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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 May 28;67(Pt 6):m816–m817. doi: 10.1107/S160053681101974X

Iodido{4-phenyl-1-[1-(1,3-thia­zol-2-yl-κN)ethyl­idene]thio­semicarbazidato-κ2 N′,S}{4-phenyl-1-[1-(1,3-thia­zol-2-yl)ethyl­idene]thio­semicarbazide-κS}mercury(II)

Samuel S R Dasary a, Sri Ranjini Arumugam a, Hongtao Yu a, Ramaiyer Venkatraman a, Frank R Fronczek b,*
PMCID: PMC3120629  PMID: 21754688

Abstract

In the title compound, [Hg(C12H11N4S2)I(C12H12N4S2)], the Hg atom is in a distorted square-pyramidal coordination, defined by the iodide ligand, by the S atom of the neutral ligand in the apical position, and by the N atom of the thia­zole ring, the thio­ureido N and the S atom of the deprotonated ligand. The deprotonated ligand intra­molecularly hydrogen bonds to the thia­zole ring N atom, while the deprotonated ligand forms an inter­molecular hydrogen bond to the thiol­ate S atom. The deprotonation of the tridentate ligand and its coordination to Hg via the S atom strikingly affects the C—S bond lengths. In the free ligand, the C—S bond distance is 1.685 (7) Å, whereas it is 1.749 (7) Å in the deprotonated ligand. Similarly, the Hg—S bond distance is slightly longer to the neutral ligand [2.6682 (18) Å] than to the deprotonated ligand [2.5202 (19) Å]. The Hg—I distance is 2.7505 (8) Å.

Related literature

For general background to thio­semicarbazones and their Hg complexes, see: Akinchan et al. (2002 ▶); Ali & Livingstone (1974 ▶); Bermejo et al. (1999 ▶, 2003 ▶); Lobana et al. (1998 ▶); Venkatraman et al. (2009 ▶); Blanz & French (1968 ▶); Campbell (1975 ▶); Casas et al. (2000 ▶); Grecu & Neamtu (1967 ▶); Pellerito & Negy (2002 ▶); Raper (1985 ▶).graphic file with name e-67-0m816-scheme1.jpg

Experimental

Crystal data

  • [Hg(C12H11N4S2)I(C12H12N4S2)]

  • M r = 879.23

  • Triclinic, Inline graphic

  • a = 8.694 (2) Å

  • b = 10.119 (2) Å

  • c = 16.801 (4) Å

  • α = 76.670 (13)°

  • β = 79.448 (12)°

  • γ = 77.190 (13)°

  • V = 1388.8 (5) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 6.99 mm−1

  • T = 90 K

  • 0.10 × 0.10 × 0.03 mm

Data collection

  • Nonius KappaCCD diffractometer with an Oxford Cryosystems Cryostream cooler

  • Absorption correction: multi-scan (SCALEPACK; Otwinowski & Minor, 1997 ▶) T min = 0.542, T max = 0.818

  • 21861 measured reflections

  • 5837 independent reflections

  • 4289 reflections with I > 2σ(I)

  • R int = 0.059

Refinement

  • R[F 2 > 2σ(F 2)] = 0.042

  • wR(F 2) = 0.085

  • S = 1.02

  • 5837 reflections

  • 346 parameters

  • H-atom parameters constrained

  • Δρmax = 1.36 e Å−3

  • Δρmin = −1.27 e Å−3

Data collection: COLLECT (Nonius, 2000 ▶); cell refinement: SCALEPACK (Otwinowski & Minor, 1997 ▶); data reduction: DENZO (Otwinowski & Minor, 1997 ▶) and SCALEPACK; program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053681101974X/vm2089sup1.cif

e-67-0m816-sup1.cif (25.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681101974X/vm2089Isup2.hkl

e-67-0m816-Isup2.hkl (279.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A D⋯A D—H⋯A
N7—H7N⋯N5 0.88 1.97 2.667 (8) 135
N4—H4N⋯S2i 0.88 2.69 3.553 (6) 167

Symmetry code: (i) Inline graphic.

Acknowledgments

Purchase of the diffractometer was made possible by grant No. LEQSF (1999–2000)-ENH-TR-13, administered by the Louisiana Board of Regents. RV acknowledges the JSU Department of Chemistry and Biochemistry for the supplies and utilization of lab facilities.

supplementary crystallographic information

Comment

Studies on thiosemicarbazones and their metal complexes has remained a fertile field of research for more than three decades due to their significant impacts in biology and chemistry (Ali & Livingstone, 1974; Campbell, 1975; Pellerito & Negy, 2002). Thiosemicarbazones are known to coordinate to many metals, potentially as tridentate ligands. The ligation can occur with the metals as a neutral molecule or, after deprotonation, as an anionic ligand (Campbell, 1975; Raper, 1985; Casas et al., 2000). Further, the metal-chelating ability is attributed to the thione-thiol tautomerism exhibited by these molecules. Some of the metal complexes are found to exhibit enhanced biological activity compared to their basic ligand (Blanz & French, 1968). Among the metals studied with thiosemicarbazones, mercury and organomercury compounds are scarce (Grecu & Neamtu, 1967; Lobana et al.,1998; Bermejo et al., 1999; Akinchan et al., 2002; Bermejo et al., 2003). Removal and remediation of many mercury species from environmental samples are very important. We report here the synthesis and structure of a mercury(II) iodide complex of the phenyl derivative of 2-acetylthiazole-3-thiosemicarbazone. The title complex is a result of interaction between two neutral ligand molecules and mercury(II) iodide in methanol. In this complex, Hg(II) is chelated by two 2-acetylthiazole-3-phenylthiosemicarbazone ligands, forming a distorted square pyramidal geometry (Fig 1). One of the two ligands is deprotonated at N3, and tridentate through its N, N, S atoms. Along with the iodide atom, it forms the square planar base. The other ligand is neutral and apical to the Hg atom, binding through its S atom. The proton NMR also provides the evidence of ligand deprotonation during metal chelation. The sharp resonance signal due to N—NH proton at 11.12 p.p.m. disappears in the spectrum of the complex. The N4 signal (at ~8.64 p.p.m.) in the ligand undergoes a downfield shift that is marked in the mercury (II) complexes, indicating coordination via the S atom. The protonated and deprotonated ligands have different conformations, differing primarily by the N–N–C–N torsion angle, which is antiperiplanar in the deprotonated ligand (torsion angle N2—N3—C6—N4 179.6 (5)°) and synperiplanar in the neutral ligand (torsion angle N6—N7—C18—N8 9.3 (9)°). Hydrogen bonding details are given in Table 1.

Experimental

To a solution of 2-acetyl thiazole thiosemicarbazone (Venkatraman et al. 2009) (1.38 g, 5 mmol) in warm methanol (50 ml) was added an equimolar methanol solution (50 ml) of mercury(II) iodide (1.36 g. 5 mmol). The mixture was stirred for about 24 h, after which time the yellow solid obtained was filtered and vacuum dried (yield ~75%). Crystals suitable for diffraction studies were obtained from the mother liquor at room temperature after a week.

Refinement

All H atoms were placed in calculated positions, guided by difference maps, with C—H bond distances 0.95–0.98 Å, N—H 0.88 Å, and thereafter refined as riding with Uiso= xUeq, where x = 1.5 for methyl H and 1.2 for all other H atoms. The highest peak in the final difference map was 1.29 Å from the Hg position.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound. Displacement ellipsoids are drawn at the 50% probability level.

Crystal data

[Hg(C12H11N4S2)I(C12H12N4S2)] Z = 2
Mr = 879.23 F(000) = 840
Triclinic, P1 Dx = 2.103 Mg m−3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.694 (2) Å Cell parameters from 5532 reflections
b = 10.119 (2) Å θ = 2.5–26.7°
c = 16.801 (4) Å µ = 6.99 mm−1
α = 76.670 (13)° T = 90 K
β = 79.448 (12)° Parallelepiped, yellow
γ = 77.190 (13)° 0.10 × 0.10 × 0.03 mm
V = 1388.8 (5) Å3

Data collection

Nonius KappaCCD diffractometer with an Oxford Cryosystems Cryostream cooler 5837 independent reflections
Radiation source: fine-focus sealed tube 4289 reflections with I > 2σ(I)
graphite Rint = 0.059
ω and φ scans θmax = 26.7°, θmin = 2.8°
Absorption correction: multi-scan (SCALEPACK; Otwinowski & Minor, 1997) h = −10→10
Tmin = 0.542, Tmax = 0.818 k = −11→12
21861 measured reflections l = −21→21

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.042 H-atom parameters constrained
wR(F2) = 0.085 w = 1/[σ2(Fo2) + (0.0336P)2] where P = (Fo2 + 2Fc2)/3
S = 1.02 (Δ/σ)max = 0.001
5837 reflections Δρmax = 1.36 e Å−3
346 parameters Δρmin = −1.27 e Å−3
0 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.00093 (17)

Special details

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)

x y z Uiso*/Ueq
Hg1 0.31186 (3) 0.89942 (3) 0.265558 (18) 0.01642 (10)
I1 0.21508 (5) 1.07878 (4) 0.12625 (3) 0.01901 (13)
S1 0.8957 (2) 0.80421 (19) 0.20242 (13) 0.0233 (4)
S2 0.1598 (2) 0.96404 (18) 0.39821 (11) 0.0190 (4)
S3 0.9843 (2) 0.36980 (18) 0.41473 (12) 0.0203 (4)
S4 0.2697 (2) 0.64537 (17) 0.26747 (11) 0.0160 (4)
N1 0.5975 (7) 0.8585 (6) 0.1973 (4) 0.0172 (13)
N2 0.5053 (6) 0.8499 (5) 0.3621 (4) 0.0140 (13)
N3 0.4585 (6) 0.8448 (6) 0.4445 (4) 0.0167 (13)
N4 0.2463 (7) 0.8923 (5) 0.5448 (4) 0.0167 (13)
H4N 0.1422 0.9187 0.5536 0.020*
N5 0.6878 (7) 0.4722 (5) 0.4101 (4) 0.0165 (13)
N6 0.7246 (6) 0.4946 (5) 0.2273 (4) 0.0148 (13)
N7 0.5745 (6) 0.5393 (5) 0.2660 (4) 0.0153 (13)
H7N 0.5599 0.5437 0.3186 0.018*
N8 0.4802 (7) 0.5470 (5) 0.1473 (4) 0.0193 (14)
H8N 0.5761 0.5022 0.1321 0.023*
C1 0.6692 (9) 0.8629 (7) 0.1192 (5) 0.0246 (18)
H1 0.6108 0.8833 0.0739 0.029*
C2 0.8316 (9) 0.8360 (7) 0.1094 (5) 0.0263 (19)
H2 0.8988 0.8352 0.0580 0.032*
C3 0.6998 (8) 0.8271 (6) 0.2493 (5) 0.0176 (16)
C4 0.6563 (8) 0.8224 (7) 0.3384 (4) 0.0162 (16)
C5 0.7824 (8) 0.7881 (7) 0.3942 (5) 0.0220 (17)
H5A 0.7641 0.8587 0.4280 0.033*
H5B 0.8875 0.7858 0.3608 0.033*
H5C 0.7778 0.6975 0.4303 0.033*
C6 0.3053 (9) 0.8937 (7) 0.4635 (4) 0.0174 (16)
C7 0.3180 (8) 0.8573 (6) 0.6171 (4) 0.0159 (16)
C8 0.4837 (8) 0.8114 (7) 0.6195 (5) 0.0199 (17)
H8 0.5544 0.7976 0.5706 0.024*
C9 0.5407 (9) 0.7870 (7) 0.6942 (5) 0.0216 (17)
H9 0.6518 0.7563 0.6957 0.026*
C10 0.4416 (9) 0.8057 (7) 0.7667 (5) 0.0222 (17)
H10 0.4838 0.7899 0.8171 0.027*
C11 0.2783 (9) 0.8484 (7) 0.7643 (5) 0.0194 (16)
H11 0.2079 0.8606 0.8135 0.023*
C12 0.2183 (9) 0.8730 (7) 0.6898 (4) 0.0198 (17)
H12 0.1068 0.9012 0.6889 0.024*
C13 0.7128 (8) 0.4433 (6) 0.4910 (4) 0.0153 (15)
H13 0.6288 0.4601 0.5345 0.018*
C14 0.8635 (8) 0.3898 (7) 0.5051 (5) 0.0206 (17)
H14 0.8980 0.3663 0.5579 0.025*
C15 0.8228 (8) 0.4387 (6) 0.3616 (4) 0.0159 (16)
C16 0.8390 (8) 0.4512 (6) 0.2728 (5) 0.0165 (16)
C17 1.0026 (8) 0.4099 (7) 0.2277 (5) 0.0194 (17)
H17A 0.9990 0.4341 0.1680 0.029*
H17B 1.0388 0.3099 0.2441 0.029*
H17C 1.0766 0.4587 0.2415 0.029*
C18 0.4504 (8) 0.5761 (7) 0.2232 (4) 0.0164 (16)
C19 0.3674 (8) 0.5833 (7) 0.0882 (4) 0.0151 (15)
C20 0.3171 (8) 0.7201 (7) 0.0526 (5) 0.0209 (17)
H20 0.3519 0.7919 0.0682 0.025*
C21 0.2147 (8) 0.7508 (8) −0.0067 (4) 0.0213 (17)
H21 0.1763 0.8444 −0.0305 0.026*
C22 0.1693 (8) 0.6466 (7) −0.0307 (4) 0.0195 (17)
H22 0.1029 0.6680 −0.0728 0.023*
C23 0.2196 (8) 0.5104 (7) 0.0058 (4) 0.0176 (16)
H23 0.1845 0.4386 −0.0096 0.021*
C24 0.3209 (8) 0.4785 (7) 0.0647 (4) 0.0151 (15)
H24 0.3581 0.3848 0.0889 0.018*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Hg1 0.01578 (16) 0.01912 (16) 0.01491 (17) −0.00140 (11) −0.00418 (11) −0.00464 (11)
I1 0.0239 (3) 0.0162 (2) 0.0163 (3) −0.0001 (2) −0.0067 (2) −0.0026 (2)
S1 0.0140 (10) 0.0241 (10) 0.0307 (12) −0.0032 (8) −0.0002 (8) −0.0058 (9)
S2 0.0186 (10) 0.0227 (9) 0.0150 (10) 0.0023 (8) −0.0049 (8) −0.0061 (8)
S3 0.0177 (10) 0.0235 (9) 0.0218 (11) −0.0023 (8) −0.0075 (8) −0.0061 (8)
S4 0.0152 (9) 0.0190 (9) 0.0153 (10) −0.0037 (8) −0.0029 (7) −0.0049 (7)
N1 0.020 (3) 0.019 (3) 0.014 (4) −0.003 (3) −0.001 (3) −0.006 (3)
N2 0.015 (3) 0.013 (3) 0.015 (3) −0.002 (2) −0.001 (3) −0.007 (2)
N3 0.013 (3) 0.020 (3) 0.015 (3) −0.001 (3) −0.001 (3) −0.003 (3)
N4 0.016 (3) 0.020 (3) 0.013 (3) 0.000 (3) −0.002 (3) −0.003 (3)
N5 0.020 (3) 0.012 (3) 0.018 (4) −0.004 (3) 0.000 (3) −0.003 (3)
N6 0.012 (3) 0.011 (3) 0.021 (4) −0.004 (2) 0.005 (3) −0.007 (3)
N7 0.019 (3) 0.020 (3) 0.007 (3) −0.003 (3) −0.004 (3) −0.003 (2)
N8 0.020 (3) 0.015 (3) 0.024 (4) 0.003 (3) −0.008 (3) −0.009 (3)
C1 0.029 (5) 0.024 (4) 0.021 (5) −0.007 (4) −0.007 (4) −0.002 (3)
C2 0.026 (4) 0.023 (4) 0.028 (5) −0.003 (4) −0.005 (4) −0.002 (4)
C3 0.020 (4) 0.009 (3) 0.020 (4) −0.001 (3) 0.004 (3) −0.001 (3)
C4 0.016 (4) 0.015 (3) 0.020 (4) −0.002 (3) −0.010 (3) −0.002 (3)
C5 0.024 (4) 0.020 (4) 0.023 (4) −0.003 (3) −0.011 (3) −0.002 (3)
C6 0.028 (4) 0.014 (3) 0.015 (4) −0.007 (3) −0.005 (3) −0.008 (3)
C7 0.024 (4) 0.011 (3) 0.014 (4) −0.004 (3) −0.007 (3) −0.003 (3)
C8 0.016 (4) 0.018 (4) 0.027 (5) −0.001 (3) −0.007 (3) −0.006 (3)
C9 0.019 (4) 0.019 (4) 0.027 (5) 0.002 (3) −0.008 (3) −0.005 (3)
C10 0.041 (5) 0.016 (4) 0.013 (4) −0.014 (4) −0.012 (4) 0.006 (3)
C11 0.030 (4) 0.015 (3) 0.017 (4) −0.010 (3) −0.006 (3) −0.004 (3)
C12 0.027 (4) 0.022 (4) 0.014 (4) −0.005 (3) −0.011 (3) −0.002 (3)
C13 0.019 (4) 0.013 (3) 0.012 (4) −0.005 (3) 0.000 (3) −0.001 (3)
C14 0.023 (4) 0.019 (4) 0.020 (4) −0.005 (3) −0.004 (3) −0.001 (3)
C15 0.021 (4) 0.010 (3) 0.020 (4) −0.004 (3) −0.008 (3) −0.003 (3)
C16 0.021 (4) 0.010 (3) 0.023 (4) −0.003 (3) −0.006 (3) −0.008 (3)
C17 0.018 (4) 0.017 (4) 0.025 (5) −0.004 (3) −0.004 (3) −0.006 (3)
C18 0.025 (4) 0.011 (3) 0.016 (4) −0.007 (3) −0.010 (3) −0.001 (3)
C19 0.014 (4) 0.020 (4) 0.007 (4) 0.001 (3) −0.001 (3) 0.000 (3)
C20 0.023 (4) 0.019 (4) 0.025 (5) 0.000 (3) −0.006 (3) −0.014 (3)
C21 0.022 (4) 0.029 (4) 0.011 (4) 0.000 (3) −0.007 (3) −0.002 (3)
C22 0.022 (4) 0.023 (4) 0.015 (4) −0.006 (3) −0.005 (3) −0.003 (3)
C23 0.015 (4) 0.025 (4) 0.020 (4) −0.010 (3) −0.005 (3) −0.011 (3)
C24 0.014 (4) 0.012 (3) 0.015 (4) −0.002 (3) −0.001 (3) 0.003 (3)

Geometric parameters (Å, °)

Hg1—N2 2.441 (6) C5—H5A 0.9800
Hg1—S2 2.5202 (19) C5—H5B 0.9800
Hg1—N1 2.525 (6) C5—H5C 0.9800
Hg1—S4 2.6682 (18) C7—C12 1.382 (10)
Hg1—I1 2.7505 (8) C7—C8 1.417 (9)
S1—C2 1.693 (8) C8—C9 1.383 (10)
S1—C3 1.730 (7) C8—H8 0.9500
S2—C6 1.749 (7) C9—C10 1.383 (10)
S3—C14 1.706 (8) C9—H9 0.9500
S3—C15 1.730 (7) C10—C11 1.394 (10)
S4—C18 1.685 (7) C10—H10 0.9500
N1—C3 1.299 (9) C11—C12 1.392 (9)
N1—C1 1.341 (9) C11—H11 0.9500
N2—C4 1.287 (8) C12—H12 0.9500
N2—N3 1.361 (8) C13—C14 1.344 (9)
N3—C6 1.321 (9) C13—H13 0.9500
N4—C6 1.366 (9) C14—H14 0.9500
N4—C7 1.403 (8) C15—C16 1.450 (10)
N4—H4N 0.8800 C16—C17 1.503 (9)
N5—C15 1.326 (9) C17—H17A 0.9800
N5—C13 1.370 (9) C17—H17B 0.9800
N6—C16 1.304 (8) C17—H17C 0.9800
N6—N7 1.376 (7) C19—C24 1.372 (9)
N7—C18 1.342 (8) C19—C20 1.382 (9)
N7—H7N 0.8800 C20—C21 1.393 (9)
N8—C18 1.340 (9) C20—H20 0.9500
N8—C19 1.454 (8) C21—C22 1.367 (10)
N8—H8N 0.8800 C21—H21 0.9500
C1—C2 1.364 (10) C22—C23 1.382 (9)
C1—H1 0.9500 C22—H22 0.9500
C2—H2 0.9500 C23—C24 1.380 (9)
C3—C4 1.468 (10) C23—H23 0.9500
C4—C5 1.503 (9) C24—H24 0.9500
N2—Hg1—S2 73.61 (13) N4—C7—C8 124.5 (6)
N2—Hg1—N1 66.52 (19) C9—C8—C7 118.9 (7)
S2—Hg1—N1 137.91 (14) C9—C8—H8 120.5
N2—Hg1—S4 101.14 (13) C7—C8—H8 120.5
S2—Hg1—S4 106.40 (6) C8—C9—C10 122.3 (7)
N1—Hg1—S4 94.22 (13) C8—C9—H9 118.8
N2—Hg1—I1 143.13 (13) C10—C9—H9 118.8
S2—Hg1—I1 113.54 (4) C9—C10—C11 118.6 (7)
N1—Hg1—I1 91.86 (13) C9—C10—H10 120.7
S4—Hg1—I1 110.31 (4) C11—C10—H10 120.7
C2—S1—C3 89.6 (4) C12—C11—C10 120.1 (7)
C6—S2—Hg1 99.8 (2) C12—C11—H11 120.0
C14—S3—C15 89.6 (4) C10—C11—H11 120.0
C18—S4—Hg1 101.0 (2) C7—C12—C11 121.3 (7)
C3—N1—C1 112.0 (6) C7—C12—H12 119.4
C3—N1—Hg1 113.2 (5) C11—C12—H12 119.4
C1—N1—Hg1 134.8 (5) C14—C13—N5 115.8 (6)
C4—N2—N3 116.5 (6) C14—C13—H13 122.1
C4—N2—Hg1 121.9 (5) N5—C13—H13 122.1
N3—N2—Hg1 121.5 (4) C13—C14—S3 110.5 (6)
C6—N3—N2 113.7 (6) C13—C14—H14 124.7
C6—N4—C7 133.0 (6) S3—C14—H14 124.7
C6—N4—H4N 113.5 N5—C15—C16 125.3 (6)
C7—N4—H4N 113.5 N5—C15—S3 113.5 (5)
C15—N5—C13 110.6 (6) C16—C15—S3 121.1 (5)
C16—N6—N7 117.3 (6) N6—C16—C15 126.4 (6)
C18—N7—N6 119.7 (6) N6—C16—C17 115.7 (6)
C18—N7—H7N 120.1 C15—C16—C17 117.9 (6)
N6—N7—H7N 120.1 C16—C17—H17A 109.5
C18—N8—C19 125.5 (6) C16—C17—H17B 109.5
C18—N8—H8N 117.2 H17A—C17—H17B 109.5
C19—N8—H8N 117.2 C16—C17—H17C 109.5
N1—C1—C2 115.3 (7) H17A—C17—H17C 109.5
N1—C1—H1 122.3 H17B—C17—H17C 109.5
C2—C1—H1 122.3 N8—C18—N7 115.6 (6)
C1—C2—S1 109.8 (6) N8—C18—S4 124.3 (5)
C1—C2—H2 125.1 N7—C18—S4 120.0 (5)
S1—C2—H2 125.1 C24—C19—C20 121.1 (6)
N1—C3—C4 124.1 (6) C24—C19—N8 118.4 (6)
N1—C3—S1 113.3 (5) C20—C19—N8 120.3 (6)
C4—C3—S1 122.5 (6) C19—C20—C21 118.8 (7)
N2—C4—C3 114.2 (6) C19—C20—H20 120.6
N2—C4—C5 125.1 (7) C21—C20—H20 120.6
C3—C4—C5 120.7 (6) C22—C21—C20 120.2 (7)
C4—C5—H5A 109.5 C22—C21—H21 119.9
C4—C5—H5B 109.5 C20—C21—H21 119.9
H5A—C5—H5B 109.5 C21—C22—C23 120.3 (7)
C4—C5—H5C 109.5 C21—C22—H22 119.8
H5A—C5—H5C 109.5 C23—C22—H22 119.8
H5B—C5—H5C 109.5 C24—C23—C22 120.1 (6)
N3—C6—N4 118.2 (6) C24—C23—H23 120.0
N3—C6—S2 129.1 (6) C22—C23—H23 120.0
N4—C6—S2 112.7 (5) C19—C24—C23 119.4 (6)
C12—C7—N4 116.6 (6) C19—C24—H24 120.3
C12—C7—C8 118.9 (7) C23—C24—H24 120.3
N2—Hg1—S2—C6 −10.2 (3) N2—N3—C6—N4 179.6 (5)
N1—Hg1—S2—C6 −29.3 (3) N2—N3—C6—S2 −0.8 (9)
S4—Hg1—S2—C6 86.9 (2) C7—N4—C6—N3 5.6 (11)
I1—Hg1—S2—C6 −151.6 (2) C7—N4—C6—S2 −174.0 (6)
N2—Hg1—S4—C18 −66.7 (3) Hg1—S2—C6—N3 11.2 (7)
S2—Hg1—S4—C18 −142.7 (3) Hg1—S2—C6—N4 −169.2 (4)
N1—Hg1—S4—C18 0.1 (3) C6—N4—C7—C12 178.0 (7)
I1—Hg1—S4—C18 93.7 (3) C6—N4—C7—C8 −0.1 (11)
N2—Hg1—N1—C3 2.4 (4) C12—C7—C8—C9 −1.5 (10)
S2—Hg1—N1—C3 22.4 (6) N4—C7—C8—C9 176.6 (6)
S4—Hg1—N1—C3 −97.9 (5) C7—C8—C9—C10 0.0 (10)
I1—Hg1—N1—C3 151.6 (4) C8—C9—C10—C11 1.2 (10)
N2—Hg1—N1—C1 −176.8 (7) C9—C10—C11—C12 −0.9 (10)
S2—Hg1—N1—C1 −156.8 (5) N4—C7—C12—C11 −176.5 (6)
S4—Hg1—N1—C1 82.9 (6) C8—C7—C12—C11 1.8 (10)
I1—Hg1—N1—C1 −27.6 (6) C10—C11—C12—C7 −0.6 (10)
S2—Hg1—N2—C4 −168.3 (5) C15—N5—C13—C14 0.5 (8)
N1—Hg1—N2—C4 −2.1 (5) N5—C13—C14—S3 −1.0 (8)
S4—Hg1—N2—C4 87.7 (5) C15—S3—C14—C13 1.0 (5)
I1—Hg1—N2—C4 −60.8 (6) C13—N5—C15—C16 177.9 (6)
S2—Hg1—N2—N3 14.3 (4) C13—N5—C15—S3 0.3 (7)
N1—Hg1—N2—N3 −179.5 (5) C14—S3—C15—N5 −0.7 (5)
S4—Hg1—N2—N3 −89.7 (4) C14—S3—C15—C16 −178.4 (6)
I1—Hg1—N2—N3 121.8 (4) N7—N6—C16—C15 3.3 (10)
C4—N2—N3—C6 170.4 (6) N7—N6—C16—C17 −177.1 (5)
Hg1—N2—N3—C6 −12.1 (7) N5—C15—C16—N6 −1.2 (11)
C16—N6—N7—C18 −175.4 (6) S3—C15—C16—N6 176.2 (5)
C3—N1—C1—C2 −0.8 (9) N5—C15—C16—C17 179.2 (6)
Hg1—N1—C1—C2 178.4 (5) S3—C15—C16—C17 −3.4 (8)
N1—C1—C2—S1 −0.1 (8) C19—N8—C18—N7 −176.6 (6)
C3—S1—C2—C1 0.6 (6) C19—N8—C18—S4 6.9 (10)
C1—N1—C3—C4 176.5 (6) N6—N7—C18—N8 9.3 (9)
Hg1—N1—C3—C4 −2.9 (8) N6—N7—C18—S4 −174.1 (4)
C1—N1—C3—S1 1.2 (7) Hg1—S4—C18—N8 −109.2 (6)
Hg1—N1—C3—S1 −178.1 (3) Hg1—S4—C18—N7 74.5 (5)
C2—S1—C3—N1 −1.1 (5) C18—N8—C19—C24 −116.1 (7)
C2—S1—C3—C4 −176.4 (6) C18—N8—C19—C20 68.1 (9)
N3—N2—C4—C3 179.0 (5) C24—C19—C20—C21 1.5 (11)
Hg1—N2—C4—C3 1.5 (8) N8—C19—C20—C21 177.1 (6)
N3—N2—C4—C5 −1.2 (9) C19—C20—C21—C22 −2.1 (11)
Hg1—N2—C4—C5 −178.7 (5) C20—C21—C22—C23 2.5 (11)
N1—C3—C4—N2 1.2 (10) C21—C22—C23—C24 −2.4 (11)
S1—C3—C4—N2 175.9 (5) C20—C19—C24—C23 −1.3 (10)
N1—C3—C4—C5 −178.7 (6) N8—C19—C24—C23 −177.0 (6)
S1—C3—C4—C5 −3.9 (9) C22—C23—C24—C19 1.8 (10)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N7—H7N···N5 0.88 1.97 2.667 (8) 135
N4—H4N···S2i 0.88 2.69 3.553 (6) 167

Symmetry codes: (i) −x, −y+2, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: VM2089).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053681101974X/vm2089sup1.cif

e-67-0m816-sup1.cif (25.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681101974X/vm2089Isup2.hkl

e-67-0m816-Isup2.hkl (279.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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