Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
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

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806032909/ci2103sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806032909/ci2103Isup2.hkl
Contains datablock I

CCDC reference: 620731

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](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

Computing details top

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]Cl2·2H2OF(000) = 808
Mr = 377.99Dx = 1.395 Mg m3
Orthorhombic, PbcnMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2n 2abCell parameters from 3938 reflections
a = 15.005 (4) Åθ = 2.5–28.2°
b = 9.591 (3) ŵ = 1.39 mm1
c = 12.505 (3) ÅT = 298 K
V = 1799.6 (9) Å3Block, blue
Z = 40.35 × 0.33 × 0.21 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1593 independent reflections
Radiation source: fine-focus sealed tube1303 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.028
φ and ω scansθmax = 25.0°, θmin = 2.5°
Absorption correction: multi-scan
(SADABS; Bruker, 1998)
h = 817
Tmin = 0.629, Tmax = 0.744k = 1111
8632 measured reflectionsl = 1414
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.038H-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 reflectionsΔρmax = 0.77 e Å3
91 parametersΔρmin = 0.89 e Å3
3 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction 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
xyzUiso*/Ueq
Ni10.50000.69497 (6)0.75000.0262 (3)
Cl10.84573 (8)0.34314 (12)0.47700 (10)0.0538 (4)
N10.5918 (2)0.8592 (4)0.7363 (3)0.0407 (8)
H1A0.62380.86660.79680.049*
H1B0.62950.84250.68180.049*
N20.5960 (2)0.5270 (3)0.7387 (3)0.0373 (8)
O10.51356 (17)0.7004 (3)0.9207 (2)0.0370 (7)
H50.56120.73950.94210.055*
H60.47140.74350.95180.055*
O20.8352 (2)0.6691 (4)0.4835 (4)0.0774 (13)
H70.82990.58090.48390.116*
H80.78310.70400.48260.116*
C10.5423 (4)0.9892 (5)0.7168 (5)0.0602 (13)
H1C0.52750.99670.64150.072*
H1D0.57901.06870.73600.072*
C20.5491 (4)0.4059 (5)0.7612 (6)0.101 (3)
H2A0.55750.38450.83630.121*
H2B0.57580.33060.72050.121*
C30.6655 (4)0.5337 (7)0.8172 (5)0.092 (2)
H3A0.63970.54630.88680.138*
H3B0.70420.61070.80140.138*
H3C0.69910.44850.81600.138*
C40.6345 (4)0.5086 (6)0.6346 (4)0.0802 (19)
H4A0.67250.42800.63500.120*
H4B0.66890.58950.61630.120*
H4C0.58790.49580.58290.120*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni10.0255 (4)0.0248 (4)0.0284 (4)0.0000.0009 (3)0.000
Cl10.0490 (7)0.0515 (7)0.0610 (7)0.0052 (5)0.0167 (5)0.0009 (5)
N10.0393 (19)0.0419 (19)0.0409 (19)0.0104 (16)0.0011 (15)0.0019 (15)
N20.0401 (18)0.0324 (18)0.0393 (18)0.0097 (15)0.0030 (14)0.0025 (14)
O10.0352 (15)0.0413 (16)0.0344 (15)0.0023 (12)0.0029 (12)0.0030 (12)
O20.047 (2)0.049 (2)0.137 (4)0.0015 (16)0.024 (2)0.021 (2)
C10.082 (4)0.032 (2)0.067 (3)0.012 (3)0.015 (3)0.003 (2)
C20.071 (4)0.037 (3)0.196 (9)0.019 (3)0.003 (5)0.012 (4)
C30.081 (4)0.115 (5)0.080 (4)0.062 (4)0.042 (3)0.036 (4)
C40.099 (4)0.084 (4)0.057 (3)0.052 (4)0.021 (3)0.001 (3)
Geometric parameters (Å, º) top
Ni1—N12.099 (3)O2—H70.85
Ni1—N1i2.099 (3)O2—H80.85
Ni1—O12.145 (3)C1—C1i1.518 (10)
Ni1—O1i2.145 (3)C1—H1C0.97
Ni1—N2i2.166 (3)C1—H1D0.97
Ni1—N22.166 (3)C2—C2i1.500 (12)
N1—C11.472 (6)C2—H2A0.97
N1—H1A0.90C2—H2B0.97
N1—H1B0.90C3—H3A0.96
N2—C21.387 (6)C3—H3B0.96
N2—C31.433 (6)C3—H3C0.96
N2—C41.435 (6)C4—H4A0.96
O1—H50.85C4—H4B0.96
O1—H60.85C4—H4C0.96
N1—Ni1—N1i82.8 (2)Ni1—O1—H6113.4
N1—Ni1—O190.06 (12)H5—O1—H6105.4
N1i—Ni1—O187.85 (11)H7—O2—H8107.7
N1—Ni1—O1i87.85 (12)N1—C1—C1i109.3 (3)
N1i—Ni1—O1i90.06 (12)N1—C1—H1C109.8
O1—Ni1—O1i177.21 (15)C1i—C1—H1C109.8
N1—Ni1—N2i178.84 (13)N1—C1—H1D109.8
N1i—Ni1—N2i96.68 (14)C1i—C1—H1D109.8
O1—Ni1—N2i90.93 (11)H1C—C1—H1D108.3
O1i—Ni1—N2i91.15 (11)N2—C2—C2i117.5 (4)
N1—Ni1—N296.68 (14)N2—C2—H2A107.9
N1i—Ni1—N2178.84 (13)C2i—C2—H2A107.9
O1—Ni1—N291.15 (11)N2—C2—H2B107.9
O1i—Ni1—N290.93 (11)C2i—C2—H2B107.9
N2i—Ni1—N283.90 (19)H2A—C2—H2B107.2
C1—N1—Ni1108.6 (3)N2—C3—H3A109.5
C1—N1—H1A110.0N2—C3—H3B109.5
Ni1—N1—H1A110.0H3A—C3—H3B109.5
C1—N1—H1B110.0N2—C3—H3C109.5
Ni1—N1—H1B110.0H3A—C3—H3C109.5
H1A—N1—H1B108.3H3B—C3—H3C109.5
C2—N2—C3105.5 (4)N2—C4—H4A109.5
C2—N2—C4106.6 (4)N2—C4—H4B109.5
C3—N2—C4109.5 (4)H4A—C4—H4B109.5
C2—N2—Ni1105.8 (3)N2—C4—H4C109.5
C3—N2—Ni1114.0 (3)H4A—C4—H4C109.5
C4—N2—Ni1114.8 (3)H4B—C4—H4C109.5
Ni1—O1—H5113.9
N1i—Ni1—N1—C113.8 (2)O1i—Ni1—N2—C3144.4 (4)
O1—Ni1—N1—C1101.7 (3)N2i—Ni1—N2—C3124.6 (4)
O1i—Ni1—N1—C176.5 (3)N1—Ni1—N2—C470.9 (4)
N2—Ni1—N1—C1167.2 (3)O1—Ni1—N2—C4161.1 (4)
N1—Ni1—N2—C2171.9 (4)O1i—Ni1—N2—C417.0 (4)
O1—Ni1—N2—C281.7 (4)N2i—Ni1—N2—C4108.1 (4)
O1i—Ni1—N2—C2100.1 (4)Ni1—N1—C1—C1i38.6 (6)
N2i—Ni1—N2—C29.1 (3)C3—N2—C2—C2i147.2 (8)
N1—Ni1—N2—C356.5 (4)C4—N2—C2—C2i96.4 (8)
O1—Ni1—N2—C333.7 (4)Ni1—N2—C2—C2i26.1 (9)
Symmetry code: (i) x+1, y, z+3/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H7···Cl10.852.293.132 (4)168
O2—H8···Cl1ii0.852.353.188 (4)168
O1—H6···Cl1iii0.852.293.139 (3)173
O1—H5···O2iv0.851.862.707 (4)177
N1—H1B···Cl1ii0.902.593.378 (4)147
N1—H1A···O2iv0.902.443.291 (6)158
Symmetry codes: (ii) x+3/2, y+1/2, z; (iii) x1/2, y+1/2, z+3/2; (iv) x+3/2, y+3/2, z+1/2.
 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

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