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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Sep 27;64(Pt 10):m1339–m1340. doi: 10.1107/S160053680803081X

(4,7-Diphenyl-1,10-phenanthroline-κ2 N,N′)diiodidomercury(II)

Mohammad Yousefi a, Rabin Rashidi Vahid a, Vahid Amani a,*, Mansour Arab Chamjangali b, Hamid Reza Khavasi c
PMCID: PMC2959289  PMID: 21201072

Abstract

In the mol­ecule of the title compound, [HgI2(C24H16N2)], the HgII atom is four-coordinated in a distorted tetra­hedral configuration by two N atoms from the bidentate 4,7-diphenyl-1,10-phenanthroline and two iodide ligands. There is a π–π contact between the pyridine and phenyl rings [centroid-to-centroid distance = 4.2387 (4) Å].

Related literature

For related literature, see: Ahmadi, Amani et al. (2008); Ahmadi, Kalateh, Ebadi et al. (2008); Ahmadi, Kalateh, Abedi et al. (2008); Ahmadi, Khalighi et al. (2008); Khalighi et al. (2008); Khavasi et al. (2008); Tadayon Pour et al. (2008); Yousefi, Khalighi et al. (2008). For related structures, see: Chen et al. (2006); Freire et al. (1999); Htoon & Ladd (1976); Yousefi, Tadayon Pour et al. (2008).graphic file with name e-64-m1339-scheme1.jpg

Experimental

Crystal data

  • [HgI2(C24H16N2)]

  • M r = 786.78

  • Monoclinic, Inline graphic

  • a = 16.673 (3) Å

  • b = 8.8964 (18) Å

  • c = 16.823 (3) Å

  • β = 109.26 (3)°

  • V = 2355.7 (9) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 9.17 mm−1

  • T = 298 (2) K

  • 0.50 × 0.48 × 0.28 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: numerical shape of crystal determined optically (X-SHAPE and X-RED; Stoe & Cie, 2005)T min = 0.016, T max = 0.080

  • 19129 measured reflections

  • 6340 independent reflections

  • 5356 reflections with I > 2σ(I)

  • R int = 0.094

Refinement

  • R[F 2 > 2σ(F 2)] = 0.067

  • wR(F 2) = 0.183

  • S = 1.23

  • 6340 reflections

  • 263 parameters

  • H-atom parameters constrained

  • Δρmax = 1.49 e Å−3

  • Δρmin = −1.10 e Å−3

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053680803081X/hk2540sup1.cif

e-64-m1339-sup1.cif (21.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053680803081X/hk2540Isup2.hkl

e-64-m1339-Isup2.hkl (304.1KB, hkl)

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

Table 1. Selected geometric parameters (Å, °).

I1—Hg1 2.6441 (8)
I2—Hg1 2.6555 (9)
N1—Hg1 2.425 (7)
N2—Hg1 2.399 (7)
N2—Hg1—N1 69.4 (2)
N2—Hg1—I1 104.08 (17)
N1—Hg1—I1 110.65 (19)
N2—Hg1—I2 107.53 (17)
N1—Hg1—I2 103.11 (19)
I1—Hg1—I2 139.97 (3)

Acknowledgments

We are grateful to the Islamic Azad University, Shahr-e-Rey Branch, for financial support.

supplementary crystallographic information

Comment

Recently, we reported the syntheses and crystal structures of [Zn(5,5'-dmbpy)Cl2], (II), (Khalighi et al., 2008), [Zn(6-mbpy)Cl2], (III), (Ahmadi, Kalateh, Abedi et al., 2008), [Cd(5,5'-dmbpy)(µ-Cl)2]n, (IV), (Ahmadi, Khalighi et al., 2008), [Hg(5,5'-dmbpy)I2], (V), (Tadayon Pour et al., 2008), [In(4,4'-dmbpy)Cl3(DMSO)], (VI), (Ahmadi, Kalateh, Ebadi et al., 2008), [Cu(5,5'-dcbpy)(en)(H2O)2].2.5H2O, (VII), (Yousefi, Khalighi et al., 2008), [Au(dmphen)Cl2][AuCl4], (VIII), (Ahmadi, Amani et al., 2008), and {[HgCl(dm4bt)]2(µ-Cl)2}, (IX), (Khavasi et al., 2008). [where 5,5'-dmbpy is 5,5'-dimethyl-2,2'-bipyridine, 6-mbpy is 6-methyl-2,2'-bipyridine, 4,4'-dmbpy is 4,4'-dimethyl-2,2'-bi- pyridine, DMSO is dimethyl sulfoxide, 5,5'-dcbpy is 2,2'-bipyridine-5,5'-di- carboxylate, en is ethylenediamine, dmphen is 4,7-diphenyl-1,10- phenanthroline and dm4bt is 2,2'-dimethyl-4,4'-bithiazole]. There are several HgII complexes, with formula, [HgI2(N—N)], such as [HgI2(bipy)], (X), [HgI2(phen)], (XI) and [HgI2(2,9-dmphen)], (XII), (Freire et al., 1999), [HgI2(bipy)][HgI2], (XIII), (Chen et al., 2006), [HgI2(4,4'-dmbpy)], (XIV), (Yousefi, Tadayon Pour et al., 2008) and [HgI2(TMDA)], (XV), (Htoon & Ladd, 1976) [where bipy is 2,2'-bipyridine, phen is 1,10-phenanthroline, dmphen is 2,9-dimethyl-1,10-phenanthroline and TMDA is tetramethylethylenediamine] have been synthesized and characterized by single crystal X-ray diffraction methods. We report herein the synthesis and crystal structure of the title compound, (I).

In the title compound, (Fig. 1), the HgII atom is four-coordinated in a distorted tetrahedral configuration by two N atoms from 4,7-diphenyl-1,10-phenanthroline and two I atoms. The Hg—I and Hg—N bond lengths and angles (Table 1) are within normal ranges, as in (X), (XI) and (XIV).

In the crystal structure, the π–π contact (Fig. 2) between the pyridine and phenyl rings, Cg3···Cg4i [symmetry code: (i) 3/2 - x, -1/2 + y, 1/2 - z, where Cg3 and Cg4 are centroids of the rings (N1/C1–C3/C10/C24) and (C4–C9), respectively] may stabilize the structure, with centroid–centroid distance of 4.2387 (4) Å.

Experimental

For the preparation of the title compound, a solution of 4,7-diphenyl-1,10-phenanthroline (0.36 g, 1.10 mmol) in acetonitrile (20 ml) was added to a solution of HgI2 (0.50 g, 1.10 mmol) in methanol (20 ml) and the resulting colorless solution was stirred for 20 min at 313 K. This solution was left to evaporate slowly at room temperature. After one week, colorless block crystals of the title compound were isolated (yield; 0.62 g, 71.6%).

Refinement

H atoms were positioned geometrically, with C—H = 0.93 Å for aromatic H and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title molecule, with the atom-numbering scheme. Displacement ellipsoids are drawn at the 40% probability level.

Fig. 2.

Fig. 2.

A partial packing diagram of the title compound.

Crystal data

[HgI2(C24H16N2)] F(000) = 1440
Mr = 786.78 Dx = 2.218 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 2356 reflections
a = 16.673 (3) Å θ = 2.1–29.3°
b = 8.8964 (18) Å µ = 9.17 mm1
c = 16.823 (3) Å T = 298 K
β = 109.26 (3)° Block, colourless
V = 2355.7 (9) Å3 0.50 × 0.48 × 0.28 mm
Z = 4

Data collection

Bruker SMART CCD area-detector diffractometer 6340 independent reflections
Radiation source: fine-focus sealed tube 5356 reflections with I > 2σ(I)
graphite Rint = 0.094
φ and ω scans θmax = 29.3°, θmin = 2.1°
Absorption correction: numerical shape of crystal determined optically h = −22→19
Tmin = 0.016, Tmax = 0.080 k = −12→12
19129 measured reflections l = −22→23

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)] = 0.067 H-atom parameters constrained
wR(F2) = 0.183 w = 1/[σ2(Fo2) + (0.085P)2 + 4.523P] where P = (Fo2 + 2Fc2)/3
S = 1.23 (Δ/σ)max = 0.009
6340 reflections Δρmax = 1.49 e Å3
263 parameters Δρmin = −1.11 e Å3
0 restraints Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0086 (6)

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 0.35746 (2) 0.27882 (4) 0.10505 (2) 0.05561 (16)
I1 0.29465 (5) 0.55290 (7) 0.06892 (4) 0.0694 (2)
I2 0.32177 (5) −0.00283 (7) 0.05316 (5) 0.0736 (2)
N1 0.5115 (5) 0.2845 (9) 0.1529 (4) 0.0545 (17)
N2 0.4136 (4) 0.2750 (8) 0.2559 (5) 0.0495 (14)
C1 0.5583 (7) 0.2946 (13) 0.1039 (6) 0.065 (2)
H1 0.5314 0.3098 0.0466 0.078*
C2 0.6448 (7) 0.2837 (13) 0.1335 (6) 0.068 (3)
H2 0.6749 0.2930 0.0960 0.081*
C3 0.6884 (6) 0.2594 (10) 0.2172 (6) 0.0524 (18)
C4 0.7831 (6) 0.2515 (11) 0.2502 (7) 0.0550 (19)
C5 0.8260 (8) 0.1623 (13) 0.2086 (9) 0.076 (3)
H5 0.7963 0.1118 0.1592 0.091*
C6 0.9151 (9) 0.1506 (14) 0.2430 (12) 0.101 (5)
H6 0.9442 0.0869 0.2182 0.122*
C7 0.9601 (9) 0.2342 (18) 0.3143 (12) 0.093 (4)
H7 1.0190 0.2274 0.3362 0.112*
C8 0.9178 (7) 0.3244 (19) 0.3510 (9) 0.086 (3)
H8 0.9477 0.3815 0.3976 0.103*
C9 0.8304 (6) 0.3327 (15) 0.3199 (7) 0.068 (2)
H9 0.8024 0.3948 0.3467 0.082*
C10 0.6399 (5) 0.2429 (10) 0.2719 (5) 0.0487 (16)
C11 0.6750 (5) 0.2082 (11) 0.3592 (6) 0.0545 (19)
H11 0.7324 0.1843 0.3816 0.065*
C12 0.6274 (5) 0.2090 (11) 0.4100 (5) 0.0534 (19)
H12 0.6527 0.1855 0.4667 0.064*
C13 0.5399 (5) 0.2448 (8) 0.3793 (5) 0.0411 (14)
C14 0.4883 (5) 0.2524 (9) 0.4320 (5) 0.0456 (15)
C15 0.5272 (6) 0.2456 (9) 0.5252 (5) 0.0478 (16)
C16 0.5965 (6) 0.3362 (12) 0.5672 (5) 0.059 (2)
H16 0.6176 0.4041 0.5370 0.071*
C17 0.6343 (7) 0.3255 (15) 0.6545 (6) 0.071 (3)
H17 0.6798 0.3875 0.6824 0.085*
C18 0.6042 (9) 0.2228 (14) 0.6993 (7) 0.078 (3)
H18 0.6300 0.2140 0.7573 0.094*
C19 0.5350 (9) 0.1323 (12) 0.6573 (7) 0.078 (3)
H19 0.5150 0.0622 0.6873 0.093*
C20 0.4958 (8) 0.1460 (11) 0.5713 (6) 0.062 (2)
H20 0.4482 0.0881 0.5441 0.075*
C21 0.4019 (6) 0.2684 (11) 0.3937 (6) 0.058 (2)
H21 0.3664 0.2743 0.4261 0.069*
C22 0.3682 (5) 0.2756 (11) 0.3070 (6) 0.058 (2)
H22 0.3094 0.2814 0.2830 0.070*
C23 0.5005 (5) 0.2597 (8) 0.2918 (5) 0.0420 (14)
C24 0.5506 (5) 0.2610 (9) 0.2361 (5) 0.0463 (15)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Hg1 0.0541 (2) 0.0529 (2) 0.0461 (2) 0.00215 (13) −0.00194 (13) 0.00031 (12)
I1 0.0728 (4) 0.0484 (3) 0.0684 (4) 0.0027 (3) −0.0018 (3) −0.0002 (3)
I2 0.0846 (5) 0.0496 (3) 0.0714 (4) 0.0056 (3) 0.0051 (3) −0.0066 (3)
N1 0.049 (3) 0.072 (5) 0.036 (3) −0.006 (3) 0.006 (3) −0.002 (3)
N2 0.041 (3) 0.054 (4) 0.047 (3) 0.001 (3) 0.006 (3) 0.001 (3)
C1 0.071 (6) 0.084 (7) 0.037 (4) −0.001 (5) 0.012 (4) 0.006 (4)
C2 0.066 (6) 0.093 (8) 0.051 (5) −0.011 (5) 0.028 (4) −0.006 (5)
C3 0.052 (4) 0.057 (4) 0.052 (4) −0.005 (4) 0.022 (4) −0.006 (4)
C4 0.051 (4) 0.055 (4) 0.066 (5) 0.000 (3) 0.029 (4) 0.000 (4)
C5 0.080 (7) 0.059 (5) 0.104 (8) −0.012 (5) 0.051 (6) −0.017 (6)
C6 0.086 (8) 0.065 (6) 0.188 (16) 0.005 (6) 0.093 (10) 0.005 (9)
C7 0.060 (6) 0.107 (10) 0.113 (11) 0.008 (7) 0.028 (7) 0.028 (9)
C8 0.057 (5) 0.111 (10) 0.085 (8) −0.001 (7) 0.017 (5) 0.003 (8)
C9 0.047 (4) 0.085 (7) 0.069 (6) −0.001 (5) 0.015 (4) −0.006 (5)
C10 0.042 (3) 0.052 (4) 0.048 (4) −0.004 (3) 0.010 (3) −0.002 (3)
C11 0.038 (3) 0.073 (6) 0.049 (4) 0.005 (3) 0.009 (3) 0.010 (4)
C12 0.045 (4) 0.071 (5) 0.037 (3) 0.002 (4) 0.004 (3) 0.007 (3)
C13 0.040 (3) 0.045 (3) 0.037 (3) −0.004 (3) 0.011 (3) 0.006 (3)
C14 0.049 (4) 0.047 (3) 0.041 (3) −0.001 (3) 0.015 (3) 0.002 (3)
C15 0.057 (4) 0.047 (4) 0.040 (4) 0.000 (3) 0.016 (3) −0.004 (3)
C16 0.063 (5) 0.063 (5) 0.048 (4) −0.011 (4) 0.013 (4) −0.001 (4)
C17 0.074 (6) 0.079 (6) 0.050 (5) −0.003 (5) 0.005 (4) −0.019 (5)
C18 0.104 (9) 0.087 (8) 0.040 (4) 0.004 (7) 0.021 (5) 0.001 (5)
C19 0.128 (10) 0.060 (5) 0.058 (5) −0.010 (6) 0.048 (6) −0.008 (5)
C20 0.091 (7) 0.051 (4) 0.052 (4) −0.006 (4) 0.033 (4) −0.004 (4)
C21 0.050 (4) 0.070 (5) 0.057 (5) 0.000 (4) 0.022 (4) −0.003 (4)
C22 0.039 (4) 0.072 (6) 0.057 (5) −0.006 (4) 0.008 (3) −0.003 (4)
C23 0.040 (3) 0.042 (3) 0.040 (3) −0.001 (3) 0.007 (3) −0.001 (3)
C24 0.047 (4) 0.044 (3) 0.039 (3) −0.002 (3) 0.003 (3) 0.007 (3)

Geometric parameters (Å, °)

I1—Hg1 2.6441 (8) C11—H11 0.9300
I2—Hg1 2.6555 (9) C12—C13 1.415 (11)
N1—Hg1 2.425 (7) C12—H12 0.9300
N2—Hg1 2.399 (7) C13—C23 1.407 (10)
C1—N1 1.312 (12) C13—C14 1.426 (10)
C1—C2 1.364 (15) C14—C21 1.379 (12)
C1—H1 0.9300 C14—C15 1.487 (11)
C2—C3 1.372 (14) C15—C20 1.389 (12)
C2—H2 0.9300 C15—C16 1.394 (12)
C3—C10 1.420 (12) C16—C17 1.398 (13)
C3—C4 1.493 (13) C16—H16 0.9300
C4—C9 1.382 (15) C17—C18 1.380 (18)
C4—C5 1.401 (14) C17—H17 0.9300
C5—C6 1.409 (19) C18—C19 1.393 (18)
C5—H5 0.9300 C18—H18 0.9300
C6—C7 1.40 (2) C19—C20 1.383 (15)
C6—H6 0.9300 C19—H19 0.9300
C7—C8 1.34 (2) C20—H20 0.9300
C7—H7 0.9300 C21—C22 1.381 (14)
C8—C9 1.378 (15) C21—H21 0.9300
C8—H8 0.9300 C22—N2 1.320 (12)
C9—H9 0.9300 C22—H22 0.9300
C10—C24 1.419 (11) C23—N2 1.379 (10)
C10—C11 1.423 (12) C23—C24 1.447 (11)
C11—C12 1.345 (13) C24—N1 1.352 (10)
N2—Hg1—N1 69.4 (2) C12—C11—C10 121.7 (8)
N2—Hg1—I1 104.08 (17) C12—C11—H11 119.1
N1—Hg1—I1 110.65 (19) C10—C11—H11 119.1
N2—Hg1—I2 107.53 (17) C11—C12—C13 121.5 (7)
N1—Hg1—I2 103.11 (19) C11—C12—H12 119.2
I1—Hg1—I2 139.97 (3) C13—C12—H12 119.2
C1—N1—C24 118.5 (8) C23—C13—C12 118.2 (7)
C1—N1—Hg1 125.3 (6) C23—C13—C14 118.5 (7)
C24—N1—Hg1 115.9 (6) C12—C13—C14 123.0 (7)
C22—N2—C23 117.4 (7) C21—C14—C13 117.8 (7)
C22—N2—Hg1 125.6 (6) C21—C14—C15 121.5 (7)
C23—N2—Hg1 116.8 (5) C13—C14—C15 120.7 (7)
N1—C1—C2 122.9 (8) C20—C15—C16 119.2 (8)
N1—C1—H1 118.6 C20—C15—C14 120.0 (8)
C2—C1—H1 118.6 C16—C15—C14 120.8 (8)
C1—C2—C3 121.6 (8) C15—C16—C17 120.3 (9)
C1—C2—H2 119.2 C15—C16—H16 119.8
C3—C2—H2 119.2 C17—C16—H16 119.8
C2—C3—C10 117.4 (8) C18—C17—C16 120.0 (11)
C2—C3—C4 121.8 (8) C18—C17—H17 120.0
C10—C3—C4 120.8 (8) C16—C17—H17 120.0
C9—C4—C5 118.6 (9) C17—C18—C19 119.7 (10)
C9—C4—C3 121.9 (8) C17—C18—H18 120.2
C5—C4—C3 119.5 (9) C19—C18—H18 120.2
C4—C5—C6 118.6 (12) C20—C19—C18 120.4 (10)
C4—C5—H5 120.7 C20—C19—H19 119.8
C6—C5—H5 120.7 C18—C19—H19 119.8
C7—C6—C5 120.5 (11) C19—C20—C15 120.3 (10)
C7—C6—H6 119.8 C19—C20—H20 119.8
C5—C6—H6 119.8 C15—C20—H20 119.8
C8—C7—C6 119.7 (12) C14—C21—C22 119.8 (8)
C8—C7—H7 120.1 C14—C21—H21 120.1
C6—C7—H7 120.1 C22—C21—H21 120.1
C7—C8—C9 120.5 (14) N2—C22—C21 124.5 (8)
C7—C8—H8 119.8 N2—C22—H22 117.7
C9—C8—H8 119.8 C21—C22—H22 117.7
C8—C9—C4 122.0 (11) N2—C23—C13 121.9 (7)
C8—C9—H9 119.0 N2—C23—C24 117.6 (7)
C4—C9—H9 119.0 C13—C23—C24 120.5 (7)
C24—C10—C3 117.0 (8) N1—C24—C10 122.6 (8)
C24—C10—C11 118.7 (7) N1—C24—C23 119.2 (7)
C3—C10—C11 124.2 (8) C10—C24—C23 118.2 (7)
C1—N1—Hg1—N2 −177.4 (9) C21—C14—C15—C20 51.1 (12)
C24—N1—Hg1—N2 9.2 (6) C13—C14—C15—C20 −129.9 (9)
C1—N1—Hg1—I1 −79.6 (9) C21—C14—C15—C16 −130.2 (10)
C24—N1—Hg1—I1 107.0 (6) C13—C14—C15—C16 48.7 (12)
C1—N1—Hg1—I2 78.6 (9) C20—C15—C16—C17 0.7 (15)
C24—N1—Hg1—I2 −94.9 (6) C14—C15—C16—C17 −177.9 (9)
C22—N2—Hg1—N1 177.5 (8) C15—C16—C17—C18 1.3 (17)
C23—N2—Hg1—N1 −7.5 (5) C16—C17—C18—C19 −1.3 (19)
C22—N2—Hg1—I1 70.4 (8) C17—C18—C19—C20 −0.7 (19)
C23—N2—Hg1—I1 −114.6 (5) C18—C19—C20—C15 2.8 (17)
C22—N2—Hg1—I2 −84.7 (7) C16—C15—C20—C19 −2.7 (15)
C23—N2—Hg1—I2 90.3 (6) C14—C15—C20—C19 175.9 (9)
N1—C1—C2—C3 0.8 (19) C13—C14—C21—C22 0.4 (14)
C1—C2—C3—C10 1.2 (16) C15—C14—C21—C22 179.4 (9)
C1—C2—C3—C4 −178.3 (10) C14—C21—C22—N2 −3.1 (16)
C2—C3—C4—C9 130.8 (11) C12—C13—C23—N2 171.4 (8)
C10—C3—C4—C9 −48.7 (14) C14—C13—C23—N2 −2.7 (11)
C2—C3—C4—C5 −47.7 (14) C12—C13—C23—C24 −9.3 (11)
C10—C3—C4—C5 132.8 (10) C14—C13—C23—C24 176.6 (7)
C9—C4—C5—C6 4.5 (17) C3—C10—C24—N1 3.7 (13)
C3—C4—C5—C6 −177.0 (10) C11—C10—C24—N1 −175.7 (8)
C4—C5—C6—C7 −4(2) C3—C10—C24—C23 −174.0 (7)
C5—C6—C7—C8 1(2) C11—C10—C24—C23 6.7 (12)
C6—C7—C8—C9 1(2) N2—C23—C24—N1 3.3 (11)
C7—C8—C9—C4 −1(2) C13—C23—C24—N1 −176.0 (7)
C5—C4—C9—C8 −2.2 (18) N2—C23—C24—C10 −179.0 (7)
C3—C4—C9—C8 179.3 (12) C13—C23—C24—C10 1.7 (11)
C2—C3—C10—C24 −3.3 (13) C21—C22—N2—C23 2.8 (14)
C4—C3—C10—C24 176.3 (8) C21—C22—N2—Hg1 177.8 (7)
C2—C3—C10—C11 176.0 (9) C13—C23—N2—C22 0.2 (12)
C4—C3—C10—C11 −4.4 (14) C24—C23—N2—C22 −179.2 (8)
C24—C10—C11—C12 −7.6 (14) C13—C23—N2—Hg1 −175.2 (6)
C3—C10—C11—C12 173.1 (9) C24—C23—N2—Hg1 5.5 (9)
C10—C11—C12—C13 −0.1 (15) C2—C1—N1—C24 −0.6 (16)
C11—C12—C13—C23 8.6 (13) C2—C1—N1—Hg1 −173.9 (9)
C11—C12—C13—C14 −177.5 (9) C10—C24—N1—C1 −1.7 (14)
C23—C13—C14—C21 2.3 (12) C23—C24—N1—C1 175.9 (9)
C12—C13—C14—C21 −171.5 (8) C10—C24—N1—Hg1 172.2 (6)
C23—C13—C14—C15 −176.7 (7) C23—C24—N1—Hg1 −10.2 (10)
C12—C13—C14—C15 9.5 (12)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HK2540).

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 I, global. DOI: 10.1107/S160053680803081X/hk2540sup1.cif

e-64-m1339-sup1.cif (21.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053680803081X/hk2540Isup2.hkl

e-64-m1339-Isup2.hkl (304.1KB, hkl)

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


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