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Both the cis, (I), and trans, (II), isomers of the title complex, [PtCl2(C4H7NO)(C2H6OS)], possess relatively undistorted square-planar geometries about the Pt atoms. For (I), cis L-Pt-L angles are in the range 88.8 (2)-91.08 (8)°, while trans angles are 178.61 (8) and 179.4 (2)°. For (II), cis L-Pt-L 86.1 (3)-93.7 (1)°, and trans L-Pt-L 175.5 (1) and 179.1 (3)°. The di­methyl sulfoxide (dmso) ligand adopts a normal pyramidal geometry in both complexes. In (I), the S=O bond essentially eclipses the adjacent Pt-N bond, while the oxazine ligand in (I) is twisted so as to avoid steric interactions with the adjacent chloride ligand. By contrast, the dmso ligand in (II) is rotated such that the S=O bond is approximately perpendicular to the square plane, while the oxazine ligand is once again twisted out of the plane by a similar amount as in (I). These are the first structural examples of square-planar platinum(II) complexes containing a 1,2-oxazine ligand.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270199013803/fr1238sup1.cif
Contains datablocks global, I, II

sft

Structure factor file (SHELXL table format) https://doi.org/10.1107/S0108270199013803/fr1238Isup2.sft
Supplementary material

sft

Structure factor file (SHELXL table format) https://doi.org/10.1107/S0108270199013803/fr1238IIsup3.sft
Supplementary material

CCDC references: 140946; 140947

Comment top

Since the discovery of the antitumor activity of cis-diamminedichloroplatinum(II) (cisplatin), a large number of square-planar platinum complexes have been studied as potential chemotherapeutic drugs which might maintain the efficacy of cisplatin without the undesirable side effects (Lippard, 1982; Rosenberg, 1985). Typically, these complexes consist of two inert cis ammine ligands and two labile cis ligands which act as leaving groups in the body, thus allowing the platinum to coordinate to the DNA of cancer cells. One complex which has achieved widespread use as an alternative to cisplatin is cis-diammine(1,1-cyclobutanedicarboxylato)platinum(II) (carboplatin). The use of 1,2-oxazines as nitrogen ligands could lead to novel compounds with increased antitumor activity or decreased toxicity due to the demonstrated biological activity of the oxazine and the easily cleaved N—O bond in the oxazine ring. Compounds (I) and (II) were obtained from an unsuccessful effort to synthesize cis-bis(3,6-dihydro-1,2-oxazine)1,1-cyclobutanedicarboxylatoplatinum(II) through an intermediate DMSO complex. They represent new members of a modest family of square planar [PtCl2(DMSO)(amine)] complexes whose structural features they share.

The cis isomer (I) of dichloro(3,6-dihydro-1,2-oxazine-N)(dimethyl sulfoxide-S)platinum(II) is shown in Fig. 1. The Pt coordination geometry (Table 1) is quite regular, with all angles within 1.4° of their ideal values. The mean devation from the PtCl2SN least squares plane is 0.011 (3) Å. The Pt—Cl distance opposite the DMSO ligand is 0.015 (3) Å longer than that opposite the oxazine ligand. This is consistent with what is observed in most of the reported cis-[PtCl2(DMSO)(amine)] complexes (Melanson & Rochon, 1977; Belsky et al., 1990, 1991; Rochon et al., 1990, 1994; Neuse et al., 1995; Caldwell et al., 1995; Cornia et al., 1997). The Pt—S and Pt—N distances are also within the reported ranges [2.184 (3)–2.225 (2) and 1.950 (6)–2.06 (1) Å, respectively], including those of two platinum 1,3-oxazine complexes (Albinati et al., 1989; Michelin et al., 1994). The pyramidal DMSO ligand is positioned so that the SO bond is nearly coplanar with the square plane [torsion angle O2–S–Pt–N −4.6 (3)°], while the S—C bonds are staggered between the Pt—Cl1 bond [torsion angle Cl1—Pt—S—C5 − 62.6 (4)°]. This arrangement is also observed when the amine ligand is 2-picoline (Melanson & Rochon, 1977), pyridine (Belsky et al., 1991), cylopentylamine (Caldwell et al., 1995), tert-butylamine (Neuse et al., 1995), and thiazole (Cornia et al., 1997). For acetonitrile, two structures have been reported, one with S O eclipsing Pt—N (Rochon et al., 1990) and one with an S—C bond approximately aligned with Pt—N (Belsky et al., 1990). The latter conformation is also found in the propionitrile complex (Rochon et al., 1994). The SO bond at 1.489 (5) Å is significantly shorter than that in the free molecule at 278 K [1.531 (5) Å] (Davies, 1981), but is at the high end of the range found in similar Pt complexes [1.44 (3)–1.48 (1) Å]. As in the free DMSO, the O—S—C angles are larger than the C—S—C angle, though the difference is smaller in the complex. The oxazine molecule shows bond distances and angles consistent with those found in non-coordinated 1,2-oxazine derivatives (Riddell et al., 1974; Holzapfel et al., 1987). It is positioned so that the N—O1 and N—C4 bonds are staggered about Cl2 [torsion angles Cl2—Pt—N—C4 62.2 (5) and Cl2–Pt–N–O1 − 63.3 (4) Å].

The trans isomer (II) is shown in Fig. 2. The Pt coordination geometry (Table 2) is slightly less regular than that of the cis isomer in that the Cl—Pt—Cl angle is closed 4.5° from ideal, causing a similar ca 3–4° distortion in the Cl2—Pt—S and Cl2—Pt—N angles. The mean deviation from the PtCl2SN plane is 0.021 (4) Å, with the two chloride ligands displaced 0.041 (4) and 0.035 (4) Å to the same side of the plane. As is the case in trans-[PtCl2(DMSO)(amine)] complexes (Melanson & Rochon, 1978; Caruso et al., 1980; Viossat et al., 1991; Lovqvist & Oskarsson, 1992; Cornia et al., 1997), the Pt—Cl bond distances are closer to one another than in (I) and within experimental error. The Pt—S distance [2.230 (3) Å] is nearly 0.01 Å longer than the longest reported distance for this type of complex, while the Pt—N distance [2.067 (9) Å] is to the high end of the reported range [2.03 (1)–2.08 (2) Å] as is the S—O bond length. The DMSO ligand is positioned quite differently from that in (I). The SO bond is almost perpendicular to the square plane [torsion angle Cl2–Pt–S–O2 100.5 (4)°], while the S—C5 bond is the closest to being in the plane [torsion angle Cl2—Pt—S—C5 − 24.6 (6)°]. A similar arrangement is found in trans-[PtCl2(DMSO)(NH3)] (Viossat et al., 1991), while other skewed orientations with the SO group directed away from the square plane are found in the pyridine (Caruso et al., 1980), piperidine (Lovqvist & Oskarsson, 1992) and thiazole (Cornia et al., 1997) complexes. Only the cytidine complex (Melanson & Rochon, 1978) differs in having the SO bond eclipsing an adjacent ligand as in (I). The bond distances and angles within the oxazine ligand do not differ significantly from those in (I). The conformation of the ring is also essentially the same [torsion angles for (I) and (II), respectively: N—C4—C3—C2 12 (1), 14 (2)°; N—O1—C1—C2 − 49.6 (8), −48 (1)°]. The ring is positioned similarly to that in the cis isomer with the N—O1 and N—C4 bonds rotated away from the adjacent Cl ligands [torsion angles Cl1—Pt—N—O1 − 55.6 (6) and Cl1—Pt—N—C4 67.9 (9)°].

Experimental top

For (I), a solution of cis-bis(dimethyl sulfoxide)(1,1-cyclobutanedicarboxylato)platinum(II) (0.502 g, 0.95 mmol) and 3,6-dihydro-1,2-oxazinium chloride (0.239 g, 1.95 mmol) in water (30 ml) was stirred at room temperature for 0.5 h. The yellow crystals which formed were collected by filtration, washed with several portions of distilled water, and dried at 323 K and 2666.45 Pa to provide cis-dichloro(3,6-dihydro-1,2-oxazine-N)(dimethyl sulfoxide-S)platinum(II) (0.269 g). For (II), to a stirred solution of cis-bis(dimethyl sulfoxide)(1,1-cyclobutanedicarboxylato)platinum(II) (0.314 g, 0.60 mmol) in water (20 ml) was added, dropwise, a solution of 3,6-dihydro-1,2-oxazine (0.149 g, 1.23 mmol) in water (5.0 ml) (pH adjusted to 4.0 with aqueous hydrochloric acid solution). The resulting solution was stirred at 328 K for 2 h and then allowed to stand at room temperature for 2 d. The volume of solution was reduced by rotary evaporation of the solvent at reduced pressure. The solid product was collected, washed repeatedly with distilled water, and dried at 323 K and 2666.45 Pa to provide trans-dichloro(3,6-dihydro-1,2-oxazine-N)(dimethyl sulfoxide-S)platinum(II) (0.167 g).

Refinement top

The minimum and maximum points on the final difference electron-density map were 1.03 and 1.27 Å, respectively, from the Pt atom. The minimum and maximum peaks in the final difference electron-density map were 1.02 Å from Pt and 1.63 Å from H9, respectively.

Computing details top

For both compounds, data collection: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1988); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: TEXSAN (Molecular Structure Corporation, 1991); program(s) used to solve structure: MITHRIL (Gilmore, 1983); program(s) used to refine structure: TEXSAN; molecular graphics: ORTEPII (Johnson, 1976); software used to prepare material for publication: TEXSAN.

Figures top
[Figure 1] Fig. 1. An ORTEPII diagram (Johnson, 1976) showing the molecular structure and atom-labelling scheme of (I). The displacement ellipsoids of the non-H atoms are shown at the 50% probability level.
[Figure 2] Fig. 2. An ORTEPII diagram (Johnson, 1976) showing the molecular structure and atom-labelling scheme of (II). The displacement ellipsoids of the non-H atoms are shown at the 50% probability level.
(I) top
Crystal data top
[PtCl2(C4H7NO)(C2H6OS)]Z = 2
Mr = 429.23F(000) = 400
Triclinic, P1Dx = 2.403 Mg m3
a = 8.177 (4) ÅMo Kα radiation, λ = 0.7107 Å
b = 8.517 (4) ÅCell parameters from 22 reflections
c = 10.297 (4) Åθ = 20.6–22.4°
α = 105.84 (3)°µ = 12.6 mm1
β = 104.42 (3)°T = 296 K
γ = 111.16 (3)°Slab, pale yellow
V = 593.2 (5) Å30.25 × 0.12 × 0.10 mm
Data collection top
Rigaku AFC6S
diffractometer
1820 reflections with I > 3σ(I)
Radiation source: X-ray tubeRint = 0.013
Graphite monochromatorθmax = 25.0°
ω–2θ scansh = 09
Absorption correction: ψ scan
(North et al., 1968)
k = 109
Tmin = 0.190, Tmax = 0.284l = 1211
2249 measured reflections3 standard reflections every 150 reflections
2089 independent reflections intensity decay: 2.3%
Refinement top
Refinement on F20 restraints
Least-squares matrix: full0 constraints
R[F2 > 2σ(F2)] = 0.026H-atom parameters not refined
wR(F2) = 0.059Weighting scheme based on measured s.u.'s w = 4Fo2/σ2(Fo2)
S = 2.23(Δ/σ)max = 0.001
2087 reflectionsΔρmax = 0.73 e Å3
118 parametersΔρmin = 1.75 e Å3
Crystal data top
[PtCl2(C4H7NO)(C2H6OS)]γ = 111.16 (3)°
Mr = 429.23V = 593.2 (5) Å3
Triclinic, P1Z = 2
a = 8.177 (4) ÅMo Kα radiation
b = 8.517 (4) ŵ = 12.6 mm1
c = 10.297 (4) ÅT = 296 K
α = 105.84 (3)°0.25 × 0.12 × 0.10 mm
β = 104.42 (3)°
Data collection top
Rigaku AFC6S
diffractometer
1820 reflections with I > 3σ(I)
Absorption correction: ψ scan
(North et al., 1968)
Rint = 0.013
Tmin = 0.190, Tmax = 0.2843 standard reflections every 150 reflections
2249 measured reflections intensity decay: 2.3%
2089 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0260 restraints
wR(F2) = 0.059H-atom parameters not refined
S = 2.23Δρmax = 0.73 e Å3
2087 reflectionsΔρmin = 1.75 e Å3
118 parameters
Special details top

Refinement. The minimum and maximum points on the final difference electron density map were 1.03 and 1.27 Å, respectively, from the Pt atom.

H atoms were located on difference electron-density maps and their positions idealized (X—H 0.95 Å) with Biso values set at 1.2 times Beq of the attached atom at the time of their inclusion.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pt0.24440 (5)0.21118 (4)0.24855 (3)0.03340 (9)
Cl10.2700 (4)0.0318 (3)0.3774 (3)0.0608 (8)
Cl20.3838 (3)0.0909 (3)0.1045 (3)0.0513 (7)
S0.1078 (3)0.3257 (3)0.3807 (2)0.0384 (6)
O10.4130 (7)0.5031 (7)0.1580 (6)0.049 (2)
O20.0728 (8)0.4734 (8)0.3483 (6)0.049 (2)
N0.2241 (9)0.3738 (8)0.1355 (7)0.037 (2)
C10.405 (1)0.651 (1)0.1163 (10)0.052 (3)
C20.255 (1)0.580 (1)0.0310 (10)0.048 (3)
C30.122 (1)0.408 (1)0.0957 (9)0.045 (3)
C40.104 (1)0.279 (1)0.0232 (8)0.042 (2)
C50.112 (1)0.153 (1)0.358 (1)0.060 (3)
C60.244 (1)0.412 (1)0.5716 (9)0.061 (3)
H10.17000.44470.17870.0448
H20.37880.72720.18610.0627
H30.52460.72230.11530.0627
H40.25500.65980.07950.0576
H50.03340.36500.19270.0543
H60.02470.21630.03570.0509
H70.14240.19210.06740.0509
H80.16030.20400.42420.0716
H90.09400.05610.37690.0716
H100.20100.10570.26030.0716
H110.35000.52750.60140.0735
H120.28800.32770.59040.0735
H130.16710.42560.62490.0735
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pt0.0378 (2)0.0339 (2)0.0299 (2)0.0156 (1)0.0139 (1)0.0153 (1)
Cl10.091 (2)0.061 (1)0.055 (1)0.045 (1)0.032 (1)0.039 (1)
Cl20.060 (1)0.049 (1)0.064 (2)0.032 (1)0.039 (1)0.027 (1)
S0.041 (1)0.050 (1)0.027 (1)0.021 (1)0.0143 (10)0.0187 (10)
O10.035 (3)0.047 (3)0.050 (4)0.007 (3)0.007 (3)0.025 (3)
O20.071 (4)0.062 (4)0.046 (4)0.046 (3)0.033 (3)0.036 (3)
N0.042 (4)0.044 (4)0.031 (4)0.020 (3)0.017 (3)0.020 (3)
C10.052 (6)0.045 (5)0.058 (6)0.015 (4)0.018 (5)0.030 (5)
C20.052 (6)0.056 (6)0.051 (6)0.025 (5)0.028 (5)0.036 (5)
C30.056 (6)0.061 (6)0.033 (5)0.031 (5)0.023 (4)0.028 (4)
C40.041 (5)0.040 (5)0.032 (5)0.011 (4)0.007 (4)0.011 (4)
C50.052 (6)0.065 (6)0.062 (6)0.020 (5)0.029 (5)0.029 (5)
C60.066 (6)0.087 (7)0.020 (4)0.040 (6)0.009 (4)0.007 (4)
Geometric parameters (Å, º) top
Pt—Cl12.310 (2)N—H10.95
Pt—Cl22.325 (2)C1—H20.95
Pt—S2.207 (2)C1—H30.95
Pt—N2.062 (6)C2—H40.95
S—O21.489 (5)C3—H50.95
S—C51.776 (9)C4—H60.95
S—C61.783 (8)C4—H70.95
O1—N1.452 (7)C5—H80.95
O1—C11.458 (9)C5—H90.95
N—C41.480 (9)C5—H100.95
C1—C21.49 (1)C6—H110.95
C2—C31.32 (1)C6—H120.95
C3—C41.47 (1)C6—H130.95
Cl1—Pt—Cl290.07 (8)C2—C1—H2109
Cl1—Pt—S91.08 (8)C2—C1—H3109
Cl1—Pt—N179.4 (2)H2—C1—H3109
Cl2—Pt—S178.61 (8)C1—C2—H4119
Cl2—Pt—N90.1 (2)C3—C2—H4119
S—Pt—N88.8 (2)C2—C3—H5119
Pt—S—O2113.8 (2)C4—C3—H5119
Pt—S—C5111.7 (3)N—C4—H6109
Pt—S—C6111.2 (3)N—C4—H7109
O2—S—C5107.9 (4)C3—C4—H6109
O2—S—C6108.9 (4)C3—C4—H7109
C5—S—C6102.7 (4)H6—C4—H7109
N—O1—C1110.2 (5)S—C5—H8109
Pt—N—O1109.8 (4)S—C5—H9109
Pt—N—C4117.1 (5)S—C5—H10109
O1—N—C4109.4 (5)H8—C5—H9109
O1—C1—C2111.6 (7)H8—C5—H10109
C1—C2—C3121.5 (8)H9—C5—H10109
C2—C3—C4122.3 (8)S—C6—H11110
N—C4—C3112.1 (6)S—C6—H12110
Pt—N—H1107S—C6—H13110
O1—N—H1107H11—C6—H12109
C4—N—H1107H11—C6—H13109
O1—C1—H2109H12—C6—H13109
O1—C1—H3109
Pt—N—O1—C1163.4 (5)O1—N—C4—C346.4 (8)
Pt—N—C4—C3172.1 (5)O1—C1—C2—C315 (1)
Cl1—Pt—S—O2174.8 (3)O2—S—Pt—N4.6 (3)
Cl1—Pt—S—C562.6 (4)N—Pt—S—C5118.0 (4)
Cl1—Pt—S—C651.4 (4)N—Pt—S—C6128.0 (4)
Cl2—Pt—N—O163.3 (4)N—O1—C1—C249.6 (8)
Cl2—Pt—N—C462.2 (5)N—C4—C3—C212 (1)
S—Pt—N—O1117.5 (4)C1—O1—N—C466.8 (7)
S—Pt—N—C4117.0 (5)C1—C2—C3—C44 (1)
(II) top
Crystal data top
[PtCl2(C4H7NO)(C2H6OS)]Dx = 2.442 Mg m3
Mr = 429.23Mo Kα radiation, λ = 0.7107 Å
Orthorhombic, PbcaCell parameters from 20 reflections
a = 16.532 (3) Åθ = 15.5–20.3°
b = 13.868 (2) ŵ = 12.8 mm1
c = 10.182 (4) ÅT = 296 K
V = 2334 (1) Å3Hexagonal plate, pale yellow
Z = 80.30 × 0.10 × 0.03 mm
F(000) = 1600
Data collection top
Rigaku AFC6S
diffractometer
1277 reflections with I > 3σ(I)
Radiation source: X-ray tubeRint = 0.00
Graphite monochromatorθmax = 25.0°
ω–2θ scansh = 019
Absorption correction: ψ scan
(North et al., 1968)
k = 016
Tmin = 0.242, Tmax = 0.681l = 120
2053 measured reflections3 standard reflections every 150 reflections
2053 independent reflections intensity decay: 0.1%
Refinement top
Refinement on F20 constraints
Least-squares matrix: fullH-atom parameters not refined
R[F2 > 2σ(F2)] = 0.032Weighting scheme based on measured s.u.'s w = 4Fo2/σ2(Fo2)
wR(F2) = 0.074(Δ/σ)max = 0.001
S = 1.71Δρmax = 1.95 e Å3
2049 reflectionsΔρmin = 2.09 e Å3
119 parametersExtinction correction: Zachariasen (1968) type 2 Gaussian isotropic
0 restraintsExtinction coefficient: 0.00000010 (5)
Crystal data top
[PtCl2(C4H7NO)(C2H6OS)]V = 2334 (1) Å3
Mr = 429.23Z = 8
Orthorhombic, PbcaMo Kα radiation
a = 16.532 (3) ŵ = 12.8 mm1
b = 13.868 (2) ÅT = 296 K
c = 10.182 (4) Å0.30 × 0.10 × 0.03 mm
Data collection top
Rigaku AFC6S
diffractometer
1277 reflections with I > 3σ(I)
Absorption correction: ψ scan
(North et al., 1968)
Rint = 0.00
Tmin = 0.242, Tmax = 0.6813 standard reflections every 150 reflections
2053 measured reflections intensity decay: 0.1%
2053 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0320 restraints
wR(F2) = 0.074H-atom parameters not refined
S = 1.71Δρmax = 1.95 e Å3
2049 reflectionsΔρmin = 2.09 e Å3
119 parameters
Special details top

Refinement. The minimum and maximum peaks in the final difference map were 1.02 Å from Pt and 1.63 Å from H9, respectively.

H atoms were located on difference electron-density maps and their positions idealized (X—H 0.95 Å) with Biso values set at 1.2 times Beq of the attached atom at the time of their inclusion.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pt0.04257 (3)0.07117 (3)0.72831 (4)0.0280 (1)
Cl10.1433 (2)0.1845 (2)0.7486 (4)0.0478 (10)
Cl20.0533 (2)0.0483 (2)0.7217 (4)0.0457 (9)
S0.0391 (2)0.1812 (2)0.6393 (3)0.0358 (9)
O10.1921 (5)0.0372 (5)0.7407 (10)0.040 (2)
O20.0767 (5)0.2498 (5)0.7326 (9)0.046 (2)
N0.1173 (6)0.0308 (6)0.8133 (10)0.035 (3)
C10.2384 (8)0.1211 (8)0.779 (1)0.046 (4)
C20.2459 (9)0.1305 (9)0.922 (2)0.053 (5)
C30.2007 (9)0.081 (1)1.006 (1)0.056 (5)
C40.1360 (10)0.0145 (9)0.954 (1)0.047 (4)
C50.118 (1)0.1284 (9)0.542 (1)0.061 (5)
C60.0137 (9)0.249 (1)0.518 (2)0.064 (5)
H10.09090.09140.80660.0419
H20.29110.11610.74180.0551
H30.21240.17700.74520.0551
H40.28500.17400.95550.0630
H50.20910.08751.09760.0669
H60.15370.05020.96430.0572
H70.08800.02431.00340.0572
H80.09520.07850.48950.0728
H90.15780.10250.59820.0728
H100.14060.17640.48730.0728
H110.02420.28160.46360.0766
H120.04800.29440.55930.0766
H130.04530.20630.46550.0766
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pt0.0253 (3)0.0279 (2)0.0308 (3)0.0011 (2)0.0000 (3)0.0041 (2)
Cl10.035 (2)0.035 (1)0.072 (3)0.009 (1)0.004 (2)0.003 (2)
Cl20.030 (2)0.038 (2)0.069 (2)0.005 (1)0.003 (2)0.001 (2)
S0.038 (2)0.033 (1)0.036 (2)0.006 (2)0.006 (2)0.006 (1)
O10.029 (5)0.036 (4)0.053 (6)0.008 (4)0.004 (5)0.006 (5)
O20.054 (5)0.046 (4)0.038 (5)0.013 (4)0.016 (5)0.007 (4)
N0.023 (6)0.034 (5)0.047 (7)0.002 (5)0.006 (6)0.000 (5)
C10.025 (7)0.041 (7)0.07 (1)0.008 (6)0.002 (9)0.006 (8)
C20.042 (10)0.046 (9)0.07 (1)0.001 (8)0.012 (10)0.000 (8)
C30.06 (1)0.063 (9)0.049 (9)0.011 (9)0.019 (8)0.004 (9)
C40.06 (1)0.059 (8)0.023 (8)0.001 (8)0.004 (8)0.003 (7)
C50.06 (1)0.051 (8)0.07 (1)0.001 (8)0.037 (10)0.006 (8)
C60.08 (1)0.055 (7)0.052 (9)0.00 (1)0.00 (1)0.017 (7)
Geometric parameters (Å, º) top
Pt—Cl12.300 (3)N—H10.95
Pt—Cl22.294 (3)C1—H20.95
Pt—S2.230 (3)C1—H30.95
Pt—N2.067 (9)C2—H40.95
S—O21.480 (8)C3—H50.95
S—C51.79 (1)C4—H60.95
S—C61.78 (1)C4—H70.95
O1—N1.44 (1)C5—H80.95
O1—C11.44 (1)C5—H90.95
N—C41.48 (1)C5—H100.95
C1—C21.47 (2)C6—H110.95
C2—C31.33 (2)C6—H120.95
C3—C41.51 (2)C6—H130.95
Cl1—Pt—Cl2175.5 (1)C2—C1—H2109
Cl1—Pt—S90.4 (1)C2—C1—H3109
Cl1—Pt—N89.8 (3)H2—C1—H3109
Cl2—Pt—S93.7 (1)C1—C2—H4118
Cl2—Pt—N86.1 (3)C3—C2—H4118
S—Pt—N179.1 (3)C2—C3—H5120
Pt—S—O2115.7 (4)C4—C3—H5120
Pt—S—C5112.5 (4)N—C4—H6108
Pt—S—C6110.2 (5)N—C4—H7108
O2—S—C5108.2 (6)C3—C4—H6109
O2—S—C6108.3 (6)C3—C4—H7109
C5—S—C6100.8 (7)H6—C4—H7109
N—O1—C1111.5 (9)S—C5—H8109
Pt—N—O1109.9 (6)S—C5—H9109
Pt—N—C4115.2 (8)S—C5—H10109
O1—N—C4109 (1)H8—C5—H9110
O1—C1—C2112 (1)H8—C5—H10109
C1—C2—C3123 (1)H9—C5—H10110
C2—C3—C4119 (1)S—C6—H11109
N—C4—C3113 (1)S—C6—H12109
Pt—N—H1107S—C6—H13109
O1—N—H1108H11—C6—H12110
C4—N—H1107H11—C6—H13109
O1—C1—H2109H12—C6—H13110
O1—C1—H3109
Pt—N—O1—C1167.5 (7)Cl2—Pt—S—C6136.2 (6)
Pt—N—C4—C3170.9 (9)Cl2—Pt—N—O1126.3 (6)
Cl1—Pt—S—O277.5 (4)Cl2—Pt—N—C4110.2 (9)
Cl1—Pt—S—C5157.4 (6)O1—N—C4—C347 (1)
Cl1—Pt—S—C645.8 (6)O1—C1—C2—C314 (2)
Cl1—Pt—N—O155.6 (6)N—O1—C1—C248 (1)
Cl1—Pt—N—C467.9 (9)N—C4—C3—C214 (2)
Cl2—Pt—S—O2100.5 (4)C1—O1—N—C465 (1)
Cl2—Pt—S—C524.6 (6)C1—C2—C3—C42 (2)

Experimental details

(I)(II)
Crystal data
Chemical formula[PtCl2(C4H7NO)(C2H6OS)][PtCl2(C4H7NO)(C2H6OS)]
Mr429.23429.23
Crystal system, space groupTriclinic, P1Orthorhombic, Pbca
Temperature (K)296296
a, b, c (Å)8.177 (4), 8.517 (4), 10.297 (4)16.532 (3), 13.868 (2), 10.182 (4)
α, β, γ (°)105.84 (3), 104.42 (3), 111.16 (3)90, 90, 90
V3)593.2 (5)2334 (1)
Z28
Radiation typeMo KαMo Kα
µ (mm1)12.612.8
Crystal size (mm)0.25 × 0.12 × 0.100.30 × 0.10 × 0.03
Data collection
DiffractometerRigaku AFC6S
diffractometer
Rigaku AFC6S
diffractometer
Absorption correctionψ scan
(North et al., 1968)
ψ scan
(North et al., 1968)
Tmin, Tmax0.190, 0.2840.242, 0.681
No. of measured, independent and
observed [I > 3σ(I)] reflections
2249, 2089, 1820 2053, 2053, 1277
Rint0.0130.00
(sin θ/λ)max1)0.5950.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.026, 0.059, 2.23 0.032, 0.074, 1.71
No. of reflections20872049
No. of parameters118119
H-atom treatmentH-atom parameters not refinedH-atom parameters not refined
Δρmax, Δρmin (e Å3)0.73, 1.751.95, 2.09

Computer programs: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1988), MSC/AFC Diffractometer Control Software, TEXSAN (Molecular Structure Corporation, 1991), MITHRIL (Gilmore, 1983), TEXSAN, ORTEPII (Johnson, 1976).

Selected geometric parameters (Å, º) for (I) top
Pt—Cl12.310 (2)O1—N1.452 (7)
Pt—Cl22.325 (2)O1—C11.458 (9)
Pt—S2.207 (2)N—C41.480 (9)
Pt—N2.062 (6)C1—C21.49 (1)
S—O21.489 (5)C2—C31.32 (1)
S—C51.776 (9)C3—C41.47 (1)
S—C61.783 (8)
Cl1—Pt—Cl290.07 (8)Pt—S—C6111.2 (3)
Cl1—Pt—S91.08 (8)O2—S—C5107.9 (4)
Cl1—Pt—N179.4 (2)O2—S—C6108.9 (4)
Cl2—Pt—S178.61 (8)C5—S—C6102.7 (4)
Cl2—Pt—N90.1 (2)N—O1—C1110.2 (5)
S—Pt—N88.8 (2)Pt—N—O1109.8 (4)
Pt—S—O2113.8 (2)Pt—N—C4117.1 (5)
Pt—S—C5111.7 (3)O1—N—C4109.4 (5)
Selected geometric parameters (Å, º) for (II) top
Pt—Cl12.300 (3)O1—N1.44 (1)
Pt—Cl22.294 (3)O1—C11.44 (1)
Pt—S2.230 (3)N—C41.48 (1)
Pt—N2.067 (9)C1—C21.47 (2)
S—O21.480 (8)C2—C31.33 (2)
S—C51.79 (1)C3—C41.51 (2)
S—C61.78 (1)
Cl1—Pt—Cl2175.5 (1)Pt—S—C6110.2 (5)
Cl1—Pt—S90.4 (1)O2—S—C5108.2 (6)
Cl1—Pt—N89.8 (3)O2—S—C6108.3 (6)
Cl2—Pt—S93.7 (1)C5—S—C6100.8 (7)
Cl2—Pt—N86.1 (3)N—O1—C1111.5 (9)
S—Pt—N179.1 (3)Pt—N—O1109.9 (6)
Pt—S—O2115.7 (4)Pt—N—C4115.2 (8)
Pt—S—C5112.5 (4)O1—N—C4109 (1)
 

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