 (17)C6—C7—H7117 (4)
N2i—Pd—N2180.0C8—C7—H7123 (4)
C1—N1—C5118.2 (5)C9—C8—C7118.6 (6)
C1—N1—Pd119.8 (4)C9—C8—H8123 (5)
C5—N1—Pd122.0 (4)C7—C8—H8118 (5)
C10—N2—C6118.1 (5)C8—C9—C10119.3 (6)
C10—N2—Pd121.1 (4)C8—C9—H9132 (4)
C6—N2—Pd120.8 (4)C10—C9—H9108 (4)
N1—C1—C2122.7 (6)N2—C10—C9121.8 (6)
N1—C1—H1113 (4)N2—C10—H10109 (3)
C2—C1—H1124 (4)C9—C10—H10128 (3)
C3—C2—C1118.8 (6)F1—B—F2113.2 (4)
C3—C2—H2120.6F1—B—F3109.8 (4)
C1—C2—H2120.6F2—B—F3109.7 (4)
C2—C3—C4119.2 (6)F1—B—F4109.0 (4)
C2—C3—H3120.4F2—B—F4109.0 (4)
C4—C3—H3120.4F3—B—F4105.8 (4)
C3—C4—C5120.4 (7)F3'—B—F4'112.4 (4)
C3—C4—H4119.8F3'—B—F2'109.7 (4)
C5—C4—H4119.8F3'—B—F1'109.4 (4)
N1—C5—C4120.7 (6)F4'—B—F2'109.4 (4)
N1—C5—H5121 (5)F4'—B—F1'109.1 (4)
C4—C5—H5117 (5)F2'—B—F1'106.6 (4)
Symmetry code: (i) x+1/2, y+1/2, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C4—H4···Cg1ii0.932.973.800 (10)150
Symmetry code: (ii) x+1/2, y+1/2, z1/2.

Experimental details

Crystal data
Chemical formula[Pd(C5H5N)4](BF4)2
Mr596.42
Crystal system, space groupMonoclinic, C2/c
Temperature (K)295
a, b, c (Å)15.640 (7), 10.886 (7), 15.711 (7)
β (°) 115.63 (3)
V3)2412 (2)
Z4
Radiation typeMo Kα
µ (mm1)0.85
Crystal size (mm)0.18 × 0.15 × 0.11
Data collection
DiffractometerEnraf–Nonius CAD-4
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
6864, 3521, 1872
Rint0.064
(sin θ/λ)max1)0.703
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.046, 0.154, 0.97
No. of reflections3521
No. of parameters217
No. of restraints20
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.96, 0.52

Computer programs: CAD-4-PC (Kretschmar, 1996), CAD-4-PC, WinGX-PC (Farrugia, 1999), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP (Brueggemann & Schmid, 1990), PLATON (Spek, 2003).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C4—H4···Cg1i0.932.973.800 (10)150
Symmetry code: (i) x+1/2, y+1/2, z1/2.
 

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds