supplementary materials


tk2250 scheme

Acta Cryst. (2008). E64, o708    [ doi:10.1107/S160053680800665X ]

1,2,4,5-Tetramethyl-3,6-diphenyl-1,2,4,5-tetraaza-3,6-diphosphinane

F. H. Kriel, J. Caddy and M. A. Fernandes

Abstract top

The title compound, C16H22N4P2, crystallizes about a centre of symmetry, leading to a chair conformation of the heterocyclic ring as is commonly found for this type of compound.

Comment top

Compound (I) has a centre of symmetry and the six-membered ring adopts a chair conformation with the phenyl groups on the phosphorous atoms being trans to each other. Reddy et al. (1994) have observed in related compounds, e.g. [HNP(Et)N(Me)]2 and [HNP(Ph)N(Me)]2, that the chair conformation was favoured over the boat conformation and was seen to readily crystallize. Bond lengths and angles in (I), with values for N—N 1.4321 (17), P—N 1.6953 (14) and 1.6984 (12), and P—Carom 1.8412 (15) Å, are in the ranges observed in related structures (Reddy et al., 1994, 1995).

Related literature top

For related structures, see: Reddy et al. (1994, 1995).

Experimental top

In an attempt to crystallize bis(diphenylphosphino)dimethylhydrazine (II) (for synthesis see Reddy et al., 1995), the worked-up diethylether reaction mixture was concentrated and kept at -20 °C for two days. Two small crystals were formed and on analysis of one of the crystals, (I) was identified. Analysis of the 31P NMR spectrum of (II) showed (I) to be present in less than 5%. Further analysis of (I) was not attempted due to the small amount of material available.

Refinement top

The H atoms were positioned geometrically and allowed to ride on their respective parent atoms, with C—H = 0.93 (Ar—H) or 0.96 (CH3) Å, and with Ueq = 1.2 (Ar—H) or 1.5 (CH3) Ueq(C).

Computing details top

Data collection: SMART-NT (Bruker, 1998); cell refinement: SAINT-Plus (Bruker, 1999); data reduction: SAINT-Plus (Bruker, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and Mercury (Macrae et al., 2006); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. Molecular structure of (I) drawn with displacement ellipsoids at the 50% probability level. Hydrogen atoms have been omitted for clarity.
1,2,4,5-Tetramethyl-3,6-diphenyl-1,2,4,5-tetraaza-3,6-diphosphinane top
Crystal data top
C16H22N4P2F000 = 704
Mr = 332.32Dx = 1.286 Mg m3
Orthorhombic, PbcaMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 899 reflections
a = 13.2879 (16) Åθ = 3.0–28.2º
b = 7.5426 (9) ŵ = 0.26 mm1
c = 17.125 (2) ÅT = 173 (2) K
V = 1716.4 (4) Å3Plates, colourless
Z = 40.38 × 0.27 × 0.26 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1591 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.031
Monochromator: graphiteθmax = 27.0º
T = 173(2) Kθmin = 2.4º
φ and ω scansh = 15→16
Absorption correction: nonek = 7→9
10040 measured reflectionsl = 21→21
1873 independent reflections
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)] = 0.030H-atom parameters constrained
wR(F2) = 0.094  w = 1/[σ2(Fo2) + (0.0506P)2 + 0.5379P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max = 0.005
1873 reflectionsΔρmax = 0.32 e Å3
100 parametersΔρmin = 0.25 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
C16H22N4P2V = 1716.4 (4) Å3
Mr = 332.32Z = 4
Orthorhombic, PbcaMo Kα
a = 13.2879 (16) ŵ = 0.26 mm1
b = 7.5426 (9) ÅT = 173 (2) K
c = 17.125 (2) Å0.38 × 0.27 × 0.26 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1873 independent reflections
Absorption correction: none1591 reflections with I > 2σ(I)
10040 measured reflectionsRint = 0.031
Refinement top
R[F2 > 2σ(F2)] = 0.030100 parameters
wR(F2) = 0.094H-atom parameters constrained
S = 1.08Δρmax = 0.32 e Å3
1873 reflectionsΔρmin = 0.25 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
C10.08579 (13)0.3217 (2)0.05297 (9)0.0359 (4)
H1A0.03640.41220.06240.054*
H1B0.14420.37370.02920.054*
H1C0.10440.26750.10160.054*
C20.17104 (11)0.0731 (2)0.08775 (8)0.0336 (3)
H2A0.21380.02770.09610.050*
H2B0.12720.08780.13190.050*
H2C0.21160.17750.08150.050*
C110.09375 (10)0.14618 (18)0.11718 (8)0.0257 (3)
C120.03662 (11)0.25669 (19)0.16564 (8)0.0295 (3)
H120.01270.32880.14380.035*
C130.05251 (13)0.2604 (2)0.24603 (9)0.0339 (3)
H130.01350.33380.27750.041*
C140.12622 (12)0.1549 (2)0.27919 (9)0.0362 (4)
H140.13590.15540.33300.043*
C150.18563 (12)0.0482 (2)0.23183 (9)0.0372 (4)
H150.23590.02150.25390.045*
C160.17020 (11)0.0452 (2)0.15125 (9)0.0307 (3)
H160.21120.02480.11990.037*
N10.04376 (10)0.18785 (15)0.00091 (7)0.0277 (3)
N20.11088 (9)0.04525 (16)0.01743 (7)0.0277 (3)
P10.08233 (3)0.16498 (5)0.01035 (2)0.02618 (14)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0509 (10)0.0263 (8)0.0304 (8)0.0060 (7)0.0051 (7)0.0052 (6)
C20.0319 (7)0.0386 (8)0.0302 (7)0.0019 (6)0.0104 (6)0.0022 (6)
C110.0285 (7)0.0237 (7)0.0250 (7)0.0039 (5)0.0019 (5)0.0006 (5)
C120.0330 (7)0.0262 (7)0.0292 (7)0.0013 (6)0.0007 (6)0.0004 (6)
C130.0375 (8)0.0345 (8)0.0298 (8)0.0014 (6)0.0017 (6)0.0076 (7)
C140.0391 (9)0.0413 (9)0.0283 (7)0.0057 (7)0.0076 (6)0.0036 (6)
C150.0339 (8)0.0385 (9)0.0392 (8)0.0016 (7)0.0129 (6)0.0017 (7)
C160.0269 (7)0.0306 (7)0.0346 (7)0.0002 (6)0.0009 (6)0.0042 (6)
N10.0323 (6)0.0226 (6)0.0282 (6)0.0037 (5)0.0036 (5)0.0076 (5)
N20.0314 (6)0.0252 (6)0.0265 (6)0.0025 (5)0.0099 (5)0.0015 (5)
P10.0307 (2)0.0230 (2)0.0248 (2)0.00033 (14)0.00652 (14)0.00337 (13)
Geometric parameters (Å, °) top
C1—N11.4583 (18)C12—H120.9300
C1—H1A0.9600C13—C141.384 (2)
C1—H1B0.9600C13—H130.9300
C1—H1C0.9600C14—C151.389 (2)
C2—N21.4605 (17)C14—H140.9300
C2—H2A0.9600C15—C161.395 (2)
C2—H2B0.9600C15—H150.9300
C2—H2C0.9600C16—H160.9300
C11—C161.398 (2)N1—N2i1.4321 (17)
C11—C121.400 (2)N1—P11.6953 (14)
C11—P11.8412 (15)N2—N1i1.4321 (17)
C12—C131.393 (2)N2—P11.6984 (12)
N1—C1—H1A109.5C12—C13—H13120.0
N1—C1—H1B109.5C13—C14—C15119.73 (14)
H1A—C1—H1B109.5C13—C14—H14120.1
N1—C1—H1C109.5C15—C14—H14120.1
H1A—C1—H1C109.5C14—C15—C16120.24 (14)
H1B—C1—H1C109.5C14—C15—H15119.9
N2—C2—H2A109.5C16—C15—H15119.9
N2—C2—H2B109.5C15—C16—C11120.72 (14)
H2A—C2—H2B109.5C15—C16—H16119.6
N2—C2—H2C109.5C11—C16—H16119.6
H2A—C2—H2C109.5N2i—N1—C1114.56 (12)
H2B—C2—H2C109.5N2i—N1—P1120.94 (9)
C16—C11—C12118.12 (13)C1—N1—P1121.23 (10)
C16—C11—P1121.12 (11)N1i—N2—C2114.43 (11)
C12—C11—P1119.90 (11)N1i—N2—P1120.04 (9)
C13—C12—C11121.04 (14)C2—N2—P1119.18 (10)
C13—C12—H12119.5N1—P1—N2106.49 (6)
C11—C12—H12119.5N1—P1—C11101.67 (6)
C14—C13—C12120.08 (14)N2—P1—C11100.84 (6)
C14—C13—H13120.0
C16—C11—C12—C132.7 (2)N2i—N1—P1—C1166.99 (11)
P1—C11—C12—C13172.18 (11)C1—N1—P1—C11134.55 (11)
C11—C12—C13—C140.5 (2)N1i—N2—P1—N137.75 (13)
C12—C13—C14—C151.3 (2)C2—N2—P1—N1112.73 (11)
C13—C14—C15—C161.0 (2)N1i—N2—P1—C1168.00 (11)
C14—C15—C16—C111.3 (2)C2—N2—P1—C11141.52 (11)
C12—C11—C16—C153.1 (2)C16—C11—P1—N1148.76 (12)
P1—C11—C16—C15172.42 (12)C12—C11—P1—N142.10 (12)
N2i—N1—P1—N238.17 (13)C16—C11—P1—N239.20 (13)
C1—N1—P1—N2120.30 (12)C12—C11—P1—N2151.65 (11)
Symmetry codes: (i) −x, −y, −z.
Acknowledgements top

The authors thank Project AuTEK (Mintek and Harmony Gold) and the University of the Witwatersrand for financial support.

references
References top

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