Literature DB >> 21202484

(Thio-cyanato-κN)bis-(thio-semicarbazide-κS)copper(I).

Li Jia, Shouxin Ma, Dacheng Li.   

Abstract

In the title complex, [Cu(CH(5)N(3)S)(2)(NCS)], the non-H part of the mol-ecule is strictly planar, lying on the mirror plane at y = 0.25. The Cu atom lies at the centre of a triangle formed by the coordination of three monodentate groups, viz. two thio-semicarbazide ligands and one NCS(-) anion. Weak inter-molecular N-H⋯S inter-actions generate a two-dimensional network.

Entities:  

Year:  2008        PMID: 21202484      PMCID: PMC2961608          DOI: 10.1107/S1600536808013068

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


Related literature

For related thio­semicarbazide metal complexes, see: Capacchi et al. (1968 ▶). For related literature, see: Chattopadhyay et al. (1991 ▶).

Experimental

Crystal data

[Cu(CH5N3S)2(NCS)] M = 303.90 Orthorhombic, a = 11.488 (2) Å b = 6.6085 (12) Å c = 14.650 (3) Å V = 1112.2 (4) Å3 Z = 4 Mo Kα radiation μ = 2.50 mm−1 T = 298 (2) K 0.38 × 0.27 × 0.24 mm

Data collection

Bruker SMART CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.44, T max = 0.55 5593 measured reflections 1077 independent reflections 947 reflections with I > 2σ(I) R int = 0.021

Refinement

R[F 2 > 2σ(F 2)] = 0.029 wR(F 2) = 0.080 S = 1.05 1077 reflections 86 parameters H-atom parameters constrained Δρmax = 0.67 e Å−3 Δρmin = −0.54 e Å−3 Data collection: SMART (Bruker, 1997 ▶); cell refinement: SAINT (Bruker, 1997 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808013068/bg2183sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808013068/bg2183Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Cu(CH5N3S)2(NCS)]F(000) = 616
Mr = 303.90Dx = 1.815 Mg m3
Orthorhombic, PnmaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2nCell parameters from 3130 reflections
a = 11.488 (2) Åθ = 2.3–28.2°
b = 6.6085 (12) ŵ = 2.50 mm1
c = 14.650 (3) ÅT = 298 K
V = 1112.2 (4) Å3Block, black
Z = 40.38 × 0.27 × 0.24 mm
Bruker SMART CCD area-detector diffractometer1077 independent reflections
Radiation source: fine-focus sealed tube947 reflections with I > 2σ(I)
graphiteRint = 0.021
φ and ω scansθmax = 25.0°, θmin = 2.3°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)h = −13→13
Tmin = 0.44, Tmax = 0.55k = −7→7
5593 measured reflectionsl = −17→10
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.029H-atom parameters constrained
wR(F2) = 0.080w = 1/[σ2(Fo2) + (0.0469P)2 + 0.712P] where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max < 0.001
1077 reflectionsΔρmax = 0.67 e Å3
86 parametersΔρmin = −0.54 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0072 (9)
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.
xyzUiso*/UeqOcc. (<1)
Cu10.28439 (4)0.25000.53244 (3)0.0689 (3)
N10.1200 (2)0.25000.25507 (19)0.0338 (6)
H1A0.14890.25000.20090.041*
H1B0.04580.25000.26250.041*
N20.3047 (2)0.25000.31376 (19)0.0361 (7)
H20.34830.25000.36150.043*
N30.3600 (2)0.25000.22780 (18)0.0348 (6)
H3A0.32440.16160.19140.052*0.50
H3B0.35550.37320.20350.052*0.50
N40.4655 (2)0.25000.7081 (2)0.0457 (8)
H4A0.52620.25000.74230.055*
H4B0.47290.25000.64960.055*
N50.3516 (2)0.25000.83438 (18)0.0349 (7)
H50.28390.25000.85940.042*
N60.4526 (2)0.25000.88959 (19)0.0414 (7)
H6A0.44260.16450.93590.062*0.50
H6B0.46470.37410.91120.062*0.50
N70.4475 (3)0.25000.4928 (2)0.0415 (7)
S10.13368 (7)0.25000.43541 (6)0.0335 (2)
S20.23512 (7)0.25000.68064 (5)0.0318 (2)
S30.68866 (8)0.25000.47665 (7)0.0528 (3)
C10.1893 (3)0.25000.3264 (2)0.0283 (7)
C20.3611 (3)0.25000.7450 (2)0.0286 (7)
C30.5450 (3)0.25000.4851 (2)0.0278 (7)
U11U22U33U12U13U23
Cu10.0292 (3)0.1520 (7)0.0256 (3)0.000−0.00124 (17)0.000
N10.0205 (13)0.0557 (17)0.0252 (13)0.000−0.0003 (10)0.000
N20.0214 (13)0.0632 (18)0.0237 (14)0.000−0.0002 (11)0.000
N30.0254 (13)0.0517 (17)0.0274 (15)0.0000.0048 (11)0.000
N40.0261 (15)0.088 (2)0.0236 (14)0.000−0.0024 (11)0.000
N50.0260 (13)0.0529 (17)0.0259 (15)0.000−0.0030 (11)0.000
N60.0339 (15)0.0617 (19)0.0285 (15)0.000−0.0088 (12)0.000
N70.0338 (18)0.0549 (19)0.0357 (16)0.0000.0011 (13)0.000
S10.0242 (4)0.0521 (5)0.0242 (4)0.0000.0021 (3)0.000
S20.0232 (4)0.0477 (5)0.0243 (4)0.000−0.0017 (3)0.000
S30.0279 (5)0.0971 (8)0.0333 (5)0.000−0.0009 (4)0.000
C10.0242 (15)0.0345 (16)0.0263 (16)0.000−0.0003 (12)0.000
C20.0256 (15)0.0335 (16)0.0265 (16)0.000−0.0038 (12)0.000
C30.0286 (18)0.0395 (18)0.0152 (14)0.0000.0017 (12)0.000
Cu1—N71.962 (3)N4—H4A0.8600
Cu1—S12.2401 (10)N4—H4B0.8600
Cu1—S22.2437 (10)N5—C21.314 (4)
N1—C11.313 (4)N5—N61.414 (4)
N1—H1A0.8600N5—H50.8600
N1—H1B0.8600N6—H6A0.8900
N2—C11.339 (4)N6—H6B0.8900
N2—N31.410 (4)N7—C31.126 (4)
N2—H20.8600S1—C11.721 (3)
N3—H3A0.8900S2—C21.727 (3)
N3—H3B0.8900S3—C31.655 (3)
N4—C21.315 (4)
N7—Cu1—S1123.38 (10)C2—N5—H5119.9
N7—Cu1—S2121.85 (10)N6—N5—H5119.9
S1—Cu1—S2114.77 (4)N5—N6—H6A109.3
C1—N1—H1A120.0N5—N6—H6B109.4
C1—N1—H1B120.0H6A—N6—H6B109.5
H1A—N1—H1B120.0C3—N7—Cu1168.5 (3)
C1—N2—N3124.7 (3)C1—S1—Cu1107.58 (11)
C1—N2—H2117.7C2—S2—Cu1108.46 (11)
N3—N2—H2117.7N1—C1—N2119.4 (3)
N2—N3—H3A109.2N1—C1—S1120.9 (2)
N2—N3—H3B109.4N2—C1—S1119.7 (2)
H3A—N3—H3B109.5N5—C2—N4119.0 (3)
C2—N4—H4A120.0N5—C2—S2118.3 (2)
C2—N4—H4B120.0N4—C2—S2122.7 (3)
H4A—N4—H4B120.0N7—C3—S3178.6 (3)
C2—N5—N6120.1 (3)
D—H···AD—HH···AD···AD—H···A
N1—H1A···S3i0.862.643.485 (3)167.
N1—H1B···N3i0.862.142.998 (4)177.
N2—H2···N70.862.243.093 (4)175.
N3—H3A···S2ii0.892.813.5481 (11)141.
N3—H3B···S2iii0.892.723.5481 (11)155.
N4—H4A···S2iv0.862.653.501 (3)170.
N4—H4B···N70.862.323.161 (4)167.
N5—H5···S3v0.862.643.342 (3)140.
N6—H6A···S1vi0.892.883.5144 (12)130.
N6—H6B···S1vii0.892.753.5144 (11)144.
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1A⋯S3i0.862.643.485 (3)167
N1—H1B⋯N3i0.862.142.998 (4)177
N2—H2⋯N70.862.243.093 (4)175
N3—H3A⋯S2ii0.892.813.5481 (11)141
N3—H3B⋯S2iii0.892.723.5481 (11)155
N4—H4A⋯S2iv0.862.653.501 (3)170
N4—H4B⋯N70.862.323.161 (4)167
N5—H5⋯S3v0.862.643.342 (3)140
N6—H6A⋯S1vi0.892.883.5144 (12)130
N6—H6B⋯S1vii0.892.753.5144 (11)144

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) ; (v) ; (vi) ; (vii) .

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