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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 25;67(Pt 7):m975–m976. doi: 10.1107/S1600536811022719

Bis(μ-5-diisopropyl­amino-1,2,3,4-tetra­zolido-κ2 N 2:N 3)bis­[(triisopropyl­phosphane)copper(I)]

Issam Kobrsi a,*, Ghada Bassioni b,
PMCID: PMC3151938  PMID: 21836950

Abstract

In the binuclear centrosymmetric crystal structure of the title compound, [Cu2(C7H14N5)2(C9H21P)2], all atoms except those of the isopropyl groups are approximately co-planar. The Cu(II) atom is in a distorted trigonal–planar CuN2P coordination. Bond angles around the amino N atom suggest sp 2 hybridization. Several intra­molecular C—H⋯N inter­actions are present involving tetra­zolate N atoms.

Related literature

For background to the coordination chemistry of anionic five-membered nitro­gen-containing heterocyclic ligands, see: Nief (2001); Rottger et al. (1994); Hitzbleck et al. (2004); Gust et al. (2001, 2002); Dezelah et al. (2004); Sebe et al. (2005); Vela et al. (2006). Complexes containing these ligands have a strong tendency to form oligomeric and polymeric structures, see: Haasnoot (2000); Zhang et al. (2006); Dinca et al. (2006). η1 Coordination is the most commonly observed binding mode in monomeric complexes containing 1,2,4-triazolato and tetra­zolato ligands, see: Hunyh et al. (2003); Jiang et al. (2004). Theoretical predictions regarding the high stability of the penta­zolate (N5 ) ion suggest that metal complexes containing this ligand might be stable enough to allow isolation, see: Frunzke et al. (2002); Lein et al. (2001); Burke et al. (2001). For our work on the synthesis, structures and mol­ecular orbital calculations of a series of Ba(alkyl­tetra­zol­ate)2(18-crown-6), K(alkyl­tetra­zolate)(18-crown-6), Ba(pen­ta­zolate)2(18-crown-6) and K(penta­zolate)(18-crown-6) complexes, which exhibited highly distorted tetra­zolato and penta­zolato ligand bonding, see: Kobrsi et al. (2005, 2006). For van der Waals radii, see: Allinger et al. (1968); Bondi (1964). graphic file with name e-67-0m975-scheme1.jpg

Experimental

Crystal data

  • [Cu2(C7H14N5)2(C9H21P)2]

  • M r = 784.02

  • Triclinic, Inline graphic

  • a = 7.3573 (6) Å

  • b = 10.8987 (8) Å

  • c = 12.7134 (9) Å

  • α = 94.273 (2)°

  • β = 96.993 (2)°

  • γ = 93.548 (2)°

  • V = 1006.43 (13) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 1.17 mm−1

  • T = 100 K

  • 0.37 × 0.28 × 0.21 mm

Data collection

  • Bruker APEXII diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2005) T min = 0.675, T max = 0.791

  • 17280 measured reflections

  • 4689 independent reflections

  • 4336 reflections with I > 2σ(I)

  • R int = 0.042

Refinement

  • R[F 2 > 2σ(F 2)] = 0.029

  • wR(F 2) = 0.079

  • S = 1.05

  • 4689 reflections

  • 218 parameters

  • H-atom parameters constrained

  • Δρmax = 0.70 e Å−3

  • Δρmin = −0.42 e Å−3

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT-Plus (Bruker, 2005); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL-Plus (Sheldrick, 2008); software used to prepare material for publication: SHELXTL-Plus (Sheldrick, 2008).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811022719/hp2003sup1.cif

e-67-0m975-sup1.cif (27.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022719/hp2003Isup2.hkl

e-67-0m975-Isup2.hkl (229.7KB, hkl)

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

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

Cu1—P1 2.1957 (5)
Cu1—N2 1.9919 (14)
Cu1—N3 1.9938 (13)
P1—Cu1—N2 126.53 (4)
P1—Cu1—N3 126.52 (4)
N2—Cu1—N3 106.96 (5)

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C3—H3A⋯N4i 0.98 2.58 3.182 (2) 119
C4—H4B⋯N4i 0.98 2.48 3.082 (2) 120
C5—H5⋯N1 1.00 2.32 2.784 (2) 107

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors would like to acknowledge Professor Charles H. Winter for his support.

supplementary crystallographic information

Comment

The coordination chemistry of anionic five-membered nitrogen heterocyclic ligands has generated considerable recent interest from several different perspectives (Nief 2001, Rottger et al. 1994, Hitzbleck et al. 2004, Gust et al. 2001, Dezelah et al. 2004, Sebe et al. 2005, Gust et al. 2002, Vela et al. 2006). Due to the presence of many nitrogen atoms in 1,2,4-triazolato and tetrazolato ligands, complexes containing these ligands have a strong tendency to form oligomeric and polymeric compounds through bridging ligand coordination modes (Haasnoot 2000, Zhang et al. 2006, Dinca et al. 2006). Furthermore, η1-coordination is the most commonly observed binding mode in monomeric complexes containing 1,2,4-triazolato and tetrazolato ligands (Jiang et al. 2004, Hunyh et al. 2003). Theoretical predictions regarding the high stability of the pentazolate (N5-) ion suggest that metal complexes containing this ligand might be stable enough to allow isolation (Frunzke et al. 2002, Lein et al. 2001, Burke et al. 2001).

Since complexes containing N5- ligands may be at the edge of isolability due to facile loss of dinitrogen, it is important to develop a knowledge base that allows the synthesis of soluble, tractable 1,2,4-triazolato and tetrazolato complexes. Presumably, the basic coordination chemistry of pentazolato ligands will share similarities with that of tetrazolato ligands.

Several years ago, we reported the synthesis, structure, and molecular orbital calculations of a series of barium complexes of the formula Ba(alkyltetrazolate)2(18-crown-6), potassium complexes of formula K(alkyltetrazolate)(18-crown-6), as well as calculations of Ba(pentazolate)2(18-crown-6) and K(pentazolate)(18-crown-6). These complexes contained highly distorted tetrazolato and pentazolato ligand bonding (Kobrsi et al. 2005, Kobrsi et al. 2006).

The present work demonstrates the stabilization of copper tetrazolate complexes using a 2-electron donor phosphane ligand. The copper complex crystallizes as a dimer having all nuclei except the isopropyl groups' in the same plane. The phosphane ligands are terminal, while each tetrazolate ligand bridges two Cu(I) centers.

While the work aimed for a monomeric complex, it can be concluded that the combination of isopropyl groups in the phosphane ligand and the tetrazolate ligand does not provide the necessary steric repulsion. However, enough steric hindrance is provided for the tetrazolate to coordinate in an N2—N3 bridging mode as opposed to the normally observed N1—N2 bridging mode.

The C1—N5—C5 angle of 120.30 (13)° and the C2—N5—C5 angle of 118.89 (13)° suggest that the N-atom of the amino group is sp2-hybridized, having its electrons donated to the aromatic ring, thus providing stability to the electron-deficient heterocycle.

Several intramolecular CH—N interactions exist between the tetrazolate's N1 and N4, and the hydrogen atoms on C9, C10, C13, C16. The CH—N distances range from 2.64 to 2.77 Å, whereas the sum of the van der Waals radii for N and H is about 2.7–3.0 Å (Bondi 1964, Allinger et al. 1968), which supports weak, attractive CH—N interactions. These types of interactions have been previously observed, where calculations have shown that these interactions provide stability to the heterocycle (Kobrsi et al. 2005, Kobrsi et al. 2006).

Experimental

A 100 ml Schlenk flask was charged with copper(I) chloride (0.300 g, 3.06 mmol), 40 ml of THF, and a stir bar under an inert atmosphere of argon. Triisopropylphosphane (0.491 g, 3.06 mmol) was added to the mixture while stirring. After 2 h, lithium 5-diisopropylamino-1,2,3,4-tetrazolate (0.536 g, 3.06 mmol) was added, and the reaction mixture was allowed to stir for 18 h at room temperature. The solvent was then removed under vacuum, the products extracted in 30 ml of hexane, and the resulting mixture filtered through a pad of celite. Single crystals were grown from a supersaturated solution at 0°C in the form of white needles. Crystalline samples were mounted in sealed thin wall capillaries under nitrogen atmosphere for X-ray data collection.

Figures

Fig. 1.

Fig. 1.

Reaction scheme for the preparation of the title compound.

Fig. 2.

Fig. 2.

A perspective view of title compound showing the labelling of the non-H atoms. Thermal ellipsoids are shown at 50% probability levels, except for H atoms.

Crystal data

[Cu2(C7H14N5)2(C9H21P)2] Z = 1
Mr = 784.02 F(000) = 420
Triclinic, P1 Dx = 1.294 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 7.3573 (6) Å Cell parameters from 8161 reflections
b = 10.8987 (8) Å θ = 2.8–28.2°
c = 12.7134 (9) Å µ = 1.17 mm1
α = 94.273 (2)° T = 100 K
β = 96.993 (2)° Fragment, colorless
γ = 93.548 (2)° 0.37 × 0.28 × 0.21 mm
V = 1006.43 (13) Å3

Data collection

Bruker APEXII diffractometer 4689 independent reflections
Radiation source: fine-focus sealed tube 4336 reflections with I > 2σ(I)
graphite Rint = 0.042
Bruker APEX2 scans θmax = 28.2°, θmin = 3.1°
Absorption correction: multi-scan (SADABS; Bruker, 2005) h = −9→9
Tmin = 0.675, Tmax = 0.791 k = −14→14
17280 measured reflections l = 0→16

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)] = 0.029 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.079 H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0402P)2 + 0.4118P] where P = (Fo2 + 2Fc2)/3
4689 reflections (Δ/σ)max = 0.001
218 parameters Δρmax = 0.70 e Å3
0 restraints Δρmin = −0.42 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.
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
Cu1 0.17941 (2) 0.40943 (2) 0.06357 (1) 0.0175 (1)
P1 0.40113 (5) 0.30668 (4) 0.13812 (3) 0.0178 (1)
N1 0.11874 (19) 0.59579 (13) 0.23257 (10) 0.0229 (4)
N2 0.06116 (17) 0.54829 (13) 0.13256 (10) 0.0204 (3)
N3 0.05711 (17) 0.38081 (13) −0.08583 (10) 0.0200 (4)
N4 0.08031 (19) 0.28290 (13) −0.15304 (10) 0.0245 (4)
N5 0.0599 (2) 0.78110 (15) 0.33143 (11) 0.0314 (4)
C1 0.0307 (2) 0.69968 (15) 0.24179 (12) 0.0231 (4)
C2 −0.0740 (2) 0.87242 (15) 0.35075 (12) 0.0238 (4)
C3 −0.0506 (2) 0.98014 (17) 0.28292 (14) 0.0302 (5)
C4 −0.2723 (2) 0.81977 (18) 0.33976 (14) 0.0316 (5)
C5 0.1839 (3) 0.74562 (18) 0.42230 (14) 0.0354 (5)
C6 0.2998 (2) 0.8553 (2) 0.47853 (14) 0.0341 (5)
C7 0.0810 (4) 0.6751 (2) 0.4980 (2) 0.0591 (8)
C8 0.4926 (2) 0.36010 (15) 0.27701 (12) 0.0246 (4)
C9 0.5791 (3) 0.49258 (17) 0.28358 (15) 0.0335 (5)
C10 0.3424 (3) 0.35205 (18) 0.34983 (13) 0.0324 (5)
C11 0.3136 (2) 0.14523 (15) 0.14860 (13) 0.0227 (4)
C12 0.4392 (2) 0.06264 (16) 0.21261 (14) 0.0265 (5)
C13 0.2369 (3) 0.07915 (17) 0.04102 (14) 0.0315 (5)
C14 0.6088 (2) 0.31413 (17) 0.06842 (13) 0.0261 (5)
C15 0.7777 (2) 0.25545 (18) 0.11955 (15) 0.0300 (5)
C16 0.5643 (2) 0.2698 (2) −0.04897 (14) 0.0360 (6)
H2 −0.04210 0.90660 0.42640 0.0290*
H3A −0.07590 0.95060 0.20750 0.0450*
H3B 0.07550 1.01720 0.29820 0.0450*
H3C −0.13640 1.04200 0.29930 0.0450*
H4A −0.28240 0.75290 0.38670 0.0470*
H4B −0.31160 0.78760 0.26590 0.0470*
H4C −0.35080 0.88490 0.35960 0.0470*
H5 0.26960 0.68830 0.39280 0.0420*
H6A 0.22370 0.90680 0.51910 0.0510*
H6B 0.35190 0.90370 0.42600 0.0510*
H6C 0.39940 0.82690 0.52710 0.0510*
H7A 0.00340 0.60680 0.45800 0.0890*
H7B 0.00410 0.73060 0.53400 0.0890*
H7C 0.16930 0.64230 0.55100 0.0890*
H8 0.59030 0.30530 0.30200 0.0290*
H9A 0.62420 0.52010 0.35780 0.0500*
H9B 0.48670 0.54700 0.25600 0.0500*
H9C 0.68160 0.49530 0.24110 0.0500*
H10A 0.24340 0.40320 0.32520 0.0490*
H10B 0.39400 0.38160 0.42270 0.0490*
H10C 0.29350 0.26620 0.34840 0.0490*
H11 0.20500 0.15240 0.18830 0.0270*
H12A 0.54300 0.04410 0.17400 0.0400*
H12B 0.36980 −0.01440 0.22250 0.0400*
H12C 0.48510 0.10550 0.28220 0.0400*
H13A 0.16230 0.00450 0.05180 0.0470*
H13B 0.33840 0.05640 0.00200 0.0470*
H13C 0.16050 0.13400 0.00010 0.0470*
H14 0.64690 0.40400 0.06980 0.0310*
H15A 0.88080 0.27150 0.07930 0.0450*
H15B 0.75040 0.16620 0.11910 0.0450*
H15C 0.80990 0.29100 0.19310 0.0450*
H16A 0.54690 0.17950 −0.05660 0.0540*
H16B 0.66580 0.29660 −0.08710 0.0540*
H16C 0.45150 0.30470 −0.07870 0.0540*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu1 0.0202 (1) 0.0177 (1) 0.0138 (1) 0.0075 (1) −0.0031 (1) −0.0010 (1)
P1 0.0195 (2) 0.0181 (2) 0.0149 (2) 0.0060 (1) −0.0031 (1) 0.0007 (1)
N1 0.0288 (7) 0.0237 (7) 0.0147 (6) 0.0109 (5) −0.0040 (5) −0.0037 (5)
N2 0.0243 (6) 0.0209 (7) 0.0150 (5) 0.0076 (5) −0.0023 (4) −0.0015 (5)
N3 0.0225 (6) 0.0214 (7) 0.0153 (6) 0.0070 (5) −0.0014 (4) −0.0024 (5)
N4 0.0302 (7) 0.0263 (7) 0.0158 (6) 0.0133 (5) −0.0039 (5) −0.0042 (5)
N5 0.0422 (8) 0.0316 (8) 0.0179 (6) 0.0223 (6) −0.0099 (6) −0.0082 (6)
C1 0.0266 (7) 0.0243 (8) 0.0175 (7) 0.0105 (6) −0.0033 (5) −0.0021 (6)
C2 0.0309 (8) 0.0226 (8) 0.0176 (7) 0.0116 (6) 0.0002 (6) −0.0031 (6)
C3 0.0348 (9) 0.0294 (9) 0.0275 (8) 0.0085 (7) 0.0046 (7) 0.0028 (7)
C4 0.0366 (9) 0.0285 (9) 0.0295 (8) 0.0031 (7) 0.0058 (7) −0.0022 (7)
C5 0.0477 (10) 0.0324 (10) 0.0223 (8) 0.0216 (8) −0.0142 (7) −0.0080 (7)
C6 0.0295 (8) 0.0473 (12) 0.0243 (8) 0.0077 (8) −0.0017 (6) 0.0003 (8)
C7 0.0697 (15) 0.0431 (13) 0.0551 (14) −0.0126 (11) −0.0350 (12) 0.0262 (11)
C8 0.0310 (8) 0.0216 (8) 0.0186 (7) 0.0077 (6) −0.0087 (6) −0.0002 (6)
C9 0.0390 (9) 0.0245 (9) 0.0319 (9) 0.0043 (7) −0.0131 (7) −0.0039 (7)
C10 0.0497 (10) 0.0301 (10) 0.0178 (7) 0.0138 (8) 0.0008 (7) 0.0009 (7)
C11 0.0234 (7) 0.0193 (7) 0.0248 (7) 0.0056 (6) −0.0015 (6) 0.0016 (6)
C12 0.0301 (8) 0.0206 (8) 0.0280 (8) 0.0069 (6) −0.0038 (6) 0.0041 (6)
C13 0.0355 (9) 0.0228 (9) 0.0320 (9) 0.0012 (7) −0.0108 (7) −0.0006 (7)
C14 0.0231 (7) 0.0303 (9) 0.0252 (8) 0.0057 (6) 0.0005 (6) 0.0047 (7)
C15 0.0213 (7) 0.0355 (10) 0.0344 (9) 0.0079 (7) 0.0012 (6) 0.0089 (7)
C16 0.0294 (8) 0.0539 (13) 0.0250 (8) 0.0029 (8) 0.0058 (7) 0.0023 (8)

Geometric parameters (Å, °)

Cu1—P1 2.1957 (5) C4—H4C 0.9800
Cu1—N2 1.9919 (14) C5—H5 1.0000
Cu1—N3 1.9938 (13) C6—H6A 0.9800
P1—C8 1.8490 (16) C6—H6B 0.9800
P1—C11 1.8559 (17) C6—H6C 0.9800
P1—C14 1.8578 (16) C7—H7A 0.9800
N1—N2 1.3445 (18) C7—H7B 0.9800
N1—C1 1.343 (2) C7—H7C 0.9800
N2—N3i 1.3164 (19) C8—H8 1.0000
N3—N4 1.3491 (19) C9—H9A 0.9800
N4—C1i 1.343 (2) C9—H9B 0.9800
N5—C1 1.378 (2) C9—H9C 0.9800
N5—C2 1.472 (2) C10—H10A 0.9800
N5—C5 1.473 (2) C10—H10B 0.9800
C2—C3 1.521 (2) C10—H10C 0.9800
C2—C4 1.521 (2) C11—H11 1.0000
C5—C6 1.505 (3) C12—H12A 0.9800
C5—C7 1.519 (3) C12—H12B 0.9800
C8—C9 1.534 (3) C12—H12C 0.9800
C8—C10 1.528 (3) C13—H13A 0.9800
C11—C12 1.535 (2) C13—H13B 0.9800
C11—C13 1.524 (2) C13—H13C 0.9800
C14—C15 1.530 (2) C14—H14 1.0000
C14—C16 1.524 (2) C15—H15A 0.9800
C2—H2 1.0000 C15—H15B 0.9800
C3—H3A 0.9800 C15—H15C 0.9800
C3—H3B 0.9800 C16—H16A 0.9800
C3—H3C 0.9800 C16—H16B 0.9800
C4—H4A 0.9800 C16—H16C 0.9800
C4—H4B 0.9800
Cu1···H15Aii 2.6200 H5···N1 2.3200
N1···N4i 2.235 (2) H6A···C2 2.8600
N2···N3 3.2030 (19) H6A···H2 2.1600
N2···N4i 2.184 (2) H6A···H7B 2.4700
N3···N2 3.2030 (19) H6A···H2viii 2.6000
N3···N1i 2.1779 (18) H6A···H3Cviii 2.5000
N4···C4i 3.082 (2) H6B···H4Cv 2.4500
N4···C3i 3.182 (2) H6C···H12Cix 2.5100
N4···N1i 2.235 (2) H7A···C1 3.0200
N1···H10A 2.6400 H7B···C2 2.9100
N1···H9B 2.7800 H7B···H2 2.4500
N1···H5 2.3200 H7B···H6A 2.4700
N1···H16Biii 2.8500 H7C···H8ix 2.4200
N2···H16Biii 2.6900 H8···C12 2.9000
N3···H15Aii 2.8900 H8···C15 2.8700
N4···H13C 2.6600 H8···H12C 2.2500
N4···H16C 2.7700 H8···H15C 2.2600
N4···H3Ai 2.5800 H8···H7Cix 2.4200
N4···H4Bi 2.4800 H9A···H4Av 2.5700
C3···N4i 3.182 (2) H9A···H10B 2.4600
C4···N4i 3.082 (2) H9B···N1 2.7800
C12···C15 3.530 (2) H9B···H10A 2.5800
C13···C16 3.440 (3) H9C···C14 2.8200
C15···C12 3.530 (2) H9C···H14 2.3000
C16···C13 3.440 (3) H9C···H15C 2.5300
C1···H7A 3.0200 H10A···N1 2.6400
C1···H4B 2.7900 H10A···H9B 2.5800
C1···H3A 2.9400 H10B···H9A 2.4600
C2···H7B 2.9100 H10C···C11 2.8000
C2···H6A 2.8600 H10C···C12 3.0400
C3···H11iv 2.9900 H10C···H11 2.3000
C6···H2 2.6300 H10C···H12C 2.4800
C7···H2 2.9000 H11···C3vi 2.9900
C7···H4A 3.0700 H11···C10 2.9200
C8···H15C 2.8000 H11···H3Bvi 2.3400
C8···H12C 2.7800 H11···H10C 2.3000
C9···H14 2.9300 H12A···C15 2.9700
C9···H15C 3.1000 H12A···H13B 2.5200
C9···H4Av 3.0900 H12A···H15B 2.1800
C10···H11 2.9200 H12B···H3Bvi 2.5100
C10···H12C 3.0500 H12B···H13A 2.5300
C11···H3Bvi 3.0900 H12C···C8 2.7800
C11···H10C 2.8000 H12C···C10 3.0500
C12···H3Bvi 3.0400 H12C···H8 2.2500
C12···H15B 2.9100 H12C···H10C 2.4800
C12···H10C 3.0400 H12C···H6Cix 2.5100
C12···H8 2.9000 H13A···H12B 2.5300
C13···H13Avii 3.0800 H13A···C13vii 3.0800
C13···H16A 2.9200 H13A···H13Avii 2.5800
C14···H9C 2.8200 H13B···C16 2.9300
C15···H8 2.8700 H13B···H12A 2.5200
C15···H12A 2.9700 H13B···H16A 2.2100
C16···H13B 2.9300 H13C···N4 2.6600
H2···C6 2.6300 H14···C9 2.9300
H2···C7 2.9000 H14···H9C 2.3000
H2···H6A 2.1600 H15A···Cu1v 2.6200
H2···H7B 2.4500 H15A···N3v 2.8900
H2···H6Aviii 2.6000 H15A···H16B 2.5300
H3A···C1 2.9400 H15B···C12 2.9100
H3A···N4i 2.5800 H15B···H12A 2.1800
H3B···C11iv 3.0900 H15B···H16A 2.5500
H3B···C12iv 3.0400 H15C···C8 2.8000
H3B···H11iv 2.3400 H15C···C9 3.1000
H3B···H12Biv 2.5100 H15C···H8 2.2600
H3C···H4C 2.4800 H15C···H9C 2.5300
H3C···H6Aviii 2.5000 H16A···C13 2.9200
H4A···C7 3.0700 H16A···H13B 2.2100
H4A···C9ii 3.0900 H16A···H15B 2.5500
H4A···H9Aii 2.5700 H16B···H15A 2.5300
H4B···C1 2.7900 H16B···N1iii 2.8500
H4B···N4i 2.4800 H16B···N2iii 2.6900
H4B···H16Ci 2.5800 H16C···N4 2.7700
H4C···H3C 2.4800 H16C···H4Bi 2.5800
H4C···H6Bii 2.4500
P1—Cu1—N2 126.53 (4) C5—C6—H6B 109.00
P1—Cu1—N3 126.52 (4) C5—C6—H6C 109.00
N2—Cu1—N3 106.96 (5) H6A—C6—H6B 109.00
Cu1—P1—C8 116.09 (5) H6A—C6—H6C 109.00
Cu1—P1—C11 109.53 (5) H6B—C6—H6C 109.00
Cu1—P1—C14 112.78 (6) C5—C7—H7A 110.00
C8—P1—C11 103.02 (7) C5—C7—H7B 110.00
C8—P1—C14 103.05 (7) C5—C7—H7C 109.00
C11—P1—C14 111.91 (8) H7A—C7—H7B 109.00
N2—N1—C1 103.91 (12) H7A—C7—H7C 109.00
Cu1—N2—N1 122.29 (10) H7B—C7—H7C 109.00
Cu1—N2—N3i 126.91 (10) P1—C8—H8 108.00
N1—N2—N3i 109.86 (13) C9—C8—H8 108.00
Cu1—N3—N4 124.44 (10) C10—C8—H8 108.00
Cu1—N3—N2i 125.54 (10) C8—C9—H9A 110.00
N2i—N3—N4 110.00 (12) C8—C9—H9B 109.00
N3—N4—C1i 103.64 (13) C8—C9—H9C 109.00
C1—N5—C2 120.27 (13) H9A—C9—H9B 109.00
C1—N5—C5 117.08 (15) H9A—C9—H9C 109.00
C2—N5—C5 118.88 (14) H9B—C9—H9C 109.00
N1—C1—N5 122.80 (14) C8—C10—H10A 109.00
N1—C1—N4i 112.59 (14) C8—C10—H10B 109.00
N4i—C1—N5 124.55 (15) C8—C10—H10C 109.00
N5—C2—C3 110.45 (13) H10A—C10—H10B 109.00
N5—C2—C4 114.69 (14) H10A—C10—H10C 109.00
C3—C2—C4 112.02 (13) H10B—C10—H10C 109.00
N5—C5—C6 111.51 (16) P1—C11—H11 105.00
N5—C5—C7 111.98 (19) C12—C11—H11 105.00
C6—C5—C7 112.07 (16) C13—C11—H11 105.00
P1—C8—C9 110.57 (11) C11—C12—H12A 109.00
P1—C8—C10 111.09 (11) C11—C12—H12B 109.00
C9—C8—C10 110.22 (14) C11—C12—H12C 109.00
P1—C11—C12 117.76 (11) H12A—C12—H12B 109.00
P1—C11—C13 112.62 (12) H12A—C12—H12C 109.00
C12—C11—C13 110.39 (14) H12B—C12—H12C 109.00
P1—C14—C15 117.04 (12) C11—C13—H13A 109.00
P1—C14—C16 111.77 (11) C11—C13—H13B 110.00
C15—C14—C16 111.12 (14) C11—C13—H13C 109.00
N5—C2—H2 106.00 H13A—C13—H13B 109.00
C3—C2—H2 106.00 H13A—C13—H13C 109.00
C4—C2—H2 106.00 H13B—C13—H13C 109.00
C2—C3—H3A 109.00 P1—C14—H14 105.00
C2—C3—H3B 109.00 C15—C14—H14 105.00
C2—C3—H3C 109.00 C16—C14—H14 105.00
H3A—C3—H3B 109.00 C14—C15—H15A 109.00
H3A—C3—H3C 109.00 C14—C15—H15B 109.00
H3B—C3—H3C 110.00 C14—C15—H15C 109.00
C2—C4—H4A 109.00 H15A—C15—H15B 110.00
C2—C4—H4B 109.00 H15A—C15—H15C 110.00
C2—C4—H4C 109.00 H15B—C15—H15C 109.00
H4A—C4—H4B 110.00 C14—C16—H16A 109.00
H4A—C4—H4C 109.00 C14—C16—H16B 109.00
H4B—C4—H4C 109.00 C14—C16—H16C 109.00
N5—C5—H5 107.00 H16A—C16—H16B 109.00
C6—C5—H5 107.00 H16A—C16—H16C 109.00
C7—C5—H5 107.00 H16B—C16—H16C 110.00
C5—C6—H6A 110.00
N2—Cu1—P1—C8 −2.92 (8) C8—P1—C14—C15 48.70 (15)
N2—Cu1—P1—C11 113.17 (7) C8—P1—C14—C16 178.45 (13)
N2—Cu1—P1—C14 −121.49 (8) C11—P1—C14—C15 −61.33 (15)
N3—Cu1—P1—C8 177.48 (7) C11—P1—C14—C16 68.43 (15)
N3—Cu1—P1—C11 −66.43 (7) C1—N1—N2—Cu1 168.56 (10)
N3—Cu1—P1—C14 58.91 (8) C1—N1—N2—N3i −1.07 (16)
P1—Cu1—N2—N1 4.13 (14) N2—N1—C1—N5 −176.03 (14)
P1—Cu1—N2—N3i 171.90 (10) N2—N1—C1—N4i 1.06 (18)
N3—Cu1—N2—N1 −176.21 (11) Cu1—N2—N3i—Cu1i 9.93 (19)
N3—Cu1—N2—N3i −8.43 (14) Cu1—N2—N3i—N4i −168.30 (10)
P1—Cu1—N3—N4 9.97 (14) N1—N2—N3i—Cu1i 178.95 (10)
P1—Cu1—N3—N2i −172.05 (10) N1—N2—N3i—N4i 0.73 (17)
N2—Cu1—N3—N4 −169.69 (12) Cu1—N3—N4—C1i 178.31 (10)
N2—Cu1—N3—N2i 8.29 (14) N2i—N3—N4—C1i 0.06 (16)
Cu1—P1—C8—C9 −62.53 (13) N3—N4—C1i—N1i 0.65 (17)
Cu1—P1—C8—C10 60.18 (13) N3—N4—C1i—N5i −176.39 (15)
C11—P1—C8—C9 177.79 (12) C2—N5—C1—N1 −162.27 (15)
C11—P1—C8—C10 −59.51 (13) C2—N5—C1—N4i 21.0 (2)
C14—P1—C8—C9 61.25 (14) C5—N5—C1—N1 −4.4 (2)
C14—P1—C8—C10 −176.04 (12) C5—N5—C1—N4i 178.88 (16)
Cu1—P1—C11—C12 −171.57 (10) C1—N5—C2—C3 −78.37 (18)
Cu1—P1—C11—C13 58.21 (13) C1—N5—C2—C4 49.4 (2)
C8—P1—C11—C12 −47.46 (13) C5—N5—C2—C3 124.14 (16)
C8—P1—C11—C13 −177.68 (12) C5—N5—C2—C4 −108.15 (18)
C14—P1—C11—C12 62.59 (14) C1—N5—C5—C6 142.57 (15)
C14—P1—C11—C13 −67.63 (14) C1—N5—C5—C7 −90.96 (19)
Cu1—P1—C14—C15 174.64 (11) C2—N5—C5—C6 −59.2 (2)
Cu1—P1—C14—C16 −55.61 (14) C2—N5—C5—C7 67.3 (2)

Symmetry codes: (i) −x, −y+1, −z; (ii) x−1, y, z; (iii) −x+1, −y+1, −z; (iv) x, y+1, z; (v) x+1, y, z; (vi) x, y−1, z; (vii) −x, −y, −z; (viii) −x, −y+2, −z+1; (ix) −x+1, −y+1, −z+1.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C3—H3A···N4i 0.98 2.58 3.182 (2) 119
C4—H4B···N4i 0.98 2.48 3.082 (2) 120
C5—H5···N1 1.00 2.32 2.784 (2) 107

Symmetry codes: (i) −x, −y+1, −z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HP2003).

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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) global, I. DOI: 10.1107/S1600536811022719/hp2003sup1.cif

e-67-0m975-sup1.cif (27.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022719/hp2003Isup2.hkl

e-67-0m975-Isup2.hkl (229.7KB, hkl)

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


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