In the centrosymmetric title compound, [Cu(C2N3)2(C10H8N2O)2], the CuII atom adopts a distorted octahedral geometry, with the equatorial plane formed by two O atoms and two N atoms of two chelating 2,2'-bipyridine N-oxide ligands. The axial positions are occupied by N atoms of two monodentate dicyanamide anions.
Supporting information
CCDC reference: 630450
Key indicators
- Single-crystal X-ray study
- T = 298 K
- Mean (C-C) = 0.002 Å
- R factor = 0.027
- wR factor = 0.083
- Data-to-parameter ratio = 15.8
checkCIF/PLATON results
No syntax errors found
Alert level B
PLAT232_ALERT_2_B Hirshfeld Test Diff (M-X) Cu1 - N4 .. 16.34 su
Alert level C
PLAT220_ALERT_2_C Large Non-Solvent N Ueq(max)/Ueq(min) ... 2.70 Ratio
PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Cu1 - O1 .. 5.38 su
PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Cu1 - N2 .. 5.10 su
PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for N5
PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C11
PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C12
0 ALERT level A = In general: serious problem
1 ALERT level B = Potentially serious problem
6 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
7 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
0 ALERT type 5 Informative message, check
Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Sheldrick, 1999); software used to prepare material for publication: SHELXTL.
Bis(2,2'-bipyridine
N-oxide)bis(dicyanamido)copper(II)
top
Crystal data top
[Cu(C2N3)2(C10H8N2O)2] | F(000) = 550 |
Mr = 540.01 | Dx = 1.595 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -p2ybc | Cell parameters from 25 reflections |
a = 10.206 (2) Å | θ = 2.1–25.3° |
b = 8.0840 (16) Å | µ = 1.02 mm−1 |
c = 13.638 (3) Å | T = 298 K |
β = 92.56 (3)° | Block, green |
V = 1124.1 (4) Å3 | 0.18 × 0.16 × 0.15 mm |
Z = 2 | |
Data collection top
Bruker SMART CCD diffractometer | 2667 independent reflections |
Radiation source: fine-focus sealed tube | 2376 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.017 |
φ and ω scans | θmax = 28.2°, θmin = 2.0° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −13→13 |
Tmin = 0.830, Tmax = 0.856 | k = −10→10 |
9715 measured reflections | l = −17→17 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.027 | H-atom parameters constrained |
wR(F2) = 0.083 | w = 1/[σ2(Fo2) + (0.0427P)2 + 0.381P] where P = (Fo2 + 2Fc2)/3 |
S = 1.01 | (Δ/σ)max < 0.001 |
2667 reflections | Δρmax = 0.32 e Å−3 |
169 parameters | Δρmin = −0.38 e Å−3 |
0 restraints | Extinction correction: SHELXL97 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0076 (13) |
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 | x | y | z | Uiso*/Ueq | |
Cu1 | 0.5000 | 0.0000 | 0.5000 | 0.02565 (10) | |
O1 | 0.35553 (10) | 0.04937 (13) | 0.40476 (8) | 0.0283 (2) | |
N1 | 0.31695 (12) | 0.20832 (15) | 0.40207 (9) | 0.0256 (3) | |
N2 | 0.60380 (12) | 0.17285 (15) | 0.43051 (9) | 0.0264 (3) | |
N3 | −0.01728 (18) | 0.1355 (3) | 0.61789 (18) | 0.0692 (6) | |
N4 | 0.40599 (15) | 0.2095 (2) | 0.61252 (12) | 0.0430 (3) | |
N5 | 0.18999 (19) | 0.2576 (3) | 0.67908 (15) | 0.0672 (6) | |
C1 | 0.18821 (15) | 0.2389 (2) | 0.41171 (12) | 0.0332 (3) | |
H1A | 0.1302 | 0.1517 | 0.4193 | 0.040* | |
C2 | 0.14285 (17) | 0.3987 (2) | 0.41028 (14) | 0.0404 (4) | |
H2A | 0.0541 | 0.4196 | 0.4172 | 0.049* | |
C3 | 0.22881 (19) | 0.5284 (2) | 0.39855 (15) | 0.0416 (4) | |
H3A | 0.1991 | 0.6372 | 0.3984 | 0.050* | |
C4 | 0.36011 (18) | 0.49340 (19) | 0.38702 (14) | 0.0355 (4) | |
H4A | 0.4189 | 0.5795 | 0.3783 | 0.043* | |
C5 | 0.40476 (14) | 0.33155 (18) | 0.38841 (11) | 0.0271 (3) | |
C6 | 0.54419 (14) | 0.29080 (18) | 0.37422 (11) | 0.0265 (3) | |
C7 | 0.61083 (16) | 0.3791 (2) | 0.30490 (12) | 0.0332 (3) | |
H7A | 0.5675 | 0.4595 | 0.2669 | 0.040* | |
C8 | 0.74220 (17) | 0.3468 (2) | 0.29267 (13) | 0.0381 (4) | |
H8A | 0.7879 | 0.4029 | 0.2454 | 0.046* | |
C9 | 0.80396 (16) | 0.2300 (2) | 0.35186 (14) | 0.0374 (4) | |
H9A | 0.8926 | 0.2071 | 0.3460 | 0.045* | |
C10 | 0.73232 (15) | 0.1473 (2) | 0.42005 (12) | 0.0325 (3) | |
H10A | 0.7752 | 0.0702 | 0.4607 | 0.039* | |
C11 | 0.08167 (18) | 0.1897 (2) | 0.64381 (14) | 0.0430 (4) | |
C12 | 0.30223 (18) | 0.2282 (2) | 0.64098 (12) | 0.0374 (4) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Cu1 | 0.02130 (15) | 0.02481 (15) | 0.03060 (15) | −0.00318 (9) | −0.00179 (10) | 0.00596 (9) |
O1 | 0.0269 (5) | 0.0231 (5) | 0.0345 (5) | −0.0011 (4) | −0.0047 (4) | −0.0001 (4) |
N1 | 0.0253 (6) | 0.0259 (6) | 0.0254 (6) | 0.0005 (5) | −0.0022 (5) | 0.0015 (5) |
N2 | 0.0232 (6) | 0.0251 (6) | 0.0309 (6) | −0.0019 (5) | 0.0003 (5) | 0.0024 (5) |
N3 | 0.0352 (9) | 0.0729 (13) | 0.1003 (16) | 0.0014 (9) | 0.0110 (10) | −0.0118 (12) |
N4 | 0.0370 (8) | 0.0441 (9) | 0.0474 (8) | −0.0061 (6) | −0.0023 (7) | −0.0022 (7) |
N5 | 0.0530 (11) | 0.0876 (15) | 0.0627 (11) | −0.0182 (10) | 0.0208 (9) | −0.0339 (11) |
C1 | 0.0235 (7) | 0.0392 (9) | 0.0366 (8) | −0.0018 (6) | −0.0006 (6) | 0.0009 (7) |
C2 | 0.0285 (8) | 0.0444 (10) | 0.0483 (9) | 0.0078 (7) | 0.0015 (7) | −0.0025 (8) |
C3 | 0.0402 (10) | 0.0328 (9) | 0.0516 (11) | 0.0105 (7) | −0.0015 (8) | −0.0023 (7) |
C4 | 0.0345 (9) | 0.0274 (8) | 0.0443 (9) | −0.0003 (6) | −0.0003 (7) | 0.0024 (6) |
C5 | 0.0262 (7) | 0.0270 (7) | 0.0278 (7) | −0.0008 (5) | −0.0005 (5) | 0.0023 (5) |
C6 | 0.0266 (7) | 0.0248 (7) | 0.0280 (7) | −0.0029 (5) | 0.0006 (5) | 0.0002 (5) |
C7 | 0.0348 (8) | 0.0307 (8) | 0.0342 (8) | −0.0021 (6) | 0.0033 (6) | 0.0063 (6) |
C8 | 0.0361 (9) | 0.0379 (9) | 0.0411 (9) | −0.0075 (7) | 0.0114 (7) | 0.0036 (7) |
C9 | 0.0265 (8) | 0.0356 (9) | 0.0508 (10) | −0.0034 (6) | 0.0082 (7) | 0.0004 (7) |
C10 | 0.0256 (7) | 0.0295 (8) | 0.0422 (8) | −0.0012 (6) | −0.0004 (6) | 0.0030 (6) |
C11 | 0.0390 (10) | 0.0425 (10) | 0.0486 (10) | 0.0055 (8) | 0.0141 (8) | 0.0004 (8) |
C12 | 0.0435 (10) | 0.0376 (9) | 0.0308 (8) | −0.0084 (7) | −0.0018 (7) | −0.0021 (7) |
Geometric parameters (Å, º) top
Cu1—O1 | 1.9620 (12) | C2—C3 | 1.381 (3) |
Cu1—O1i | 1.9620 (12) | C2—H2A | 0.9300 |
Cu1—N2 | 2.0156 (13) | C3—C4 | 1.385 (3) |
Cu1—N2i | 2.0156 (13) | C3—H3A | 0.9300 |
Cu1—N4 | 2.5052 (17) | C4—C5 | 1.385 (2) |
O1—N1 | 1.3439 (16) | C4—H4A | 0.9300 |
N1—C1 | 1.3492 (19) | C5—C6 | 1.482 (2) |
N1—C5 | 1.3584 (19) | C6—C7 | 1.387 (2) |
N2—C10 | 1.3417 (19) | C7—C8 | 1.383 (2) |
N2—C6 | 1.3516 (19) | C7—H7A | 0.9300 |
N3—C11 | 1.142 (3) | C8—C9 | 1.377 (3) |
N4—C12 | 1.154 (2) | C8—H8A | 0.9300 |
N5—C12 | 1.301 (3) | C9—C10 | 1.381 (2) |
N5—C11 | 1.307 (3) | C9—H9A | 0.9300 |
C1—C2 | 1.372 (2) | C10—H10A | 0.9300 |
C1—H1A | 0.9300 | | |
| | | |
O1—Cu1—O1i | 180.00 (5) | C2—C3—H3A | 120.6 |
O1—Cu1—N2 | 86.73 (5) | C4—C3—H3A | 120.6 |
O1i—Cu1—N2 | 93.27 (5) | C5—C4—C3 | 120.71 (16) |
O1—Cu1—N2i | 93.27 (5) | C5—C4—H4A | 119.6 |
O1i—Cu1—N2i | 86.73 (5) | C3—C4—H4A | 119.6 |
N2—Cu1—N2i | 180.0 | N1—C5—C4 | 118.41 (14) |
O1—Cu1—N4 | 88.34 (5) | N1—C5—C6 | 119.88 (13) |
O1i—Cu1—N4 | 91.66 (5) | C4—C5—C6 | 121.70 (14) |
N2—Cu1—N4 | 92.46 (6) | N2—C6—C7 | 121.89 (14) |
N2i—Cu1—N4 | 87.54 (6) | N2—C6—C5 | 119.56 (13) |
N1—O1—Cu1 | 115.04 (8) | C7—C6—C5 | 118.52 (14) |
O1—N1—C1 | 117.27 (12) | C8—C7—C6 | 119.49 (15) |
O1—N1—C5 | 120.70 (12) | C8—C7—H7A | 120.3 |
C1—N1—C5 | 122.02 (13) | C6—C7—H7A | 120.3 |
C10—N2—C6 | 117.77 (13) | C9—C8—C7 | 118.67 (15) |
C10—N2—Cu1 | 118.68 (10) | C9—C8—H8A | 120.7 |
C6—N2—Cu1 | 121.56 (10) | C7—C8—H8A | 120.7 |
C12—N4—Cu1 | 132.57 (13) | C8—C9—C10 | 118.99 (15) |
C12—N5—C11 | 121.47 (18) | C8—C9—H9A | 120.5 |
N1—C1—C2 | 120.06 (15) | C10—C9—H9A | 120.5 |
N1—C1—H1A | 120.0 | N2—C10—C9 | 123.12 (15) |
C2—C1—H1A | 120.0 | N2—C10—H10A | 118.4 |
C1—C2—C3 | 120.05 (16) | C9—C10—H10A | 118.4 |
C1—C2—H2A | 120.0 | N3—C11—N5 | 175.4 (2) |
C3—C2—H2A | 120.0 | N4—C12—N5 | 174.90 (19) |
C2—C3—C4 | 118.73 (16) | | |
Symmetry code: (i) −x+1, −y, −z+1. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
C4—H4A···N4ii | 0.93 | 2.47 | 3.386 (2) | 169 |
Symmetry code: (ii) −x+1, −y+1, −z+1. |