Bis(η³-2-tert-butyl-1-trimethyl­silyl-3-phenyl-1-aza­all­yl)nickel(II)

Abstract

The title compound, [Ni(C₁₅H₂₄NSi)₂], is a homoleptic metal–η³-aza­allyl centrosymmetric complex containing two aza­allyl ligands bound in an η³-manner to an Ni^II atom located on a center of symmetry. The overall coordination about the Ni^II atom is square-planar. The C and N atoms of the aza­allyl group are sp ²-hybridized. The uneven Ni—C and Ni—N distances [2.045 (5)/2.060 (6) and 1.916 (5) Å] are influenced by a steric hindering effect from the nearby benzene ring.

Related literature

For metal-mediated reactions, see: Blystone (1989 ▶). For related 1-aza­allyl complexes including some main group elements and transition metals, see: Avent et al. (2004 ▶); Caro et al. (2001 ▶); Hitchcock et al. (2000 ▶). For related cobalt–η³-allyl complexes, see: Yuan et al. (2007 ▶).

Experimental

Crystal data

• [Ni(C₁₅H₂₄NSi)₂]

• M _r = 551.59

• Monoclinic,

• a = 10.309 (6) Å

• b = 9.289 (6) Å

• c = 16.521 (9) Å

• β = 94.84 (2)°

• V = 1576.4 (16) ų

• Z = 2

• Mo Kα radiation

• μ = 0.71 mm⁻¹

• T = 213 K

• 0.30 × 0.30 × 0.20 mm

Data collection

• Siemens SMART CCD area-detector diffractometer

• Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T _min = 0.815, T _max = 0.871

• 7488 measured reflections

• 2776 independent reflections

• 2446 reflections with I > 2σ(I)

• R _int = 0.061

Refinement

• R[F ² > 2σ(F ²)] = 0.096

• wR(F ²) = 0.186

• S = 1.36

• 2776 reflections

• 166 parameters

• H-atom parameters constrained

• Δρ_max = 0.63 e Å⁻³

• Δρ_min = −1.22 e Å⁻³

Data collection: SMART (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97.

Supplementary Material

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

supplementary crystallographic information

Comment

Metal-η³-allyl complexes are well known to play an important role in many metal-mediated reactions (Blystone et al., 1989). Lappert and co-workers have prepared a variety of 1-azaallyl complexes containing main group elements and transition metals (Avent et al., 2004; Caro et al., 2001; Hitchcock et al., 2000). Recently, Yuan and co-workers have prepared related Cobalt η^3^-allyl complexes (Yuan et al., 2007). As part of an subsequent investigation of metal-η³-azaallyl complexes, we have prepared the title complex, [Ni(C₃₀H₄₈N₂Si₂)₂], (I),

The title compound is a homoleptic metal-η³-azaallyl centrosymmetric complex containing two azaallyl ligands bound in an η³ manner to a Ni^II atom located at the center of symmetry, thereby, forming two nonplanar 4-membered rings, N/C8/C7/Ni (Fig. 1). The dihedral angle between the N/C7/Ni and C8/C7/Ni planes is 49.0 (3)°. The C and N atoms of the azaallyl group are sp²– hybridized with the N—C8 bond [1.355 (7) Å] showing double-bond character. The uneven Ni—C7, Ni—C8 and Ni—N distances [2.045 (5), 2.060 (6)Å, and 1.916 (5)Å] are influenced by a steric hindered effect from the nearby benzene ring (C1—C6).

Experimental

All manipulations were carried out under argon or in vacuo using standard Schlenk techniques. The title complex was synthesized according to literature methods (Hitchcock et al., 2000; Avent et al., 2004). To a solution of trimethylsilylmethyltolulithium (6 mmol) in diethyl ether(20 ml), tert-butyl nitrile (6 mmol) was added at ca 273 K and the solution was stirred for 15 min and then for 5 h at room temperature. To this solution, NiCl₂(3 mmol) was added at ca 200 K and the suspension was stirred for 15 min and then for 5 h at room temperature. The mixture was filtered and the filtrate was carefully concentrated under a vacuum until yellow crystals of the title compound appeared.

Refinement

All H atoms were positioned geometrically, with CH = 0.96– 0.98 Å, CH₃ = 0.96Å and refined as riding, allowing for free rotation of the methyl groups. The U_iso(H) values were set at 1.18-1.21 U_eq(CH) or 1.5U_eq(CH₃).

Figures

Fig. 1.

View of the title molecule showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are omitted for clarity. The symmetry operator for i is –X, –Y, –Z.

Crystal data

[Ni(C15H24NSi)2]	F(000) = 596
Mr = 551.59	Dx = 1.162 Mg m−3
Monoclinic, P21/n	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn	Cell parameters from 1405 reflections
a = 10.309 (6) Å	θ = 2.4–26.7°
b = 9.289 (6) Å	µ = 0.71 mm−1
c = 16.521 (9) Å	T = 213 K
β = 94.84 (2)°	Block, yellow
V = 1576.4 (16) Å3	0.30 × 0.30 × 0.20 mm
Z = 2

Data collection

Siemens SMART CCD area-detector diffractometer	2776 independent reflections
Radiation source: fine-focus sealed tube	2446 reflections with I > 2σ(I)
graphite	Rint = 0.061
φ and ω scans	θmax = 25.0°, θmin = 2.3°
Absorption correction: multi-scan (SADABS; Bruker, 2009)	h = −12→9
Tmin = 0.815, Tmax = 0.871	k = −9→11
7488 measured reflections	l = −19→19

Refinement

Refinement on F2	Primary atom site location: structure-invariant direct methods
Least-squares matrix: full	Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.096	Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.186	H-atom parameters constrained
S = 1.36	w = 1/[σ2(Fo2) + (0.0426P)2 + 3.0952P] where P = (Fo2 + 2Fc2)/3
2776 reflections	(Δ/σ)max < 0.001
166 parameters	Δρmax = 0.63 e Å−3
0 restraints	Δρmin = −1.22 e Å−3

Special details

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 (Ų)

	x	y	z	Uiso*/Ueq
Ni	0.5000	0.5000	0.0000	0.0230 (3)
N	0.5562 (5)	0.5466 (5)	0.1104 (3)	0.0258 (11)
Si	0.60753 (18)	0.6959 (2)	0.16563 (10)	0.0343 (5)
C1	0.6907 (6)	0.2919 (7)	0.0403 (4)	0.0319 (15)
C2	0.7162 (8)	0.1682 (7)	−0.0031 (4)	0.0461 (18)
H2	0.6477	0.1078	−0.0208	0.055*
C3	0.8420 (9)	0.1330 (10)	−0.0205 (5)	0.067 (3)
H3	0.8575	0.0502	−0.0498	0.080*
C4	0.9421 (9)	0.2215 (11)	0.0060 (6)	0.071 (3)
H4	1.0265	0.1984	−0.0052	0.086*
C5	0.9199 (7)	0.3447 (9)	0.0491 (5)	0.057 (2)
H5	0.9887	0.4047	0.0670	0.068*
C6	0.7934 (7)	0.3781 (7)	0.0655 (4)	0.0404 (17)
H6	0.7783	0.4615	0.0944	0.048*
C7	0.5535 (6)	0.3120 (6)	0.0600 (3)	0.0288 (14)
H7	0.4961	0.2299	0.0465	0.035*
C8	0.5045 (6)	0.4128 (6)	0.1139 (3)	0.0264 (13)
C9	0.3895 (6)	0.3787 (7)	0.1648 (4)	0.0354 (15)
C10	0.3392 (9)	0.2272 (9)	0.1507 (6)	0.079 (3)
H10A	0.2748	0.2066	0.1878	0.119*
H10B	0.4100	0.1603	0.1594	0.119*
H10C	0.3009	0.2184	0.0959	0.119*
C11	0.4382 (8)	0.3936 (10)	0.2540 (4)	0.064 (2)
H11A	0.3679	0.3754	0.2872	0.096*
H11B	0.4706	0.4894	0.2641	0.096*
H11C	0.5069	0.3255	0.2671	0.096*
C12	0.2786 (7)	0.4838 (9)	0.1442 (5)	0.063 (2)
H12A	0.2472	0.4728	0.0881	0.095*
H12B	0.3093	0.5805	0.1534	0.095*
H12C	0.2092	0.4646	0.1779	0.095*
C13	0.7233 (8)	0.6372 (9)	0.2517 (4)	0.059 (2)
H13A	0.6765	0.5887	0.2914	0.088*
H13B	0.7669	0.7198	0.2760	0.088*
H13C	0.7864	0.5728	0.2320	0.088*
C14	0.4802 (8)	0.8102 (8)	0.2082 (5)	0.063 (2)
H14A	0.4187	0.8418	0.1650	0.094*
H14B	0.5206	0.8925	0.2350	0.094*
H14C	0.4358	0.7551	0.2465	0.094*
C15	0.6989 (9)	0.8097 (9)	0.0976 (5)	0.066 (3)
H15A	0.7616	0.7517	0.0727	0.099*
H15B	0.7430	0.8852	0.1286	0.099*
H15C	0.6394	0.8512	0.0562	0.099*

Atomic displacement parameters (Ų)

	U11	U22	U33	U12	U13	U23
Ni	0.0255 (6)	0.0245 (6)	0.0189 (5)	−0.0018 (5)	0.0021 (4)	0.0027 (5)
N	0.029 (3)	0.027 (3)	0.022 (2)	0.007 (2)	0.006 (2)	0.003 (2)
Si	0.0386 (11)	0.0359 (10)	0.0281 (9)	−0.0032 (8)	0.0005 (8)	−0.0048 (8)
C1	0.035 (4)	0.033 (4)	0.028 (3)	0.007 (3)	0.003 (3)	0.014 (3)
C2	0.057 (5)	0.040 (4)	0.042 (4)	0.011 (4)	0.008 (4)	0.007 (3)
C3	0.074 (7)	0.058 (6)	0.072 (6)	0.030 (5)	0.025 (5)	0.008 (5)
C4	0.048 (6)	0.082 (7)	0.088 (7)	0.032 (5)	0.028 (5)	0.027 (6)
C5	0.035 (5)	0.074 (6)	0.061 (5)	0.007 (4)	0.003 (4)	0.019 (4)
C6	0.038 (4)	0.046 (4)	0.038 (4)	0.001 (3)	0.006 (3)	0.008 (3)
C7	0.041 (4)	0.020 (3)	0.025 (3)	−0.003 (3)	−0.001 (3)	0.004 (3)
C8	0.022 (3)	0.030 (3)	0.027 (3)	−0.008 (3)	−0.002 (3)	0.013 (3)
C9	0.033 (4)	0.043 (4)	0.031 (3)	−0.007 (3)	0.010 (3)	0.002 (3)
C10	0.090 (7)	0.067 (6)	0.088 (7)	−0.036 (5)	0.054 (6)	−0.007 (5)
C11	0.058 (5)	0.099 (7)	0.037 (4)	0.002 (5)	0.016 (4)	0.013 (4)
C12	0.043 (5)	0.079 (6)	0.070 (5)	0.003 (4)	0.022 (4)	0.028 (5)
C13	0.061 (6)	0.067 (5)	0.046 (4)	−0.006 (4)	−0.012 (4)	−0.005 (4)
C14	0.067 (6)	0.054 (5)	0.066 (5)	0.012 (4)	−0.001 (4)	−0.022 (4)
C15	0.089 (7)	0.062 (5)	0.048 (5)	−0.043 (5)	0.007 (4)	−0.001 (4)

Geometric parameters (Å, °)

Ni—N	1.916 (5)	C7—H7	0.9800
Ni—Ni	1.916 (5)	C8—C9	1.544 (8)
Ni—C8	2.045 (5)	C9—C10	1.511 (10)
Ni—C8i	2.045 (5)	C9—C12	1.521 (10)
Ni—C7i	2.060 (6)	C9—C11	1.523 (9)
Ni—C7	2.060 (6)	C10—H10A	0.9600
N—C8	1.355 (7)	C10—H10B	0.9600
N—Si	1.720 (5)	C10—H10C	0.9600
Si—C15	1.857 (7)	C11—H11A	0.9600
Si—C13	1.860 (8)	C11—H11B	0.9600
Si—C14	1.871 (7)	C11—H11C	0.9600
C1—C6	1.365 (9)	C12—H12A	0.9600
C1—C2	1.390 (9)	C12—H12B	0.9600
C1—C7	1.490 (8)	C12—H12C	0.9600
C2—C3	1.390 (10)	C13—H13A	0.9600
C2—H2	0.9300	C13—H13B	0.9600
C3—C4	1.362 (12)	C13—H13C	0.9600
C3—H3	0.9300	C14—H14A	0.9600
C4—C5	1.377 (11)	C14—H14B	0.9600
C4—H4	0.9300	C14—H14C	0.9600
C5—C6	1.389 (9)	C15—H15A	0.9600
C5—H5	0.9300	C15—H15B	0.9600
C6—H6	0.9300	C15—H15C	0.9600
C7—C8	1.414 (8)
N—Ni—Ni	180.0	N—C8—C7	114.7 (5)
N—Ni—C8	39.8 (2)	N—C8—C9	122.3 (5)
Ni—Ni—C8	140.2 (2)	C7—C8—C9	122.6 (5)
N—Ni—C8i	140.2 (2)	N—C8—Ni	64.9 (3)
Ni—Ni—C8i	39.8 (2)	C7—C8—Ni	70.4 (3)
C8—Ni—C8i	180.0	C9—C8—Ni	128.6 (4)
N—Ni—C7i	108.3 (2)	C10—C9—C12	108.8 (7)
Ni—Ni—C7i	71.7 (2)	C10—C9—C11	108.4 (6)
C8—Ni—C7i	139.7 (2)	C12—C9—C11	109.8 (6)
C8i—Ni—C7i	40.3 (2)	C10—C9—C8	112.1 (5)
N—Ni—C7	71.7 (2)	C12—C9—C8	110.1 (5)
Ni—Ni—C7	108.3 (2)	C11—C9—C8	107.7 (5)
C8—Ni—C7	40.3 (2)	C9—C10—H10A	109.5
C8i—Ni—C7	139.7 (2)	C9—C10—H10B	109.5
C7i—Ni—C7	180.0	H10A—C10—H10B	109.5
C8—N—Si	145.2 (4)	C9—C10—H10C	109.5
C8—N—Ni	75.2 (3)	H10A—C10—H10C	109.5
Si—N—Ni	137.9 (3)	H10B—C10—H10C	109.5
N—Si—C15	106.7 (3)	C9—C11—H11A	109.5
N—Si—C13	108.5 (3)	C9—C11—H11B	109.5
C15—Si—C13	107.7 (4)	H11A—C11—H11B	109.5
N—Si—C14	117.6 (3)	C9—C11—H11C	109.5
C15—Si—C14	108.2 (4)	H11A—C11—H11C	109.5
C13—Si—C14	107.7 (4)	H11B—C11—H11C	109.5
C6—C1—C2	117.8 (6)	C9—C12—H12A	109.5
C6—C1—C7	125.8 (6)	C9—C12—H12B	109.5
C2—C1—C7	116.2 (6)	H12A—C12—H12B	109.5
C1—C2—C3	121.4 (8)	C9—C12—H12C	109.5
C1—C2—H2	119.3	H12A—C12—H12C	109.5
C3—C2—H2	119.3	H12B—C12—H12C	109.5
C4—C3—C2	119.1 (8)	Si—C13—H13A	109.5
C4—C3—H3	120.5	Si—C13—H13B	109.5
C2—C3—H3	120.5	H13A—C13—H13B	109.5
C3—C4—C5	120.9 (8)	Si—C13—H13C	109.5
C3—C4—H4	119.6	H13A—C13—H13C	109.5
C5—C4—H4	119.6	H13B—C13—H13C	109.5
C4—C5—C6	119.1 (8)	Si—C14—H14A	109.5
C4—C5—H5	120.5	Si—C14—H14B	109.5
C6—C5—H5	120.5	H14A—C14—H14B	109.5
C1—C6—C5	121.8 (7)	Si—C14—H14C	109.5
C1—C6—H6	119.1	H14A—C14—H14C	109.5
C5—C6—H6	119.1	H14B—C14—H14C	109.5
C8—C7—C1	128.1 (5)	Si—C15—H15A	109.5
C8—C7—Ni	69.3 (3)	Si—C15—H15B	109.5
C1—C7—Ni	102.8 (4)	H15A—C15—H15B	109.5
C8—C7—H7	114.7	Si—C15—H15C	109.5
C1—C7—H7	114.7	H15A—C15—H15C	109.5
Ni—C7—H7	114.7	H15B—C15—H15C	109.5

Symmetry codes: (i) −x+1, −y+1, −z.