1377m cmϪ1. 1H NMR: δ 1.56 (s, 45H, Cp*), 7.37–7.57 (m, 15H,
Ph). ES mass spectrum (MeOH containing NaOMe, m/z): 1420,
[M ϩ Na]ϩ; 955, [M ϩ Na Ϫ Ru{PhC4(CN)4}]ϩ.
Table 2 Selected bond distances (Å) and angles (Њ) for 4 and 5
4
5
Ru–P
Ru(1)–C(Cp*)
(av.)
Ru(2)–C(Cp*)
(av.)
Ru(3)–C(Cp*)
(av.)
2.3618(8)
2.194–2.271(2)
2.24(3)
2.179–2.276(3)
2.22(4)
3
᎐
Reaction of Ru{ꢀ -CHPh᎐CHC᎐CPh(C᎐CPh)}(PPh )Cp*
᎐
᎐
᎐
3
2.171–2.283(6)
2.22(4)
2.172–2.298(5)
2.23(5)
2.174–2.305(5)
2.23(6)
(7) with tcne. When tcne (8 mg, 0.06 mmol) was added to a
solution of Ru{η -CHPh᎐CHC᎐CPh(C᎐CPh)}(PPh )Cp* (7)
3
᎐
᎐
᎐
᎐
3
(50 mg, 0.06 mmol) in benzene (5 ml), the mixture immediately
turned dark green. After 30 min at rt, no starting complex
was present. Evaporation, extraction of the residue with thf
and separation by preparative t.l.c. (acetone–hexane 3/7) gave
two closely running deep green bands as the major product.
Dark green solids were obtained after extraction (Rf 0.49, 10
mg; Rf 0.47, 19.5 mg). Both materials have identical physical
properties and are probably isomers. Rechromatography of
each band separately also generates two green bands. Crystal
structures of products from each band were determined,
but were identical, suggesting that in each case, the same
isomer is preferentially crystallised. The complex was identified
Ru(1)–C(14)
Ru(2)–C(11)
Ru(2)–C(12)
Ru(2)–C(13)
Ru(2)–C(21)
Ru(2)–C(22)
Ru(2)–C(23)
Ru(3)–C(31)
Ru(3)–C(32)
Ru(3)–C(33)
Ru(1)–N(11)
Ru(2)–N(11)
Ru(3)–N(141)
C(11)–C(12)
C(11)–C(111)
C(12)–C(13)
C(13)–C(14)
C(14)–C(141)
C(21)–C(22)
C(21)–C(211)
C(23)–C(24)
C(31)–C(32)
C(32)–C(33)
C(33)–C(34)
C–CN (av.)
C(111)–N(111)
C(141)–N(141)
C(211)–N(211)
C–N (av.)
2.032(2)
2.234(5)
2.159(4)
1.980(5)
2.226(5) [Ru(1)]
2.155(5) [Ru(1)]
1.975(5) [Ru(1)]
2.198(4)
2.171(5)
1.969(5)
2.044(4) [N(111)]
2.074(4) [N(211)]
2.031(4)
1.466(7)
1.432(7)
1.422(7)
1.347(7)
1.432(7)
1.475(7)
1.433(7)
1.358(7)
1.471(7)
1.429(7)
1.356(7)
1.436(7)
1.149(7)
1.143(6)
2.242(2)
2.163(2)
1.986(3)
2.034(2) [N(211)]
2.049(2) [N(141)]
as
Ru{η1,η2(N,C)-C(CH᎐CHPh)᎐CPhC[CPh᎐C(CN) ]᎐
᎐ ᎐ ᎐ ᎐
2
C(CN)(C᎐N)}(PPh )Cp* (6) by X-ray crystallography. Anal.
Found: C, 74.03; H, 5.18; N, 5.98. Calc. for C58H47N4P2Ru: C,
᎐
3
1.363(6)
74.74; H, 5.08; N, 6.01%; M, 932. IR (CH2Cl2): ν(CN) 2230w,
1.483(4)
1.368(4)
1.461(4)
1.458(4)
1.432(3)
1.353(4)
2208s; other bands at 1597m, 1561m, 1524w, 1490s, 1371s cmϪ1
.
1H NMR: δ 1.44 [d, J(HP) 1.4 Hz, 15H, Cp*], 3.34 [d, J(HH)
16 Hz, 1H, ᎐CH], 4.41 [d, J(HH) 16 Hz, 1H, ᎐CH], 5.92–7.33
᎐
᎐
(m, 30H, Ph). 31P NMR: δ 48.75 (s), 50.34 (s). ES mass
spectrum (CH2Cl2–MeOH, m/z): 934, [M ϩ 2H]ϩ; 672,
[M ϩ 2H Ϫ PPh3]ϩ.
Structure determinations
1.44(1)
Full spheres of diffraction data were measured at ca. 153 K
using a Bruker AXS CCD area-detector instrument. Ntot
reflections were merged to Nunique (Rint quoted) after
“empirical”/multiscan absorption correction (proprietary
software), No with F > 4σ(F) being used in the full matrix
least squares refinement. All data were measured using
monochromatic Mo-Kα radiation, λ = 0.71073 Å. Anisotropic
thermal parameter forms were refined for the non-hydrogen
atoms, (x, y, z, Uiso)H being constrained at estimated values.
Conventional residuals R, Rw on |F| are given [weights: (σ2(F) ϩ
0.0004F 2)Ϫ1]. Neutral atom complex scattering factors
were used; computation used the Xtal 3.7 program system.14
Pertinent results are given in the Figures (which show non-
hydrogen atoms with 50% probability amplitude displacement
envelopes and hydrogen atoms with arbitrary radii of 0.1 Å)
and Tables 1–3.
1.170(3)
1.146(3)
1.142(6)
1.149(7)
1.144(8)
P–Ru(1)–C(14)
P–Ru(1)–N(211)
94.31(9)
86.75(7)
87.90(9)
68.6(1)
C(14)–Ru(1)–N(211)
C(21)–Ru(2)–C(23)
C(11)–Ru(2)–N(211)
C(13)–Ru(2)–N(211)
C(21)–Ru(2)–N(141)
C(23)–Ru(2)–N(141)
C(31)–Ru(3)–N(141)
C(33)–Ru(3)–N(141)
C(12)–C(11)–C(111)
C(11)–C(12)–C(13)
C(12)–C(13)–C(14)
C(13)–C(14)–C(141)
C(22)–C(21)–C(211)
C(21)–C(22)–C(23)
C(22)–C(23)–C(24)
C(31)–C(32)–C(33)
C(32)–C(33)–C(34)
Ru(1)–N(111)–C(111)
Ru(2)–N(211)–C(211)
Ru(3)–C(141)–N(141)
Ru(1)–C(14)–C(13)
Ru(1)–C(14)–C(141)
C(11)–C(111)–N(111)
C(14)–C(141)–N(141)
C(21)–C(211)–N(211)
89.7(2)
89.1(2)
88.58(8)
91.06(9)
88.4(2)a
91.9(2)a
90.0(2)
89.6(2)
117.1(4)
110.2(4)
140.2(4)
122.4(5)
123.6(3)
127.6(3)
115.9(2)
120.4(2)
111.3(2)
132.0(2)
Variata. Complex 3. (x, y, z, Uiso)H were refined. Difference
map residues were modelled as methanol, seemingly hydrogen-
bonded to CN(41) of the cyanocarbon ligand [N(41) ؒ ؒ ؒ H,O-
(x, 2 Ϫ y, z) 1.90(4), 2.915(3) Å]. C(41)–N(41) [1.158(3) Å] may
be slightly elongated in consequence.
Complex 4. Difference map residues were most satisfactorily
modelled as two MeCN molecules, one disordered over two sets
of sites, occupancies set at 0.5 after trial refinement.
Complex 5. Difference map residues were modelled as three
Me2CO molecules; displacement amplitudes on the latter
were high, particularly on molecule ‘3’ which was refined with
isotropic displacement parameters and constrained geometries.
CCDC reference numbers 165410–165413.
111.6(4)
139.7(5)
166.9(4)
164.0(4)
177.9(4)
170.4(2)
132.1(2)
111.9(2)
174.8(5)
179.4(5)
175.6(5)
171.2(3)
172.9(2)
a Values for C(21)–Ru(1)–N(111), C(23)–Ru(1)–N(111).
(m, 25H, Ph). 31P NMR: δ 43.58 (s, PPh3). ES mass spectrum
(MeOH containing NaOMe, m/z): 1217, [M ϩ Na]ϩ; 1194, Mϩ;
955, [M ϩ Na Ϫ PPh3]ϩ.
lographic data in CIF or other electronic format.
Band 3 (Rf 0.32) gave orange crystals (acetone–hexane) of
Acknowledgements
{Ru[η3-C(CN) ᎐CPhC᎐C(CN) ]Cp*} (5) (46 mg, 52%). Anal.
᎐
᎐
2
2
3
Found: C, 61.52; H, 4.40; N, 11.52. Calc. for C72H60N12Ru3: C,
61.92; H, 4.33; N, 12.03%; M, 1397. IR (CH2Cl2): ν(CN)
2215m, 2126w; other bands at 1603m, 1493w, 1449m, 1417m,
This work was supported by the Australian Research Council.
We thank Professor Brian Nicholson (University of Waikato,
New Zealand) for the mass spectra. We are grateful to Johnson
3632
J. Chem. Soc., Dalton Trans., 2001, 3627–3633