Download citation
Download citation
link to html
The crystal structure of the title compound, [Pt(C6H7N)2(C20H16N4)](PF6)2·C3H6O·0.5H2O, is composed of a bivalent square-planar platinum(II) complex, two PF6- counter-ions and solvent mol­ecules. The di-2-pyridylquinoxaline ligands are known to confer an `L shape' on square-planar platinum(II) complexes, which also display inter­calating properties. The structural characterization reported here is a contribution to a wide-ranging study focused on structural and dynamical analyses of these substrates, which may provide better insight into their biological mechanisms and activities. The expected `L-shaped' skeleton of the metallic complex combined with the antiparallel orientation of substituted pyridines (anti conformation) generates chiral objects, found in the solid state as a racemic mixture.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270105040163/rb1020sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270105040163/rb1020Isup2.hkl
Contains datablock I

CCDC reference: 296328

Comment top

Many platinum complexes show biological properties related to their reactivity toward duplex DNA (Sundquist & Lippard, 1990). Beyond cisDDP (cisplatinum) activity (Harder & Rosenberg, 1970) due to the formation of covalent DNA complexes, some aromatic species were found to react with DNA through intercalation (Lerman, 1961). The intercalation was demonstrated to occur also for Pt coordination complexes bearing wide, flat aromatic groups (Barton & Lippard, 1979). The great interest in these substrates led to careful characterizations of metal complexes with extended flat moieties both by NMR and by X-ray crystallography; beyond the solid-state structure, the solution dynamic behavior is, of course, also related to their activity (Rotondo et al., 2003). Among the wide variety of complexes obtained using substituted pyridyls as ligands, those containing 6,7-dimethyl-2,3-bis-2-pyridylquinoxaline (DMeDPQ) were found to coordinate PtII as a symmetrical seven-membered bis(pyridyl)metal chelate ring (Escuer et al., 1989). The resulting `L-shaped' complexes possess intercalating properties (Cusumano et al., 2004). Moreover, the L-shaped skeleton is prochiral, so that the combination with non-symmetrical ancillary ligands gives optically active complexes. For the [Pt(DMeDPQ)(3-Mepy)2]2+ cation, 3-methylpyridyl (3-Mepy) ligands are roughly perpendicular to the coordination plane. When the methyl groups of the 3-Mepy ligands are on the same side of the coordination plane, two Cs symmetric conformations will be generated (syn-up and syn-down); alternatively, the methyl groups can be placed on opposite sides, resulting in the loss of the mirror plane and the consequent development of two chiral C1 enantiomeric conformers, anti-C and anti-A (see scheme).

Because the free 3-Mepy rotation is observed in solution, all of the four conformers give rise to an averaged NMR signal (Rotondo et al., 2004). In the solid state only the chiral conformers (perhaps because they are thermodynamically favoured) are detected, and since the space group is centrosymmetric, the crystal contains a racemic mixture. The asymmetric unit of the title compound, (I), is occupied by one PtII cation complex, two hexafluorophosphate ions, an acetone molecule and a water molecule with 50% occupancy. The metal is bound to four pyridyl N atoms (Table 1 and Fig. 1). The four coordinating N atoms are positioned around platinum(II) in the typical square-planar geometry, the maximum deviation from the mean plane being 0.028?(5) Å (for N1). All the pyridyl rings are almost perfectly planar, as is the fused quinoline system. The angle between the metal coordination plane and the plane of the fused quinoline system is 75.8?(2)°, leading to the known L-shaped arrangement (Fig. 1). Even though all four pyridyl rings tend to flip away from the coordination plane, the strained DMeDPQ pyridyl rings are less tilted than free pyridyl ligands [the angles of the mean planes with respect to the coordination plane are 71.4?(3) and 70.2 ?(3)° versus 81.3?(3) and 83.1?(3)°, respectively]. This configuration confirms the previous hypothesis of Rotondo et al. (2004) regarding the stiffness of the DMeDPQ ligand often affecting partner ligands.

The crystal packing of (I) is mainly stabilized by conventional and unconventional intermolecular hydrogen interactions of types O—H···F, O—H···N and C—H···F (Table 2 and Fig. 2). The close proximity between an F atom and the metal centre should be noted [Pt1···F4 = 3.503?(1) Å, and the angle between the vector Pt1···F4 and the normal to the coordination plane is 8.1?(2)°]. This interaction characterizes many Pt complexes devoid of steric hindrance in the apical position; F4 is indeed located on the side opposite the cumbersome quinoline system. As is the case with most cationic complexes, the cations of (I) are held together mainly through interactions with anion and solvent groups (Fig. 2).

Experimental top

The title complex was prepared as described by Rotondo et al. (2004); colorless crystals suitable for X-ray analysis were obtained by slow evaporation from acetone.

Refinement top

The space group of (I) was hypothesized to be centrosymmetric during the data-reduction procedure and finally confirmed by subsequent evaluation (Orpen et al., 1992). All H atoms were treated as riding, with methyl C—H distances of 0.96 Å and aromatic C—H distances of 0.93 Å. The Uiso(H) values were fixed by the `riding-model' technique, being 1.2Ueq(C) for aromatic and 1.5Ueq(C) for methyl H atoms. The water molecule was located in a Fourier difference analysis and refined as a rigid group, while its occupancy factor was calculated by linking it to a free variable; the value found after ten least-squares cycles was fixed in order to reduce the number of parameters.

Structure description top

Many platinum complexes show biological properties related to their reactivity toward duplex DNA (Sundquist & Lippard, 1990). Beyond cisDDP (cisplatinum) activity (Harder & Rosenberg, 1970) due to the formation of covalent DNA complexes, some aromatic species were found to react with DNA through intercalation (Lerman, 1961). The intercalation was demonstrated to occur also for Pt coordination complexes bearing wide, flat aromatic groups (Barton & Lippard, 1979). The great interest in these substrates led to careful characterizations of metal complexes with extended flat moieties both by NMR and by X-ray crystallography; beyond the solid-state structure, the solution dynamic behavior is, of course, also related to their activity (Rotondo et al., 2003). Among the wide variety of complexes obtained using substituted pyridyls as ligands, those containing 6,7-dimethyl-2,3-bis-2-pyridylquinoxaline (DMeDPQ) were found to coordinate PtII as a symmetrical seven-membered bis(pyridyl)metal chelate ring (Escuer et al., 1989). The resulting `L-shaped' complexes possess intercalating properties (Cusumano et al., 2004). Moreover, the L-shaped skeleton is prochiral, so that the combination with non-symmetrical ancillary ligands gives optically active complexes. For the [Pt(DMeDPQ)(3-Mepy)2]2+ cation, 3-methylpyridyl (3-Mepy) ligands are roughly perpendicular to the coordination plane. When the methyl groups of the 3-Mepy ligands are on the same side of the coordination plane, two Cs symmetric conformations will be generated (syn-up and syn-down); alternatively, the methyl groups can be placed on opposite sides, resulting in the loss of the mirror plane and the consequent development of two chiral C1 enantiomeric conformers, anti-C and anti-A (see scheme).

Because the free 3-Mepy rotation is observed in solution, all of the four conformers give rise to an averaged NMR signal (Rotondo et al., 2004). In the solid state only the chiral conformers (perhaps because they are thermodynamically favoured) are detected, and since the space group is centrosymmetric, the crystal contains a racemic mixture. The asymmetric unit of the title compound, (I), is occupied by one PtII cation complex, two hexafluorophosphate ions, an acetone molecule and a water molecule with 50% occupancy. The metal is bound to four pyridyl N atoms (Table 1 and Fig. 1). The four coordinating N atoms are positioned around platinum(II) in the typical square-planar geometry, the maximum deviation from the mean plane being 0.028?(5) Å (for N1). All the pyridyl rings are almost perfectly planar, as is the fused quinoline system. The angle between the metal coordination plane and the plane of the fused quinoline system is 75.8?(2)°, leading to the known L-shaped arrangement (Fig. 1). Even though all four pyridyl rings tend to flip away from the coordination plane, the strained DMeDPQ pyridyl rings are less tilted than free pyridyl ligands [the angles of the mean planes with respect to the coordination plane are 71.4?(3) and 70.2 ?(3)° versus 81.3?(3) and 83.1?(3)°, respectively]. This configuration confirms the previous hypothesis of Rotondo et al. (2004) regarding the stiffness of the DMeDPQ ligand often affecting partner ligands.

The crystal packing of (I) is mainly stabilized by conventional and unconventional intermolecular hydrogen interactions of types O—H···F, O—H···N and C—H···F (Table 2 and Fig. 2). The close proximity between an F atom and the metal centre should be noted [Pt1···F4 = 3.503?(1) Å, and the angle between the vector Pt1···F4 and the normal to the coordination plane is 8.1?(2)°]. This interaction characterizes many Pt complexes devoid of steric hindrance in the apical position; F4 is indeed located on the side opposite the cumbersome quinoline system. As is the case with most cationic complexes, the cations of (I) are held together mainly through interactions with anion and solvent groups (Fig. 2).

Computing details top

Data collection: XSCANS (Siemens, 1993); cell refinement: XSCANS; data reduction: XPREPW (Bruker, 1997); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XPW (Bruker, 1997); software used to prepare material for publication: PARST97 (Nardelli, 1995) and WinGX-PC (Version 1.6.4.05; Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. The cation of (I), showing the L-shaped scaffold with the atom-labeling scheme. Displacements ellipsoids are drawn at the 30% probability level for all non-H atoms.
[Figure 2] Fig. 2. The crystal packing of (I), with intermolecular interactions drawn as dotted lines; several atoms have been labeled for ease of correlation with Table 2. H atoms not involved in intermolecular interactions have been omitted for clarity. The atom marked with an asterisk (*) is at the symmetry position (1/2 - x, 1/2 + y, 3/2 - z).
(6,7-Dimethyl-2,3-di-2-pyridylquinoxaline)bis(3-methylpyridine)platinum(II) bis(hexafluorophosphate) acetone solvate 0.5-hydrate top
Crystal data top
[Pt(C20H16N4)(C6H7N)2](PF6)2·C3H6O·0.5H2OF(000) = 2068
Mr = 1050.74Dx = 1.705 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 26 reflections
a = 9.815 (3) Åθ = 3.9–12.5°
b = 13.105 (3) ŵ = 3.60 mm1
c = 32.039 (7) ÅT = 298 K
β = 96.620 (15)°Prism, colourless
V = 4093.6 (18) Å30.22 × 0.18 × 0.08 mm
Z = 4
Data collection top
Bruker P4
diffractometer
Rint = 0.065
ω scansθmax = 25°, θmin = 2.0°
Absorption correction: empirical (using intensity measurements)
(North et al., 1968)
h = 111
Tmin = 0.506, Tmax = 0.757k = 115
9390 measured reflectionsl = 3838
7214 independent reflections3 standard reflections every 196 reflections
3904 reflections with I > 2σ(I) intensity decay: 6.8%
Refinement top
Refinement on F26 restraints
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.067 w = 1/[σ2(Fo2) + (0.023P)2 + 10.6011P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.122(Δ/σ)max = 0.002
S = 1.02Δρmax = 0.83 e Å3
7214 reflectionsΔρmin = 0.71 e Å3
532 parameters
Crystal data top
[Pt(C20H16N4)(C6H7N)2](PF6)2·C3H6O·0.5H2OV = 4093.6 (18) Å3
Mr = 1050.74Z = 4
Monoclinic, P21/nMo Kα radiation
a = 9.815 (3) ŵ = 3.60 mm1
b = 13.105 (3) ÅT = 298 K
c = 32.039 (7) Å0.22 × 0.18 × 0.08 mm
β = 96.620 (15)°
Data collection top
Bruker P4
diffractometer
3904 reflections with I > 2σ(I)
Absorption correction: empirical (using intensity measurements)
(North et al., 1968)
Rint = 0.065
Tmin = 0.506, Tmax = 0.7573 standard reflections every 196 reflections
9390 measured reflections intensity decay: 6.8%
7214 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0676 restraints
wR(F2) = 0.122H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.023P)2 + 10.6011P]
where P = (Fo2 + 2Fc2)/3
7214 reflectionsΔρmax = 0.83 e Å3
532 parametersΔρmin = 0.71 e Å3
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*/UeqOcc. (<1)
Pt10.49093 (5)0.20441 (4)0.615543 (15)0.03917 (14)
N10.4041 (10)0.3138 (8)0.6480 (3)0.048 (3)
C20.4703 (14)0.3991 (10)0.6602 (4)0.055 (4)
H20.55910.40760.65340.066*
C30.4153 (15)0.4741 (11)0.6820 (5)0.066 (4)
H30.4650.53250.69040.079*
C40.2847 (17)0.4608 (11)0.6910 (5)0.075 (5)
H40.24360.51150.70560.09*
C50.2115 (14)0.3735 (10)0.6791 (4)0.059 (4)
H50.12340.36380.68640.071*
C60.2721 (13)0.3012 (11)0.6560 (3)0.048 (3)
C70.2009 (10)0.2047 (11)0.6419 (3)0.042 (3)
N80.1467 (10)0.1542 (8)0.6711 (3)0.048 (3)
C90.0776 (13)0.0685 (10)0.6601 (4)0.048 (3)
C100.0251 (13)0.0056 (11)0.6899 (4)0.060 (4)
H100.03850.02440.71810.072*
C110.0441 (14)0.0809 (11)0.6792 (5)0.060 (4)
C120.0674 (13)0.1143 (10)0.6357 (5)0.061 (4)
C130.0168 (15)0.0515 (10)0.6063 (5)0.066 (4)
H130.03090.07040.57820.079*
C140.0542 (11)0.0385 (9)0.6170 (4)0.040 (3)
N150.1067 (10)0.0959 (8)0.5869 (3)0.047 (3)
C160.1777 (11)0.1770 (9)0.5983 (3)0.038 (3)
C170.2267 (12)0.2365 (8)0.5637 (3)0.037 (3)
C180.1371 (12)0.2734 (9)0.5310 (4)0.047 (3)
H180.04330.26220.53020.056*
C190.1891 (14)0.3272 (9)0.4992 (4)0.060 (4)
H190.12920.3550.47760.073*
C200.3281 (14)0.3401 (10)0.4993 (4)0.062 (4)
H200.36440.37380.47750.074*
C210.4110 (12)0.3008 (11)0.5331 (4)0.054 (3)
H210.50540.3090.53380.065*
N220.3634 (9)0.2512 (7)0.5652 (3)0.043 (3)
C230.0992 (16)0.1473 (11)0.7129 (4)0.093 (6)
H23A0.07920.11520.73990.14*
H23B0.05620.21310.71350.14*
H23C0.19660.1550.70650.14*
C240.1449 (14)0.2096 (12)0.6238 (4)0.091 (5)
H24A0.09560.26720.63630.137*
H24B0.15540.21680.59370.137*
H24C0.23370.20610.63350.137*
N250.5684 (9)0.0925 (7)0.5818 (3)0.039 (2)
C260.5179 (14)0.0012 (10)0.5833 (4)0.060 (4)
H260.45150.01570.60090.072*
C270.5639 (17)0.0766 (11)0.5587 (5)0.080 (5)
H270.530.14250.56060.096*
C280.6566 (15)0.0576 (12)0.5320 (5)0.075 (5)
H280.68580.10920.51530.09*
C290.7076 (13)0.0403 (11)0.5300 (4)0.054 (4)
C300.6614 (13)0.1125 (10)0.5557 (4)0.050 (3)
H300.69620.17840.5550.06*
C310.8129 (13)0.0666 (11)0.5005 (4)0.080 (5)
H31A0.77190.11060.47860.12*
H31B0.8440.00520.48840.12*
H31C0.88930.10080.5160.12*
N320.6133 (10)0.1672 (7)0.6678 (3)0.044 (3)
C330.7379 (13)0.2082 (12)0.6750 (4)0.060 (4)
H330.77110.24510.65350.072*
C340.8197 (14)0.1987 (13)0.7125 (5)0.075 (4)
H340.90650.22820.71620.09*
C350.7717 (15)0.1449 (11)0.7447 (4)0.066 (4)
H350.82320.14080.77090.079*
C360.6470 (16)0.0976 (11)0.7375 (4)0.062 (4)
C370.5671 (14)0.1115 (10)0.6993 (4)0.061 (4)
H370.48030.08220.69510.073*
C380.5895 (19)0.0333 (14)0.7703 (5)0.123 (7)
H38A0.66060.00950.78390.184*
H38B0.51640.00840.75720.184*
H38C0.5550.07690.79080.184*
P10.8492 (5)0.4298 (3)0.58960 (14)0.0694 (12)
F10.9960 (14)0.4519 (14)0.5992 (5)0.246 (9)
F20.8824 (15)0.3148 (8)0.5899 (4)0.181 (6)
F30.8115 (16)0.5435 (8)0.5889 (4)0.172 (6)
F40.7015 (11)0.3964 (12)0.5819 (4)0.200 (6)
F50.8687 (15)0.4354 (10)0.5433 (3)0.178 (6)
F60.8313 (15)0.4253 (8)0.6364 (3)0.162 (5)
P20.1088 (6)0.3141 (4)0.82095 (17)0.0943 (16)
F70.0379 (11)0.3664 (9)0.8178 (4)0.165 (5)
F80.2520 (11)0.2630 (10)0.8264 (4)0.174 (6)
F90.0507 (15)0.2211 (11)0.7999 (7)0.259 (9)
F100.131 (2)0.3544 (13)0.7791 (4)0.252 (9)
F110.0813 (17)0.2771 (16)0.8635 (5)0.269 (10)
F120.1619 (13)0.4114 (12)0.8392 (6)0.227 (8)
C390.632 (3)0.4384 (16)0.4268 (7)0.202 (13)
H39A0.69390.46910.40920.303*
H39B0.61280.48620.4480.303*
H39C0.54880.41980.410.303*
C400.8350 (17)0.3230 (16)0.4351 (6)0.144 (9)
H40A0.89660.37780.44390.216*
H40B0.82970.3150.40520.216*
H40C0.86820.26090.44860.216*
C410.697 (2)0.3465 (14)0.4470 (5)0.091 (6)
O420.6383 (12)0.2900 (10)0.4682 (4)0.109 (4)
O430.325 (2)0.172 (2)0.7534 (8)0.122 (9)0.5
H43A0.25050.1980.76890.183*0.5
H43B0.28430.11740.73430.183*0.5
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pt10.0421 (2)0.0388 (2)0.0369 (2)0.0005 (4)0.00563 (18)0.0011 (3)
N10.050 (7)0.055 (8)0.035 (5)0.003 (7)0.005 (5)0.003 (6)
C20.059 (10)0.053 (9)0.056 (9)0.003 (8)0.021 (8)0.001 (8)
C30.063 (11)0.046 (9)0.088 (12)0.005 (9)0.006 (9)0.017 (9)
C40.084 (12)0.054 (10)0.087 (12)0.020 (10)0.007 (10)0.040 (9)
C50.059 (9)0.055 (9)0.066 (10)0.005 (8)0.013 (8)0.018 (8)
C60.056 (8)0.046 (8)0.038 (7)0.006 (9)0.004 (6)0.005 (8)
C70.027 (6)0.064 (8)0.036 (6)0.001 (8)0.009 (5)0.003 (8)
N80.056 (7)0.051 (7)0.041 (6)0.007 (6)0.022 (6)0.016 (5)
C90.050 (9)0.043 (8)0.054 (9)0.009 (7)0.016 (7)0.003 (7)
C100.065 (10)0.066 (10)0.050 (9)0.005 (9)0.011 (8)0.009 (8)
C110.056 (9)0.062 (10)0.062 (10)0.009 (8)0.002 (8)0.019 (8)
C120.047 (9)0.046 (9)0.088 (12)0.005 (8)0.007 (8)0.017 (9)
C130.064 (10)0.057 (9)0.071 (11)0.008 (9)0.011 (9)0.011 (8)
C140.033 (7)0.039 (7)0.046 (8)0.003 (6)0.004 (6)0.003 (7)
N150.062 (7)0.041 (6)0.043 (6)0.006 (6)0.018 (6)0.001 (5)
C160.038 (7)0.045 (9)0.033 (7)0.005 (6)0.006 (6)0.002 (6)
C170.037 (7)0.037 (7)0.039 (7)0.005 (6)0.011 (6)0.009 (6)
C180.032 (7)0.048 (9)0.059 (8)0.001 (6)0.000 (6)0.003 (7)
C190.070 (10)0.046 (9)0.064 (9)0.003 (8)0.005 (8)0.023 (7)
C200.058 (9)0.070 (10)0.057 (9)0.012 (8)0.002 (8)0.023 (8)
C210.051 (8)0.057 (8)0.054 (8)0.004 (9)0.009 (7)0.008 (9)
N220.040 (6)0.045 (6)0.045 (6)0.001 (5)0.012 (5)0.005 (5)
C230.118 (14)0.090 (12)0.078 (11)0.028 (11)0.036 (11)0.020 (10)
C240.095 (12)0.077 (11)0.107 (12)0.021 (12)0.031 (10)0.008 (12)
N250.033 (6)0.043 (7)0.040 (6)0.008 (5)0.002 (5)0.003 (5)
C260.070 (10)0.035 (8)0.076 (11)0.001 (8)0.013 (8)0.011 (8)
C270.106 (14)0.048 (10)0.092 (13)0.028 (10)0.034 (11)0.001 (9)
C280.073 (12)0.079 (13)0.076 (12)0.021 (10)0.022 (10)0.025 (10)
C290.047 (9)0.060 (10)0.056 (9)0.018 (8)0.011 (7)0.001 (8)
C300.053 (9)0.037 (8)0.060 (9)0.010 (7)0.005 (7)0.014 (7)
C310.070 (10)0.095 (12)0.079 (11)0.017 (10)0.031 (9)0.024 (10)
N320.038 (6)0.037 (6)0.058 (7)0.007 (5)0.011 (5)0.003 (5)
C330.053 (8)0.070 (9)0.055 (8)0.002 (10)0.003 (7)0.002 (10)
C340.052 (9)0.081 (11)0.089 (11)0.011 (11)0.006 (9)0.002 (12)
C350.062 (10)0.080 (11)0.052 (9)0.001 (9)0.014 (8)0.000 (9)
C360.080 (11)0.060 (10)0.044 (9)0.006 (9)0.001 (9)0.010 (8)
C370.063 (10)0.061 (9)0.061 (9)0.011 (8)0.014 (8)0.012 (8)
C380.142 (18)0.131 (17)0.092 (14)0.033 (15)0.008 (13)0.035 (13)
P10.071 (3)0.065 (3)0.073 (3)0.017 (3)0.014 (2)0.005 (2)
F10.111 (11)0.33 (2)0.28 (2)0.094 (14)0.052 (12)0.059 (16)
F20.264 (16)0.092 (9)0.212 (13)0.034 (10)0.135 (12)0.031 (9)
F30.290 (18)0.078 (8)0.164 (11)0.026 (10)0.094 (12)0.015 (7)
F40.077 (8)0.274 (18)0.242 (16)0.031 (11)0.014 (9)0.069 (14)
F50.277 (16)0.182 (12)0.089 (8)0.057 (12)0.077 (10)0.033 (8)
F60.290 (16)0.127 (9)0.075 (7)0.035 (11)0.039 (9)0.009 (7)
P20.098 (4)0.081 (4)0.098 (4)0.010 (3)0.014 (3)0.008 (3)
F70.097 (9)0.142 (10)0.251 (15)0.002 (8)0.004 (9)0.019 (10)
F80.127 (9)0.207 (15)0.176 (11)0.069 (10)0.027 (8)0.043 (10)
F90.210 (15)0.118 (11)0.42 (3)0.029 (12)0.096 (16)0.102 (16)
F100.41 (3)0.242 (18)0.118 (10)0.120 (19)0.095 (14)0.069 (12)
F110.243 (17)0.38 (3)0.200 (14)0.070 (18)0.085 (13)0.185 (17)
F120.137 (11)0.191 (15)0.36 (2)0.066 (11)0.051 (13)0.153 (16)
C390.29 (3)0.125 (19)0.21 (3)0.09 (2)0.08 (2)0.064 (19)
C400.087 (14)0.20 (3)0.152 (19)0.032 (16)0.048 (13)0.046 (18)
C410.124 (17)0.096 (15)0.051 (10)0.015 (13)0.008 (11)0.010 (10)
O420.129 (10)0.104 (9)0.100 (9)0.013 (10)0.035 (8)0.000 (9)
O430.12 (2)0.14 (3)0.10 (2)0.007 (19)0.003 (16)0.003 (16)
Geometric parameters (Å, º) top
Pt1—N322.005 (10)C26—C271.371 (17)
Pt1—N12.017 (10)C26—H260.93
Pt1—N222.019 (9)C27—C281.342 (18)
Pt1—N252.022 (9)C27—H270.93
N1—C21.328 (15)C28—C291.382 (18)
N1—C61.360 (14)C28—H280.93
C2—C31.354 (16)C29—C301.366 (16)
C2—H20.93C29—C311.517 (17)
C3—C41.359 (18)C30—H300.93
C3—H30.93C31—H31A0.96
C4—C51.381 (17)C31—H31B0.96
C4—H40.93C31—H31C0.96
C5—C61.377 (16)N32—C331.331 (14)
C5—H50.93N32—C371.365 (14)
C6—C71.491 (18)C33—C341.373 (16)
C7—N81.308 (13)C33—H330.93
C7—C161.436 (14)C34—C351.377 (18)
N8—C91.338 (14)C34—H340.93
C9—C101.404 (16)C35—C361.368 (18)
C9—C141.429 (16)C35—H350.93
C10—C111.345 (17)C36—C371.388 (16)
C10—H100.93C36—C381.507 (19)
C11—C121.452 (18)C37—H370.93
C11—C231.534 (16)C38—H38A0.96
C12—C131.385 (17)C38—H38B0.96
C12—C241.489 (17)C38—H38C0.96
C13—C141.393 (16)P1—F11.468 (13)
C13—H130.93P1—F41.506 (11)
C14—N151.371 (14)P1—F51.518 (10)
N15—C161.300 (13)P1—F61.530 (10)
C16—C171.478 (14)P1—F31.535 (11)
C17—N221.351 (13)P1—F21.542 (11)
C17—C181.376 (14)P2—F121.472 (13)
C18—C191.382 (15)P2—F91.475 (13)
C18—H180.93P2—F101.479 (13)
C19—C201.375 (16)P2—F111.499 (13)
C19—H190.93P2—F81.549 (11)
C20—C211.378 (15)P2—F71.587 (12)
C20—H200.93C39—C411.48 (2)
C21—N221.345 (13)C39—H39A0.96
C21—H210.93C39—H39B0.96
C23—H23A0.96C39—H39C0.96
C23—H23B0.96C40—C411.48 (2)
C23—H23C0.96C40—H40A0.96
C24—H24A0.96C40—H40B0.96
C24—H24B0.96C40—H40C0.96
C24—H24C0.96C41—O421.195 (17)
N25—C261.327 (14)O43—H43A0.9919
N25—C301.332 (13)O43—H43B0.992
N32—Pt1—N189.4 (4)C28—C27—H27119.2
N32—Pt1—N22175.7 (4)C26—C27—H27119.2
N1—Pt1—N2286.3 (4)C27—C28—C29118.6 (14)
N32—Pt1—N2592.5 (4)C27—C28—H28120.7
N1—Pt1—N25177.1 (4)C29—C28—H28120.7
N22—Pt1—N2591.7 (4)C30—C29—C28117.9 (13)
C2—N1—C6119.4 (12)C30—C29—C31121.0 (14)
C2—N1—Pt1121.8 (9)C28—C29—C31121.1 (13)
C6—N1—Pt1118.7 (9)N25—C30—C29122.7 (12)
N1—C2—C3123.5 (13)N25—C30—H30118.6
N1—C2—H2118.2C29—C30—H30118.6
C3—C2—H2118.2C29—C31—H31A109.5
C2—C3—C4117.3 (14)C29—C31—H31B109.5
C2—C3—H3121.3H31A—C31—H31B109.5
C4—C3—H3121.3C29—C31—H31C109.5
C3—C4—C5121.3 (14)H31A—C31—H31C109.5
C3—C4—H4119.3H31B—C31—H31C109.5
C5—C4—H4119.3C33—N32—C37117.8 (11)
C6—C5—C4118.4 (13)C33—N32—Pt1119.7 (9)
C6—C5—H5120.8C37—N32—Pt1122.0 (9)
C4—C5—H5120.8N32—C33—C34123.2 (14)
N1—C6—C5119.8 (13)N32—C33—H33118.4
N1—C6—C7118.0 (12)C34—C33—H33118.4
C5—C6—C7122.1 (12)C33—C34—C35119.1 (14)
N8—C7—C16122.5 (12)C33—C34—H34120.4
N8—C7—C6115.2 (10)C35—C34—H34120.4
C16—C7—C6121.8 (11)C36—C35—C34118.9 (14)
C7—N8—C9118.1 (11)C36—C35—H35120.6
N8—C9—C10121.9 (13)C34—C35—H35120.6
N8—C9—C14120.3 (12)C35—C36—C37119.6 (14)
C10—C9—C14117.7 (12)C35—C36—C38122.4 (14)
C11—C10—C9122.3 (13)C37—C36—C38118.0 (15)
C11—C10—H10118.8N32—C37—C36121.3 (13)
C9—C10—H10118.8N32—C37—H37119.3
C10—C11—C12121.2 (13)C36—C37—H37119.3
C10—C11—C23120.4 (14)C36—C38—H38A109.5
C12—C11—C23118.4 (13)C36—C38—H38B109.5
C13—C12—C11116.4 (13)H38A—C38—H38B109.5
C13—C12—C24122.4 (14)C36—C38—H38C109.5
C11—C12—C24121.3 (13)H38A—C38—H38C109.5
C12—C13—C14123.0 (13)H38B—C38—H38C109.5
C12—C13—H13118.5F1—P1—F4174.1 (10)
C14—C13—H13118.5F1—P1—F588.0 (9)
N15—C14—C13120.7 (12)F4—P1—F594.6 (8)
N15—C14—C9119.9 (11)F1—P1—F691.3 (9)
C13—C14—C9119.4 (12)F4—P1—F686.2 (8)
C16—N15—C14118.9 (10)F5—P1—F6179.1 (9)
N15—C16—C7120.0 (11)F1—P1—F392.3 (9)
N15—C16—C17115.5 (10)F4—P1—F393.1 (9)
C7—C16—C17124.5 (11)F5—P1—F389.8 (7)
N22—C17—C18121.4 (11)F6—P1—F389.8 (7)
N22—C17—C16117.1 (11)F1—P1—F289.5 (9)
C18—C17—C16121.5 (11)F4—P1—F285.2 (8)
C17—C18—C19118.9 (11)F5—P1—F290.2 (7)
C17—C18—H18120.6F6—P1—F290.3 (7)
C19—C18—H18120.6F3—P1—F2178.3 (9)
C20—C19—C18120.8 (13)F12—P2—F9175.7 (11)
C20—C19—H19119.6F12—P2—F1088.3 (11)
C18—C19—H19119.6F9—P2—F1088.3 (11)
C19—C20—C21116.8 (12)F12—P2—F1190.6 (11)
C19—C20—H20121.6F9—P2—F1192.7 (11)
C21—C20—H20121.6F10—P2—F11177.3 (10)
N22—C21—C20123.8 (12)F12—P2—F893.1 (8)
N22—C21—H21118.1F9—P2—F889.6 (8)
C20—C21—H21118.1F10—P2—F891.8 (9)
C21—N22—C17118.3 (10)F11—P2—F890.7 (8)
C21—N22—Pt1121.3 (8)F12—P2—F785.9 (8)
C17—N22—Pt1120.4 (8)F9—P2—F791.6 (8)
C11—C23—H23A109.5F10—P2—F790.9 (8)
C11—C23—H23B109.5F11—P2—F786.6 (8)
H23A—C23—H23B109.5F8—P2—F7177.1 (8)
C11—C23—H23C109.5C41—C39—H39A109.5
H23A—C23—H23C109.5C41—C39—H39B109.5
H23B—C23—H23C109.5H39A—C39—H39B109.5
C12—C24—H24A109.5C41—C39—H39C109.5
C12—C24—H24B109.5H39A—C39—H39C109.5
H24A—C24—H24B109.5H39B—C39—H39C109.5
C12—C24—H24C109.5C41—C40—H40A109.5
H24A—C24—H24C109.5C41—C40—H40B109.5
H24B—C24—H24C109.5H40A—C40—H40B109.5
C26—N25—C30119.4 (11)C41—C40—H40C109.5
C26—N25—Pt1119.2 (9)H40A—C40—H40C109.5
C30—N25—Pt1121.3 (9)H40B—C40—H40C109.5
N25—C26—C27119.8 (13)O42—C41—C39123 (2)
N25—C26—H26120.1O42—C41—C40122.1 (19)
C27—C26—H26120.1C39—C41—C40114.5 (18)
C28—C27—C26121.6 (15)H43A—O43—H43B107
N32—Pt1—N1—C272.1 (10)N15—C16—C17—N22122.2 (11)
N22—Pt1—N1—C2107.1 (9)C7—C16—C17—N2259.4 (15)
N32—Pt1—N1—C6110.7 (9)N15—C16—C17—C1856.3 (15)
N22—Pt1—N1—C670.1 (9)C7—C16—C17—C18122.1 (13)
C6—N1—C2—C32.8 (19)N22—C17—C18—C190.6 (17)
Pt1—N1—C2—C3179.9 (10)C16—C17—C18—C19179.0 (11)
N1—C2—C3—C41 (2)C17—C18—C19—C202.8 (19)
C2—C3—C4—C51 (2)C18—C19—C20—C213 (2)
C3—C4—C5—C63 (2)C19—C20—C21—N220 (2)
C2—N1—C6—C54.4 (18)C20—C21—N22—C171.9 (19)
Pt1—N1—C6—C5178.4 (9)C20—C21—N22—Pt1175.7 (10)
C2—N1—C6—C7179.9 (10)C18—C17—N22—C211.7 (17)
Pt1—N1—C6—C72.6 (14)C16—C17—N22—C21176.8 (10)
C4—C5—C6—N14.3 (19)C18—C17—N22—Pt1175.9 (8)
C4—C5—C6—C7179.8 (12)C16—C17—N22—Pt15.5 (13)
N1—C6—C7—N8126.1 (12)N1—Pt1—N22—C21109.8 (10)
C5—C6—C7—N849.5 (16)N25—Pt1—N22—C2172.3 (10)
N1—C6—C7—C1662.0 (15)N1—Pt1—N22—C1767.8 (9)
C5—C6—C7—C16122.4 (13)N25—Pt1—N22—C17110.1 (9)
C16—C7—N8—C96.1 (17)N32—Pt1—N25—C2684.4 (9)
C6—C7—N8—C9177.9 (10)N22—Pt1—N25—C2696.2 (9)
C7—N8—C9—C10175.2 (11)N32—Pt1—N25—C30100.9 (9)
C7—N8—C9—C145.3 (17)N22—Pt1—N25—C3078.5 (9)
N8—C9—C10—C11179.8 (12)C30—N25—C26—C271.4 (19)
C14—C9—C10—C110.8 (19)Pt1—N25—C26—C27176.3 (10)
C9—C10—C11—C120 (2)N25—C26—C27—C282 (2)
C9—C10—C11—C23179.8 (12)C26—C27—C28—C291 (2)
C10—C11—C12—C131 (2)C27—C28—C29—C301 (2)
C23—C11—C12—C13179.5 (13)C27—C28—C29—C31179.8 (13)
C10—C11—C12—C24179.5 (13)C26—N25—C30—C290.1 (18)
C23—C11—C12—C241 (2)Pt1—N25—C30—C29174.6 (9)
C11—C12—C13—C141 (2)C28—C29—C30—N251 (2)
C24—C12—C13—C14179.1 (12)C31—C29—C30—N25179.6 (11)
C12—C13—C14—N15177.4 (12)N1—Pt1—N32—C3394.2 (10)
C12—C13—C14—C90 (2)N25—Pt1—N32—C3387.9 (10)
N8—C9—C14—N152.3 (18)N1—Pt1—N32—C3776.9 (10)
C10—C9—C14—N15178.2 (11)N25—Pt1—N32—C37100.9 (10)
N8—C9—C14—C13179.4 (11)C37—N32—C33—C341 (2)
C10—C9—C14—C131.1 (18)Pt1—N32—C33—C34170.1 (12)
C13—C14—N15—C16176.9 (11)N32—C33—C34—C350 (2)
C9—C14—N15—C160.1 (17)C33—C34—C35—C364 (2)
C14—N15—C16—C70.5 (16)C34—C35—C36—C375 (2)
C14—N15—C16—C17178.0 (10)C34—C35—C36—C38177.2 (15)
N8—C7—C16—N153.8 (18)C33—N32—C37—C360.1 (19)
C6—C7—C16—N15175.1 (11)Pt1—N32—C37—C36171.4 (10)
N8—C7—C16—C17174.6 (11)C35—C36—C37—N323 (2)
C6—C7—C16—C173.3 (17)C38—C36—C37—N32178.8 (13)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O43—H43A···F80.992.032.79 (3)132
O43—H43A···F90.992.323.29 (3)166
O43—H43A···F100.992.43.23 (3)140
O43—H43B···N80.992.353.00 (3)122
C3—H3···F9i0.932.53.30 (2)144
C35—H35···F9ii0.932.553.241 (19)132
C26—H26···F12iii0.932.513.41 (2)161
C33—H33···F60.932.513.275 (19)140
Symmetry codes: (i) x+1/2, y+1/2, z+3/2; (ii) x+1, y, z; (iii) x+1/2, y1/2, z+3/2.

Experimental details

Crystal data
Chemical formula[Pt(C20H16N4)(C6H7N)2](PF6)2·C3H6O·0.5H2O
Mr1050.74
Crystal system, space groupMonoclinic, P21/n
Temperature (K)298
a, b, c (Å)9.815 (3), 13.105 (3), 32.039 (7)
β (°) 96.620 (15)
V3)4093.6 (18)
Z4
Radiation typeMo Kα
µ (mm1)3.60
Crystal size (mm)0.22 × 0.18 × 0.08
Data collection
DiffractometerBruker P4
Absorption correctionEmpirical (using intensity measurements)
(North et al., 1968)
Tmin, Tmax0.506, 0.757
No. of measured, independent and
observed [I > 2σ(I)] reflections
9390, 7214, 3904
Rint0.065
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.067, 0.122, 1.02
No. of reflections7214
No. of parameters532
No. of restraints6
H-atom treatmentH-atom parameters constrained
w = 1/[σ2(Fo2) + (0.023P)2 + 10.6011P]
where P = (Fo2 + 2Fc2)/3
Δρmax, Δρmin (e Å3)0.83, 0.71

Computer programs: XSCANS (Siemens, 1993), XSCANS, XPREPW (Bruker, 1997), SIR97 (Altomare et al., 1999), SHELXL97 (Sheldrick, 1997), XPW (Bruker, 1997), PARST97 (Nardelli, 1995) and WinGX-PC (Version 1.6.4.05; Farrugia, 1999).

Selected geometric parameters (Å, º) top
Pt1—N322.005 (10)Pt1—N222.019 (9)
Pt1—N12.017 (10)Pt1—N252.022 (9)
N32—Pt1—N189.4 (4)N32—Pt1—N2592.5 (4)
N1—Pt1—N2286.3 (4)N22—Pt1—N2591.7 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O43—H43A···F80.992.032.79 (3)132
O43—H43A···F90.992.323.29 (3)166
O43—H43A···F100.992.43.23 (3)140
O43—H43B···N80.992.353.00 (3)122
C3—H3···F9i0.932.53.30 (2)144
C35—H35···F9ii0.932.553.241 (19)132
C26—H26···F12iii0.932.513.41 (2)161
C33—H33···F60.932.513.275 (19)140
Symmetry codes: (i) x+1/2, y+1/2, z+3/2; (ii) x+1, y, z; (iii) x+1/2, y1/2, z+3/2.
 

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