supplementary materials


Acta Cryst. (2007). E63, m1734    [ doi:10.1107/S1600536807024051 ]

Tetrapyridinecopper(I) hexafluoridophosphate(V)

G. Horvat, T. Portada, V. Stilinovic and V. Tomisic

Abstract top

The crystal structure of the title compound, [Cu(C5H5N)4]PF6, consists of discrete [Cu(C5H5N)4]+ and PF6- ions. Both the cations and the anions are located on \overline{4} axes. The pyridine ligands are bonded to the Cu+ ion in an almost perfectly tetrahedral coordination geometry, with Cu-N = 2.061 (3) Å and N-Cu-N angles of 110.00 (9) and 108.42 (17)°.

Comment top

The crystal structure of (I) consists of discrete tetrakis(pyridine)copper(I) and hexafluorophosphate(V) ions. The copper and phosphorus atoms are placed in 2a and 2c special positions of the space group respectively. The coordination of copper is almost perfectly tetrahedral with N—Cu—N angles 110.00 (9)° and 108.42 (17)°. The planes of the pyridine rings are at angles of 79.38° and 65.93°.

The hexafluorophosphate anions are octahedral and slightly elongated along z axes with F—P—F angles in the range 89.4 (3)° - 90.6 (3)° and P—F bond lengths 1.527 (4) Å and 1.553 (5) Å.

The shortest intermolecular distance is a C—H···F contact of 3.445 Å

Related literature top

The only previously described structure containing tetrakis(pyridine)copper(I) cations is the perchlorate salt described by Nilsson & Oskarsson (1981, 1982). It crystallized in the same space group as the title compound with analogous placement of the ions. The Cu atom was almost perfectly tetrahedrally coordinated.

Experimental top

The title compound was obtained unintentionally while attempting to crystallize a coordination compound of copper(I) with a bisoxazoline ligand. Tetrakis(acetonitrile)copper(I) hexafluorophosphate(V) (10 mg) and bisoxazoline (20 mg) were dissolved in a mixture of pyridine and toluene (10 ml, 1:1) and heated to boiling. The resulting solution was cooled to room temperature and left to slowly evaporate. Colourless crystals of (I) were obtained after 4 days.

Refinement top

All H atoms were placed geometrically and included in the refinement in the riding-model approximation, with C—H distances 0.93 with Uiso = 1.2Ueq of the carrier atom.

Computing details top

Data collection: CrysAlis CCD (Oxford Diffraction, 2003); cell refinement: CrysAlis RED (Oxford Diffraction, 2003); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999) and PARST95 (Nardelli, 1995).

Figures top
[Figure 1] Fig. 1. View of (I) with the atom labeling scheme. Displacement ellipsoids are shown at 20% probability. Hydrogen atoms are shown as spheres of arbitrary radius.
[Figure 2] Fig. 2. Crystal packing of (I) viewed along the z axis.
Tetrapyridinecopper(I) hexafluoridophosphate(V) top
Crystal data top
[Cu(C5H5N)4]PF6Dx = 1.547 Mg m3
Mr = 524.91Mo Kα radiation, λ = 0.71073 Å
Tetragonal, I4Cell parameters from 1485 reflections
Hall symbol: I -4θ = 4.6–32.0°
a = 12.600 (2) ŵ = 1.10 mm1
c = 7.0983 (14) ÅT = 295 K
V = 1126.9 (3) Å3Prism, colourless
Z = 20.39 × 0.19 × 0.14 mm
F(000) = 532
Data collection top
Oxford Diffraction Xcalibur CCD area-detector
diffractometer
1212 independent reflections
Radiation source: fine–focus sealed tube1074 reflections with I > 2σ(I)
graphiteRint = 0.041
ω scansθmax = 27.0°, θmin = 4.6°
Absorption correction: analytical
(Alcock, 1970)
h = 1616
Tmin = 0.616, Tmax = 0.791k = 1615
4610 measured reflectionsl = 99
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0713P)2]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.044(Δ/σ)max = 0.003
wR(F2) = 0.118Δρmax = 0.23 e Å3
S = 1.09Δρmin = 0.21 e Å3
1212 reflectionsAbsolute structure: Flack (1983), with 551 Friedel pairs
73 parametersFlack parameter: 0.01 (3)
1 restraint
Crystal data top
[Cu(C5H5N)4]PF6Z = 2
Mr = 524.91Mo Kα radiation
Tetragonal, I4µ = 1.10 mm1
a = 12.600 (2) ÅT = 295 K
c = 7.0983 (14) Å0.39 × 0.19 × 0.14 mm
V = 1126.9 (3) Å3
Data collection top
Oxford Diffraction Xcalibur CCD area-detector
diffractometer
1212 independent reflections
Absorption correction: analytical
(Alcock, 1970)
1074 reflections with I > 2σ(I)
Tmin = 0.616, Tmax = 0.791Rint = 0.041
4610 measured reflectionsθmax = 27.0°
Refinement top
R[F2 > 2σ(F2)] = 0.044H-atom parameters constrained
wR(F2) = 0.118Δρmax = 0.23 e Å3
S = 1.09Δρmin = 0.21 e Å3
1212 reflectionsAbsolute structure: Flack (1983), with 551 Friedel pairs
73 parametersFlack parameter: 0.01 (3)
1 restraint
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cu10000.0670 (3)
P10.500.250.0556 (4)
C50.0527 (3)0.2144 (3)0.1582 (6)0.0663 (9)
H50.0070.23820.06430.08*
N10.0734 (2)0.1106 (2)0.1698 (4)0.0594 (7)
C40.0961 (3)0.2872 (3)0.2790 (7)0.0770 (12)
H40.07890.35870.26910.092*
C30.1657 (4)0.2524 (4)0.4157 (7)0.0828 (12)
H30.19560.29980.5010.099*
C20.1896 (5)0.1477 (4)0.4225 (7)0.0879 (13)
H20.23860.12250.50960.105*
C10.1414 (3)0.0798 (3)0.3012 (6)0.0702 (10)
H10.15690.00790.31090.084*
F20.500.4688 (6)0.156 (2)
F10.3816 (3)0.0255 (6)0.2479 (10)0.196 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0591 (4)0.0591 (4)0.0828 (6)000
P10.0555 (6)0.0555 (6)0.0558 (9)000
C50.061 (2)0.0560 (19)0.082 (2)0.0073 (17)0.0066 (18)0.0021 (18)
N10.0593 (16)0.0497 (14)0.0694 (16)0.0001 (12)0.0014 (13)0.0025 (12)
C40.078 (3)0.058 (2)0.095 (3)0.0017 (19)0.010 (2)0.012 (2)
C30.085 (3)0.083 (3)0.080 (2)0.016 (2)0.001 (2)0.024 (2)
C20.101 (3)0.091 (3)0.072 (2)0.010 (3)0.020 (2)0.001 (2)
C10.078 (2)0.059 (2)0.074 (2)0.0019 (19)0.0111 (18)0.0089 (17)
F20.178 (6)0.227 (7)0.062 (3)0.019 (5)00
F10.0681 (19)0.323 (8)0.198 (5)0.030 (3)0.012 (3)0.014 (5)
Geometric parameters (Å, °) top
Cu1—N12.061 (3)C5—C41.369 (6)
Cu1—N1i2.061 (3)C5—H50.93
Cu1—N1ii2.061 (3)N1—C11.324 (5)
Cu1—N1iii2.061 (3)C4—C31.379 (7)
P1—F1iv1.526 (4)C4—H40.93
P1—F11.526 (4)C3—C21.354 (7)
P1—F1v1.526 (4)C3—H30.93
P1—F1vi1.526 (4)C2—C11.357 (7)
P1—F2iv1.553 (5)C2—H20.93
P1—F21.553 (5)C1—H10.93
C5—N11.337 (5)
N1—Cu1—N1i110.00 (9)F2iv—P1—F2180
N1—Cu1—N1ii110.00 (9)N1—C5—C4122.6 (4)
N1i—Cu1—N1ii108.42 (17)N1—C5—H5118.7
N1—Cu1—N1iii108.42 (17)C4—C5—H5118.7
N1i—Cu1—N1iii110.00 (9)C1—N1—C5117.1 (3)
N1ii—Cu1—N1iii110.00 (9)C1—N1—Cu1120.3 (2)
F1iv—P1—F190.006 (6)C5—N1—Cu1122.6 (3)
F1iv—P1—F1v90.006 (6)C5—C4—C3118.8 (4)
F1—P1—F1v178.9 (6)C5—C4—H4120.6
F1iv—P1—F1vi178.9 (6)C3—C4—H4120.6
F1—P1—F1vi90.006 (6)C2—C3—C4118.4 (4)
F1v—P1—F1vi90.006 (6)C2—C3—H3120.8
F1iv—P1—F2iv90.6 (3)C4—C3—H3120.8
F1—P1—F2iv89.4 (3)C3—C2—C1119.5 (5)
F1v—P1—F2iv89.4 (3)C3—C2—H2120.3
F1vi—P1—F2iv90.6 (3)C1—C2—H2120.3
F1iv—P1—F289.4 (3)N1—C1—C2123.5 (4)
F1—P1—F290.6 (3)N1—C1—H1118.2
F1v—P1—F290.6 (3)C2—C1—H1118.2
F1vi—P1—F289.4 (3)
Symmetry codes: (i) −y, x, −z; (ii) y, −x, −z; (iii) −x, −y, z; (iv) y+1/2, −x+1/2, −z+1/2; (v) −x+1, −y, z; (vi) −y+1/2, x−1/2, −z+1/2.
Acknowledgements top

The authors thank the Ministry of Science, Education and Sport, Republic of Croatia, for financial support of this work through grant Nos. 119–1193079-3069, 119–1191342-2960 and 098–0982914-2935.

references
References top

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