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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Jan 21;68(Pt 2):m190. doi: 10.1107/S1600536812001845

{3,14-Dimethyl-2,6,13,17-tetra­aza­tricyclo­[16.4.0.07,12]docosane-κ4 N,N′,N′′,N′′′)bis­(nitrato-κO)copper(II)

Jong-Ha Choi a, Md Abdus Subhan a, Seik Weng Ng b,c,*
PMCID: PMC3274913  PMID: 22346860

Abstract

The CuII atom in the title compound, [Cu(NO3)2(C20H40N4)], is N,N′,N′′,N′′′-chelated by the macrocyclic ligand: the four N atoms form a square, above and below which are located the O atoms of the nitrate ions. The metal atom exists in a tetra­gonally distorted octa­hedron, on a special position of Inline graphic site symmetry. One of the amino groups is hydrogen bonded to an O atom of the nitrate ion. The other amino group is hydrogen bonded to O atom of an adjacent mol­ecule, generating a supra­molecular dimeric hydrogen-bonded dinuclear aggregate.

Related literature

For the synthesis of the cyclam, see: Choi et al. (2012). For similar copper nitrate–cyclam adducts, see: Amadei et al. (1999); Choi et al. (2001, 2006); Dong et al. (1999); Liu & Chu (2010).graphic file with name e-68-0m190-scheme1.jpg

Experimental

Crystal data

  • [Cu(NO3)2(C20H40N4)]

  • M r = 524.12

  • Triclinic, Inline graphic

  • a = 8.2552 (10) Å

  • b = 8.8074 (11) Å

  • c = 9.1399 (10) Å

  • α = 67.879 (12)°

  • β = 68.780 (11)°

  • γ = 75.096 (11)°

  • V = 568.23 (12) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 1.01 mm−1

  • T = 100 K

  • 0.30 × 0.20 × 0.10 mm

Data collection

  • Agilent SuperNova Dual diffractometer with an Atlas detector

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) T min = 0.751, T max = 0.906

  • 4122 measured reflections

  • 2332 independent reflections

  • 1963 reflections with I > 2σ(I)

  • R int = 0.064

Refinement

  • R[F 2 > 2σ(F 2)] = 0.052

  • wR(F 2) = 0.132

  • S = 1.02

  • 2332 reflections

  • 159 parameters

  • 2 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.96 e Å−3

  • Δρmin = −0.68 e Å−3

Data collection: CrysAlis PRO (Agilent, 2011); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812001845/xu5440sup1.cif

e-68-0m190-sup1.cif (18KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812001845/xu5440Isup2.hkl

e-68-0m190-Isup2.hkl (114.6KB, hkl)

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

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

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯O2i 0.88 (1) 2.15 (2) 2.992 (3) 160 (3)
N2—H2⋯O3ii 0.88 (1) 2.23 (2) 2.961 (3) 140 (3)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

We thank Andong National University and the Ministry of Higher Education of Malaysia (grant No. UM·C/HIR/MOHE/SC/12) for supporting this study.

supplementary crystallographic information

Comment

The macrocycle, cyclam (1,4,8,11-tetraazacyclotetradecane), forms a large number of complexes with copper(II) salts in which the macrocle chelates in a tetradentate matter. In same cases, the counterion bonded to the metal atoms and in other cases, the metal atom exists in square-pyramidal geometry as the counterion is far away. The crystal structure of copper nitrate–cyclam has not been reported; the crystal structures of other substituted cyclams have the metal atom in a tetragonally elongated octahedral geometry (Amadei et al., 1999; Choi et al., 2006; Choi et al., 2001; Dong et al., 1999; Liu & Chu, 2010). The CuII atom in the title compound (Scheme I) is similarly chelated by the macrocyclic ligand in a tetragonally distorted octahedron (Fig.1). The atom lies on a special position of –1 site symmetry. One of the amino groups is hydrogen-bonded to an O atom of the nitrate ion. The other amino group is hydrogen-bonded to O atom of an adjacent molecule to generate a hydrogen-bonded dinuclear molecule (Table 1).

Experimental

The macrocycle co-crystal, 3,14-dimethyl-2,6,13,17-tetraazatricyclo(16.4.0.07,12)docosane (naphthalen-1-yl)methanol prepared as described (Choi et al., 2012). Copper nitrate trihydrate (0.242 g, 1 mmol) dissolved in methanol (10 ml) was mixed with a suspension of the macrocycle co-crystal (0.163 g, 2.5 mmol) dissolved in methanol (10 ml). The mixture was heated for 30 minutes and then set aside for the growth of purple crystals.

Refinement

Carbon-bound H-atoms were placed in calculated positions [C–H 0.99 to 1.00 Å, Uiso(H) 1.2 to 1.5Ueq(C)] and were included in the refinement in the riding model approximation.

The amino H-atoms were located in a difference Fourier map, and were refined with a distance restraint of N–H 0.88±0.01 Å; their temperature factors were refined.

Figures

Fig. 1.

Fig. 1.

Thermal ellipsoid plot (Barbour, 2001) of Cu(NO3)2(C20H40N4) at the 70% probability level; hydrogen atoms are drawn as spheres of arbitrary radius.

Crystal data

[Cu(NO3)2(C20H40N4)] Z = 1
Mr = 524.12 F(000) = 279
Triclinic, P1 Dx = 1.532 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.2552 (10) Å Cell parameters from 1668 reflections
b = 8.8074 (11) Å θ = 2.5–27.5°
c = 9.1399 (10) Å µ = 1.01 mm1
α = 67.879 (12)° T = 100 K
β = 68.780 (11)° Prism, purple
γ = 75.096 (11)° 0.30 × 0.20 × 0.10 mm
V = 568.23 (12) Å3

Data collection

Agilent SuperNova Dual diffractometer with an Atlas detector 2332 independent reflections
Radiation source: SuperNova (Mo) X-ray Source 1963 reflections with I > 2σ(I)
Mirror Rint = 0.064
Detector resolution: 10.4041 pixels mm-1 θmax = 26.5°, θmin = 2.5°
ω scan h = −7→10
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) k = −10→11
Tmin = 0.751, Tmax = 0.906 l = −11→10
4122 measured reflections

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)] = 0.052 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.132 H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.0874P)2] where P = (Fo2 + 2Fc2)/3
2332 reflections (Δ/σ)max = 0.001
159 parameters Δρmax = 0.96 e Å3
2 restraints Δρmin = −0.68 e Å3

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

x y z Uiso*/Ueq
Cu1 0.5000 0.5000 0.5000 0.0158 (2)
N1 0.5570 (3) 0.5225 (3) 0.2605 (3) 0.0152 (5)
H1 0.473 (3) 0.481 (4) 0.257 (4) 0.022 (9)*
N2 0.6852 (3) 0.2945 (3) 0.5073 (3) 0.0154 (5)
H2 0.777 (3) 0.342 (3) 0.484 (4) 0.014 (8)*
N3 0.8305 (3) 0.6621 (3) 0.5099 (3) 0.0193 (6)
O1 0.7574 (3) 0.6375 (3) 0.4223 (3) 0.0228 (5)
O2 0.7518 (3) 0.6441 (3) 0.6596 (3) 0.0280 (5)
O3 0.9780 (3) 0.7070 (3) 0.4452 (3) 0.0260 (5)
C1 0.5512 (4) 0.6927 (4) 0.1448 (4) 0.0201 (6)
H1A 0.5787 0.6891 0.0312 0.024*
H1B 0.6413 0.7475 0.1460 0.024*
C2 0.7261 (4) 0.4161 (4) 0.2131 (4) 0.0171 (6)
H2A 0.8227 0.4708 0.2045 0.020*
C3 0.7647 (4) 0.3870 (4) 0.0493 (4) 0.0203 (6)
H3A 0.7728 0.4940 −0.0408 0.024*
H3B 0.6675 0.3379 0.0528 0.024*
C4 0.9369 (4) 0.2708 (4) 0.0141 (4) 0.0207 (6)
H4A 0.9581 0.2509 −0.0913 0.025*
H4B 1.0353 0.3236 0.0023 0.025*
C5 0.9308 (4) 0.1064 (4) 0.1531 (4) 0.0206 (6)
H5A 1.0448 0.0348 0.1299 0.025*
H5B 0.8386 0.0494 0.1593 0.025*
C6 0.8921 (4) 0.1347 (4) 0.3181 (4) 0.0196 (6)
H6A 0.9906 0.1813 0.3155 0.024*
H6B 0.8821 0.0275 0.4079 0.024*
C7 0.7216 (4) 0.2533 (4) 0.3538 (4) 0.0169 (6)
H7 0.6221 0.2001 0.3659 0.020*
C8 0.6715 (4) 0.1477 (4) 0.6603 (4) 0.0177 (6)
H8 0.7896 0.0787 0.6487 0.021*
C9 0.6290 (4) 0.2073 (4) 0.8083 (4) 0.0192 (6)
H9A 0.6398 0.1093 0.9053 0.023*
H9B 0.7189 0.2758 0.7851 0.023*
C10 0.5417 (4) 0.0404 (4) 0.6826 (4) 0.0206 (6)
H10A 0.5752 0.0052 0.5846 0.031*
H10B 0.4238 0.1039 0.6971 0.031*
H10C 0.5422 −0.0573 0.7804 0.031*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu1 0.0102 (3) 0.0195 (3) 0.0187 (3) −0.00213 (18) −0.0034 (2) −0.0080 (2)
N1 0.0079 (11) 0.0190 (13) 0.0199 (13) −0.0024 (9) −0.0025 (10) −0.0087 (10)
N2 0.0119 (12) 0.0181 (13) 0.0187 (12) −0.0057 (9) −0.0030 (10) −0.0077 (10)
N3 0.0125 (12) 0.0193 (13) 0.0287 (15) −0.0028 (9) −0.0085 (11) −0.0076 (11)
O1 0.0175 (11) 0.0303 (12) 0.0264 (11) −0.0086 (9) −0.0087 (9) −0.0097 (10)
O2 0.0239 (12) 0.0397 (14) 0.0253 (12) −0.0131 (10) −0.0032 (10) −0.0138 (10)
O3 0.0137 (11) 0.0310 (13) 0.0362 (13) −0.0103 (9) −0.0086 (10) −0.0078 (10)
C1 0.0147 (14) 0.0264 (17) 0.0190 (15) −0.0034 (12) −0.0033 (12) −0.0084 (13)
C2 0.0079 (13) 0.0242 (16) 0.0223 (15) −0.0026 (11) −0.0026 (11) −0.0122 (13)
C3 0.0184 (15) 0.0252 (17) 0.0207 (15) −0.0028 (12) −0.0053 (12) −0.0115 (13)
C4 0.0163 (15) 0.0252 (16) 0.0216 (15) −0.0010 (12) −0.0021 (12) −0.0131 (13)
C5 0.0155 (15) 0.0241 (16) 0.0258 (16) −0.0010 (12) −0.0039 (12) −0.0151 (13)
C6 0.0146 (14) 0.0233 (16) 0.0224 (15) −0.0003 (11) −0.0047 (12) −0.0110 (13)
C7 0.0123 (14) 0.0232 (15) 0.0197 (15) −0.0042 (11) −0.0033 (11) −0.0120 (12)
C8 0.0117 (14) 0.0210 (15) 0.0196 (15) −0.0015 (11) −0.0049 (11) −0.0057 (12)
C9 0.0174 (15) 0.0215 (15) 0.0198 (15) −0.0012 (11) −0.0067 (12) −0.0077 (12)
C10 0.0163 (15) 0.0216 (16) 0.0253 (16) −0.0057 (11) −0.0048 (12) −0.0081 (13)

Geometric parameters (Å, °)

Cu1—N1 2.007 (2) C3—H3A 0.9900
Cu1—N1i 2.007 (2) C3—H3B 0.9900
Cu1—N2i 2.044 (2) C4—C5 1.523 (4)
Cu1—N2 2.044 (2) C4—H4A 0.9900
Cu1—O1 2.463 (2) C4—H4B 0.9900
N1—C1 1.475 (4) C5—C6 1.527 (4)
N1—C2 1.486 (3) C5—H5A 0.9900
N1—H1 0.879 (10) C5—H5B 0.9900
N2—C7 1.487 (4) C6—C7 1.532 (4)
N2—C8 1.496 (4) C6—H6A 0.9900
N2—H2 0.878 (10) C6—H6B 0.9900
N3—O3 1.241 (3) C7—H7 1.0000
N3—O2 1.251 (3) C8—C10 1.517 (4)
N3—O1 1.265 (3) C8—C9 1.525 (4)
C1—C9i 1.524 (4) C8—H8 1.0000
C1—H1A 0.9900 C9—C1i 1.524 (4)
C1—H1B 0.9900 C9—H9A 0.9900
C2—C3 1.520 (4) C9—H9B 0.9900
C2—C7 1.521 (4) C10—H10A 0.9800
C2—H2A 1.0000 C10—H10B 0.9800
C3—C4 1.530 (4) C10—H10C 0.9800
N1—Cu1—N1i 180.0 H3A—C3—H3B 108.1
N1—Cu1—N2i 95.20 (9) C5—C4—C3 110.9 (2)
N1i—Cu1—N2i 84.80 (9) C5—C4—H4A 109.5
N1—Cu1—N2 84.80 (9) C3—C4—H4A 109.5
N1i—Cu1—N2 95.20 (9) C5—C4—H4B 109.5
N2i—Cu1—N2 180.000 (1) C3—C4—H4B 109.5
N1—Cu1—O1 87.75 (8) H4A—C4—H4B 108.1
N1i—Cu1—O1 92.25 (8) C4—C5—C6 110.4 (2)
N2i—Cu1—O1 97.63 (8) C4—C5—H5A 109.6
N2—Cu1—O1 82.37 (8) C6—C5—H5A 109.6
C1—N1—C2 113.1 (2) C4—C5—H5B 109.6
C1—N1—Cu1 116.33 (18) C6—C5—H5B 109.6
C2—N1—Cu1 108.35 (17) H5A—C5—H5B 108.1
C1—N1—H1 106 (2) C5—C6—C7 111.2 (2)
C2—N1—H1 108 (2) C5—C6—H6A 109.4
Cu1—N1—H1 104 (2) C7—C6—H6A 109.4
C7—N2—C8 114.3 (2) C5—C6—H6B 109.4
C7—N2—Cu1 107.58 (17) C7—C6—H6B 109.4
C8—N2—Cu1 121.32 (18) H6A—C6—H6B 108.0
C7—N2—H2 102 (2) N2—C7—C2 107.0 (2)
C8—N2—H2 111 (2) N2—C7—C6 113.1 (2)
Cu1—N2—H2 98 (2) C2—C7—C6 111.3 (2)
O3—N3—O2 120.9 (2) N2—C7—H7 108.4
O3—N3—O1 119.5 (2) C2—C7—H7 108.4
O2—N3—O1 119.6 (2) C6—C7—H7 108.4
N3—O1—Cu1 131.16 (18) N2—C8—C10 112.4 (2)
N1—C1—C9i 111.0 (2) N2—C8—C9 108.9 (2)
N1—C1—H1A 109.4 C10—C8—C9 112.8 (3)
C9i—C1—H1A 109.4 N2—C8—H8 107.5
N1—C1—H1B 109.4 C10—C8—H8 107.5
C9i—C1—H1B 109.4 C9—C8—H8 107.5
H1A—C1—H1B 108.0 C1i—C9—C8 116.4 (2)
N1—C2—C3 114.3 (2) C1i—C9—H9A 108.2
N1—C2—C7 107.1 (2) C8—C9—H9A 108.2
C3—C2—C7 111.1 (2) C1i—C9—H9B 108.2
N1—C2—H2A 108.0 C8—C9—H9B 108.2
C3—C2—H2A 108.0 H9A—C9—H9B 107.3
C7—C2—H2A 108.0 C8—C10—H10A 109.5
C2—C3—C4 110.7 (2) C8—C10—H10B 109.5
C2—C3—H3A 109.5 H10A—C10—H10B 109.5
C4—C3—H3A 109.5 C8—C10—H10C 109.5
C2—C3—H3B 109.5 H10A—C10—H10C 109.5
C4—C3—H3B 109.5 H10B—C10—H10C 109.5
N2i—Cu1—N1—C1 35.3 (2) Cu1—N1—C2—C7 42.3 (2)
N2—Cu1—N1—C1 −144.7 (2) N1—C2—C3—C4 −177.7 (2)
O1—Cu1—N1—C1 −62.11 (19) C7—C2—C3—C4 −56.3 (3)
N2i—Cu1—N1—C2 164.12 (17) C2—C3—C4—C5 57.5 (3)
N2—Cu1—N1—C2 −15.88 (17) C3—C4—C5—C6 −57.2 (3)
O1—Cu1—N1—C2 66.66 (18) C4—C5—C6—C7 56.0 (3)
N1—Cu1—N2—C7 −14.16 (18) C8—N2—C7—C2 178.5 (2)
N1i—Cu1—N2—C7 165.84 (18) Cu1—N2—C7—C2 40.6 (2)
O1—Cu1—N2—C7 −102.58 (18) C8—N2—C7—C6 −58.6 (3)
N1—Cu1—N2—C8 −148.4 (2) Cu1—N2—C7—C6 163.59 (19)
N1i—Cu1—N2—C8 31.6 (2) N1—C2—C7—N2 −55.2 (3)
O1—Cu1—N2—C8 123.1 (2) C3—C2—C7—N2 179.4 (2)
O3—N3—O1—Cu1 166.62 (19) N1—C2—C7—C6 −179.2 (2)
O2—N3—O1—Cu1 −14.8 (4) C3—C2—C7—C6 55.3 (3)
N1—Cu1—O1—N3 −172.7 (2) C5—C6—C7—N2 −175.7 (2)
N1i—Cu1—O1—N3 7.3 (2) C5—C6—C7—C2 −55.2 (3)
N2i—Cu1—O1—N3 92.4 (2) C7—N2—C8—C10 −52.7 (3)
N2—Cu1—O1—N3 −87.6 (2) Cu1—N2—C8—C10 78.8 (3)
C2—N1—C1—C9i 175.8 (2) C7—N2—C8—C9 −178.4 (2)
Cu1—N1—C1—C9i −57.8 (3) Cu1—N2—C8—C9 −46.9 (3)
C1—N1—C2—C3 −63.6 (3) N2—C8—C9—C1i 67.3 (3)
Cu1—N1—C2—C3 165.83 (19) C10—C8—C9—C1i −58.2 (3)
C1—N1—C2—C7 172.8 (2)

Symmetry codes: (i) −x+1, −y+1, −z+1.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1···O2i 0.88 (1) 2.15 (2) 2.992 (3) 160 (3)
N2—H2···O3ii 0.88 (1) 2.23 (2) 2.961 (3) 140 (3)

Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+2, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5440).

References

  1. Agilent (2011). CrysAlis PRO Agilent Technologies, Yarnton, England.
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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/S1600536812001845/xu5440sup1.cif

e-68-0m190-sup1.cif (18KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812001845/xu5440Isup2.hkl

e-68-0m190-Isup2.hkl (114.6KB, hkl)

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


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