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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2015 Aug 6;71(Pt 9):m154–m155. doi: 10.1107/S2056989015014176

Crystal structure of bis­[μ-1,2-bis­(di­phenyl­phosphan­yl)ethane-κ2 P:P′]bis[(N,N′-di­ethyl­thio­urea-κS)iodidocopper(I)]

Ladawan Khongsichan a, Arunpatcha Nimthong-Roldán b, Chaveng Pakawatchai a, Sumpun Wongnawa a,*
PMCID: PMC4555430  PMID: 26396862

Abstract

The binuclear title complex, [Cu2I2(C26H24P2)2(C5H12N2S)2], lies about an inversion centre. The CuI atom displays a distorted tetra­hedral coordination geometry defined by one S atom of an N,N′-di­ethyl­thio­urea ligand, two P atoms derived from two bridging 1,2-bis­(di­phenyl­phosphan­yl)ethane (dppe) ligands and one iodide ion. The dppe ligand bridges two symmetry-related CuI ions, forming a 10-membered Cu2P4C4 ring. An intra­molecular N—H⋯I hydrogen bond is noted. In the crystal, N—H⋯I hydrogen bonds link complex mol­ecules into layers parallel to (-101).

Keywords: crystal structure; copper(I) complex; N,N′-di­ethyl­thio­urea; N—H⋯I hydrogen bonding

Related literature  

For background to the coordination chemistry of copper(I) halides and pseudohalides, see: Dennehy et al. (2011); Oshio et al. (1996); Seward et al. (2003). For their potential applications, see: Corey et al. (1987); Dias et al. (2006). For relevant examples of discrete complexes, see: Dennehy et al. (2009).graphic file with name e-71-0m154-scheme1.jpg

Experimental  

Crystal data  

  • [Cu2I2(C26H24P2)2(C5H12N2S)2]

  • M r = 1442.11

  • Monoclinic, Inline graphic

  • a = 12.2150 (8) Å

  • b = 15.1836 (9) Å

  • c = 17.1801 (10) Å

  • β = 96.414 (2)°

  • V = 3166.4 (3) Å3

  • Z = 2

  • Cu Kα radiation

  • μ = 10.37 mm−1

  • T = 100 K

  • 0.16 × 0.15 × 0.08 mm

Data collection  

  • Bruker Prospector CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2013) T min = 0.433, T max = 0.753

  • 23236 measured reflections

  • 5564 independent reflections

  • 5556 reflections with I > 2σ(I)

  • R int = 0.028

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.025

  • wR(F 2) = 0.063

  • S = 1.13

  • 5564 reflections

  • 345 parameters

  • H-atom parameters constrained

  • Δρmax = 0.98 e Å−3

  • Δρmin = −0.92 e Å−3

Data collection: APEX2 (Bruker, 2013); cell refinement: SAINT (Bruker, 2013); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2015 (Sheldrick, 2015) and SHELXLE (Hübschle et al., 2011); molecular graphics: Mercury (Macrae et al., 2008); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989015014176/tk5371sup1.cif

e-71-0m154-sup1.cif (801.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015014176/tk5371Isup2.hkl

e-71-0m154-Isup2.hkl (442.7KB, hkl)

. DOI: 10.1107/S2056989015014176/tk5371fig1.tif

The structure of title complex with displacement ellipsoids drawn at the 50% propbability level. All H atoms are omitted for clarity.

. DOI: 10.1107/S2056989015014176/tk5371fig2.tif

Part of the crystal structure showing intra/inter-mol­ecular N—H⋯I hydrogen bonds forming a layers as dashed lines.

CCDC reference: 1415379

Additional supporting information: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (, ).

DHA DH HA D A DHA
N1H1I1i 0.88 2.80 3.622(2) 156
N2H2I1 0.88 2.70 3.5517(19) 162

Symmetry code: (i) Inline graphic.

Acknowledgments

We gratefully acknowledge financial support from the Strategic Scholarships Fellowships Frontier Research Networks (Specific for Southern Region), the Commission on Higher Education, Ministry of Education, and the Department of Chemistry and Graduate School, Prince of Songkla University. LK would like to thank Dr Matthias Zeller of Youngstown State University, Ohio, USA, for suggestions and assistance with the X-ray structure refinement.

supplementary crystallographic information

S0.1. Synthesis and crystallization

N,N'-Di­ethyl­thio­urea (0.07 g, 0.5 mmol) was dissolved in 30 cm3 of aceto­nitrile in a round flask equipped with reflux condenser and magnetic stirrer at 333 K and then CuI (0.1 g, 0.5 mmol) was added. The mixture was stirred for 2 h. 1,2-bis­(di­phenyl­phosphanyl)ethane (0.2 g, 0.5 mmol) was added and the reaction mixture was heated under reflux for 5 h where upon the precipitate gradually disappeared. The resulting clear solution was filtered and left to evaporate at room temperature. The colorless crystals, which deposited after standing for several days were filtered off and washed with acetone and dried in vacuo (M. pt = 557 K). Elemental analysis, calculated for [Cu2I2(C26H24P2)2(C5H12N2S)2]: C, 51.59; H, 4.97; N, 3.88; S, 4.44%, found: C, 55.69; H, 5.22; N, 3.62; S, 4.61%.

S0.2. Refinement

The (-1 8 3) reflection was affected by the beam-stop and was omitted from the final cycles of refinement. H atoms bonded to C and N atoms were included in their calculated positions and were refined using a riding model using bond lengths of 0.95–0.99 Å and Uiso(H) = 1.2–1.5Ueq(C), and N—H = 0.88 Å (NH) and Uiso(H) = 1.2Ueq(N). The (-1 8 3) reflection was omitted owing to poor agreement.

S1. Comment

Coordination complexes of copper(I) halides or pseudo-halides with mixed P and S donor ligands have been of inter­est in coordination chemistry (Dennehy et al., 2011; Oshio et al., 1996; Sewead et al., 2003) due to their applications such as magnetism (Oshio et al., 1996) and biological or medicinal activities (Corey et al., 1987; Dias et al., 2006). In this work, a mixed ligand complex of copper(I) iodide with 1,2-bis­(di­phenyl­phosphanyl)ethane (dppe) and N,N'-di­ethyl­thio­urea (detu) is reported. The binuclear copper(I) complex lies across an inversion center. The µ2-dppe bridges between CuI centers leads to a 10-membered Cu2P4C4 rhomboid, see Fig. 1. The Cu1—P1 and Cu1—P2 bond lengths are 2.2681 (6) and 2.2813 (6)Å, respectively. These values are slightly shorter than the equivalent distances found in [Cu(tsac)(PPh3)2], [Cu4(tsac)4(PPh3)3], [Cu2(tsac)2(dppm)2] and [Cu4(tsac)4(dppm)2], which are in the range 2.2799 (5) and 2.3119 (5) Å (Dennehy et al., 2009). There is an intra­molecular N2—H2···I1 hydrogen bond. In the crystal, inter­molecular N1—H1···I1 hydrogen bonds link complex molecules into a two-dimensional supra­molecular network parallel to (-101) (Fig. 2. and Table 1)

Figures

Fig. 1.

Fig. 1.

The structure of title complex with displacement ellipsoids drawn at the 50% propbability level. All H atoms are omitted for clarity.

Fig. 2.

Fig. 2.

Part of the crystal structure showing intra/inter-molecular N—H···I hydrogen bonds forming a layers as dashed lines.

Crystal data

[Cu2I2(C26H24P2)2(C5H12N2S)2] F(000) = 1456
Mr = 1442.11 Dx = 1.513 Mg m3
Monoclinic, P21/n Cu Kα radiation, λ = 1.54178 Å
a = 12.2150 (8) Å Cell parameters from 9846 reflections
b = 15.1836 (9) Å θ = 3.9–66.7°
c = 17.1801 (10) Å µ = 10.37 mm1
β = 96.414 (2)° T = 100 K
V = 3166.4 (3) Å3 Block, colourless
Z = 2 0.16 × 0.15 × 0.08 mm

Data collection

Bruker Prospector CCD diffractometer 5564 independent reflections
Radiation source: I-mu-S microsource X-ray tube 5556 reflections with I > 2σ(I)
Laterally graded multilayer (Goebel) mirror monochromator Rint = 0.028
ω and phi scans θmax = 67.0°, θmin = 3.9°
Absorption correction: multi-scan (SADABS; Bruker, 2013) h = −14→12
Tmin = 0.433, Tmax = 0.753 k = −18→17
23236 measured reflections l = −20→20

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.025 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.063 H-atom parameters constrained
S = 1.13 w = 1/[σ2(Fo2) + (0.0315P)2 + 3.4263P] where P = (Fo2 + 2Fc2)/3
5564 reflections (Δ/σ)max = 0.003
345 parameters Δρmax = 0.98 e Å3
0 restraints Δρmin = −0.92 e Å3

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
I1 0.71658 (2) 0.56133 (2) 0.16309 (2) 0.01039 (6)
Cu1 0.51704 (2) 0.64264 (2) 0.12681 (2) 0.00798 (8)
S1 0.48147 (4) 0.74104 (3) 0.22620 (3) 0.01238 (12)
P1 0.39142 (4) 0.53264 (3) 0.12684 (3) 0.00711 (11)
P2 0.52134 (4) 0.70642 (3) 0.00696 (3) 0.00768 (11)
N1 0.58767 (16) 0.88958 (13) 0.27366 (12) 0.0163 (4)
H1 0.6493 0.9171 0.2902 0.020*
N2 0.69626 (15) 0.77334 (13) 0.24764 (11) 0.0122 (4)
H2 0.7019 0.7167 0.2380 0.015*
C1 0.59546 (18) 0.80593 (15) 0.25058 (12) 0.0109 (4)
C2 0.4851 (2) 0.93892 (15) 0.27369 (17) 0.0198 (5)
H2A 0.4929 0.9817 0.3174 0.024*
H2B 0.4250 0.8977 0.2827 0.024*
C3 0.4547 (3) 0.9875 (2) 0.19789 (19) 0.0348 (7)
H3A 0.5135 1.0289 0.1891 0.052*
H3B 0.3859 1.0199 0.2007 0.052*
H3C 0.4448 0.9452 0.1546 0.052*
C4 0.79787 (18) 0.82441 (16) 0.25912 (14) 0.0149 (5)
H4A 0.8076 0.8487 0.3129 0.018*
H4B 0.7936 0.8743 0.2218 0.018*
C5 0.89514 (18) 0.76646 (16) 0.24646 (14) 0.0162 (5)
H5A 0.8813 0.7370 0.1956 0.024*
H5B 0.9055 0.7222 0.2881 0.024*
H5C 0.9617 0.8027 0.2475 0.024*
C11 0.38548 (18) 0.47611 (14) 0.22045 (13) 0.0103 (4)
C12 0.45710 (18) 0.50116 (14) 0.28549 (13) 0.0124 (4)
H12 0.5106 0.5456 0.2807 0.015*
C13 0.4500 (2) 0.46061 (16) 0.35789 (13) 0.0161 (5)
H13 0.4989 0.4777 0.4022 0.019*
C14 0.3723 (2) 0.39590 (16) 0.36541 (14) 0.0196 (5)
H14 0.3673 0.3692 0.4149 0.024*
C15 0.3015 (2) 0.36998 (17) 0.30053 (15) 0.0201 (5)
H15 0.2486 0.3250 0.3055 0.024*
C16 0.30793 (19) 0.40978 (16) 0.22830 (14) 0.0149 (5)
H16 0.2594 0.3918 0.1840 0.018*
C21 0.24971 (18) 0.57205 (14) 0.10553 (14) 0.0109 (4)
C22 0.1845 (2) 0.55542 (16) 0.03495 (15) 0.0188 (5)
H22 0.2117 0.5190 −0.0035 0.023*
C23 0.0792 (2) 0.59235 (18) 0.02086 (16) 0.0240 (5)
H23 0.0359 0.5819 −0.0277 0.029*
C24 0.0375 (2) 0.64380 (17) 0.07685 (17) 0.0246 (6)
H24 −0.0346 0.6678 0.0674 0.029*
C25 0.1021 (2) 0.66008 (18) 0.14715 (17) 0.0245 (6)
H25 0.0739 0.6953 0.1860 0.029*
C26 0.2072 (2) 0.62539 (17) 0.16094 (14) 0.0177 (5)
H26 0.2510 0.6381 0.2088 0.021*
C27 0.39162 (19) 0.44094 (13) 0.05650 (13) 0.0098 (4)
H27A 0.3228 0.4068 0.0578 0.012*
H27B 0.3910 0.4658 0.0032 0.012*
C28 0.51050 (17) 0.62207 (14) −0.07137 (12) 0.0090 (4)
H28A 0.4406 0.5891 −0.0713 0.011*
H28B 0.5110 0.6507 −0.1231 0.011*
C31 0.40910 (19) 0.78228 (15) −0.02656 (12) 0.0126 (4)
C32 0.4258 (2) 0.87216 (18) −0.03567 (19) 0.0302 (6)
H32 0.4977 0.8963 −0.0252 0.036*
C33 0.3369 (3) 0.9266 (2) −0.0601 (2) 0.0432 (8)
H33 0.3488 0.9880 −0.0658 0.052*
C34 0.2325 (3) 0.8932 (2) −0.07599 (18) 0.0343 (7)
H34 0.1728 0.9310 −0.0933 0.041*
C35 0.2148 (2) 0.8042 (2) −0.06672 (16) 0.0279 (6)
H35 0.1427 0.7805 −0.0779 0.033*
C36 0.3023 (2) 0.74917 (18) −0.04106 (15) 0.0205 (5)
H36 0.2893 0.6883 −0.0333 0.025*
C41 0.64463 (18) 0.76671 (14) −0.01297 (13) 0.0114 (4)
C42 0.7191 (2) 0.79247 (18) 0.04993 (15) 0.0239 (6)
H42 0.7029 0.7809 0.1018 0.029*
C43 0.8164 (3) 0.8347 (2) 0.03845 (17) 0.0333 (7)
H43 0.8658 0.8524 0.0823 0.040*
C44 0.8419 (2) 0.8513 (2) −0.03605 (18) 0.0315 (7)
H44 0.9092 0.8794 −0.0440 0.038*
C45 0.7686 (3) 0.8267 (3) −0.09912 (18) 0.0423 (9)
H45 0.7856 0.8383 −0.1508 0.051*
C46 0.6708 (3) 0.7853 (2) −0.08813 (15) 0.0316 (7)
H46 0.6209 0.7694 −0.1323 0.038*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
I1 0.01029 (9) 0.00674 (9) 0.01363 (9) 0.00312 (4) −0.00089 (6) −0.00191 (4)
Cu1 0.00902 (16) 0.00693 (16) 0.00820 (15) −0.00076 (11) 0.00197 (12) −0.00022 (11)
S1 0.0096 (2) 0.0109 (3) 0.0175 (3) −0.00149 (19) 0.0049 (2) −0.0069 (2)
P1 0.0074 (2) 0.0068 (3) 0.0076 (2) −0.00001 (19) 0.00262 (19) −0.00070 (19)
P2 0.0097 (3) 0.0057 (2) 0.0078 (2) 0.00084 (19) 0.00168 (19) 0.00046 (19)
N1 0.0105 (9) 0.0122 (10) 0.0262 (11) −0.0006 (8) 0.0025 (8) −0.0094 (8)
N2 0.0100 (9) 0.0092 (9) 0.0174 (9) 0.0010 (7) 0.0012 (7) −0.0073 (7)
C1 0.0121 (10) 0.0117 (11) 0.0096 (10) 0.0003 (8) 0.0036 (8) −0.0022 (8)
C2 0.0172 (12) 0.0122 (12) 0.0315 (14) 0.0030 (9) 0.0091 (11) −0.0075 (9)
C3 0.0314 (15) 0.0299 (16) 0.0441 (17) 0.0096 (13) 0.0083 (13) 0.0068 (13)
C4 0.0112 (11) 0.0149 (11) 0.0185 (11) −0.0007 (9) 0.0012 (9) −0.0063 (9)
C5 0.0105 (10) 0.0172 (12) 0.0208 (12) −0.0002 (9) 0.0011 (9) −0.0089 (9)
C11 0.0117 (10) 0.0088 (10) 0.0112 (10) 0.0041 (8) 0.0052 (8) 0.0014 (8)
C12 0.0144 (10) 0.0090 (10) 0.0146 (11) 0.0020 (8) 0.0051 (9) −0.0004 (8)
C13 0.0214 (12) 0.0149 (11) 0.0124 (11) 0.0049 (10) 0.0030 (9) −0.0003 (9)
C14 0.0248 (12) 0.0197 (13) 0.0164 (11) 0.0054 (10) 0.0115 (10) 0.0085 (9)
C15 0.0170 (11) 0.0186 (12) 0.0260 (13) −0.0024 (10) 0.0088 (10) 0.0076 (10)
C16 0.0106 (10) 0.0166 (12) 0.0181 (11) −0.0015 (9) 0.0036 (9) 0.0029 (9)
C21 0.0088 (10) 0.0093 (10) 0.0151 (11) −0.0017 (8) 0.0033 (9) 0.0016 (8)
C22 0.0156 (12) 0.0219 (13) 0.0185 (12) 0.0035 (9) 0.0002 (10) −0.0044 (9)
C23 0.0166 (12) 0.0239 (14) 0.0297 (14) 0.0046 (11) −0.0059 (10) 0.0002 (11)
C24 0.0120 (11) 0.0191 (13) 0.0425 (16) 0.0048 (10) 0.0023 (11) 0.0007 (11)
C25 0.0191 (12) 0.0202 (13) 0.0358 (15) 0.0057 (10) 0.0105 (11) −0.0064 (11)
C26 0.0175 (12) 0.0161 (12) 0.0200 (12) 0.0017 (9) 0.0042 (10) −0.0048 (9)
C27 0.0112 (11) 0.0082 (11) 0.0101 (10) 0.0002 (8) 0.0017 (8) −0.0020 (7)
C28 0.0111 (10) 0.0075 (10) 0.0085 (10) 0.0002 (8) 0.0016 (8) −0.0017 (8)
C31 0.0175 (11) 0.0123 (11) 0.0088 (10) 0.0062 (9) 0.0039 (8) 0.0011 (8)
C32 0.0274 (14) 0.0171 (13) 0.0456 (17) 0.0059 (11) 0.0025 (12) 0.0054 (12)
C33 0.045 (2) 0.0210 (15) 0.064 (2) 0.0149 (14) 0.0092 (17) 0.0142 (15)
C34 0.0319 (15) 0.0399 (18) 0.0315 (15) 0.0273 (14) 0.0049 (12) 0.0107 (13)
C35 0.0188 (13) 0.0409 (17) 0.0238 (13) 0.0122 (12) 0.0018 (10) −0.0045 (12)
C36 0.0179 (12) 0.0221 (13) 0.0218 (12) 0.0057 (10) 0.0042 (10) −0.0024 (10)
C41 0.0149 (11) 0.0054 (10) 0.0140 (11) −0.0001 (8) 0.0027 (9) 0.0020 (8)
C42 0.0278 (14) 0.0278 (14) 0.0154 (12) −0.0125 (11) 0.0003 (10) 0.0057 (10)
C43 0.0305 (15) 0.0388 (17) 0.0285 (15) −0.0211 (13) −0.0067 (12) 0.0108 (13)
C44 0.0245 (14) 0.0330 (16) 0.0371 (16) −0.0154 (12) 0.0042 (12) 0.0131 (13)
C45 0.0434 (18) 0.063 (2) 0.0220 (14) −0.0303 (17) 0.0116 (13) 0.0075 (14)
C46 0.0358 (16) 0.0455 (18) 0.0128 (12) −0.0229 (14) 0.0002 (11) 0.0039 (12)

Geometric parameters (Å, º)

I1—Cu1 2.7412 (4) C21—C26 1.394 (3)
Cu1—P1 2.2681 (6) C21—C22 1.398 (4)
Cu1—P2 2.2813 (6) C22—C23 1.399 (4)
Cu1—S1 2.3457 (6) C22—H22 0.9500
S1—C1 1.719 (2) C23—C24 1.380 (4)
P1—C21 1.829 (2) C23—H23 0.9500
P1—C11 1.832 (2) C24—C25 1.389 (4)
P1—C27 1.844 (2) C24—H24 0.9500
P2—C41 1.827 (2) C25—C26 1.384 (4)
P2—C31 1.834 (2) C25—H25 0.9500
P2—C28 1.852 (2) C26—H26 0.9500
N1—C1 1.337 (3) C27—C28i 1.530 (3)
N1—C2 1.459 (3) C27—H27A 0.9900
N1—H1 0.8800 C27—H27B 0.9900
N2—C1 1.333 (3) C28—C27i 1.530 (3)
N2—C4 1.458 (3) C28—H28A 0.9900
N2—H2 0.8800 C28—H28B 0.9900
C2—C3 1.507 (4) C31—C32 1.391 (4)
C2—H2A 0.9900 C31—C36 1.394 (4)
C2—H2B 0.9900 C32—C33 1.391 (4)
C3—H3A 0.9800 C32—H32 0.9500
C3—H3B 0.9800 C33—C34 1.371 (5)
C3—H3C 0.9800 C33—H33 0.9500
C4—C5 1.514 (3) C34—C35 1.381 (5)
C4—H4A 0.9900 C34—H34 0.9500
C4—H4B 0.9900 C35—C36 1.389 (4)
C5—H5A 0.9800 C35—H35 0.9500
C5—H5B 0.9800 C36—H36 0.9500
C5—H5C 0.9800 C41—C42 1.389 (3)
C11—C12 1.393 (3) C41—C46 1.393 (3)
C11—C16 1.399 (3) C42—C43 1.384 (4)
C12—C13 1.399 (3) C42—H42 0.9500
C12—H12 0.9500 C43—C44 1.374 (4)
C13—C14 1.382 (4) C43—H43 0.9500
C13—H13 0.9500 C44—C45 1.378 (5)
C14—C15 1.389 (4) C44—H44 0.9500
C14—H14 0.9500 C45—C46 1.381 (4)
C15—C16 1.390 (3) C45—H45 0.9500
C15—H15 0.9500 C46—H46 0.9500
C16—H16 0.9500
P1—Cu1—P2 113.37 (2) C15—C16—H16 119.8
P1—Cu1—S1 106.77 (2) C11—C16—H16 119.8
P2—Cu1—S1 114.30 (2) C26—C21—C22 118.6 (2)
P1—Cu1—I1 104.637 (18) C26—C21—P1 118.01 (18)
P2—Cu1—I1 106.669 (17) C22—C21—P1 123.33 (18)
S1—Cu1—I1 110.709 (17) C21—C22—C23 120.1 (2)
C1—S1—Cu1 109.37 (7) C21—C22—H22 119.9
C21—P1—C11 101.52 (10) C23—C22—H22 119.9
C21—P1—C27 100.74 (10) C24—C23—C22 120.6 (2)
C11—P1—C27 102.98 (10) C24—C23—H23 119.7
C21—P1—Cu1 112.59 (7) C22—C23—H23 119.7
C11—P1—Cu1 116.01 (8) C23—C24—C25 119.3 (2)
C27—P1—Cu1 120.36 (7) C23—C24—H24 120.4
C41—P2—C31 103.26 (10) C25—C24—H24 120.4
C41—P2—C28 101.76 (10) C26—C25—C24 120.5 (2)
C31—P2—C28 102.47 (10) C26—C25—H25 119.8
C41—P2—Cu1 118.97 (7) C24—C25—H25 119.8
C31—P2—Cu1 117.28 (7) C25—C26—C21 120.9 (2)
C28—P2—Cu1 110.82 (7) C25—C26—H26 119.5
C1—N1—C2 125.3 (2) C21—C26—H26 119.5
C1—N1—H1 117.4 C28i—C27—P1 114.89 (15)
C2—N1—H1 117.4 C28i—C27—H27A 108.5
C1—N2—C4 124.98 (19) P1—C27—H27A 108.5
C1—N2—H2 117.5 C28i—C27—H27B 108.5
C4—N2—H2 117.5 P1—C27—H27B 108.5
N2—C1—N1 117.4 (2) H27A—C27—H27B 107.5
N2—C1—S1 120.29 (17) C27i—C28—P2 108.66 (14)
N1—C1—S1 122.29 (17) C27i—C28—H28A 110.0
N1—C2—C3 112.4 (2) P2—C28—H28A 110.0
N1—C2—H2A 109.1 C27i—C28—H28B 110.0
C3—C2—H2A 109.1 P2—C28—H28B 110.0
N1—C2—H2B 109.1 H28A—C28—H28B 108.3
C3—C2—H2B 109.1 C32—C31—C36 118.7 (2)
H2A—C2—H2B 107.9 C32—C31—P2 122.5 (2)
C2—C3—H3A 109.5 C36—C31—P2 118.77 (18)
C2—C3—H3B 109.5 C33—C32—C31 119.8 (3)
H3A—C3—H3B 109.5 C33—C32—H32 120.1
C2—C3—H3C 109.5 C31—C32—H32 120.1
H3A—C3—H3C 109.5 C34—C33—C32 121.2 (3)
H3B—C3—H3C 109.5 C34—C33—H33 119.4
N2—C4—C5 109.97 (19) C32—C33—H33 119.4
N2—C4—H4A 109.7 C33—C34—C35 119.6 (3)
C5—C4—H4A 109.7 C33—C34—H34 120.2
N2—C4—H4B 109.7 C35—C34—H34 120.2
C5—C4—H4B 109.7 C34—C35—C36 120.0 (3)
H4A—C4—H4B 108.2 C34—C35—H35 120.0
C4—C5—H5A 109.5 C36—C35—H35 120.0
C4—C5—H5B 109.5 C35—C36—C31 120.8 (3)
H5A—C5—H5B 109.5 C35—C36—H36 119.6
C4—C5—H5C 109.5 C31—C36—H36 119.6
H5A—C5—H5C 109.5 C42—C41—C46 117.8 (2)
H5B—C5—H5C 109.5 C42—C41—P2 118.50 (18)
C12—C11—C16 119.4 (2) C46—C41—P2 123.68 (18)
C12—C11—P1 119.57 (17) C43—C42—C41 121.2 (2)
C16—C11—P1 121.03 (17) C43—C42—H42 119.4
C11—C12—C13 119.8 (2) C41—C42—H42 119.4
C11—C12—H12 120.1 C44—C43—C42 120.3 (3)
C13—C12—H12 120.1 C44—C43—H43 119.8
C14—C13—C12 120.5 (2) C42—C43—H43 119.8
C14—C13—H13 119.7 C43—C44—C45 119.2 (3)
C12—C13—H13 119.7 C43—C44—H44 120.4
C13—C14—C15 119.9 (2) C45—C44—H44 120.4
C13—C14—H14 120.0 C44—C45—C46 120.8 (3)
C15—C14—H14 120.0 C44—C45—H45 119.6
C14—C15—C16 120.0 (2) C46—C45—H45 119.6
C14—C15—H15 120.0 C45—C46—C41 120.7 (3)
C16—C15—H15 120.0 C45—C46—H46 119.6
C15—C16—C11 120.3 (2) C41—C46—H46 119.6
C4—N2—C1—N1 −7.2 (3) P1—C21—C26—C25 177.6 (2)
C4—N2—C1—S1 173.37 (18) C21—P1—C27—C28i −165.70 (16)
C2—N1—C1—N2 174.1 (2) C11—P1—C27—C28i −61.09 (18)
C2—N1—C1—S1 −6.5 (3) Cu1—P1—C27—C28i 69.95 (17)
Cu1—S1—C1—N2 −33.6 (2) C41—P2—C28—C27i 66.78 (16)
Cu1—S1—C1—N1 146.99 (17) C31—P2—C28—C27i 173.40 (15)
C1—N1—C2—C3 −90.6 (3) Cu1—P2—C28—C27i −60.70 (15)
C1—N2—C4—C5 −176.4 (2) C41—P2—C31—C32 −20.2 (2)
C21—P1—C11—C12 −123.32 (18) C28—P2—C31—C32 −125.7 (2)
C27—P1—C11—C12 132.67 (18) Cu1—P2—C31—C32 112.8 (2)
Cu1—P1—C11—C12 −0.9 (2) C41—P2—C31—C36 161.93 (18)
C21—P1—C11—C16 54.8 (2) C28—P2—C31—C36 56.5 (2)
C27—P1—C11—C16 −49.2 (2) Cu1—P2—C31—C36 −65.11 (19)
Cu1—P1—C11—C16 177.20 (16) C36—C31—C32—C33 −1.1 (4)
C16—C11—C12—C13 −0.7 (3) P2—C31—C32—C33 −178.9 (3)
P1—C11—C12—C13 177.45 (17) C31—C32—C33—C34 −0.4 (5)
C11—C12—C13—C14 −0.1 (3) C32—C33—C34—C35 0.8 (5)
C12—C13—C14—C15 0.8 (4) C33—C34—C35—C36 0.3 (4)
C13—C14—C15—C16 −0.7 (4) C34—C35—C36—C31 −1.9 (4)
C14—C15—C16—C11 −0.1 (4) C32—C31—C36—C35 2.2 (4)
C12—C11—C16—C15 0.8 (3) P2—C31—C36—C35 −179.84 (19)
P1—C11—C16—C15 −177.35 (18) C31—P2—C41—C42 114.9 (2)
C11—P1—C21—C26 56.7 (2) C28—P2—C41—C42 −139.1 (2)
C27—P1—C21—C26 162.44 (19) Cu1—P2—C41—C42 −17.1 (2)
Cu1—P1—C21—C26 −68.06 (19) C31—P2—C41—C46 −67.9 (2)
C11—P1—C21—C22 −127.0 (2) C28—P2—C41—C46 38.1 (3)
C27—P1—C21—C22 −21.2 (2) Cu1—P2—C41—C46 160.1 (2)
Cu1—P1—C21—C22 108.27 (19) C46—C41—C42—C43 −0.4 (4)
C26—C21—C22—C23 0.3 (4) P2—C41—C42—C43 177.0 (2)
P1—C21—C22—C23 −176.0 (2) C41—C42—C43—C44 −0.7 (5)
C21—C22—C23—C24 −1.5 (4) C42—C43—C44—C45 1.1 (5)
C22—C23—C24—C25 1.2 (4) C43—C44—C45—C46 −0.4 (6)
C23—C24—C25—C26 0.2 (4) C44—C45—C46—C41 −0.7 (6)
C24—C25—C26—C21 −1.3 (4) C42—C41—C46—C45 1.1 (5)
C22—C21—C26—C25 1.1 (4) P2—C41—C46—C45 −176.2 (3)

Symmetry code: (i) −x+1, −y+1, −z.

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N1—H1···I1ii 0.88 2.80 3.622 (2) 156
N2—H2···I1 0.88 2.70 3.5517 (19) 162

Symmetry code: (ii) −x+3/2, y+1/2, −z+1/2.

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: TK5371).

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 datablock(s) I. DOI: 10.1107/S2056989015014176/tk5371sup1.cif

e-71-0m154-sup1.cif (801.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015014176/tk5371Isup2.hkl

e-71-0m154-Isup2.hkl (442.7KB, hkl)

. DOI: 10.1107/S2056989015014176/tk5371fig1.tif

The structure of title complex with displacement ellipsoids drawn at the 50% propbability level. All H atoms are omitted for clarity.

. DOI: 10.1107/S2056989015014176/tk5371fig2.tif

Part of the crystal structure showing intra/inter-mol­ecular N—H⋯I hydrogen bonds forming a layers as dashed lines.

CCDC reference: 1415379

Additional supporting information: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Crystallographic Communications are provided here courtesy of International Union of Crystallography

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