A. Gopalan Nair et al. / Inorganic Chemistry Communications 45 (2014) 51–54
53
relative to the CH2 protons in N-cyanoacetylurethane, which appear
at δ 4.06.
The 1H NMR spectrum of 7 was more complex. All four aromatic CH
protons from the p-cymene ligand are inequivalent. Each appears as a
doublet due to 3J(HH) coupling, with three of the signals showing addi-
tional resolved long-range coupling, presumably cross-ring 4J ‘W’-
coupling [16]. Two of the protons clearly form an AB type pattern, with
more intense inner lines. The methyl groups of the cymene iso-propyl
substituent are inequivalent and appear as two doublets at δ 1.08 and
1.23, with coupling to the iso-propyl CH proton. The protons of the ethyl
group also show a more complex pattern in 7 compared to 6. The CH3 pro-
tons appear as a triplet, but the CH2 protons (Fig. 1) are diastereotopic and
each appears as a resonance approximating to a doublet of quartets due to
2J(HH) geminal coupling, together with 3J(HH) coupling to the CH3 pro-
tons in an ABX3 spin system. The ruthenalactam proton appears at δ 2.2
as a doublet due to phosphorus coupling [3J(PH) 8.6 Hz], while the
CH(CH3)2 proton from the p-cymene ligand gives a quintet at δ 2.63.
In order to unequivocally characterise the ruthenalactam ring system,
an X-ray structure determination was carried out on the p-cymene com-
plex 7, which gave a small number of crystals suitable for study [17]. The
molecular structure is shown in Fig. 2 together with selected bond lengths
and angles. The complex contains the typical ‘piano-stool’ arrangement of
an η6 p-cymene ligand, the chelating N,C-bonded ligand (confirming the
formation of the ruthenalactam ring), and a triphenylphosphine. The
ruthenalactam ring system pays a strong resemblance to the correspond-
ing platinalactam ring in [Pt{CH(CN)C(O)N(CO2Et)}(cod)] [1], (cod =
cyclo-octa-1,5-diene) which is the only other structurally characterised
four-membered ring metallalactam derived from N-cyanoacetylurethane.
The Ru–C–C–N ring is highly planar, with a fold angle between the
N(1)–Ru(1)–C(1) and C(1)–C(2)–N(1) planes of only 1.84°. The torsion
angles Ru(1)–C(1)–C(2)–O(1) and Ru(1)–N(1)–C(2)–O(1) [both
178.8(2)°] corroborate this planarity. The N(1)–Ru(1)–C(1) bite angle of
the metallacyclic ligand is 64.49(7)°, which is comparable to the angle
of 67.0(3)° in the platinum complex [Pt{CH(CN)C(O)N(CO2Et)}(cod)]
[1]. The CO2 group of the ester substituent is also reasonably coplanar
Ru
Pt
Fig. 3. A comparison of the metallalactam rings of [Ru{CH(CN)C(O)N(CO2Et)}(PPh3)(η6-p-
cymene)] 7 (left) and [Pt{CH(CN)C(O)N(CO2Et)}(cod)] (right, cod = cyclo-octa-1,5-
diene), showing the different arrangements of the CO2Et substituent with respect to the
metallalactam ring.
with the ruthenalactam ring, with C(2)–N(1)–C(4)–O(2) and Ru(1)–
N(1)–C(4)–O(3) torsion angles of 169.6(2) and 172.1(1)° respectively.
The Ru–N and Ru–CH(CN) bond distances of 7 are in the expected
range, for example the Ru–C(1) bond distance of 2.1654(19) Å is identical
to that of 2.169(4) Å in the cyanoalkyl complex [Ru{CH(CN)SO2Ph}(η5-
C5H5)(CO)(PPh3)] [18]. The Ru–C and Ru–N bonds of 7 are larger by
0.0788 and 0.0964 Å respectively, when compared to [Pt{CH(CN)C(O)
N(CO2Et)}(cod)], consistent with the 0.1 Å greater covalent radius of ru-
thenium. The C_O bond distances of 7 [C(2)–O(1) 1.209(3) and C(4)–
O(2) 1.222(3) Å] are also comparable to the corresponding distances in
[Pt{CH(CN)C(O)N(CO2Et)}(cod)] [1.196(9) and 1.215(9) Å]. The cyano
group, C(3)–N(2), is directed towards the p-cymene ring, and the
ruthenalactam hydrogen points H(1) towards the PPh3 ligand [with a
H(1)⋯H(22) non-bonded distance of 2.4537(1) Å]. This arrangement pre-
sumably arises in order to minimise steric interactions between the CN
group and the PPh3 ligand.
The most significant difference between [Ru{CH(CN)C(O)N
(CO2Et)}(PPh3)(η6-p-cymene)] and [Pt{CH(CN)C(O)N(CO2Et)}(cod)]
involves the orientation of the ester substituent. In [Pt{CH(CN)C(O)
N(CO2Et)}(cod)] the OEt group is proximal to the platinum atom, where-
as in [Ru{CH(CN)C(O)N(CO2Et)}(PPh3)(η6-p-cymene)] it is distal, as
shown in the comparison in Fig. 3. This is presumably due to the greater
steric bulk of the p-cymene and PPh3 ligands in the Ru complex. The p-
cymene ligand bonds slightly asymmetrically to the ruthenium, as a re-
sult of the steric effects involving the PPh3 ligand; the Ru(1)–C(13) and
Ru(1)–C(14) bonds – those closest to the PPh3 ligand – are the two lon-
gest Ru–C(cymene) bond lengths.
C(12)
C(13)
C(11)
C(10)
C(17)
C(19)
C(18)
N(2)
C(14)
C(16)
Ru(1)
C(31)
C(3)
O(1)
C(1)
C(2)
N(1)
C(41)
P(1)
O(2)
This study indicates that metallalactam complexes of another plati-
num group metal can be readily synthesised by a simple one-pot proce-
dure; investigations into metallalactam complexes of other metals are in
progress.
C(4)
O(3)
C(21)
C(5)
Acknowledgments
C(6)
We thank the University of Waikato for financial support of this
work and Dr. Tania Groutso (University of Auckland) for collection of
the X-ray data set.
Fig. 2. Molecular structure of the complex [Ru{CH(CN)C(O)N(CO2Et)}(PPh3)(η6-p-
cymene)] 7. Only the ipso carbons of the triphenylphosphine ligand are shown for clarity.
Selected bond lengths (Å) and angles (°): Ru(1)–P(1) 2.3259(5), Ru(1)–N(1) 2.0948(17),
Ru(1)–C(1) 2.1654(19), N(1)–C(2) 1.377(3), C(1)–C(2) 1.539(3), C(2)–O(1) 1.209(3),
C(1)–C(3) 1.451(3), C(3)–N(2) 1.150(3), N(1)–C(4) 1.367(3), Ru–C(cymene) range
2.217(2) to 2.277(2), mean 2.244(2), C(1)–Ru(1)–N(1) 64.49(7), Ru(1)–N(1)–C(2)
100.62(12), N(1)–C(2)–C(1) 102.36(16), Ru(1)–C(1)–C(2) 92.50(12), C(1)–C(3)–N(2)
177.5(2), P(1)–Ru(1)–N(1) 89.02(5), P(1)–Ru(1)–C(1) 85.65(6).
Appendix A. Supplementary material
CCDC 976610 contains the supplementary crystallographic data for
this paper. These data can be obtained free of charge from The Cambridge