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In the title complex, [Ni(C10H9O2)2(C10H17N)2], the Ni atom, which occupies a special position at an inversion centre, has an octa­hedral environment formed by four O atoms of two chelate benzoyl­acetonates [Ni—O 2.0409 (16) and 2.0187 (16) Å, and O—Ni—O 90.36 (6)°] and two N atoms of the adamantylamine ligands [Ni—N = 2.176 (2) Å]. The amine H atoms of the adamantylamine ligands do not participate in any hydrogen bonds, due to their steric shielding and the lack of accessible acceptors.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805004216/ya6237sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805004216/ya6237Isup2.hkl
Contains datablock I

CCDC reference: 269893

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.041
  • wR factor = 0.103
  • Data-to-parameter ratio = 14.6

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT420_ALERT_2_C D-H Without Acceptor N - H1N ... ? PLAT420_ALERT_2_C D-H Without Acceptor N - H2N ... ?
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 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 2 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: CrysAlis CCD (Oxford Diffraction, 2003); cell refinement: CrysAlis RED (Oxford Diffraction, 2003); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Bis(adamantylamine-κN)bis(1-phenylbutane-1,3-dionato-κO,O')nickel(II) top
Crystal data top
[Ni(C10H9O2)2(C10H17N)2]Z = 1
Mr = 683.55F(000) = 366
Triclinic, P1Dx = 1.271 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 6.738 (3) ÅCell parameters from 4811 reflections
b = 12.028 (3) Åθ = 2.1–30.4°
c = 12.063 (3) ŵ = 0.59 mm1
α = 70.02 (3)°T = 295 K
β = 86.88 (3)°Plate, green
γ = 76.45 (3)°0.6 × 0.3 × 0.1 mm
V = 892.8 (5) Å3
Data collection top
Oxford Diffraction Xcalibur 3 CCD area-detector
diffractometer
3129 independent reflections
Radiation source: fine-focus sealed tube2545 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.034
ω scansθmax = 25.0°, θmin = 4.2°
Absorption correction: analytical
(Alcock, 1970)
h = 88
Tmin = 0.810, Tmax = 0.941k = 1414
12713 measured reflectionsl = 1414
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)] = 0.041Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.057P)2]
where P = (Fo2 + 2Fc2)/3
3129 reflections(Δ/σ)max < 0.001
215 parametersΔρmax = 0.21 e Å3
0 restraintsΔρmin = 0.26 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*/Ueq
Ni1.00000.00000.00000.04476 (18)
O11.1488 (2)0.13748 (13)0.06614 (13)0.0474 (4)
O20.7838 (2)0.10678 (13)0.06509 (13)0.0471 (4)
N1.2002 (3)0.04761 (17)0.15284 (16)0.0507 (5)
H1N1.32610.07270.12850.061*
H2N1.19890.02380.16190.061*
C11.2466 (4)0.3200 (2)0.0943 (3)0.0687 (8)
H1A1.38680.27650.07850.103*
H1C1.21940.38330.06030.103*
H1B1.22110.35510.17800.103*
C21.1097 (3)0.2340 (2)0.0411 (2)0.0464 (5)
C30.9510 (4)0.2669 (2)0.0286 (2)0.0538 (6)
H30.94820.33660.04640.065*
C40.7962 (3)0.20688 (19)0.07441 (18)0.0424 (5)
C50.6233 (3)0.2615 (2)0.13816 (19)0.0443 (5)
C60.4898 (4)0.1919 (2)0.1984 (2)0.0557 (6)
H60.51240.11130.20240.067*
C70.3237 (4)0.2402 (3)0.2527 (2)0.0691 (7)
H70.23620.19180.29390.083*
C80.2865 (4)0.3597 (3)0.2461 (2)0.0711 (8)
H80.17240.39300.28120.085*
C90.4182 (5)0.4290 (3)0.1879 (3)0.0782 (8)
H90.39440.50960.18390.094*
C100.5866 (4)0.3807 (2)0.1348 (2)0.0663 (7)
H100.67640.42870.09630.080*
C111.1935 (3)0.13326 (19)0.27463 (18)0.0421 (5)
C120.9817 (4)0.1023 (2)0.3217 (2)0.0568 (6)
H12A0.88020.10630.27010.068*
H12B0.95310.02010.32390.068*
C130.9698 (4)0.1921 (3)0.4462 (2)0.0703 (8)
H130.83290.17200.47630.084*
C141.0120 (4)0.3199 (3)0.4415 (2)0.0746 (8)
H14A1.00160.37720.51970.090*
H14B0.91180.32500.38970.090*
C151.2238 (4)0.3517 (2)0.3963 (2)0.0580 (6)
H151.25060.43430.39330.070*
C161.2359 (4)0.2623 (2)0.2723 (2)0.0500 (6)
H16A1.37070.28280.24190.060*
H16B1.13660.26790.22030.060*
C171.3522 (4)0.1274 (2)0.3572 (2)0.0612 (7)
H17A1.48770.14720.32740.073*
H17B1.32800.04550.35950.073*
C181.1275 (5)0.1851 (3)0.5277 (2)0.0780 (9)
H18B1.10010.10380.53180.094*
H18A1.11890.24160.60660.094*
C191.3819 (4)0.3451 (2)0.4777 (2)0.0628 (7)
H19B1.51790.36650.44900.075*
H19A1.37470.40220.55640.075*
C201.3403 (4)0.2163 (2)0.4814 (2)0.0621 (7)
H201.44170.21110.53360.075*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni0.0561 (3)0.0350 (2)0.0437 (3)0.01306 (18)0.00447 (19)0.01273 (18)
O10.0563 (10)0.0419 (9)0.0455 (9)0.0160 (7)0.0056 (7)0.0142 (7)
O20.0530 (9)0.0386 (8)0.0538 (9)0.0164 (7)0.0085 (7)0.0177 (7)
N0.0599 (12)0.0450 (11)0.0485 (11)0.0182 (9)0.0016 (9)0.0133 (9)
C10.0774 (18)0.0589 (16)0.080 (2)0.0354 (14)0.0188 (15)0.0264 (14)
C20.0517 (14)0.0423 (13)0.0472 (13)0.0153 (10)0.0031 (11)0.0141 (11)
C30.0623 (15)0.0437 (13)0.0656 (16)0.0208 (11)0.0085 (12)0.0264 (12)
C40.0504 (13)0.0370 (12)0.0402 (12)0.0116 (10)0.0011 (10)0.0121 (9)
C50.0525 (14)0.0411 (12)0.0404 (12)0.0098 (10)0.0029 (10)0.0151 (10)
C60.0608 (16)0.0512 (14)0.0598 (16)0.0176 (12)0.0098 (12)0.0227 (12)
C70.0706 (18)0.0729 (19)0.0677 (18)0.0205 (14)0.0209 (14)0.0291 (15)
C80.0768 (19)0.0722 (19)0.0621 (17)0.0018 (15)0.0148 (14)0.0320 (15)
C90.100 (2)0.0541 (16)0.084 (2)0.0104 (16)0.0244 (17)0.0351 (15)
C100.0839 (19)0.0468 (15)0.0741 (19)0.0200 (13)0.0216 (15)0.0275 (13)
C110.0477 (13)0.0372 (11)0.0400 (12)0.0085 (9)0.0008 (10)0.0121 (9)
C120.0589 (15)0.0546 (15)0.0465 (14)0.0081 (11)0.0004 (11)0.0178 (11)
C130.0570 (16)0.088 (2)0.0473 (15)0.0041 (14)0.0123 (13)0.0156 (14)
C140.0750 (19)0.080 (2)0.0558 (17)0.0296 (15)0.0060 (14)0.0006 (14)
C150.0747 (17)0.0373 (13)0.0579 (15)0.0091 (11)0.0029 (13)0.0126 (11)
C160.0534 (14)0.0444 (13)0.0518 (14)0.0034 (10)0.0025 (11)0.0210 (11)
C170.0719 (17)0.0494 (14)0.0619 (16)0.0173 (12)0.0150 (13)0.0136 (12)
C180.105 (2)0.0722 (19)0.0447 (15)0.0062 (16)0.0003 (15)0.0217 (14)
C190.0655 (16)0.0507 (15)0.0562 (16)0.0010 (12)0.0079 (13)0.0063 (12)
C200.0758 (18)0.0562 (15)0.0511 (15)0.0108 (13)0.0195 (13)0.0137 (12)
Geometric parameters (Å, º) top
Ni—O2i2.0187 (16)C10—H100.9300
Ni—O12.0409 (16)C11—C121.519 (3)
Ni—O22.0187 (16)C11—C161.520 (3)
Ni—O1i2.0409 (16)C11—C171.529 (3)
Ni—N2.176 (2)C12—C131.532 (3)
Ni—Ni2.176 (2)C12—H12A0.9700
O1—C21.263 (3)C12—H12B0.9700
O2—C41.269 (3)C13—C141.516 (4)
N—C111.484 (3)C13—C181.522 (4)
N—H1N0.9000C13—H130.9800
N—H2N0.9000C14—C151.511 (4)
C1—C21.505 (3)C14—H14A0.9700
C1—H1A0.9600C14—H14B0.9700
C1—H1C0.9600C15—C191.521 (4)
C1—H1B0.9600C15—C161.526 (3)
C2—C31.392 (3)C15—H150.9800
C3—C41.390 (3)C16—H16A0.9700
C3—H30.9300C16—H16B0.9700
C4—C51.506 (3)C17—C201.526 (3)
C5—C61.380 (3)C17—H17A0.9700
C5—C101.383 (3)C17—H17B0.9700
C6—C71.376 (3)C18—C201.521 (4)
C6—H60.9300C18—H18B0.9700
C7—C81.376 (4)C18—H18A0.9700
C7—H70.9300C19—C201.524 (4)
C8—C91.362 (4)C19—H19B0.9700
C8—H80.9300C19—H19A0.9700
C9—C101.379 (4)C20—H200.9800
C9—H90.9300
O2i—Ni—O2180.00 (12)C12—C11—C16109.00 (19)
O2i—Ni—O1i90.36 (6)N—C11—C17112.02 (18)
O2—Ni—O1i89.64 (6)C12—C11—C17109.3 (2)
O2i—Ni—O189.64 (6)C16—C11—C17108.34 (19)
O2—Ni—O190.36 (6)C11—C12—C13109.60 (19)
O1i—Ni—O1180.00 (6)C11—C12—H12A109.7
O2i—Ni—N88.90 (7)C13—C12—H12A109.7
O2—Ni—N91.10 (7)C11—C12—H12B109.7
O1i—Ni—N97.28 (7)C13—C12—H12B109.7
O1—Ni—N82.72 (7)H12A—C12—H12B108.2
O2i—Ni—Ni91.10 (7)C14—C13—C18109.4 (2)
O2—Ni—Ni88.90 (7)C14—C13—C12109.3 (2)
O1i—Ni—Ni82.72 (7)C18—C13—C12109.9 (2)
O1—Ni—Ni97.28 (7)C14—C13—H13109.4
N—Ni—Ni180.00 (6)C18—C13—H13109.4
C2—O1—Ni124.67 (14)C12—C13—H13109.4
C4—O2—Ni125.71 (14)C15—C14—C13109.5 (2)
C11—N—Ni130.22 (14)C15—C14—H14A109.8
C11—N—H1N104.7C13—C14—H14A109.8
Ni—N—H1N104.7C15—C14—H14B109.8
C11—N—H2N104.7C13—C14—H14B109.8
Ni—N—H2N104.7H14A—C14—H14B108.2
H1N—N—H2N105.7C14—C15—C19110.1 (2)
C2—C1—H1A109.5C14—C15—C16109.0 (2)
C2—C1—H1C109.5C19—C15—C16109.9 (2)
H1A—C1—H1C109.5C14—C15—H15109.3
C2—C1—H1B109.5C19—C15—H15109.3
H1A—C1—H1B109.5C16—C15—H15109.3
H1C—C1—H1B109.5C11—C16—C15110.23 (19)
O1—C2—C3125.6 (2)C11—C16—H16A109.6
O1—C2—C1115.8 (2)C15—C16—H16A109.6
C3—C2—C1118.5 (2)C11—C16—H16B109.6
C4—C3—C2127.1 (2)C15—C16—H16B109.6
C4—C3—H3116.5H16A—C16—H16B108.1
C2—C3—H3116.5C20—C17—C11110.5 (2)
O2—C4—C3124.8 (2)C20—C17—H17A109.6
O2—C4—C5114.84 (19)C11—C17—H17A109.6
C3—C4—C5120.4 (2)C20—C17—H17B109.6
C6—C5—C10118.2 (2)C11—C17—H17B109.6
C6—C5—C4119.0 (2)H17A—C17—H17B108.1
C10—C5—C4122.8 (2)C20—C18—C13109.7 (2)
C7—C6—C5120.9 (2)C20—C18—H18B109.7
C7—C6—H6119.5C13—C18—H18B109.7
C5—C6—H6119.6C20—C18—H18A109.7
C6—C7—C8120.3 (3)C13—C18—H18A109.7
C6—C7—H7119.9H18B—C18—H18A108.2
C8—C7—H7119.9C15—C19—C20109.1 (2)
C9—C8—C7119.4 (2)C15—C19—H19B109.9
C9—C8—H8120.3C20—C19—H19B109.9
C7—C8—H8120.3C15—C19—H19A109.9
C8—C9—C10120.6 (3)C20—C19—H19A109.9
C8—C9—H9119.7H19B—C19—H19A108.3
C10—C9—H9119.7C18—C20—C19109.0 (2)
C9—C10—C5120.7 (2)C18—C20—C17109.4 (2)
C9—C10—H10119.7C19—C20—C17109.4 (2)
C5—C10—H10119.7C18—C20—H20109.7
N—C11—C12108.83 (18)C19—C20—H20109.7
N—C11—C16109.31 (18)C17—C20—H20109.7
Symmetry code: (i) x+2, y, z.
 

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