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The title mononuclear copper(II) complex, [CuCl(C18H26N4)]ClO4, shows a square-pyramidal coordination with the diethyl­amino N atom at the apical position. Large anisotropies in the displacement parameters of the non-H atoms of the ligand seem to be due to rotational disorder of the ClO4- anion.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S010827010000559X/qa0280sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S010827010000559X/qa0280Isup2.hkl
Contains datablock I

CCDC reference: 145642

Comment top

DNA degradation by the copper(II) complexes with tripodal ligands has been investigated by one (YN) of the authors (Kobayashi et al., 1996, 1998). The structure of [Cu(Et2py)Cl]ClO4 (where py is pyridine), (I), is reported here.

The Ueq values of the perchlorate O1, O2, O3 and O4 atoms are in the range 0.207 (3)–0.349 (6) Å2, suggesting a rotational disorder of the ClO4- anion.

Experimental top

The ligand and its chlorocopper(II) complex were prepared as described previously (Kobayashi et al., 1998). Crystals of the title compound were grown from an aqueous methanol solution.

Refinement top

Positional parameters of all the H atoms were calculated geometrically and fixed with U(H) = 1.2Ueq(parent atom).

Computing details top

Data collection: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1993); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: TEXSAN (Molecular Structure Corporation, 1999); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: TEXSAN; software used to prepare material for publication: TEXSAN.

(I) top
Crystal data top
[CuCl(C18H26N4)]ClO4Dx = 1.522 Mg m3
Mr = 496.88Mo Kα radiation, λ = 0.71073 Å
Monoclinic, P21/cCell parameters from 25 reflections
a = 12.513 (2) Åθ = 10–15°
b = 14.613 (2) ŵ = 1.29 mm1
c = 12.569 (2) ÅT = 298 K
β = 109.34 (1)°Plate-like, blue
V = 2168.6 (1) Å30.65 × 0.55 × 0.3 mm
Z = 4
Data collection top
Rigaku AFC-5S
diffractometer
Rint = 0.025
θ–2θ scansθmax = 27.5°
Absorption correction: integration
(Coppens et al., 1965)
h = 016
Tmin = 0.469, Tmax = 0.701k = 019
5399 measured reflectionsl = 1616
4971 independent reflections3 standard reflections every 100 reflections
2593 reflections with I > 2σ(I) intensity decay: none
Refinement top
Refinement on F2H-atom parameters not refined
R[F2 > 2σ(F2)] = 0.064 w = 1/[σ2(Fo2) + (0.05(Fo2 + 2Fc2)/3)2]
wR(F2) = 0.161(Δ/σ)max = 0.003
S = 1.51Δρmax = 0.45 e Å3
4971 reflectionsΔρmin = 0.43 e Å3
262 parameters
Crystal data top
[CuCl(C18H26N4)]ClO4V = 2168.6 (1) Å3
Mr = 496.88Z = 4
Monoclinic, P21/cMo Kα radiation
a = 12.513 (2) ŵ = 1.29 mm1
b = 14.613 (2) ÅT = 298 K
c = 12.569 (2) Å0.65 × 0.55 × 0.3 mm
β = 109.34 (1)°
Data collection top
Rigaku AFC-5S
diffractometer
2593 reflections with I > 2σ(I)
Absorption correction: integration
(Coppens et al., 1965)
Rint = 0.025
Tmin = 0.469, Tmax = 0.7013 standard reflections every 100 reflections
5399 measured reflections intensity decay: none
4971 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.064262 parameters
wR(F2) = 0.161H-atom parameters not refined
S = 1.51Δρmax = 0.45 e Å3
4971 reflectionsΔρmin = 0.43 e Å3
Special details top

Refinement. Refinement using reflections with F2 > 0.0 σ(F2). The weighted R-factor (wR) and goodness of fit (S) are based on F2. R-factor (gt) are based on F. The threshold expression of F2 > 2.0 σ(F2) is used only for calculating R-factor (gt).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cu10.13286 (5)0.09364 (4)0.08692 (4)0.0726 (2)
Cl10.0406 (1)0.1487 (1)0.08547 (9)0.0953 (4)
Cl20.6570 (1)0.1021 (1)0.4177 (1)0.0904 (5)
O10.6045 (10)0.0359 (6)0.343 (1)0.349 (6)
O20.6027 (6)0.1143 (7)0.4878 (5)0.283 (5)
O30.6409 (5)0.1734 (4)0.3466 (7)0.207 (3)
O40.7669 (5)0.0787 (6)0.4624 (5)0.225 (3)
N10.2373 (3)0.0122 (3)0.0379 (4)0.083 (1)
N20.2031 (4)0.0329 (3)0.2407 (3)0.107 (2)
N30.0124 (4)0.1289 (4)0.1526 (4)0.094 (2)
N40.2679 (3)0.2086 (3)0.1642 (3)0.070 (1)
C10.2573 (5)0.0163 (4)0.0587 (6)0.095 (2)
C20.3355 (7)0.0375 (5)0.0822 (8)0.133 (3)
C30.3944 (9)0.0989 (8)0.003 (1)0.176 (5)
C40.3748 (9)0.1041 (7)0.095 (1)0.175 (4)
C50.2933 (5)0.0473 (4)0.1175 (6)0.113 (2)
C60.2621 (6)0.0503 (6)0.2241 (7)0.143 (3)
C70.1065 (8)0.0154 (6)0.2852 (4)0.133 (3)
C80.0206 (7)0.0882 (5)0.2473 (6)0.123 (3)
C90.052 (1)0.1070 (7)0.3150 (9)0.158 (5)
C100.127 (1)0.1712 (9)0.270 (1)0.183 (6)
C110.1431 (6)0.2142 (6)0.1692 (9)0.141 (3)
C120.0694 (6)0.1909 (5)0.1128 (6)0.107 (2)
C130.2833 (6)0.1013 (5)0.3176 (4)0.128 (2)
C140.3450 (5)0.1561 (4)0.2588 (4)0.106 (2)
C150.3259 (5)0.2324 (3)0.0805 (4)0.089 (2)
C160.4263 (5)0.2951 (4)0.1207 (5)0.110 (2)
C170.2243 (5)0.2898 (4)0.2047 (4)0.092 (2)
C180.1487 (6)0.3488 (4)0.1148 (6)0.119 (2)
H10.21480.05900.11490.1136*
H20.34880.03230.15290.1592*
H30.44960.13820.01730.2116*
H40.41670.14720.15080.2102*
H50.33020.05740.28750.1710*
H60.21350.10200.22000.1710*
H70.07240.04260.25760.1600*
H80.13520.01430.36610.1600*
H90.04570.07610.38430.1894*
H100.17550.18950.31170.2196*
H110.20230.25840.13950.1691*
H120.07730.22030.04230.1282*
H130.24020.14190.34780.1539*
H140.33720.06870.37810.1539*
H150.38960.11580.23010.1276*
H160.39400.19810.31150.1276*
H170.35090.17620.05680.1071*
H180.27090.26100.01710.1071*
H190.48350.26750.18330.1316*
H200.45610.30550.06050.1316*
H210.40340.35230.14390.1316*
H220.18260.26980.25230.1104*
H230.28780.32610.24810.1104*
H240.12420.40010.14840.1422*
H250.18910.37020.06670.1422*
H260.08390.31400.07100.1422*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0845 (4)0.0706 (4)0.0452 (3)0.0047 (3)0.0022 (2)0.0046 (3)
Cl10.1100 (10)0.098 (1)0.0514 (6)0.0286 (8)0.0089 (6)0.0018 (6)
Cl20.1005 (10)0.101 (1)0.0743 (8)0.0337 (8)0.0350 (7)0.0212 (8)
O10.38 (1)0.189 (8)0.39 (2)0.023 (9)0.01 (1)0.14 (1)
O20.198 (7)0.56 (2)0.138 (5)0.118 (8)0.115 (5)0.057 (7)
O30.160 (5)0.164 (5)0.305 (9)0.063 (4)0.089 (5)0.122 (6)
O40.137 (4)0.37 (1)0.176 (5)0.129 (6)0.061 (4)0.135 (6)
N10.081 (3)0.062 (2)0.082 (3)0.001 (2)0.006 (2)0.002 (2)
N20.129 (4)0.090 (3)0.059 (2)0.036 (3)0.024 (2)0.025 (2)
N30.109 (4)0.097 (3)0.072 (3)0.045 (3)0.023 (3)0.012 (3)
N40.078 (2)0.068 (2)0.051 (2)0.009 (2)0.006 (2)0.001 (2)
C10.094 (4)0.067 (3)0.107 (4)0.003 (3)0.011 (3)0.026 (3)
C20.103 (5)0.093 (5)0.195 (8)0.018 (4)0.040 (5)0.066 (5)
C30.107 (6)0.113 (8)0.28 (2)0.022 (5)0.026 (9)0.06 (1)
C40.103 (6)0.082 (5)0.28 (1)0.023 (5)0.021 (8)0.006 (8)
C50.089 (4)0.063 (3)0.140 (6)0.005 (3)0.023 (4)0.013 (4)
C60.134 (6)0.112 (5)0.130 (6)0.008 (5)0.026 (4)0.069 (5)
C70.190 (7)0.139 (6)0.055 (3)0.107 (6)0.018 (4)0.008 (3)
C80.156 (7)0.100 (5)0.089 (4)0.075 (5)0.009 (4)0.007 (4)
C90.22 (1)0.157 (9)0.124 (7)0.122 (8)0.097 (8)0.059 (7)
C100.24 (1)0.18 (1)0.17 (1)0.14 (1)0.13 (1)0.10 (1)
C110.114 (5)0.147 (7)0.177 (8)0.058 (5)0.070 (6)0.083 (7)
C120.090 (4)0.111 (5)0.117 (5)0.029 (4)0.029 (4)0.034 (4)
C130.147 (5)0.138 (5)0.057 (3)0.069 (5)0.023 (3)0.026 (3)
C140.108 (4)0.094 (4)0.075 (3)0.023 (3)0.027 (3)0.016 (3)
C150.101 (4)0.076 (4)0.084 (3)0.017 (3)0.021 (3)0.007 (3)
C160.102 (4)0.106 (4)0.115 (5)0.023 (4)0.028 (3)0.009 (4)
C170.109 (4)0.082 (4)0.081 (3)0.013 (3)0.026 (3)0.012 (3)
C180.126 (5)0.077 (4)0.133 (5)0.007 (4)0.016 (4)0.006 (4)
Geometric parameters (Å, º) top
Cu1—Cl12.240 (1)C6—H60.960
Cu1—N12.008 (5)C7—C81.47 (1)
Cu1—N22.042 (4)C7—H70.960
Cu1—N32.011 (5)C7—H80.960
Cu1—N42.352 (4)C8—C91.46 (1)
Cl2—O11.354 (9)C9—C101.32 (2)
Cl2—O21.292 (5)C9—H90.960
Cl2—O31.343 (5)C10—C111.37 (1)
Cl2—O41.346 (5)C10—H100.960
N1—C11.321 (7)C11—C121.379 (9)
N1—C51.335 (7)C11—H110.960
N2—C61.472 (10)C12—H120.960
N2—C71.511 (8)C13—C141.471 (8)
N2—C131.517 (7)C13—H130.960
N3—C81.304 (8)C13—H140.960
N3—C121.334 (8)C14—H150.960
N4—C141.474 (6)C14—H160.960
N4—C151.503 (6)C15—C161.500 (8)
N4—C171.467 (6)C15—H170.960
C1—C21.361 (8)C15—H180.960
C1—H10.960C16—H190.960
C2—C31.36 (1)C16—H200.960
C2—H20.960C16—H210.960
C3—C41.33 (2)C17—C181.485 (8)
C3—H30.960C17—H220.960
C4—C51.42 (1)C17—H230.960
C4—H40.960C18—H240.960
C5—C61.52 (1)C18—H250.960
C6—H50.960C18—H260.960
Cl1···C10i3.480 (10)O3···C4vii3.35 (1)
Cl1···C7ii3.518 (6)O3···C143.504 (9)
O1···C143.53 (1)O4···C7v3.337 (9)
O1···C16iii3.58 (1)O4···C9vi3.39 (1)
O2···C16iv3.443 (8)O4···C10vi3.40 (1)
O2···C6v3.575 (9)C2···C11ii3.452 (9)
O2···C143.593 (9)C2···C10ii3.48 (1)
O3···C10vi3.35 (1)C3···C11ii3.57 (1)
Cl1—Cu1—N195.5 (1)N2—C7—H7109.3
Cl1—Cu1—N2173.7 (1)N2—C7—H8109.3
Cl1—Cu1—N395.1 (2)C8—C7—H7109.3
Cl1—Cu1—N4102.26 (9)C8—C7—H8109.3
N1—Cu1—N285.0 (2)H7—C7—H8109.5
N1—Cu1—N3158.4 (2)N3—C8—C7116.8 (8)
N1—Cu1—N495.6 (1)N3—C8—C9124.7 (9)
N2—Cu1—N382.5 (2)C7—C8—C9118.4 (8)
N2—Cu1—N484.0 (1)C8—C9—C10112 (1)
N3—Cu1—N4100.4 (1)C8—C9—H9123.9
O1—Cl2—O2108.9 (7)C10—C9—H9123.9
O1—Cl2—O399.5 (7)C9—C10—C11126 (1)
O1—Cl2—O4107.5 (6)C9—C10—H10116.9
O2—Cl2—O3110.4 (5)C11—C10—H10116.9
O2—Cl2—O4116.5 (4)C10—C11—C12116 (1)
O3—Cl2—O4112.5 (4)C10—C11—H11121.8
Cu1—N1—C1126.6 (4)C12—C11—H11121.8
Cu1—N1—C5112.9 (5)N3—C12—C11122.4 (8)
C1—N1—C5120.4 (6)N3—C12—H12118.8
Cu1—N2—C6107.7 (4)C11—C12—H12118.8
Cu1—N2—C7106.1 (4)N2—C13—C14112.7 (5)
Cu1—N2—C13107.6 (3)N2—C13—H13108.7
C6—N2—C7114.4 (6)N2—C13—H14108.7
C6—N2—C13112.2 (5)C14—C13—H13108.7
C7—N2—C13108.5 (5)C14—C13—H14108.7
Cu1—N3—C8114.6 (6)H13—C13—H14109.5
Cu1—N3—C12127.3 (4)N4—C14—C13112.1 (5)
C8—N3—C12118.1 (7)N4—C14—H15108.8
Cu1—N4—C1498.7 (3)N4—C14—H16108.8
Cu1—N4—C15108.9 (3)C13—C14—H15108.8
Cu1—N4—C17115.0 (3)C13—C14—H16108.8
C14—N4—C15110.2 (4)H15—C14—H16109.5
C14—N4—C17111.1 (4)N4—C15—C16116.8 (4)
C15—N4—C17112.1 (4)N4—C15—H17107.6
N1—C1—C2122.8 (6)N4—C15—H18107.6
N1—C1—H1118.6C16—C15—H17107.6
C2—C1—H1118.6C16—C15—H18107.6
C1—C2—C3118.4 (9)H17—C15—H18109.5
C1—C2—H2120.8C15—C16—H19109.5
C3—C2—H2120.8C15—C16—H20109.5
C2—C3—C4119 (1)C15—C16—H21109.5
C2—C3—H3120.3H19—C16—H20109.5
C4—C3—H3120.3H19—C16—H21109.5
C3—C4—C5121 (1)H20—C16—H21109.5
C3—C4—H4119.4N4—C17—C18114.9 (4)
C5—C4—H4119.4N4—C17—H22108.1
N1—C5—C4117.7 (8)N4—C17—H23108.1
N1—C5—C6117.2 (6)C18—C17—H22108.1
C4—C5—C6125.1 (8)C18—C17—H23108.1
N2—C6—C5112.9 (5)H22—C17—H23109.5
N2—C6—H5108.6C17—C18—H24109.5
N2—C6—H6108.6C17—C18—H25109.5
C5—C6—H5108.6C17—C18—H26109.5
C5—C6—H6108.6H24—C18—H25109.5
H5—C6—H6109.5H24—C18—H26109.5
N2—C7—C8110.3 (5)H25—C18—H26109.5
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x, y, z; (iii) x+1, y1/2, z+1/2; (iv) x, y+1/2, z+1/2; (v) x+1, y, z+1; (vi) x+1, y, z; (vii) x+1, y+1/2, z+1/2.

Experimental details

Crystal data
Chemical formula[CuCl(C18H26N4)]ClO4
Mr496.88
Crystal system, space groupMonoclinic, P21/c
Temperature (K)298
a, b, c (Å)12.513 (2), 14.613 (2), 12.569 (2)
β (°) 109.34 (1)
V3)2168.6 (1)
Z4
Radiation typeMo Kα
µ (mm1)1.29
Crystal size (mm)0.65 × 0.55 × 0.3
Data collection
DiffractometerRigaku AFC-5S
diffractometer
Absorption correctionIntegration
(Coppens et al., 1965)
Tmin, Tmax0.469, 0.701
No. of measured, independent and
observed [I > 2σ(I)] reflections
5399, 4971, 2593
Rint0.025
(sin θ/λ)max1)0.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.064, 0.161, 1.51
No. of reflections4971
No. of parameters262
No. of restraints?
H-atom treatmentH-atom parameters not refined
Δρmax, Δρmin (e Å3)0.45, 0.43

Computer programs: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1993), MSC/AFC Diffractometer Control Software, TEXSAN (Molecular Structure Corporation, 1999), SIR92 (Altomare et al., 1994), TEXSAN.

Selected bond lengths (Å) top
Cu1—Cl12.240 (1)Cu1—N32.011 (5)
Cu1—N12.008 (5)Cu1—N42.352 (4)
Cu1—N22.042 (4)
 

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