Literature DB >> 21577723

Bis(1,3-dibutylthiourea)dicyanido-mercury(II).

Saeed Ahmad, Haseeba Sadaf, Mehmet Akkurt, Shahzad Sharif, Islam Ullah Khan.   

Abstract

In the title compound, [Hg(CN)(2)(C(9)H(20)N(2)S)(2)], the Hg atom lies on a twofold rotation axis. There is only half a mol-ecule in the asymmetric unit. The Hg atom has a distorted tetra-hedral coordination involving the S atoms of two 1-butyl-3-propyl-thio-urea groups and the C atoms of the two CN(-) anions. In the crystal packing, adjacent mol-ecules are connected by inter-molecular N-H⋯N and N-H⋯S hydrogen bonds, forming infinite chains in three dimensions.

Entities:  

Year:  2009        PMID: 21577723      PMCID: PMC2970451          DOI: 10.1107/S1600536809035594

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


Related literature

For the coordination chemistry of thio­urea-type ligands, see: Nadeem et al. (2009 ▶, 2008 ▶); Zoufalá et al. (2007 ▶); Khan et al. (2007 ▶); Hanif et al. (2007 ▶); Fuks et al. (2005 ▶); Moro et al. (2009 ▶); Matesanz & Souza (2007 ▶). For crystallographic reports about mercury(II) complexes containing thio­amides, see: Popovic et al. (2000 ▶, 2002 ▶); Pavlović et al. (2000 ▶); Jiang et al. (2001 ▶); Wu et al. (2004 ▶). For the spectroscopy and structural chemistry of cyanide complexes of silver(I) and gold(I) with thio­nes, see: Hanif et al. (2007 ▶); Wu et al. (2004 ▶); Ahmad, Isab & Ashraf (2002 ▶); Ahmad, Isab & Perzanowski (2002 ▶); Ashraf et al. (2002 ▶); Ahmad & Isab (2001 ▶); Ahmad (2004 ▶).

Experimental

Crystal data

[Hg(CN)2(C9H20N2S)2] M = 629.31 Monoclinic, a = 17.4692 (3) Å b = 9.5928 (2) Å c = 17.4699 (4) Å β = 111.540 (1)° V = 2723.12 (10) Å3 Z = 4 Mo Kα radiation μ = 5.82 mm−1 T = 296 K 0.14 × 0.15 × 0.17 mm

Data collection

Bruker Kappa APEXII CCD area-detector diffractometer Absorption correction: none 15120 measured reflections 3372 independent reflections 2918 reflections with I > 2σ(I) R int = 0.032

Refinement

R[F 2 > 2σ(F 2)] = 0.022 wR(F 2) = 0.044 S = 1.02 3372 reflections 134 parameters H-atom parameters constrained Δρmax = 0.40 e Å−3 Δρmin = −0.72 e Å−3 Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶) and PLATON (Spek, 2009 ▶). Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809035594/bt5052sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809035594/bt5052Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Hg(CN)2(C9H20N2S)2]F(000) = 1256
Mr = 629.31Dx = 1.535 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 6609 reflections
a = 17.4692 (3) Åθ = 2.5–27.2°
b = 9.5928 (2) ŵ = 5.82 mm1
c = 17.4699 (4) ÅT = 296 K
β = 111.540 (1)°Irregular, white
V = 2723.12 (10) Å30.17 × 0.15 × 0.14 mm
Z = 4
Bruker Kappa APEXII CCD area-detector diffractometer2918 reflections with I > 2σ(I)
Radiation source: sealed tubeRint = 0.032
graphiteθmax = 28.3°, θmin = 2.5°
φ and ω scansh = −23→23
15120 measured reflectionsk = −12→12
3372 independent reflectionsl = −20→23
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) = 0.044H-atom parameters constrained
S = 1.02w = 1/[σ2(Fo2) + (0.0211P)2], where P = (Fo2 + 2Fc2)/3
3372 reflections(Δ/σ)max = 0.001
134 parametersΔρmax = 0.40 e Å3
0 restraintsΔρmin = −0.72 e Å3
Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles
Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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*/Ueq
Hg11.000000.20478 (1)0.750000.0405 (1)
S11.08516 (3)0.39691 (7)0.86634 (4)0.0414 (2)
N10.86048 (15)0.1224 (3)0.81955 (17)0.0718 (10)
N21.11488 (12)0.5094 (2)0.74219 (12)0.0422 (7)
N31.22801 (11)0.4758 (2)0.85840 (12)0.0411 (7)
C10.91098 (16)0.1498 (3)0.79668 (17)0.0475 (9)
C21.14750 (13)0.4655 (2)0.81878 (15)0.0341 (7)
C31.16093 (17)0.5591 (3)0.69240 (17)0.0548 (10)
C41.10347 (17)0.6051 (3)0.60900 (17)0.0534 (10)
C51.0548 (2)0.7334 (4)0.6094 (2)0.0633 (12)
C60.9979 (3)0.7767 (4)0.5243 (3)0.0875 (17)
C71.27223 (15)0.4387 (3)0.94375 (16)0.0441 (8)
C81.27906 (17)0.5571 (3)1.00242 (16)0.0473 (9)
C91.3311 (2)0.5232 (3)1.09034 (17)0.0586 (11)
C101.3434 (3)0.6466 (4)1.1477 (2)0.0795 (14)
H21.062100.508800.719500.0510*
H31.256500.507100.831200.0490*
H3A1.196000.485000.686300.0660*
H3B1.195800.636600.720200.0660*
H4A1.135300.622300.574700.0640*
H4B1.065500.529700.584100.0640*
H5A1.092400.809300.634200.0760*
H5B1.022400.716500.643300.0760*
H6A1.028800.785500.489100.1310*
H6B0.973000.864600.527500.1310*
H6C0.955800.707500.502400.1310*
H7A1.327100.407800.950100.0530*
H7B1.244300.361200.958100.0530*
H8A1.224300.582500.999500.0570*
H8B1.302500.637300.985100.0570*
H9A1.384500.490401.092700.0700*
H9B1.305200.448201.109200.0700*
H10A1.367600.722201.128500.1190*
H10B1.379100.620401.202100.1190*
H10C1.291100.675401.148700.1190*
U11U22U33U12U13U23
Hg10.0323 (1)0.0459 (1)0.0478 (1)0.00000.0199 (1)0.0000
S10.0359 (3)0.0566 (4)0.0340 (3)−0.0115 (3)0.0154 (3)−0.0005 (3)
N10.0516 (14)0.104 (2)0.0668 (17)−0.0297 (15)0.0300 (13)−0.0046 (17)
N20.0326 (10)0.0594 (14)0.0352 (12)−0.0068 (9)0.0133 (9)0.0057 (11)
N30.0313 (10)0.0545 (13)0.0383 (12)−0.0043 (9)0.0136 (9)0.0051 (10)
C10.0385 (13)0.0553 (16)0.0463 (16)−0.0125 (12)0.0126 (12)−0.0037 (14)
C20.0330 (11)0.0369 (13)0.0340 (14)−0.0030 (9)0.0142 (10)−0.0015 (11)
C30.0473 (15)0.076 (2)0.0491 (17)−0.0018 (14)0.0270 (14)0.0144 (15)
C40.0563 (16)0.069 (2)0.0396 (16)−0.0019 (14)0.0232 (13)0.0039 (15)
C50.076 (2)0.066 (2)0.052 (2)0.0065 (17)0.0285 (17)0.0103 (16)
C60.084 (3)0.101 (3)0.074 (3)0.026 (2)0.025 (2)0.020 (2)
C70.0353 (12)0.0476 (15)0.0446 (16)0.0040 (11)0.0089 (11)0.0054 (13)
C80.0477 (14)0.0466 (15)0.0427 (16)0.0038 (12)0.0110 (12)0.0064 (13)
C90.0665 (19)0.0565 (19)0.0433 (17)0.0044 (15)0.0090 (15)0.0050 (15)
C100.107 (3)0.066 (2)0.051 (2)−0.005 (2)0.012 (2)−0.0008 (19)
Hg1—S12.7424 (7)C3—H3A0.9700
Hg1—C12.072 (3)C3—H3B0.9700
Hg1—S1i2.7424 (7)C4—H4A0.9700
Hg1—C1i2.072 (3)C4—H4B0.9700
S1—C21.724 (2)C5—H5A0.9700
N1—C11.125 (4)C5—H5B0.9700
N2—C21.316 (3)C6—H6A0.9600
N2—C31.465 (4)C6—H6B0.9600
N3—C21.324 (3)C6—H6C0.9600
N3—C71.449 (3)C7—H7A0.9700
N2—H20.8600C7—H7B0.9700
N3—H30.8600C8—H8A0.9700
C3—C41.500 (4)C8—H8B0.9700
C4—C51.497 (5)C9—H9A0.9700
C5—C61.512 (6)C9—H9B0.9700
C7—C81.505 (4)C10—H10A0.9600
C8—C91.505 (4)C10—H10B0.9600
C9—C101.514 (5)C10—H10C0.9600
S1···C13.693 (3)H3A···N32.8500
S1···C83.684 (3)H3A···H32.3700
S1···N2i3.479 (2)H3A···H10Cvi2.5200
S1···H7B2.6700H3B···N32.7400
S1···H2i2.6800H3B···H32.2200
S1···H6Aii3.1900H3B···H5A2.5000
N1···N3iii2.991 (3)H3B···N1iv2.7600
N1···C3iii3.431 (4)H4A···H6A2.4700
N2···S1i3.479 (2)H4B···H22.4000
N3···N1iv2.991 (3)H4B···H6C2.5700
N1···H3Biii2.7600H5A···H3B2.5000
N1···H3iii2.2000H5A···H7Avii2.5600
N2···H5B2.7400H5B···N22.7400
N3···H3A2.8500H5B···H22.3500
N3···H3B2.7400H6A···H4A2.4700
C1···S13.693 (3)H6A···S1vi3.1900
C1···C2i3.574 (4)H6C···H4B2.5700
C3···N1iv3.431 (4)H7A···H9A2.4500
C8···S13.684 (3)H7A···H5Aviii2.5600
C1···H10Bv3.0100H7B···S12.6700
C3···H32.4400H7B···H9B2.6000
C5···H22.8600H7B···H7Bix2.5500
H2···C52.8600H8A···H10C2.5900
H2···H4B2.4000H8B···H10A2.4800
H2···H5B2.3500H9A···H7A2.4500
H2···S1i2.6800H9B···H7B2.6000
H3···C32.4400H10A···H8B2.4800
H3···H3A2.3700H10B···C1x3.0100
H3···H3B2.2200H10C···H8A2.5900
H3···N1iv2.2000H10C···H3Aii2.5200
S1—Hg1—C199.25 (8)C4—C5—H5A109.00
S1—Hg1—S1i95.55 (2)C4—C5—H5B109.00
S1—Hg1—C1i100.45 (8)C6—C5—H5A109.00
S1i—Hg1—C1100.45 (8)C6—C5—H5B109.00
C1—Hg1—C1i150.51 (11)H5A—C5—H5B108.00
S1i—Hg1—C1i99.25 (8)C5—C6—H6A109.00
Hg1—S1—C299.56 (8)C5—C6—H6B109.00
C2—N2—C3125.5 (2)C5—C6—H6C109.00
C2—N3—C7125.6 (2)H6A—C6—H6B109.00
C2—N2—H2117.00H6A—C6—H6C110.00
C3—N2—H2117.00H6B—C6—H6C109.00
C2—N3—H3117.00N3—C7—H7A109.00
C7—N3—H3117.00N3—C7—H7B109.00
Hg1—C1—N1177.4 (3)C8—C7—H7A109.00
S1—C2—N2119.84 (19)C8—C7—H7B109.00
S1—C2—N3120.95 (18)H7A—C7—H7B108.00
N2—C2—N3119.2 (2)C7—C8—H8A109.00
N2—C3—C4110.8 (2)C7—C8—H8B109.00
C3—C4—C5114.6 (2)C9—C8—H8A109.00
C4—C5—C6113.0 (3)C9—C8—H8B109.00
N3—C7—C8113.2 (2)H8A—C8—H8B108.00
C7—C8—C9113.5 (2)C8—C9—H9A109.00
C8—C9—C10113.1 (3)C8—C9—H9B109.00
N2—C3—H3A109.00C10—C9—H9A109.00
N2—C3—H3B109.00C10—C9—H9B109.00
C4—C3—H3A109.00H9A—C9—H9B108.00
C4—C3—H3B109.00C9—C10—H10A109.00
H3A—C3—H3B108.00C9—C10—H10B109.00
C3—C4—H4A109.00C9—C10—H10C109.00
C3—C4—H4B109.00H10A—C10—H10B110.00
C5—C4—H4A109.00H10A—C10—H10C109.00
C5—C4—H4B109.00H10B—C10—H10C110.00
H4A—C4—H4B108.00
C1—Hg1—S1—C2−169.87 (11)C7—N3—C2—S1−2.8 (3)
S1i—Hg1—S1—C2−68.30 (8)C7—N3—C2—N2176.7 (2)
C1i—Hg1—S1—C232.19 (11)C2—N3—C7—C8−88.9 (3)
Hg1—S1—C2—N251.24 (18)N2—C3—C4—C567.9 (3)
Hg1—S1—C2—N3−129.28 (17)C3—C4—C5—C6179.8 (3)
C3—N2—C2—S1−174.74 (19)N3—C7—C8—C9−175.0 (2)
C3—N2—C2—N35.8 (3)C7—C8—C9—C10175.2 (3)
C2—N2—C3—C4−178.1 (2)
D—H···AD—HH···AD···AD—H···A
N2—H2···S1i0.862.683.479 (2)155
N3—H3···N1iv0.862.202.991 (3)153
C7—H7B···S10.972.673.070 (3)105
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N2—H2⋯S1i0.862.683.479 (2)155
N3—H3⋯N1ii0.862.202.991 (3)153
C7—H7B⋯S10.972.673.070 (3)105

Symmetry codes: (i) ; (ii) .

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