Literature DB >> 24109273

Dichloridobis[3-(4-chloro-phen-yl)-2,N,N-trimethyl-2,3-di-hydro-1,2,4-oxa-diazole-5-amine-κN (4)]platinum(II)-4-chloro-benzaldehyde (1/1).

Andreii S Kritchenkov1, Vladislav V Gurzhiy, Nadezhda A Bokach, Valentina A Kalibabchuk.   

Abstract

In the title 1:1 co-crystal, [PtCl2(C11H14ClN3O)2]·C7H5ClO, the coordination polyhedron of the Pt(II) atom is slightly distorted square-planar with the chloride and 2,3-di-hydro-1,2,4-oxa-diazole ligands mutually trans, as the Pt atom lies on an inversion center. The 4-chloro-benzaldehyde mol-ecules are statistically disordered about an inversion centre with equal occupancies for the two positions. The Pt(II) complex forms a three-dimensional structure through C-H⋯Cl and weaker C-H⋯O inter-actions with the 4-chloro-benzaldehyde mol-ecule.

Entities:  

Year:  2013        PMID: 24109273      PMCID: PMC3793686          DOI: 10.1107/S1600536813017376

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For the synthesis of platinum complexes with 2,3-di­hydro-1,2,4-oxa­diazole ligands, see: Bokach et al. (2011 ▶); Kritchenkov et al. (2011 ▶). For related structures, see: Bokach et al. (2003 ▶, 2011 ▶); Kritchenkov et al. (2011 ▶); Bokach & Kukushkin (2006 ▶); Gushchin et al. (2008 ▶); Kuznetsov & Kukushkin (2006 ▶); Fritsky et al. (2006 ▶); Penkova et al. (2009 ▶). For standard bond lengths, see: see: Allen et al. (1987 ▶).

Experimental

Crystal data

[PtCl2(C11H15ClN3O)2]·C7H5ClO M = 887.97 Triclinic, a = 8.46436 (18) Å b = 9.38481 (19) Å c = 11.4373 (3) Å α = 101.0381 (18)° β = 104.9553 (19)° γ = 96.3847 (17)° V = 849.07 (3) Å3 Z = 1 Mo Kα radiation μ = 4.57 mm−1 T = 100 K 0.17 × 0.11 × 0.09 mm

Data collection

Agilent Xcalibur Eos diffractometer Absorption correction: multi-scan (DENZO/SCALEPACK; Otwinowski & Minor, 1997 ▶) T min = 0.933, T max = 1.000 13908 measured reflections 3892 independent reflections 3888 reflections with I > 2σ(I) R int = 0.036

Refinement

R[F 2 > 2σ(F 2)] = 0.022 wR(F 2) = 0.054 S = 1.06 3892 reflections 211 parameters H-atom parameters constrained Δρmax = 1.63 e Å−3 Δρmin = −1.21 e Å−3 Data collection: CrysAlis PRO (Agilent, 2012 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SIR2004 (Burla et al., 2005 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: OLEX2 (Dolomanov et al., 2009 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813017376/sj5329sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813017376/sj5329Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[PtCl2(C11H15ClN3O)2]·C7H5ClOZ = 1
Mr = 887.97F(000) = 438
Triclinic, P1Dx = 1.737 Mg m3
a = 8.46436 (18) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.38481 (19) ÅCell parameters from 9801 reflections
c = 11.4373 (3) Åθ = 2.5–31.7°
α = 101.0381 (18)°µ = 4.57 mm1
β = 104.9553 (19)°T = 100 K
γ = 96.3847 (17)°Prism, colourless
V = 849.07 (3) Å30.17 × 0.11 × 0.09 mm
Agilent Xcalibur Eos diffractometer3892 independent reflections
Radiation source: Enhance (Mo) X-ray Source3888 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.036
Detector resolution: 16.2096 pixels mm-1θmax = 27.5°, θmin = 2.5°
ω scansh = −10→10
Absorption correction: multi-scan (DENZO/SCALEPACK; Otwinowski & Minor, 1997)k = −12→12
Tmin = 0.933, Tmax = 1.000l = −14→14
13908 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.022Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.054H-atom parameters constrained
S = 1.06w = 1/[σ2(Fo2) + (0.0326P)2] where P = (Fo2 + 2Fc2)/3
3892 reflections(Δ/σ)max < 0.001
211 parametersΔρmax = 1.63 e Å3
0 restraintsΔρmin = −1.21 e Å3
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.
Refinement. Refinement of F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > 2sigma(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/UeqOcc. (<1)
Pt10.50000.50000.00000.01562 (5)
O10.8747 (3)0.5755 (3)0.34126 (19)0.0321 (5)
N20.9212 (3)0.4486 (3)0.2650 (2)0.0290 (6)
H20.99720.47860.22730.035*
C30.7596 (4)0.3810 (3)0.1742 (3)0.0243 (6)
H30.69360.32030.21120.029*
N40.6856 (3)0.5130 (3)0.1552 (2)0.0209 (5)
C50.7499 (4)0.6134 (3)0.2577 (3)0.0240 (6)
N60.7135 (3)0.7450 (3)0.2956 (2)0.0281 (6)
C70.5711 (4)0.8001 (4)0.2268 (3)0.0334 (7)
H7A0.60500.85520.17230.050*
H7B0.52930.86270.28430.050*
H7C0.48560.71860.17880.050*
C80.8131 (5)0.8425 (4)0.4142 (3)0.0451 (10)
H8A0.76420.82720.47880.068*
H8B0.81630.94320.40770.068*
H8C0.92390.82090.43380.068*
C90.9849 (5)0.3574 (4)0.3496 (3)0.0452 (10)
H9A1.08130.41290.41340.068*
H9B1.01420.27210.30450.068*
H9C0.90120.32720.38690.068*
C100.7869 (4)0.2884 (3)0.0606 (3)0.0230 (6)
C110.7575 (5)0.1367 (4)0.0400 (3)0.0342 (7)
H110.71560.09190.09410.041*
C120.7907 (5)0.0506 (4)−0.0617 (3)0.0434 (9)
H120.7705−0.0516−0.07650.052*
C130.8532 (5)0.1191 (4)−0.1391 (3)0.0365 (8)
Cl140.89823 (18)0.01398 (12)−0.26699 (9)0.0619 (3)
C150.8828 (4)0.2708 (4)−0.1219 (3)0.0306 (7)
H150.92430.3150−0.17640.037*
C160.8483 (4)0.3547 (3)−0.0206 (3)0.0257 (6)
H160.86670.4569−0.00700.031*
Cl170.34015 (9)0.32493 (9)0.05713 (7)0.03003 (16)
C190.5885 (5)0.4816 (5)0.6159 (4)0.0510 (11)
H190.64740.46860.69270.061*
C200.5665 (6)0.3740 (5)0.5084 (4)0.0493 (11)
C180.4783 (5)0.3921 (5)0.3929 (4)0.0479 (10)
H180.46430.31900.32170.057*
Cl210.6390 (5)0.2036 (3)0.5142 (4)0.0640 (9)0.50
C210.659 (3)0.2527 (18)0.522 (2)0.081 (2)0.50
H210.72550.25010.60050.097*0.50
O20.6509 (12)0.1563 (8)0.4337 (7)0.081 (2)0.50
U11U22U33U12U13U23
Pt10.01892 (8)0.01346 (8)0.01130 (7)0.00185 (5)0.00020 (5)0.00142 (5)
O10.0370 (12)0.0334 (13)0.0173 (10)0.0180 (10)−0.0050 (9)−0.0037 (9)
N20.0311 (13)0.0305 (15)0.0193 (12)0.0135 (11)−0.0004 (10)−0.0033 (10)
C30.0280 (14)0.0236 (15)0.0188 (13)0.0079 (12)0.0013 (11)0.0045 (11)
N40.0246 (12)0.0176 (12)0.0159 (11)0.0040 (9)−0.0003 (9)0.0011 (9)
C50.0251 (14)0.0276 (16)0.0151 (13)0.0071 (12)0.0000 (11)0.0017 (11)
N60.0340 (14)0.0236 (13)0.0170 (11)0.0097 (11)−0.0048 (10)−0.0049 (10)
C70.0394 (18)0.0260 (17)0.0250 (15)0.0147 (14)−0.0038 (13)−0.0047 (13)
C80.045 (2)0.040 (2)0.0297 (17)0.0138 (16)−0.0096 (15)−0.0164 (15)
C90.053 (2)0.048 (2)0.0264 (17)0.0291 (19)−0.0062 (16)0.0022 (16)
C100.0247 (14)0.0207 (15)0.0178 (13)0.0064 (11)−0.0022 (11)0.0006 (11)
C110.051 (2)0.0262 (17)0.0257 (15)0.0055 (15)0.0084 (15)0.0094 (13)
C120.074 (3)0.0135 (16)0.0358 (18)0.0094 (16)0.0061 (18)0.0007 (14)
C130.054 (2)0.0323 (19)0.0212 (15)0.0222 (16)0.0059 (15)−0.0002 (13)
Cl140.1140 (10)0.0441 (6)0.0333 (5)0.0409 (6)0.0248 (6)0.0019 (4)
C150.0342 (16)0.0305 (17)0.0308 (16)0.0112 (13)0.0120 (14)0.0087 (13)
C160.0235 (14)0.0187 (15)0.0309 (15)0.0017 (11)0.0043 (12)0.0022 (12)
Cl170.0284 (4)0.0283 (4)0.0350 (4)0.0005 (3)0.0072 (3)0.0162 (3)
C190.067 (3)0.069 (3)0.037 (2)0.037 (2)0.027 (2)0.028 (2)
C200.071 (3)0.058 (3)0.044 (2)0.042 (2)0.037 (2)0.028 (2)
C180.067 (3)0.058 (3)0.0366 (19)0.031 (2)0.0315 (19)0.0178 (18)
Cl210.100 (2)0.059 (2)0.0583 (16)0.0507 (19)0.0399 (15)0.0301 (19)
C210.145 (7)0.062 (5)0.059 (4)0.064 (5)0.043 (4)0.023 (4)
O20.145 (7)0.062 (5)0.059 (4)0.064 (5)0.043 (4)0.023 (4)
Pt1—N42.018 (2)C9—H9B0.9600
Pt1—N4i2.018 (2)C9—H9C0.9600
Pt1—Cl172.3087 (7)C10—C111.381 (4)
Pt1—Cl17i2.3087 (7)C10—C161.385 (4)
O1—N21.490 (3)C11—H110.9300
O1—C51.360 (3)C11—C121.394 (5)
N2—H20.9100C12—H120.9300
N2—C31.474 (4)C12—C131.364 (5)
N2—C91.452 (4)C13—Cl141.754 (3)
C3—H30.9800C13—C151.385 (5)
C3—N41.476 (4)C15—H150.9300
C3—C101.505 (4)C15—C161.387 (4)
N4—C51.301 (4)C16—H160.9300
C5—N61.325 (4)C19—H190.9300
N6—C71.464 (4)C19—C201.389 (6)
N6—C81.467 (4)C19—C18ii1.378 (6)
C7—H7A0.9600C20—C181.391 (5)
C7—H7B0.9600C20—Cl211.782 (5)
C7—H7C0.9600C20—C211.465 (18)
C8—H8A0.9600C18—C19ii1.378 (6)
C8—H8B0.9600C18—H180.9300
C8—H8C0.9600C21—H210.9300
C9—H9A0.9600C21—O21.20 (2)
N4—Pt1—N4i180.0N2—C9—H9A109.5
N4i—Pt1—Cl1790.47 (7)N2—C9—H9B109.5
N4—Pt1—Cl1789.53 (7)N2—C9—H9C109.5
N4i—Pt1—Cl17i89.53 (7)H9A—C9—H9B109.5
N4—Pt1—Cl17i90.47 (7)H9A—C9—H9C109.5
Cl17—Pt1—Cl17i180.0H9B—C9—H9C109.5
C5—O1—N2103.2 (2)C11—C10—C3119.9 (3)
O1—N2—H2111.8C11—C10—C16119.8 (3)
C3—N2—O1101.1 (2)C16—C10—C3120.2 (3)
C3—N2—H2111.8C10—C11—H11119.9
C9—N2—O1106.0 (2)C10—C11—C12120.1 (3)
C9—N2—H2111.8C12—C11—H11119.9
C9—N2—C3113.6 (3)C11—C12—H12120.6
N2—C3—H3110.1C13—C12—C11118.8 (3)
N2—C3—N4101.0 (2)C13—C12—H12120.6
N2—C3—C10109.5 (2)C12—C13—Cl14119.9 (3)
N4—C3—H3110.1C12—C13—C15122.6 (3)
N4—C3—C10115.5 (2)C15—C13—Cl14117.5 (3)
C10—C3—H3110.1C13—C15—H15121.1
C3—N4—Pt1119.50 (17)C13—C15—C16117.8 (3)
C5—N4—Pt1133.5 (2)C16—C15—H15121.1
C5—N4—C3106.5 (2)C10—C16—C15120.9 (3)
N4—C5—O1114.1 (3)C10—C16—H16119.6
N4—C5—N6131.3 (3)C15—C16—H16119.6
N6—C5—O1114.5 (2)C20—C19—H19120.4
C5—N6—C7123.4 (2)C18ii—C19—H19120.4
C5—N6—C8120.6 (3)C18ii—C19—C20119.1 (4)
C7—N6—C8115.9 (3)C19—C20—C18121.0 (4)
N6—C7—H7A109.5C19—C20—Cl21121.3 (3)
N6—C7—H7B109.5C19—C20—C21116.0 (9)
N6—C7—H7C109.5C18—C20—Cl21117.5 (4)
H7A—C7—H7B109.5C18—C20—C21122.5 (9)
H7A—C7—H7C109.5C21—C20—Cl2111.6 (10)
H7B—C7—H7C109.5C19ii—C18—C20119.9 (4)
N6—C8—H8A109.5C19ii—C18—H18120.1
N6—C8—H8B109.5C20—C18—H18120.1
N6—C8—H8C109.5C20—C21—H21119.7
H8A—C8—H8B109.5O2—C21—C20120.5 (17)
H8A—C8—H8C109.5O2—C21—H21119.7
H8B—C8—H8C109.5
Pt1—N4—C5—O1179.0 (2)C9—N2—C3—C10−88.6 (3)
Pt1—N4—C5—N60.1 (5)C10—C3—N4—Pt141.0 (3)
O1—N2—C3—N436.0 (3)C10—C3—N4—C5−146.2 (3)
O1—N2—C3—C10158.3 (2)C10—C11—C12—C130.5 (5)
O1—C5—N6—C7−172.6 (3)C11—C10—C16—C15−0.7 (4)
O1—C5—N6—C84.9 (5)C11—C12—C13—Cl14179.4 (3)
N2—O1—C5—N416.2 (3)C11—C12—C13—C15−1.1 (6)
N2—O1—C5—N6−164.7 (3)C12—C13—C15—C160.7 (5)
N2—C3—N4—Pt1159.05 (18)C13—C15—C16—C100.2 (5)
N2—C3—N4—C5−28.1 (3)Cl14—C13—C15—C16−179.7 (2)
N2—C3—C10—C11105.8 (3)C16—C10—C11—C120.4 (5)
N2—C3—C10—C16−71.3 (3)Cl17—Pt1—N4—C361.0 (2)
C3—N4—C5—O17.6 (3)Cl17i—Pt1—N4—C3−119.0 (2)
C3—N4—C5—N6−171.3 (3)Cl17i—Pt1—N4—C570.5 (3)
C3—C10—C11—C12−176.7 (3)Cl17—Pt1—N4—C5−109.5 (3)
C3—C10—C16—C15176.4 (3)C19—C20—C18—C19ii0.1 (8)
N4i—Pt1—N4—C315 (24)C19—C20—C21—O2−178.3 (15)
N4i—Pt1—N4—C5−155 (24)C18ii—C19—C20—C18−0.1 (7)
N4—C3—C10—C11−141.0 (3)C18ii—C19—C20—Cl21−176.3 (4)
N4—C3—C10—C1641.9 (4)C18ii—C19—C20—C21172.0 (11)
N4—C5—N6—C76.3 (6)C18—C20—C21—O2−6 (3)
N4—C5—N6—C8−176.2 (4)Cl21—C20—C18—C19ii176.4 (4)
C5—O1—N2—C3−32.6 (3)Cl21—C20—C21—O261 (4)
C5—O1—N2—C9−151.3 (3)C21—C20—C18—C19ii−171.4 (11)
C9—N2—C3—N4149.1 (3)
D—H···AD—HH···AD···AD—H···A
C8—H8···O2iii0.962.583.378 (9)141
C12—H12···Cl17iv0.932.703.589 (4)160
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
C8—H8⋯O2i 0.962.583.378 (9)141
C12—H12⋯Cl17ii 0.932.703.589 (4)160

Symmetry codes: (i) ; (ii) .

  7 in total

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6.  Novel tailoring reaction for two adjacent coordinated nitriles giving platinum 1,3,5-triazapentadiene complexes.

Authors:  Pavel V Gushchin; Marina R Tyan; Nadezhda A Bokach; Mikhail D Revenco; Matti Haukka; Meng-Jiy Wang; Cheng-Hsuan Lai; Pi-Tai Chou; Vadim Yu Kukushkin
Journal:  Inorg Chem       Date:  2008-12-15       Impact factor: 5.165

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Authors:  Larysa V Penkova; Anna Maciag; Elena V Rybak-Akimova; Matti Haukka; Vadim A Pavlenko; Turganbay S Iskenderov; Henryk Kozłowski; Franc Meyer; Igor O Fritsky
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