In the title compound, [Ni(C2H8N2)(C6H16N2)(H2O)2]Cl2·2H2O, the NiII ion, located on a twofold axis, is coordinated by four N atoms of the ethylenediamine and N,N,N',N'-tetramethylethylenediamine ligands and two water molecules in a distorted octahedral geometry. Hydrogen bonds between ethylenediamine, water molecules and chloride ions help to construct a three-dimensional supramolecular architecture.
Supporting information
CCDC reference: 620731
Key indicators
- Single-crystal X-ray study
- T = 298 K
- Mean
(C-C) = 0.009 Å
- R factor = 0.038
- wR factor = 0.112
- Data-to-parameter ratio = 17.5
checkCIF/PLATON results
No syntax errors found
Alert level B
PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ?
PLAT242_ALERT_2_B Check Low Ueq as Compared to Neighbors for N2
Alert level C
PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ?
PLAT341_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 9
0 ALERT level A = In general: serious problem
2 ALERT level B = Potentially serious problem
2 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
2 ALERT type 2 Indicator that the structure model may be wrong or deficient
1 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, 1998); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.
Diaqua(ethylenediamine)(
N,
N,
N',
N'-tetramethylethylenediamine)nickel(II) dichloride dihydrate
top
Crystal data top
[Ni(C2H8N2)(C6H16N2)(H2O)2]Cl2·2H2O | F(000) = 808 |
Mr = 377.99 | Dx = 1.395 Mg m−3 |
Orthorhombic, Pbcn | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2n 2ab | Cell parameters from 3938 reflections |
a = 15.005 (4) Å | θ = 2.5–28.2° |
b = 9.591 (3) Å | µ = 1.39 mm−1 |
c = 12.505 (3) Å | T = 298 K |
V = 1799.6 (9) Å3 | Block, blue |
Z = 4 | 0.35 × 0.33 × 0.21 mm |
Data collection top
Bruker SMART CCD area-detector diffractometer | 1593 independent reflections |
Radiation source: fine-focus sealed tube | 1303 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.028 |
φ and ω scans | θmax = 25.0°, θmin = 2.5° |
Absorption correction: multi-scan (SADABS; Bruker, 1998) | h = −8→17 |
Tmin = 0.629, Tmax = 0.744 | k = −11→11 |
8632 measured reflections | l = −14→14 |
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)] = 0.038 | H-atom parameters constrained |
wR(F2) = 0.112 | w = 1/[σ2(Fo2) + (0.0503P)2 + 3.0865P] where P = (Fo2 + 2Fc2)/3 |
S = 1.09 | (Δ/σ)max = 0.001 |
1593 reflections | Δρmax = 0.77 e Å−3 |
91 parameters | Δρmin = −0.89 e Å−3 |
3 restraints | Extinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0173 (16) |
Special details top
Experimental. The IUCr checkCIF software suggested the possibility of lattice centering
or cell halving. But we were unable to see any evidence for these from the
reflection data. |
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 | |
Ni1 | 0.5000 | 0.69497 (6) | 0.7500 | 0.0262 (3) | |
Cl1 | 0.84573 (8) | 0.34314 (12) | 0.47700 (10) | 0.0538 (4) | |
N1 | 0.5918 (2) | 0.8592 (4) | 0.7363 (3) | 0.0407 (8) | |
H1A | 0.6238 | 0.8666 | 0.7968 | 0.049* | |
H1B | 0.6295 | 0.8425 | 0.6818 | 0.049* | |
N2 | 0.5960 (2) | 0.5270 (3) | 0.7387 (3) | 0.0373 (8) | |
O1 | 0.51356 (17) | 0.7004 (3) | 0.9207 (2) | 0.0370 (7) | |
H5 | 0.5612 | 0.7395 | 0.9421 | 0.055* | |
H6 | 0.4714 | 0.7435 | 0.9518 | 0.055* | |
O2 | 0.8352 (2) | 0.6691 (4) | 0.4835 (4) | 0.0774 (13) | |
H7 | 0.8299 | 0.5809 | 0.4839 | 0.116* | |
H8 | 0.7831 | 0.7040 | 0.4826 | 0.116* | |
C1 | 0.5423 (4) | 0.9892 (5) | 0.7168 (5) | 0.0602 (13) | |
H1C | 0.5275 | 0.9967 | 0.6415 | 0.072* | |
H1D | 0.5790 | 1.0687 | 0.7360 | 0.072* | |
C2 | 0.5491 (4) | 0.4059 (5) | 0.7612 (6) | 0.101 (3) | |
H2A | 0.5575 | 0.3845 | 0.8363 | 0.121* | |
H2B | 0.5758 | 0.3306 | 0.7205 | 0.121* | |
C3 | 0.6655 (4) | 0.5337 (7) | 0.8172 (5) | 0.092 (2) | |
H3A | 0.6397 | 0.5463 | 0.8868 | 0.138* | |
H3B | 0.7042 | 0.6107 | 0.8014 | 0.138* | |
H3C | 0.6991 | 0.4485 | 0.8160 | 0.138* | |
C4 | 0.6345 (4) | 0.5086 (6) | 0.6346 (4) | 0.0802 (19) | |
H4A | 0.6725 | 0.4280 | 0.6350 | 0.120* | |
H4B | 0.6689 | 0.5895 | 0.6163 | 0.120* | |
H4C | 0.5879 | 0.4958 | 0.5829 | 0.120* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Ni1 | 0.0255 (4) | 0.0248 (4) | 0.0284 (4) | 0.000 | −0.0009 (3) | 0.000 |
Cl1 | 0.0490 (7) | 0.0515 (7) | 0.0610 (7) | 0.0052 (5) | −0.0167 (5) | 0.0009 (5) |
N1 | 0.0393 (19) | 0.0419 (19) | 0.0409 (19) | −0.0104 (16) | 0.0011 (15) | −0.0019 (15) |
N2 | 0.0401 (18) | 0.0324 (18) | 0.0393 (18) | 0.0097 (15) | −0.0030 (14) | −0.0025 (14) |
O1 | 0.0352 (15) | 0.0413 (16) | 0.0344 (15) | 0.0023 (12) | −0.0029 (12) | −0.0030 (12) |
O2 | 0.047 (2) | 0.049 (2) | 0.137 (4) | −0.0015 (16) | 0.024 (2) | 0.021 (2) |
C1 | 0.082 (4) | 0.032 (2) | 0.067 (3) | −0.012 (3) | 0.015 (3) | 0.003 (2) |
C2 | 0.071 (4) | 0.037 (3) | 0.196 (9) | 0.019 (3) | 0.003 (5) | 0.012 (4) |
C3 | 0.081 (4) | 0.115 (5) | 0.080 (4) | 0.062 (4) | −0.042 (3) | −0.036 (4) |
C4 | 0.099 (4) | 0.084 (4) | 0.057 (3) | 0.052 (4) | 0.021 (3) | 0.001 (3) |
Geometric parameters (Å, º) top
Ni1—N1 | 2.099 (3) | O2—H7 | 0.85 |
Ni1—N1i | 2.099 (3) | O2—H8 | 0.85 |
Ni1—O1 | 2.145 (3) | C1—C1i | 1.518 (10) |
Ni1—O1i | 2.145 (3) | C1—H1C | 0.97 |
Ni1—N2i | 2.166 (3) | C1—H1D | 0.97 |
Ni1—N2 | 2.166 (3) | C2—C2i | 1.500 (12) |
N1—C1 | 1.472 (6) | C2—H2A | 0.97 |
N1—H1A | 0.90 | C2—H2B | 0.97 |
N1—H1B | 0.90 | C3—H3A | 0.96 |
N2—C2 | 1.387 (6) | C3—H3B | 0.96 |
N2—C3 | 1.433 (6) | C3—H3C | 0.96 |
N2—C4 | 1.435 (6) | C4—H4A | 0.96 |
O1—H5 | 0.85 | C4—H4B | 0.96 |
O1—H6 | 0.85 | C4—H4C | 0.96 |
| | | |
N1—Ni1—N1i | 82.8 (2) | Ni1—O1—H6 | 113.4 |
N1—Ni1—O1 | 90.06 (12) | H5—O1—H6 | 105.4 |
N1i—Ni1—O1 | 87.85 (11) | H7—O2—H8 | 107.7 |
N1—Ni1—O1i | 87.85 (12) | N1—C1—C1i | 109.3 (3) |
N1i—Ni1—O1i | 90.06 (12) | N1—C1—H1C | 109.8 |
O1—Ni1—O1i | 177.21 (15) | C1i—C1—H1C | 109.8 |
N1—Ni1—N2i | 178.84 (13) | N1—C1—H1D | 109.8 |
N1i—Ni1—N2i | 96.68 (14) | C1i—C1—H1D | 109.8 |
O1—Ni1—N2i | 90.93 (11) | H1C—C1—H1D | 108.3 |
O1i—Ni1—N2i | 91.15 (11) | N2—C2—C2i | 117.5 (4) |
N1—Ni1—N2 | 96.68 (14) | N2—C2—H2A | 107.9 |
N1i—Ni1—N2 | 178.84 (13) | C2i—C2—H2A | 107.9 |
O1—Ni1—N2 | 91.15 (11) | N2—C2—H2B | 107.9 |
O1i—Ni1—N2 | 90.93 (11) | C2i—C2—H2B | 107.9 |
N2i—Ni1—N2 | 83.90 (19) | H2A—C2—H2B | 107.2 |
C1—N1—Ni1 | 108.6 (3) | N2—C3—H3A | 109.5 |
C1—N1—H1A | 110.0 | N2—C3—H3B | 109.5 |
Ni1—N1—H1A | 110.0 | H3A—C3—H3B | 109.5 |
C1—N1—H1B | 110.0 | N2—C3—H3C | 109.5 |
Ni1—N1—H1B | 110.0 | H3A—C3—H3C | 109.5 |
H1A—N1—H1B | 108.3 | H3B—C3—H3C | 109.5 |
C2—N2—C3 | 105.5 (4) | N2—C4—H4A | 109.5 |
C2—N2—C4 | 106.6 (4) | N2—C4—H4B | 109.5 |
C3—N2—C4 | 109.5 (4) | H4A—C4—H4B | 109.5 |
C2—N2—Ni1 | 105.8 (3) | N2—C4—H4C | 109.5 |
C3—N2—Ni1 | 114.0 (3) | H4A—C4—H4C | 109.5 |
C4—N2—Ni1 | 114.8 (3) | H4B—C4—H4C | 109.5 |
Ni1—O1—H5 | 113.9 | | |
| | | |
N1i—Ni1—N1—C1 | −13.8 (2) | O1i—Ni1—N2—C3 | 144.4 (4) |
O1—Ni1—N1—C1 | −101.7 (3) | N2i—Ni1—N2—C3 | −124.6 (4) |
O1i—Ni1—N1—C1 | 76.5 (3) | N1—Ni1—N2—C4 | −70.9 (4) |
N2—Ni1—N1—C1 | 167.2 (3) | O1—Ni1—N2—C4 | −161.1 (4) |
N1—Ni1—N2—C2 | 171.9 (4) | O1i—Ni1—N2—C4 | 17.0 (4) |
O1—Ni1—N2—C2 | 81.7 (4) | N2i—Ni1—N2—C4 | 108.1 (4) |
O1i—Ni1—N2—C2 | −100.1 (4) | Ni1—N1—C1—C1i | 38.6 (6) |
N2i—Ni1—N2—C2 | −9.1 (3) | C3—N2—C2—C2i | 147.2 (8) |
N1—Ni1—N2—C3 | 56.5 (4) | C4—N2—C2—C2i | −96.4 (8) |
O1—Ni1—N2—C3 | −33.7 (4) | Ni1—N2—C2—C2i | 26.1 (9) |
Symmetry code: (i) −x+1, y, −z+3/2. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H7···Cl1 | 0.85 | 2.29 | 3.132 (4) | 168 |
O2—H8···Cl1ii | 0.85 | 2.35 | 3.188 (4) | 168 |
O1—H6···Cl1iii | 0.85 | 2.29 | 3.139 (3) | 173 |
O1—H5···O2iv | 0.85 | 1.86 | 2.707 (4) | 177 |
N1—H1B···Cl1ii | 0.90 | 2.59 | 3.378 (4) | 147 |
N1—H1A···O2iv | 0.90 | 2.44 | 3.291 (6) | 158 |
Symmetry codes: (ii) −x+3/2, y+1/2, z; (iii) x−1/2, y+1/2, −z+3/2; (iv) −x+3/2, −y+3/2, z+1/2. |