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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Oct 15;64(Pt 11):m1402. doi: 10.1107/S1600536808032376

[2,6-Bis(di-tert-butyl­phosphinometh­yl)­phen­yl-κ3 P,C 1,P′](nitrato-κO)nickel(II)

Brian J Boro a, Diane A Dickie a, Eileen N Duesler a, Karen I Goldberg b, Richard A Kemp a,c,*
PMCID: PMC2959575  PMID: 21580852

Abstract

The NiII atom in the title compound, [Ni(C24H43P2)(NO3)], adopts a distorted square-planar geometry with the P atoms in a trans arrangement. The compound contains a twofold rotational axis with the nitrate group offset from this axis, except for an O atom of the nitrate group, generating two positions of 50% occupancy for the other atoms of the nitrate group.

Related literature

The synthetic preparation was adopted from that employed to prepare the Pd analogue (Cámpora et al., 2004). For the crystallographic characterization of the Pd analogue, see: Olsson et al. (2007). For the crystallographic characterization of the starting {2,6-bis­[(di-tert-butyl­phosphino)meth­yl]phenyl}chloridonickel complex, see: Boro et al. (2008). For related literature, see: Denney et al. (2006); Johansson et al. (2007); Keith et al. (2006).graphic file with name e-64-m1402-scheme1.jpg

Experimental

Crystal data

  • [Ni(C24H43P2)(NO3)]

  • M r = 514.24

  • Orthorhombic, Inline graphic

  • a = 24.0023 (14) Å

  • b = 12.6350 (6) Å

  • c = 17.6528 (6) Å

  • V = 5353.5 (4) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.87 mm−1

  • T = 225 (2) K

  • 0.50 × 0.40 × 0.20 mm

Data collection

  • Bruker X8 APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2004) T min = 0.671, T max = 0.846

  • 33484 measured reflections

  • 4078 independent reflections

  • 3703 reflections with I > 2σ(I)

  • R int = 0.037

Refinement

  • R[F 2 > 2σ(F 2)] = 0.030

  • wR(F 2) = 0.099

  • S = 0.81

  • 4078 reflections

  • 156 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.38 e Å−3

  • Δρmin = −0.38 e Å−3

  • Absolute structure: Flack (1983), 1976 Freidel pairs

  • Flack parameter: 0.012 (10)

Data collection: APEX2 (Bruker, 2007); cell refinement: APEX2; data reduction: APEX2; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: publCIF (Westrip, 2008).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808032376/at2643sup1.cif

e-64-m1402-sup1.cif (18.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808032376/at2643Isup2.hkl

e-64-m1402-Isup2.hkl (200.2KB, hkl)

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

Acknowledgments

Funding was provided by the Natural Sciences and Engineering Research Council of Canada (NSERC PDF to DAD) and the Department of Energy (DE-FG02-06ER15765). The diffractometer was purchased via a National Science Foundation CRIF:MU award to the University of New Mexico (CHE-0443580). Sandia is a multiprogram laboratory operated by Sandia Corporation, a Lockheed Martin Company, for the US Department of Energy under contract No. DE-AC04-94AL85000.

supplementary crystallographic information

Comment

The title compound, (I) (Fig. 1), was prepared from {2,6-bis[(di-tert-butylphosphino)methyl]phenyl}chloridonickel(II) (Boro et al., 2008) via a synthesis adopted from the preparation of the Pd analogue (Cámpora et al., 2004). Our research has been directed towards the activation of molecular oxygen using pincer complexes of the late transition metals (Denney et al., 2006; Keith et al., 2006). Compound (I) was prepared as a precursor along the path of the attempted synthesis of a NiII-hydroperoxide.

The compound is bisected by a twofold rotational axis running through C4, C1, Ni1, and O3. The nitrate group is offset from this axis with a C1—Ni1—O1 angle of 164.64 (11)°. As a result of this symmetry induced disorder the nitrate group occupies two positions each with 50% occupancy. The Ni1—O1 bond length 1.976 (3) Å is significantly shorter than the corresponding Pd—O bond length 2.164 (2) Å in the Pd analogue (Johansson et al. 2007). This not surprising, given the smaller size of the Ni atom. The M—C and M—P bonds were also shorter in the Ni compound compared to the Pd. The P—M—P angle, however was closer to the ideal linear geometry with Ni (168.87 (3)°) than Pd (163.41 (3)°).

In their report on the Pd analogue of (I), Johansson et al. (2007) observed non-traditional hydrogen bonding between one of the nitrato O atoms and a hydrogen from the methylene arm of the pincer ligand to form a zigzag chain. The C—H···O interaction measured 3.263 (4) Å (C···O) with an angle of 137°. The same pattern is observed in I (Fig. 2) between C5—H5b···O2, with corresponding measurements of 3.5616 (54) Å and 171.81 (18)°.

Experimental

{2,6-Bis[(di-tert-butylphosphino)methyl]phenyl}chloronickel(II) (0.135 g, 0.28 mmol) and AgNO3 (0.05 g, 0.29 mmol) were combined with THF (20 ml) and the solution was stirred at room temperature for 48 h. The THF was then removed under vacuum and the product was extracted into diethyl ether (15 ml). After filtering, the solution was layered with hexanes and placed in a 238 K freezer. The product crystallized as orange-brown prisms.

Yield 0.118 g, 82%. 1H NMR (250 MHz, C6D6): 6.93 (d, JHH = 7.5 Hz, 1H, Ar-Hpara), 6.68 (t, JHH = 7.5 Hz, 2H, Ar-Hmeta), 2.80 (virtual t, 4H, JHP = 7.15 Hz,CH2), 1.25 (virtual t, 36H, J = 13.1 Hz C(CH3)3) p.p.m.. 13C{1H} (63 MHz, C6D6): 152.8 (t, 2JPC = 11.6 Hz, Ar-Cipso), 147.1 (virtual t, JCP= 32.3 Hz, Ar-Cortho), 125.8 (s, Ar-Cpara), 122.1 (virtual t, JCP = 15.8 Hz, Ar-Cpara), 34.5 (virtual t, JCP = 13.2 Hz, PCH2), 32.7 (virtual t, JCP = 24.6 Hz, PC(CH3)3), 29.6 (s, CH3) p.p.m.. 31P{1H} (101 MHz, C6D6): 69.5 (s) p.p.m..

Refinement

Hydrogen atoms were included at geometrically idealized positions with C—H distances at the range of 0.93 - 0.98 Å and were treated as riding on their respective heavy atoms. The isotropic thermal parameters of the hydrogen atoms were fixed at 1.2 or 1.5 Ueq of the parent atom.

Figures

Fig. 1.

Fig. 1.

View of the title compound showing full numbering scheme. Ellipsoids are shown at 50% probability and hydrogen atoms have been removed for clarity. Only one of the two symmetry equivalent positions for the nitrate group is shown.

Fig. 2.

Fig. 2.

Hydrogen bonding in (I). For clarity the tert-butyl substituents on P have been removed.

Crystal data

[Ni(C24H43P2)(NO3)] F(000) = 2208
Mr = 514.24 Dx = 1.276 Mg m3
Orthorhombic, Fdd2 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: F 2 -2d Cell parameters from 9535 reflections
a = 24.0023 (14) Å θ = 2.2–30.3°
b = 12.6350 (6) Å µ = 0.87 mm1
c = 17.6528 (6) Å T = 225 K
V = 5353.5 (4) Å3 Cut-prism, orange–brown
Z = 8 0.50 × 0.40 × 0.20 mm

Data collection

Bruker SMART CCD area-detector diffractometer 4078 independent reflections
Radiation source: fine-focus sealed tube 3703 reflections with I > 2σ(I)
graphite Rint = 0.037
φ and ω scans θmax = 30.5°, θmin = 2.9°
Absorption correction: multi-scan (SADABS; Bruker, 2004) h = −34→34
Tmin = 0.671, Tmax = 0.846 k = −18→18
33484 measured reflections l = −25→25

Refinement

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)] = 0.030 H-atom parameters constrained
wR(F2) = 0.099 w = 1/[σ2(Fo2) + (0.1P)2 + 0.25P] where P = (Fo2 + 2Fc2)/3
S = 0.81 (Δ/σ)max = 0.001
4078 reflections Δρmax = 0.38 e Å3
156 parameters Δρmin = −0.38 e Å3
1 restraint Absolute structure: Flack (1983), 1976 Freidel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.012 (10)

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 (Å2)

x y z Uiso*/Ueq Occ. (<1)
Ni1 0.2500 0.2500 0.594610 (14) 0.02536 (9)
P1 0.232841 (19) 0.07823 (3) 0.58242 (3) 0.02639 (10)
C1 0.2500 0.2500 0.48634 (16) 0.0263 (5)
C2 0.22870 (9) 0.16438 (14) 0.44415 (10) 0.0293 (3)
C3 0.22918 (11) 0.16401 (17) 0.36544 (11) 0.0381 (4)
H3 0.2153 0.1051 0.3390 0.046*
C4 0.2500 0.2500 0.32575 (19) 0.0443 (8)
H4 0.2500 0.2500 0.2725 0.053*
C5 0.20438 (10) 0.07210 (16) 0.48626 (12) 0.0357 (4)
H5A 0.2149 0.0054 0.4618 0.043*
H5B 0.1636 0.0770 0.4875 0.043*
C6 0.17578 (10) 0.02125 (17) 0.64252 (13) 0.0356 (4)
C7 0.15103 (12) −0.08133 (18) 0.60934 (17) 0.0492 (6)
H7A 0.1803 −0.1337 0.6038 0.074*
H7B 0.1348 −0.0665 0.5602 0.074*
H7C 0.1225 −0.1082 0.6431 0.074*
C8 0.13040 (11) 0.1061 (2) 0.64349 (17) 0.0490 (5)
H8A 0.1001 0.0833 0.6759 0.073*
H8B 0.1166 0.1170 0.5925 0.073*
H8C 0.1458 0.1718 0.6627 0.073*
C9 0.19464 (14) 0.00157 (19) 0.72359 (15) 0.0484 (6)
H9A 0.1623 −0.0057 0.7561 0.073*
H9B 0.2171 0.0607 0.7408 0.073*
H9C 0.2166 −0.0628 0.7256 0.073*
C10 0.29710 (10) −0.00713 (16) 0.58017 (16) 0.0434 (5)
C11 0.33545 (12) 0.0368 (3) 0.5189 (2) 0.0635 (9)
H11A 0.3615 −0.0176 0.5032 0.095*
H11B 0.3558 0.0970 0.5388 0.095*
H11C 0.3134 0.0590 0.4757 0.095*
C12 0.32896 (19) 0.0019 (4) 0.6540 (3) 0.100 (2)
H12A 0.3293 −0.0663 0.6793 0.150*
H12B 0.3110 0.0538 0.6864 0.150*
H12C 0.3669 0.0240 0.6437 0.150*
C13 0.28517 (17) −0.1214 (3) 0.5629 (4) 0.106 (2)
H13A 0.2705 −0.1274 0.5118 0.159*
H13B 0.2580 −0.1484 0.5986 0.159*
H13C 0.3193 −0.1621 0.5670 0.159*
N1 0.2619 (2) 0.2312 (5) 0.7546 (2) 0.0478 (13) 0.50
O1 0.22947 (16) 0.2640 (3) 0.70255 (19) 0.0394 (7) 0.50
O2 0.3061 (2) 0.1884 (5) 0.7355 (3) 0.0732 (13) 0.50
O3 0.2500 0.2500 0.8206 (2) 0.0869 (14)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ni1 0.03377 (16) 0.01934 (13) 0.02296 (14) −0.00129 (11) 0.000 0.000
P1 0.0305 (2) 0.01967 (19) 0.0290 (2) 0.00015 (15) 0.00072 (17) 0.00082 (15)
C1 0.0312 (13) 0.0241 (12) 0.0238 (11) 0.0033 (8) 0.000 0.000
C2 0.0344 (8) 0.0280 (8) 0.0256 (8) 0.0006 (7) −0.0019 (7) −0.0025 (6)
C3 0.0478 (11) 0.0397 (11) 0.0267 (9) −0.0013 (8) −0.0025 (8) −0.0070 (7)
C4 0.059 (2) 0.0497 (19) 0.0237 (12) 0.0046 (13) 0.000 0.000
C5 0.0468 (11) 0.0289 (9) 0.0314 (9) −0.0077 (8) −0.0027 (8) −0.0030 (7)
C6 0.0378 (10) 0.0323 (8) 0.0368 (10) −0.0059 (8) 0.0047 (8) 0.0017 (7)
C7 0.0514 (13) 0.0399 (11) 0.0564 (14) −0.0172 (10) 0.0099 (11) −0.0066 (9)
C8 0.0387 (11) 0.0530 (13) 0.0552 (14) 0.0026 (10) 0.0096 (10) −0.0039 (11)
C9 0.0621 (16) 0.0468 (14) 0.0364 (11) −0.0120 (11) 0.0025 (10) 0.0099 (9)
C10 0.0380 (10) 0.0317 (10) 0.0606 (15) 0.0095 (7) 0.0119 (10) 0.0072 (9)
C11 0.0397 (12) 0.0590 (16) 0.092 (2) 0.0147 (12) 0.0217 (15) 0.0184 (17)
C12 0.061 (2) 0.168 (6) 0.070 (3) 0.056 (3) −0.0012 (18) 0.028 (2)
C13 0.069 (2) 0.0339 (14) 0.215 (7) 0.0129 (13) 0.034 (3) −0.011 (2)
N1 0.057 (4) 0.052 (4) 0.0350 (19) −0.016 (2) −0.0114 (18) 0.0079 (18)
O1 0.0488 (17) 0.0462 (17) 0.0233 (14) −0.0022 (15) 0.0012 (13) −0.0048 (12)
O2 0.054 (2) 0.104 (4) 0.062 (3) 0.012 (3) −0.011 (2) 0.019 (3)
O3 0.098 (3) 0.137 (4) 0.0265 (13) −0.012 (2) 0.000 0.000

Geometric parameters (Å, °)

Ni1—C1 1.911 (3) C7—H7C 0.9700
Ni1—O1i 1.976 (3) C8—H8A 0.9700
Ni1—O1 1.976 (3) C8—H8B 0.9700
Ni1—P1i 2.2195 (4) C8—H8C 0.9700
Ni1—P1 2.2195 (4) C9—H9A 0.9700
P1—C5 1.831 (2) C9—H9B 0.9700
P1—C6 1.876 (2) C9—H9C 0.9700
P1—C10 1.882 (2) C10—C13 1.503 (4)
C1—C2i 1.409 (2) C10—C12 1.516 (6)
C1—C2 1.409 (2) C10—C11 1.525 (4)
C2—C3 1.389 (3) C11—H11A 0.9700
C2—C5 1.501 (3) C11—H11B 0.9700
C3—C4 1.386 (3) C11—H11C 0.9700
C3—H3 0.9400 C12—H12A 0.9700
C4—C3i 1.386 (3) C12—H12B 0.9700
C4—H4 0.9400 C12—H12C 0.9700
C5—H5A 0.9800 C13—H13A 0.9700
C5—H5B 0.9800 C13—H13B 0.9700
C6—C9 1.521 (3) C13—H13C 0.9700
C6—C8 1.528 (4) N1—O3 1.223 (5)
C6—C7 1.541 (3) N1—O2 1.239 (7)
C7—H7A 0.9700 N1—O1 1.273 (5)
C7—H7B 0.9700 O3—N1i 1.223 (5)
C1—Ni1—O1i 164.64 (11) C6—C8—H8B 109.5
C1—Ni1—O1 164.64 (11) H8A—C8—H8B 109.5
C1—Ni1—P1i 84.437 (14) C6—C8—H8C 109.5
O1i—Ni1—P1i 97.74 (10) H8A—C8—H8C 109.5
O1—Ni1—P1i 93.00 (10) H8B—C8—H8C 109.5
C1—Ni1—P1 84.435 (14) C6—C9—H9A 109.5
O1i—Ni1—P1 93.00 (10) C6—C9—H9B 109.5
O1—Ni1—P1 97.74 (10) H9A—C9—H9B 109.5
P1i—Ni1—P1 168.87 (3) C6—C9—H9C 109.5
C5—P1—C6 103.63 (10) H9A—C9—H9C 109.5
C5—P1—C10 105.18 (12) H9B—C9—H9C 109.5
C6—P1—C10 112.97 (10) C13—C10—C12 110.1 (3)
C5—P1—Ni1 101.56 (7) C13—C10—C11 108.7 (3)
C6—P1—Ni1 117.12 (7) C12—C10—C11 106.1 (3)
C10—P1—Ni1 114.22 (8) C13—C10—P1 113.5 (2)
C2i—C1—C2 116.2 (3) C12—C10—P1 110.6 (2)
C2i—C1—Ni1 121.90 (13) C11—C10—P1 107.52 (16)
C2—C1—Ni1 121.90 (13) C10—C11—H11A 109.5
C3—C2—C1 121.9 (2) C10—C11—H11B 109.5
C3—C2—C5 119.73 (18) H11A—C11—H11B 109.5
C1—C2—C5 118.39 (19) C10—C11—H11C 109.5
C4—C3—C2 120.4 (2) H11A—C11—H11C 109.5
C4—C3—H3 119.8 H11B—C11—H11C 109.5
C2—C3—H3 119.8 C10—C12—H12A 109.5
C3i—C4—C3 119.3 (3) C10—C12—H12B 109.5
C3i—C4—H4 120.4 H12A—C12—H12B 109.5
C3—C4—H4 120.4 C10—C12—H12C 109.5
C2—C5—P1 106.33 (13) H12A—C12—H12C 109.5
C2—C5—H5A 110.5 H12B—C12—H12C 109.5
P1—C5—H5A 110.5 C10—C13—H13A 109.5
C2—C5—H5B 110.5 C10—C13—H13B 109.5
P1—C5—H5B 110.5 H13A—C13—H13B 109.5
H5A—C5—H5B 108.7 C10—C13—H13C 109.5
C9—C6—C8 108.4 (2) H13A—C13—H13C 109.5
C9—C6—C7 109.6 (2) H13B—C13—H13C 109.5
C8—C6—C7 108.6 (2) O1i—N1—O3 165.1 (6)
C9—C6—P1 112.18 (18) O1i—N1—O2 64.8 (4)
C8—C6—P1 104.93 (15) O3—N1—O2 123.0 (4)
C7—C6—P1 112.90 (16) O3—N1—O1 118.8 (4)
C6—C7—H7A 109.5 O2—N1—O1 117.9 (5)
C6—C7—H7B 109.5 N1i—O1—O2i 69.6 (4)
H7A—C7—H7B 109.5 O2i—O1—N1 104.4 (4)
C6—C7—H7C 109.5 N1i—O1—Ni1 152.8 (5)
H7A—C7—H7C 109.5 O2i—O1—Ni1 133.8 (4)
H7B—C7—H7C 109.5 N1—O1—Ni1 121.0 (3)
C6—C8—H8A 109.5

Symmetry codes: (i) −x+1/2, −y+1/2, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: AT2643).

References

  1. Boro, B. J., Dickie, D. A., Goldberg, K. I. & Kemp, R. A. (2008). Acta Cryst. E64, m1304. [DOI] [PMC free article] [PubMed]
  2. Brandenburg, K. (1999). DIAMOND Crystal Impact GbR, Bonn, Germany.
  3. Bruker (2004). SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Bruker (2007). APEX2 Bruker AXS Inc., Madison, Wisconsin, USA.
  5. Cámpora, J., Palma, P., del Rio, D. & Álvarez, E. (2004). Organometallics, 23, 1652–1655.
  6. Denney, M. C., Smythe, N. A., Cetto, K. L., Kemp, R. A. & Goldberg, K. I. (2006). J. Am. Chem. Soc.128, 2508–2509. [DOI] [PubMed]
  7. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  8. Johansson, R., Öhrström, L. & Wendt, O. F. (2007). Cryst. Growth Des.7, 1974–1979.
  9. Keith, J. M., Muller, R. P., Kemp, R. A., Goldberg, K. I., Goddard, W. A. III & Oxgaard, J. (2006). Inorg. Chem.45, 9631–9633. [DOI] [PubMed]
  10. Olsson, D., Janse van Rensburg, J. M. & Wendt, O. F. (2007). Acta Cryst. E63, m1969. [DOI] [PMC free article] [PubMed]
  11. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  12. Westrip, S. P. (2008). publCIF In preparation.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808032376/at2643sup1.cif

e-64-m1402-sup1.cif (18.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808032376/at2643Isup2.hkl

e-64-m1402-Isup2.hkl (200.2KB, hkl)

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


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