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The crystal structure of the title compound, [PtCl2(C25H22NPS)]·0.5CH2Cl2, was determined to establish the coordination properties of the (phosphan­yl)benzyl­idene–methanamine ligand to platinum. In the unit cell two mol­ecules of cis-[PtCl2(C25H22NPS)] are accompanied by a dichloro­methane solvent mol­ecule. The square-planar Pt2+ coordination sphere is slightly distorted with the bidentate ligand coordinated via the P and the amine N atoms, and the Cl atoms located cis at the two remaining coordination sites. Parts of the thiophene ring and the solvate molecule were modeled as disordered with occupancy ratios of 0.55 (2):0.45 (2) and 0.302 (10):0.198 (10), respectively. Weak C—H...Cl inter­actions stabilize the crystal packing.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536811056108/nr2014sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536811056108/nr2014Isup2.hkl
Contains datablock I

CCDC reference: 867951

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C) = 0.006 Å
  • Disorder in main residue
  • R factor = 0.028
  • wR factor = 0.058
  • Data-to-parameter ratio = 19.8

checkCIF/PLATON results

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Alert level C PLAT042_ALERT_1_C Calc. and Reported MoietyFormula Strings Differ ? PLAT045_ALERT_1_C Calculated and Reported Z Differ by ............ 0.25 Ratio PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 3.4 Ratio PLAT910_ALERT_3_C Missing # of FCF Reflections Below Th(Min) ..... 1 PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.600 7 PLAT912_ALERT_4_C Missing # of FCF Reflections Above STh/L= 0.600 8 PLAT913_ALERT_3_C Missing # of Very Strong Reflections in FCF .... 1
Alert level G PLAT002_ALERT_2_G Number of Distance or Angle Restraints on AtSite 14 PLAT003_ALERT_2_G Number of Uiso or Uij Restrained Atom Sites .... 9 PLAT005_ALERT_5_G No _iucr_refine_instructions_details in CIF .... ? PLAT244_ALERT_4_G Low 'Solvent' Ueq as Compared to Neighbors of C26A PLAT244_ALERT_4_G Low 'Solvent' Ueq as Compared to Neighbors of C26B PLAT301_ALERT_3_G Note: Main Residue Disorder ................... 10 Perc. PLAT302_ALERT_4_G Note: Anion/Solvent Disorder ................... 100 Perc. PLAT432_ALERT_2_G Short Inter X...Y Contact C2A .. C2A .. 3.18 Ang. PLAT811_ALERT_5_G No ADDSYM Analysis: Too Many Excluded Atoms .... ! PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 146
0 ALERT level A = Most likely a serious problem - resolve or explain 0 ALERT level B = A potentially serious problem, consider carefully 7 ALERT level C = Check. Ensure it is not caused by an omission or oversight 10 ALERT level G = General information/check it is not something unexpected 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 4 ALERT type 2 Indicator that the structure model may be wrong or deficient 5 ALERT type 3 Indicator that the structure quality may be low 4 ALERT type 4 Improvement, methodology, query or suggestion 2 ALERT type 5 Informative message, check

Comment top

Platinum complexes with (phosphanyl)benzylidene-methanamine ligands have been used as catalysts or catalyst precursors for a variety of organic reactions. Our group and others have recently been interested in these types of complexes and have reported several of these types of complexes (Chiririwa et al., 2011; Chiririwa & Meijboom, 2011a, 2011b, 2011c; Ghilardi et al., 1992; Sanchez et al., (1998, 2001) and Coleman et al., 2001).

The title compound (see Fig. 1) crystallize with a dichloromethane solvate, disordered over an inversion center, for each pair of cis-[PtCl2(C25H21NSP)] molecules. The square planar Pt coordination sphere is slightly distorted (Pt1 displaced -0.0275 (7)) Å from the plane formed by Pt1, P1, N1, Cl1 and Cl2 respectively; r.m.s. deviation of fitted atoms = 0.0423 Å). The distortion is featured most prominently in the N1—Pt1—P1 angle of 86.17 (10)° versus. Cl1—Pt1—Cl2 = 89.08 (4)°, indicating some ring strain induced by the chelation of the bidentate ligand. The average Pt—N and Pt—P bond lengths of 2.030 (3) and 2.2089 (9) Å, respectively are in the range expected for similar platinum(II) complexes (Ankersmit et al.(1996)). The initial refinement model of the compound showed some large displacement parameters for the thiophene moiety as well as the dichloromethane solvent. These disorders were elucidated to give an improved model (details can be found under the experimental refinement section). Two weak C—H···Cl interactions (Steiner, 1996) aid in the stabilization of the crystal structure (see Table 1, Fig. 2).

Related literature top

For background to related structures, see: Chiririwa et al. (2011); Chiririwa & Meijboom (2011a,b,c); Ghilardi et al. (1992); Sanchez et al. (1998, 2001); Coleman et al. (2001). For Pt—N and Pt—P bond lengths in similar platinum(II) complexes, see: Ankersmit et al. (1996). For background to weak hydrogen-bonding interactions, see Steiner (1996).

Experimental top

To a dry CH2Cl2 (10 ml) solution of the precursor [Pt(COD)Cl2] was added an equimolar amount of (2-(diphenylphosphanyl) benzylidene)(thiophen-2-yl)methanamine in CH2Cl2 (10 ml), and stirred at room temperature for 2 hrs. The solvent was reduced and the complex precipitated out on addition of hexane, filtered off, washed with Et2O (2×5 ml) and dried under vacuum for 4 hrs affording a yellow precipitate in 72% yield. Crystals suitable for X-ray structure determination were obtained by recrystallization form a CH2Cl2-hexane mixture at room temperature.

Refinement top

All hydrogen atoms were positioned in geometrically idealized positions with C—H = 0.99 Å and 0.95 Å for methylene and aromatic H atoms respectively. All hydrogen atoms were allowed to ride on their parent atoms with Uiso(H) = 1.2Ueq. A disorder refinement model was applied to the thiophene that showed large displacements at C2, C3 and S1. Geometrical (FLAT) restraints were applied to keep the rings C1, C2A/B, C3A/B, C4, S1A/B planar. Ellipsoid displacement (SIMU and DELU) restraints were also applied to the disordered moiety. The occupation parameters of the two disordered tiophene fragments were linked to a free variable so that the two sites add to unity. This showed a distribution of 0.54903:0.45097., The dichloromethane solvate was also refined as disordered on two positions in the asymmetric unit. This resulted in four disordered positions for each dichloromethane at each solvent accessible site in the crystal lattice. The occupancies of these sites were linked to a free variable to add to unity and refined to a ratio of 0.60331:0.39669 (based on the asymmetric unit fraction). To keep refinement stable geometrical (DIFX and DANG) restraints were applied to the C—Cl bonds and Cl···Cl distances All the above restraints were applied with the default standard deviations. The atoms of the solvate molecule was left isotropic due to the extensive nature of the disorder. The highest residual electron density of 0.84 e.Å-3 is 0.89 Å from Pt1 representing no physical meaning.

Computing details top

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT and XPREP (Bruker, 2007); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2005); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. View of title compound showing displacement ellipsoids (drawn at a 30% probability level) and labeling. For clarity: a) hydrogen atoms omitted, b) bonds in part B of the disordered thiophene indicated with dotted lines, and c) minor component as well as symmetry generated disordered parts of dichloromethane created by inversion center omitted.
[Figure 2] Fig. 2. Partial packing diagram of title compound to illustrate the weak hydrogen bonding stabilizing crystal packing. All disordered components omitted for clarity.
Dichlorido{N-[2-(diphenylphosphanyl)benzylidene]-2-(thiophen-2- yl)ethanamine-κ2P,N}platinum(II) dichloromethane hemisolvate top
Crystal data top
[PtCl2(C25H22NPS)]·0.5CH2Cl2F(000) = 1372
Mr = 707.92Dx = 1.842 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 5962 reflections
a = 9.9635 (7) Åθ = 2.6–28.2°
b = 19.0185 (14) ŵ = 5.97 mm1
c = 16.0155 (9) ÅT = 173 K
β = 122.751 (3)°Block, yellow
V = 2552.3 (3) Å30.08 × 0.05 × 0.03 mm
Z = 4
Data collection top
Bruker APEXII 4K-CCD
diffractometer
6593 independent reflections
Graphite monochromator5165 reflections with I > 2σ(I)
Detector resolution: 8.4 pixels mm-1Rint = 0.052
ϕ and ω scansθmax = 28.7°, θmin = 2.1°
Absorption correction: multi-scan
(SADABS; Bruker, 2007)
h = 1313
Tmin = 0.647, Tmax = 0.841k = 2525
30158 measured reflectionsl = 2121
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)] = 0.028Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.058H-atom parameters constrained
S = 1.01 w = 1/[σ2(Fo2) + (0.0216P)2 + 0.6014P]
where P = (Fo2 + 2Fc2)/3
6593 reflections(Δ/σ)max = 0.002
333 parametersΔρmax = 0.84 e Å3
146 restraintsΔρmin = 0.62 e Å3
Crystal data top
[PtCl2(C25H22NPS)]·0.5CH2Cl2V = 2552.3 (3) Å3
Mr = 707.92Z = 4
Monoclinic, P21/cMo Kα radiation
a = 9.9635 (7) ŵ = 5.97 mm1
b = 19.0185 (14) ÅT = 173 K
c = 16.0155 (9) Å0.08 × 0.05 × 0.03 mm
β = 122.751 (3)°
Data collection top
Bruker APEXII 4K-CCD
diffractometer
6593 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2007)
5165 reflections with I > 2σ(I)
Tmin = 0.647, Tmax = 0.841Rint = 0.052
30158 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.028146 restraints
wR(F2) = 0.058H-atom parameters constrained
S = 1.01Δρmax = 0.84 e Å3
6593 reflectionsΔρmin = 0.62 e Å3
333 parameters
Special details top

Experimental. The intensity data was collected on a Bruker Apex-II 4 K CCD diffractometer using an exposure time of 80 s/frame. A total of 1315 frames were collected with a frame width of 0.5° covering up to θ = 28.72° with 99.8% completeness accomplished.

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Pt10.557569 (15)0.701063 (7)0.420321 (11)0.02063 (4)
Cl10.38212 (12)0.79833 (5)0.36520 (9)0.0382 (2)
Cl20.57723 (11)0.70634 (5)0.56946 (7)0.0318 (2)
P10.73311 (10)0.61536 (5)0.46437 (7)0.01889 (18)
N10.5342 (4)0.69787 (16)0.2864 (2)0.0278 (7)
C10.1129 (5)0.6300 (2)0.1049 (3)0.0385 (10)
C2A0.0513 (10)0.5796 (8)0.0305 (9)0.056 (4)0.55 (2)
H2A0.11370.54370.02640.067*0.55 (2)
C3A0.1149 (10)0.5875 (9)0.0387 (9)0.056 (4)0.55 (2)
H3A0.17580.55780.09470.067*0.55 (2)
S1A0.0359 (10)0.6794 (6)0.0932 (7)0.060 (2)0.55 (2)
C2B0.0654 (13)0.6113 (12)0.0100 (8)0.069 (5)0.45 (2)
H2B0.1360.59340.00760.083*0.45 (2)
C3B0.0994 (13)0.6213 (13)0.0587 (8)0.060 (5)0.45 (2)
H3B0.15010.61360.12810.072*0.45 (2)
S1B0.0452 (11)0.6648 (7)0.1052 (7)0.0434 (19)0.45 (2)
C40.1785 (5)0.6432 (3)0.0158 (3)0.0511 (12)
H4A0.2860.65880.05530.061*0.45 (2)
H4B0.29120.64610.04840.061*0.55 (2)
C50.2814 (5)0.6328 (2)0.1939 (3)0.0382 (10)
H5A0.34040.59120.19320.046*
H5B0.27950.63060.2550.046*
C60.3689 (5)0.6990 (2)0.1964 (3)0.0369 (10)
H6A0.37280.70150.1360.044*
H6B0.31150.7410.19790.044*
C70.6488 (5)0.6932 (2)0.2717 (3)0.0318 (9)
H70.62030.69550.20470.038*
C80.8184 (5)0.68468 (19)0.3477 (3)0.0272 (8)
C90.8769 (4)0.64993 (18)0.4383 (3)0.0229 (8)
C101.0409 (4)0.64245 (19)0.5044 (3)0.0267 (8)
H101.08090.61810.56520.032*
C111.1464 (5)0.6705 (2)0.4817 (3)0.0345 (10)
H111.25810.66620.5280.041*
C121.0910 (5)0.7042 (2)0.3935 (4)0.0422 (11)
H121.16390.7230.37840.051*
C130.9267 (5)0.7108 (2)0.3254 (3)0.0365 (10)
H130.88820.73320.26350.044*
C140.8472 (4)0.58128 (18)0.5904 (3)0.0209 (7)
C150.9314 (4)0.6271 (2)0.6700 (3)0.0273 (8)
H150.92950.67620.65860.033*
C161.0187 (5)0.6010 (2)0.7665 (3)0.0341 (9)
H161.07630.63230.82080.041*
C171.0217 (5)0.5291 (2)0.7835 (3)0.0331 (9)
H171.07990.51140.84950.04*
C180.9395 (5)0.4836 (2)0.7041 (3)0.0302 (9)
H180.9430.43440.71560.036*
C190.8526 (4)0.50892 (19)0.6080 (3)0.0246 (8)
H190.79640.47730.55380.029*
C200.6463 (4)0.53857 (17)0.3865 (3)0.0201 (7)
C210.7114 (4)0.50677 (19)0.3381 (3)0.0255 (8)
H210.80310.52650.34320.031*
C220.6429 (5)0.4463 (2)0.2825 (3)0.0306 (9)
H220.68850.42460.250.037*
C230.5093 (5)0.4177 (2)0.2741 (3)0.0318 (9)
H230.4630.37620.23610.038*
C240.4419 (4)0.44923 (19)0.3211 (3)0.0288 (9)
H240.34940.42950.3150.035*
C250.5098 (4)0.50953 (18)0.3769 (3)0.0234 (8)
H250.46330.53130.40880.028*
C26A0.485 (3)0.5266 (10)0.0366 (13)0.070 (6)*0.302 (10)
H26A0.51870.56560.06250.084*0.302 (10)
H26B0.36930.52030.08430.084*0.302 (10)
Cl3A0.5086 (19)0.5549 (5)0.0677 (8)0.099 (3)*0.302 (10)
Cl4A0.5746 (14)0.4531 (5)0.0434 (8)0.121 (4)*0.302 (10)
C26B0.564 (3)0.5398 (9)0.0142 (17)0.047 (7)*0.198 (10)
H26C0.65720.55020.01850.057*0.198 (10)
H26D0.46760.56120.0720.057*0.198 (10)
Cl3B0.591 (3)0.5697 (8)0.0906 (11)0.122 (5)*0.198 (10)
Cl4B0.5390 (15)0.4497 (6)0.0105 (12)0.090 (4)*0.198 (10)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pt10.01969 (7)0.01735 (7)0.02733 (8)0.00077 (6)0.01435 (6)0.00296 (7)
Cl10.0329 (5)0.0267 (5)0.0624 (7)0.0114 (4)0.0307 (5)0.0171 (5)
Cl20.0343 (5)0.0353 (5)0.0322 (5)0.0034 (4)0.0221 (4)0.0041 (4)
P10.0200 (4)0.0179 (4)0.0209 (5)0.0001 (3)0.0125 (4)0.0013 (4)
N10.0254 (16)0.0288 (17)0.0290 (18)0.0021 (14)0.0145 (14)0.0078 (15)
C10.030 (2)0.057 (3)0.022 (2)0.0020 (19)0.0097 (17)0.0003 (19)
C2A0.026 (4)0.097 (9)0.036 (6)0.011 (5)0.011 (4)0.024 (6)
C3A0.027 (4)0.096 (9)0.029 (6)0.004 (5)0.005 (4)0.022 (6)
S1A0.048 (2)0.036 (3)0.068 (4)0.0109 (17)0.012 (2)0.009 (2)
C2B0.033 (5)0.141 (14)0.029 (6)0.006 (8)0.014 (4)0.018 (8)
C3B0.038 (6)0.113 (13)0.020 (5)0.002 (7)0.009 (4)0.006 (7)
S1B0.042 (2)0.051 (5)0.033 (2)0.013 (2)0.0175 (18)0.005 (2)
C40.033 (2)0.059 (3)0.040 (3)0.009 (2)0.006 (2)0.002 (2)
C50.030 (2)0.041 (2)0.028 (2)0.0028 (18)0.0059 (18)0.0048 (19)
C60.030 (2)0.046 (3)0.026 (2)0.0025 (19)0.0096 (18)0.013 (2)
C70.039 (2)0.030 (2)0.032 (2)0.0017 (18)0.0224 (19)0.0090 (18)
C80.032 (2)0.024 (2)0.036 (2)0.0011 (15)0.0254 (19)0.0005 (16)
C90.0273 (19)0.0202 (18)0.028 (2)0.0018 (15)0.0195 (17)0.0026 (16)
C100.0253 (19)0.027 (2)0.030 (2)0.0024 (15)0.0171 (18)0.0036 (17)
C110.026 (2)0.031 (2)0.051 (3)0.0060 (17)0.024 (2)0.010 (2)
C120.041 (2)0.035 (2)0.071 (3)0.004 (2)0.044 (3)0.003 (2)
C130.045 (3)0.031 (2)0.051 (3)0.0018 (18)0.038 (2)0.012 (2)
C140.0195 (17)0.0241 (18)0.0217 (19)0.0019 (14)0.0129 (15)0.0023 (15)
C150.0240 (19)0.027 (2)0.026 (2)0.0034 (15)0.0108 (17)0.0019 (16)
C160.029 (2)0.041 (2)0.022 (2)0.0067 (18)0.0081 (17)0.0068 (19)
C170.029 (2)0.046 (3)0.022 (2)0.0037 (18)0.0123 (18)0.0061 (19)
C180.033 (2)0.027 (2)0.029 (2)0.0060 (17)0.0162 (18)0.0084 (17)
C190.029 (2)0.0231 (19)0.023 (2)0.0015 (15)0.0149 (17)0.0030 (15)
C200.0224 (17)0.0174 (17)0.0195 (18)0.0007 (14)0.0107 (15)0.0001 (14)
C210.0245 (19)0.029 (2)0.025 (2)0.0007 (16)0.0151 (17)0.0014 (16)
C220.034 (2)0.033 (2)0.024 (2)0.0030 (17)0.0154 (18)0.0066 (17)
C230.031 (2)0.0207 (19)0.031 (2)0.0014 (16)0.0092 (18)0.0039 (17)
C240.026 (2)0.025 (2)0.031 (2)0.0041 (16)0.0123 (17)0.0000 (17)
C250.0268 (19)0.0220 (18)0.027 (2)0.0008 (15)0.0179 (16)0.0008 (16)
Geometric parameters (Å, º) top
Pt1—N12.029 (3)C10—H100.95
Pt1—P12.2087 (9)C11—C121.367 (6)
Pt1—Cl22.2907 (10)C11—H110.95
Pt1—Cl12.3638 (9)C12—C131.397 (6)
P1—C201.808 (4)C12—H120.95
P1—C141.818 (4)C13—H130.95
P1—C91.818 (4)C14—C151.390 (5)
N1—C71.288 (5)C14—C191.400 (5)
N1—C61.490 (5)C15—C161.391 (5)
C1—C2B1.373 (11)C15—H150.95
C1—C2A1.388 (10)C16—C171.391 (6)
C1—C51.504 (5)C16—H160.95
C1—S1A1.678 (9)C17—C181.383 (5)
C1—S1B1.711 (9)C17—H170.95
C2A—C3A1.416 (9)C18—C191.381 (5)
C2A—H2A0.95C18—H180.95
C3A—C41.382 (10)C19—H190.95
C3A—H3A0.95C20—C211.389 (5)
S1A—C41.690 (9)C20—C251.397 (5)
C2B—C3B1.410 (11)C21—C221.387 (5)
C2B—H2B0.95C21—H210.95
C3B—C41.362 (11)C22—C231.376 (5)
C3B—H3B0.95C22—H220.95
S1B—C41.704 (10)C23—C241.386 (5)
C4—H4A0.95C23—H230.95
C4—H4B0.95C24—C251.385 (5)
C5—C61.519 (5)C24—H240.95
C5—H5A0.99C25—H250.95
C5—H5B0.99C26A—Cl3A1.647 (16)
C6—H6A0.99C26A—Cl4A1.692 (15)
C6—H6B0.99C26A—H26A0.99
C7—C81.462 (6)C26A—H26B0.99
C7—H70.95C26B—Cl3B1.648 (16)
C8—C131.397 (5)C26B—Cl4B1.737 (16)
C8—C91.403 (5)C26B—H26C0.99
C9—C101.393 (5)C26B—H26D0.99
C10—C111.391 (5)
N1—Pt1—P186.20 (9)C13—C8—C7116.9 (4)
N1—Pt1—Cl2178.38 (9)C9—C8—C7124.0 (3)
P1—Pt1—Cl295.34 (3)C10—C9—C8119.6 (3)
N1—Pt1—Cl189.42 (9)C10—C9—P1122.3 (3)
P1—Pt1—Cl1174.06 (3)C8—C9—P1118.1 (3)
Cl2—Pt1—Cl189.08 (4)C11—C10—C9120.3 (4)
C20—P1—C14104.86 (16)C11—C10—H10119.9
C20—P1—C9106.01 (16)C9—C10—H10119.9
C14—P1—C9106.69 (16)C12—C11—C10120.7 (4)
C20—P1—Pt1112.03 (12)C12—C11—H11119.7
C14—P1—Pt1121.94 (11)C10—C11—H11119.7
C9—P1—Pt1104.23 (12)C11—C12—C13119.7 (4)
C7—N1—C6116.7 (3)C11—C12—H12120.1
C7—N1—Pt1126.1 (3)C13—C12—H12120.1
C6—N1—Pt1117.2 (2)C8—C13—C12120.6 (4)
C2B—C1—C5126.7 (6)C8—C13—H13119.7
C2A—C1—C5125.9 (5)C12—C13—H13119.7
C2B—C1—S1A105.5 (6)C15—C14—C19119.6 (3)
C2A—C1—S1A109.7 (5)C15—C14—P1120.0 (3)
C5—C1—S1A123.5 (4)C19—C14—P1120.4 (3)
C2B—C1—S1B109.7 (6)C14—C15—C16119.9 (4)
C2A—C1—S1B106.8 (5)C14—C15—H15120
C5—C1—S1B122.8 (4)C16—C15—H15120
C1—C2A—C3A112.6 (7)C17—C16—C15120.2 (4)
C1—C2A—H2A123.7C17—C16—H16119.9
C3A—C2A—H2A123.7C15—C16—H16119.9
C4—C3A—C2A112.6 (7)C18—C17—C16119.7 (4)
C4—C3A—H3A123.7C18—C17—H17120.1
C2A—C3A—H3A123.7C16—C17—H17120.1
C1—S1A—C494.9 (5)C19—C18—C17120.5 (4)
C1—C2B—C3B112.8 (8)C19—C18—H18119.7
C1—C2B—H2B123.6C17—C18—H18119.7
C3B—C2B—H2B123.6C18—C19—C14120.0 (4)
C4—C3B—C2B113.3 (8)C18—C19—H19120
C4—C3B—H3B123.4C14—C19—H19120
C2B—C3B—H3B123.4C21—C20—C25119.1 (3)
C4—S1B—C193.2 (4)C21—C20—P1122.9 (3)
C3B—C4—S1A104.7 (6)C25—C20—P1118.0 (3)
C3A—C4—S1A109.6 (5)C22—C21—C20120.2 (3)
C3B—C4—S1B109.9 (6)C22—C21—H21119.9
C3A—C4—S1B107.4 (5)C20—C21—H21119.9
C3B—C4—H4A120.7C23—C22—C21120.3 (4)
C3A—C4—H4A125.2C23—C22—H22119.9
S1A—C4—H4A125.2C21—C22—H22119.9
S1B—C4—H4A126C22—C23—C24120.2 (4)
C3B—C4—H4B125.1C22—C23—H23119.9
C3A—C4—H4B118.3C24—C23—H23119.9
S1A—C4—H4B128.9C25—C24—C23119.8 (4)
S1B—C4—H4B125C25—C24—H24120.1
C1—C5—C6112.6 (3)C23—C24—H24120.1
C1—C5—H5A109.1C24—C25—C20120.4 (3)
C6—C5—H5A109.1C24—C25—H25119.8
C1—C5—H5B109.1C20—C25—H25119.8
C6—C5—H5B109.1Cl3A—C26A—Cl4A123.0 (11)
H5A—C5—H5B107.8Cl3A—C26A—H26A106.6
N1—C6—C5109.4 (3)Cl4A—C26A—H26A106.6
N1—C6—H6A109.8Cl3A—C26A—H26B106.6
C5—C6—H6A109.8Cl4A—C26A—H26B106.6
N1—C6—H6B109.8H26A—C26A—H26B106.6
C5—C6—H6B109.8Cl3B—C26B—Cl4B104.7 (12)
H6A—C6—H6B108.2Cl3B—C26B—H26C110.8
N1—C7—C8126.5 (4)Cl4B—C26B—H26C110.8
N1—C7—H7116.7Cl3B—C26B—H26D110.8
C8—C7—H7116.7Cl4B—C26B—H26D110.8
C13—C8—C9119.1 (4)H26C—C26B—H26D108.9
N1—Pt1—P1—C2059.67 (15)Pt1—N1—C7—C84.2 (6)
Cl2—Pt1—P1—C20119.82 (12)N1—C7—C8—C13152.5 (4)
N1—Pt1—P1—C14174.99 (16)N1—C7—C8—C930.0 (6)
Cl2—Pt1—P1—C145.52 (14)C13—C8—C9—C100.3 (5)
N1—Pt1—P1—C954.51 (15)C7—C8—C9—C10177.7 (4)
Cl2—Pt1—P1—C9126.00 (13)C13—C8—C9—P1179.1 (3)
P1—Pt1—N1—C743.9 (3)C7—C8—C9—P11.7 (5)
Cl1—Pt1—N1—C7132.1 (3)C20—P1—C9—C10105.8 (3)
P1—Pt1—N1—C6134.3 (3)C14—P1—C9—C105.6 (3)
Cl1—Pt1—N1—C649.8 (3)Pt1—P1—C9—C10135.8 (3)
C2B—C1—C2A—C3A82.1 (14)C20—P1—C9—C873.6 (3)
C5—C1—C2A—C3A174.8 (7)C14—P1—C9—C8175.0 (3)
S1A—C1—C2A—C3A5.3 (10)Pt1—P1—C9—C844.7 (3)
S1B—C1—C2A—C3A18.3 (10)C8—C9—C10—C111.3 (5)
C1—C2A—C3A—C40.7 (12)P1—C9—C10—C11179.3 (3)
C2B—C1—S1A—C425.5 (9)C9—C10—C11—C121.6 (6)
C2A—C1—S1A—C46.6 (7)C10—C11—C12—C130.2 (6)
C5—C1—S1A—C4176.4 (4)C9—C8—C13—C121.8 (6)
S1B—C1—S1A—C486 (3)C7—C8—C13—C12179.3 (4)
C2A—C1—C2B—C3B86.2 (15)C11—C12—C13—C81.5 (6)
C5—C1—C2B—C3B173.5 (9)C20—P1—C14—C15179.5 (3)
S1A—C1—C2B—C3B16.4 (13)C9—P1—C14—C1567.3 (3)
S1B—C1—C2B—C3B3.8 (12)Pt1—P1—C14—C1552.0 (3)
C1—C2B—C3B—C43.9 (16)C20—P1—C14—C190.4 (3)
C2B—C1—S1B—C48.0 (9)C9—P1—C14—C19111.8 (3)
C2A—C1—S1B—C424.5 (8)Pt1—P1—C14—C19128.9 (2)
C5—C1—S1B—C4178.2 (4)C19—C14—C15—C160.9 (5)
S1A—C1—S1B—C481 (2)P1—C14—C15—C16180.0 (3)
C2B—C3B—C4—C3A81.7 (14)C14—C15—C16—C170.1 (6)
C2B—C3B—C4—S1A21.9 (13)C15—C16—C17—C181.0 (6)
C2B—C3B—C4—S1B9.7 (15)C16—C17—C18—C191.0 (6)
C2A—C3A—C4—C3B82.5 (13)C17—C18—C19—C140.1 (6)
C2A—C3A—C4—S1A4.1 (11)C15—C14—C19—C180.9 (5)
C2A—C3A—C4—S1B17.4 (11)P1—C14—C19—C18180.0 (3)
C1—S1A—C4—C3B27.5 (9)C14—P1—C20—C2198.8 (3)
C1—S1A—C4—C3A6.2 (8)C9—P1—C20—C2113.8 (4)
C1—S1A—C4—S1B88 (2)Pt1—P1—C20—C21126.9 (3)
C1—S1B—C4—C3B10.1 (10)C14—P1—C20—C2579.7 (3)
C1—S1B—C4—C3A24.2 (8)C9—P1—C20—C25167.6 (3)
C1—S1B—C4—S1A78 (2)Pt1—P1—C20—C2554.5 (3)
C2B—C1—C5—C679.4 (13)C25—C20—C21—C221.1 (5)
C2A—C1—C5—C6118.0 (10)P1—C20—C21—C22177.5 (3)
S1A—C1—C5—C673.9 (8)C20—C21—C22—C230.5 (6)
S1B—C1—C5—C689.1 (7)C21—C22—C23—C240.2 (6)
C7—N1—C6—C5113.9 (4)C22—C23—C24—C250.3 (6)
Pt1—N1—C6—C564.4 (4)C23—C24—C25—C200.3 (6)
C1—C5—C6—N1179.9 (4)C21—C20—C25—C241.0 (5)
C6—N1—C7—C8174.0 (4)P1—C20—C25—C24177.6 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C7—H7···Cl2i0.952.713.486 (4)139
C12—H12···Cl1ii0.952.713.639 (4)168
Symmetry codes: (i) x, y+3/2, z1/2; (ii) x+1, y, z.

Experimental details

Crystal data
Chemical formula[PtCl2(C25H22NPS)]·0.5CH2Cl2
Mr707.92
Crystal system, space groupMonoclinic, P21/c
Temperature (K)173
a, b, c (Å)9.9635 (7), 19.0185 (14), 16.0155 (9)
β (°) 122.751 (3)
V3)2552.3 (3)
Z4
Radiation typeMo Kα
µ (mm1)5.97
Crystal size (mm)0.08 × 0.05 × 0.03
Data collection
DiffractometerBruker APEXII 4K-CCD
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2007)
Tmin, Tmax0.647, 0.841
No. of measured, independent and
observed [I > 2σ(I)] reflections
30158, 6593, 5165
Rint0.052
(sin θ/λ)max1)0.676
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.028, 0.058, 1.01
No. of reflections6593
No. of parameters333
No. of restraints146
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.84, 0.62

Computer programs: APEX2 (Bruker, 2007), SAINT (Bruker, 2007), SAINT and XPREP (Bruker, 2007), SIR97 (Altomare et al., 1999), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg & Putz, 2005), WinGX (Farrugia, 1999).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C7—H7···Cl2i0.952.713.486 (4)139
C12—H12···Cl1ii0.952.713.639 (4)167.5
Symmetry codes: (i) x, y+3/2, z1/2; (ii) x+1, y, z.
 

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