Download citation
Download citation
link to html
In the title binuclear copper(II) complex, [Cu2Cl3(CH3O)(C10H9N3)2], the metal centers adopt distorted trigonal bipyramidal five-coordinate geometry. The mol­ecule possesses a C2 axis, on which lie the bridging Cl anion and the methoxy group. The non-bridging coordinated Cl ions participate in N—H...Cl and C—H...Cl inter- and intramolecular hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803026151/su6053sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803026151/su6053Isup2.hkl
Contains datablock I

CCDC reference: 227759

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.042
  • wR factor = 0.096
  • Data-to-parameter ratio = 17.3

checkCIF/PLATON results

No syntax errors found



Alert level A PLAT707_ALERT_1_A D...A Calc 20.101(3), Rep 3.188(3), Dev.. 5637.67 Sigma N2 -CL2 1.555 3.566 PLAT707_ALERT_1_A D...A Calc 21.591(4), Rep 3.717(4), Dev.. 4468.50 Sigma C3 -CL1 1.555 5.445 PLAT726_ALERT_1_A H...A Calc 19.71690, Rep 2.32000, Dev.. 17.40 Ang. H2A -CL2 1.555 3.566 PLAT726_ALERT_1_A H...A Calc 21.10100, Rep 2.83000, Dev.. 18.27 Ang. H3A -CL1 1.555 5.445 PLAT728_ALERT_1_A D-H..A Calc 114.67, Rep 170.00, Dev. 55.33 Deg. N2 -H2A -CL2 1.555 1.555 3.566 PLAT728_ALERT_1_A D-H..A Calc 119.91, Rep 156.00, Dev. 36.09 Deg. C3 -H3A -CL1 1.555 1.555 5.445
6 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 0 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 6 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: COLLECT (Nonius, 1998); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Sheldrick, 1997); software used to prepare material for publication: SHELXTL.

µ-chloro-µ-methoxy-bis[chloro(di-2-pyridylamine)copper(II)] top
Crystal data top
[Cu2Cl3(CH3O)(C10H9N3)2]F(000) = 1224
Mr = 606.87Dx = 1.750 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from all reflections
a = 16.9245 (3) Åθ = 2.3–27.5°
b = 7.6655 (2) ŵ = 2.22 mm1
c = 19.2417 (4) ÅT = 150 K
β = 112.6724 (9)°Plate, green
V = 2303.41 (9) Å30.10 × 0.10 × 0.02 mm
Z = 4
Data collection top
Nonius KappaCCD
diffractometer
2633 independent reflections
Radiation source: fine-focus sealed tube2028 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.066
φ and ω scansθmax = 27.5°, θmin = 2.3°
Absorption correction: multi-scan
Blessing, 1995
h = 2121
Tmin = 0.836, Tmax = 0.965k = 99
9609 measured reflectionsl = 2424
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.042Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.096H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0447P)2 + 3.9941P]
where P = (Fo2 + 2Fc2)/3
2633 reflections(Δ/σ)max = 0.001
152 parametersΔρmax = 0.81 e Å3
0 restraintsΔρmin = 0.54 e Å3
Special details top

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) top
xyzUiso*/UeqOcc. (<1)
Cu0.01537 (2)0.55208 (5)0.33904 (2)0.02169 (15)
Cl10.00000.79493 (15)0.25000.0251 (3)
Cl20.13860 (5)0.38716 (12)0.40850 (5)0.0285 (2)
O10.00000.4194 (4)0.25000.0224 (7)
N10.10866 (16)0.5208 (4)0.33323 (15)0.0206 (6)
N20.08074 (16)0.6477 (4)0.45286 (15)0.0236 (6)
H2A0.10040.65000.48910.028*
N30.04158 (16)0.7120 (4)0.42653 (15)0.0240 (6)
C10.1664 (2)0.4450 (5)0.27081 (19)0.0252 (7)
H1A0.14840.41270.23160.030*
C20.2497 (2)0.4125 (5)0.2613 (2)0.0270 (8)
H2B0.28760.35430.21750.032*
C30.2776 (2)0.4663 (5)0.31709 (19)0.0267 (8)
H3A0.33540.44860.31120.032*
C40.2210 (2)0.5449 (5)0.38045 (19)0.0256 (8)
H4A0.23870.58200.41930.031*
C50.1359 (2)0.5702 (4)0.38714 (18)0.0207 (7)
C60.0009 (2)0.7218 (4)0.47249 (18)0.0224 (7)
C70.0337 (2)0.8075 (5)0.54221 (18)0.0264 (7)
H7A0.00310.81030.57450.032*
C80.1119 (2)0.8870 (5)0.5634 (2)0.0313 (8)
H8A0.13670.94320.61100.038*
C90.1549 (2)0.8844 (5)0.5141 (2)0.0349 (9)
H9A0.20810.94300.52620.042*
C100.1181 (2)0.7953 (5)0.4483 (2)0.0305 (8)
H10A0.14780.79100.41530.037*
C110.00000.2346 (7)0.25000.0363 (13)
H11A0.00870.19200.19950.054*0.50
H11B0.04630.19200.26420.054*0.50
H11C0.05500.19200.28630.054*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu0.0155 (2)0.0314 (3)0.0187 (2)0.00132 (17)0.00716 (16)0.00178 (17)
Cl10.0241 (6)0.0278 (6)0.0224 (6)0.0000.0077 (5)0.000
Cl20.0190 (4)0.0456 (5)0.0210 (4)0.0057 (3)0.0077 (3)0.0022 (4)
O10.0203 (16)0.0259 (18)0.0221 (17)0.0000.0093 (13)0.000
N10.0172 (13)0.0281 (15)0.0168 (13)0.0003 (11)0.0069 (11)0.0014 (12)
N20.0198 (14)0.0359 (17)0.0179 (14)0.0014 (12)0.0104 (11)0.0018 (12)
N30.0192 (14)0.0318 (16)0.0214 (15)0.0021 (12)0.0083 (12)0.0005 (12)
C10.0217 (16)0.0326 (19)0.0208 (17)0.0002 (15)0.0077 (14)0.0003 (15)
C20.0228 (17)0.0288 (19)0.0247 (18)0.0036 (14)0.0039 (14)0.0010 (15)
C30.0158 (16)0.036 (2)0.0286 (19)0.0003 (14)0.0093 (14)0.0060 (16)
C40.0186 (16)0.036 (2)0.0245 (18)0.0063 (15)0.0113 (14)0.0033 (16)
C50.0189 (16)0.0248 (17)0.0195 (16)0.0022 (13)0.0087 (13)0.0039 (14)
C60.0184 (16)0.0231 (17)0.0205 (17)0.0033 (13)0.0018 (13)0.0023 (14)
C70.0290 (18)0.0286 (19)0.0191 (17)0.0039 (15)0.0067 (14)0.0007 (15)
C80.0302 (19)0.029 (2)0.0242 (19)0.0003 (15)0.0013 (15)0.0030 (16)
C90.0216 (18)0.037 (2)0.038 (2)0.0063 (16)0.0038 (16)0.0003 (18)
C100.0242 (18)0.038 (2)0.030 (2)0.0051 (16)0.0103 (15)0.0007 (17)
C110.033 (3)0.035 (3)0.036 (3)0.0000.009 (2)0.000
Geometric parameters (Å, º) top
Cu—O11.9220 (17)C4—C51.408 (4)
Cu—N31.990 (3)C6—C71.403 (5)
Cu—N12.072 (3)C7—C81.368 (5)
Cu—Cl22.3633 (9)C8—C91.402 (5)
Cu—Cl12.4748 (10)C9—C101.360 (5)
Cl1—Cui2.4748 (10)N2—H2A0.8810
O1—C111.416 (6)C1—H1A0.9490
O1—Cui1.9220 (17)C2—H2B0.9508
N1—C51.342 (4)C3—H3A0.9501
N1—C11.353 (4)C4—H4A0.9498
N2—C61.378 (4)C7—H7A0.9501
N2—C51.383 (4)C8—H8A0.9509
N3—C61.339 (4)C9—H9A0.9514
N3—C101.356 (4)C10—H10A0.9503
C1—C21.374 (5)C11—H11A0.9809
C2—C31.391 (5)C11—H11B0.9800
C3—C41.367 (5)C11—H11C0.9797
O1—Cu—N3171.81 (10)N2—C6—C7117.3 (3)
O1—Cu—N196.00 (8)C8—C7—C6119.5 (3)
N3—Cu—N190.44 (11)C7—C8—C9119.1 (3)
O1—Cu—Cl290.44 (6)C10—C9—C8117.7 (3)
N3—Cu—Cl289.47 (8)N3—C10—C9124.4 (3)
N1—Cu—Cl2128.56 (8)C5—N2—H2A113.86
O1—Cu—Cl180.73 (8)C6—N2—H2A113.86
N3—Cu—Cl192.97 (9)N1—C1—H1A118.33
N1—Cu—Cl1102.45 (7)C2—C1—H1A118.34
Cl2—Cu—Cl1128.92 (3)C1—C2—H2B120.71
Cui—Cl1—Cu82.44 (4)C3—C2—H2B120.62
C11—O1—Cu121.95 (8)C2—C3—H3A120.37
C11—O1—Cui121.95 (8)C4—C3—H3A120.33
Cu—O1—Cui116.09 (16)C3—C4—H4A120.60
C5—N1—C1117.5 (3)C5—C4—H4A120.55
C5—N1—Cu124.7 (2)C6—C7—H7A120.27
C1—N1—Cu117.9 (2)C8—C7—H7A120.22
C6—N2—C5132.3 (3)C7—C8—H8A120.38
C6—N3—C10117.4 (3)C9—C8—H8A120.47
C6—N3—Cu126.3 (2)C8—C9—H9A121.15
C10—N3—Cu115.2 (2)C10—C9—H9A121.04
N1—C1—C2123.3 (3)N3—C10—H10A117.71
C1—C2—C3118.7 (3)C9—C10—H10A117.98
C4—C3—C2119.3 (3)O1—C11—H11A109.44
C3—C4—C5118.9 (3)O1—C11—H11B109.46
N1—C5—N2121.0 (3)O1—C11—H11C109.47
N1—C5—C4122.3 (3)H11A—C11—H11B109.54
N2—C5—C4116.7 (3)H11A—C11—H11C109.50
N3—C6—N2121.0 (3)H11B—C11—H11C109.41
N3—C6—C7121.7 (3)
Symmetry code: (i) x, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···Cl2ii0.882.323.188 (3)170
C1—H1A···Cl2i0.952.773.684 (4)162
C1—H1A···O10.952.403.000 (4)121
C3—H3A···Cl1iii0.952.833.717 (4)156
C9—H9A···Cl2iv0.952.743.672 (4)168
C11—H11A···Cl2i0.982.803.264 (2)109
C11—H11C···Cl20.982.683.264 (2)118
Symmetry codes: (i) x, y, z+1/2; (ii) x+1/2, y+3/2, z+1; (iii) x1, y1, z; (iv) x+1/2, y+3/2, z+1.
 

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds