1
is dramatic. In the H NMR spectrum of Pd(1H MeCN
Fig. 1d) the resonances corresponding to H , H and H are
alkyl
2
)Cl
2
(
G
g
shifted significantly upfield, indicating that each macrocycle is
9
located preferentially over the aliphatic region of the other. The
X-ray crystal structure (Fig. 2c and d) shows a similar geometry
exists in the solid state. An additional feature of the X-ray crystal
structure of Pd(1H
2
)Cl
Pd–Cl HNCO hydrogen bonds between adjacent molecules
Fig. 2d). The negligible change in the chemical shift of the amide
protons (H ) between 1H (Fig. 1a) and Pd(1H )Cl MeCN
Fig. 1d) suggests this interaction is weak in solution, nevertheless
2
MeCN is the presence of intermolecular
…
(
C
2
2
2
6
(
10
it has been successfully utilised to direct the formation of
pseudorotaxanes.
The three catenanes 1H2, Pd1 and Pd(1H
directly interconvertible (Scheme 1): the palladium complexes
are de-metallated with KCN; Pd(1H )Cl MeCN is converted
into Pd1 by treatment with NaH, and the reverse reaction is
2 2
)Cl MeCN are all
2
2
1
1
promoted by HCl in MeCN. It is interesting to note the
macrocycles adopt similar positions and orientations in Pd1 and
2
1H but in the former they are locked in place by a coordination
bond whereas in the latter they are held in the thermodynamic
minimum only by weak and dynamic H-bonds. The preferred
2 2
co-conformation of Pd(1H )Cl MeCN is very different to the
other two, presumably on steric grounds, and as such its formation
from either of the others corresponds to a large amplitude
rotational switch. It is rare to find such a rich variation in structure
and dynamics made possible through simple manipulation of
coordination modes.
6
7
Fig. 2 X-Ray crystal structures of: (a) 1H
2
,
(b) Pd1, (c)
MeCN (single molecule view; note the change of position
and orientation of the yellow macrocycle compared to Pd1 and 1H ) and
d) adjacent molecules of Pd(1H )Cl MeCN showing intermolecular
8
2 2
Pd(1H )Cl
2
(
2
2
…
Pd–Cl HN hydrogen bonding. Carbon atoms of the bis-amide macro-
cycle are shown in light blue and those of the tetra-ether macrocycle and
coordinated acetonitrile molecule in yellow; oxygen atoms are red,
nitrogen dark blue, hydrogen white, palladium grey, chlorine green. For
clarity only amide hydrogen atoms are shown. Selected bond lengths for
Notes and references
1 V. Balzani, A. Credi, F. M. Raymo and J. F. Stoddart, Angew. Chem.,
Int. Ed., 2000, 39, 3348; J.-P. Sauvage, Chem. Commun., 2005, 1507;
K. Kinbara and T. Aida, Chem. Rev., 2005, 105, 1377.
2
For examples of catenanes which undergo stimuli-induced half-rotations
see: M. Cesario, C. O. Dietrich-Buchecker, J. Guilhem, C. Pascard and
J.-P. Sauvage, J. Chem. Soc., Chem. Commun, 1985, 244; A. Livoreil,
C. O. Dietrich-Buchecker and J.-P. Sauvage, J. Am. Chem. Soc., 1994,
˚
Pd(1H
Selected bond angles for Pd(1H
N5 104.1.
2
)Cl
2
MeCN [A]: N2H–N5 2.21; N11H–N5 2.31; N5–N41 12.93.
2
)Cl MeCN [u]: N2–H–N5 108.8; N11–H–
2
1
16, 9399; D. B. Amabilino, C. O. Dietrich-Buchecker, A. Livoreil,
L. P e´ rez-Garc ´ı a, J.-P. Sauvage and J. F. Stoddart, J. Am. Chem. Soc,
996, 118, 3905; D. A. Leigh, K. Moody, J. P. Smart, K. J. Watson and
1
resonances indicate a p-stacking arrangement between the benzylic
A. M. Z. Slawin, Angew. Chem., Int. Ed. Engl., 1996, 35, 306; A. Livoreil,
J. P. Sauvage, N. Armaroli, V. Balzani, L. Flamigni and B. Ventura,
J. Am. Chem. Soc., 1997, 119, 12114; C. P. Collier, G. Mattersteig,
E. W. Wong, Y. Luo, K. Beverly, J. Sampaio, F. M. Raymo,
J. F. Stoddart and J. R. Heath, Science, 2000, 289, 1172; V. Balzani,
A. Credi, S. J. Langford, F. M. Raymo, J. F. Stoddart and M. Venturi,
J. Am. Chem. Soc., 2000, 122, 3542; D. W. Steuerman, H. R. Tseng,
A. J. Peters, A. H. Flood, J. O. Jeppesen, K. A. Nielsen, J. F. Stoddart
and J. R. Heath, Angew. Chem., Int. Ed., 2004, 43, 6486; B. Korybut-
Daszkiewicz, A. Wie c¸ kowska, R. Bilewicz, S. Domagala and
K. W o´ zniak, Angew. Chem., Int. Ed., 2004, 43, 1668.
amide rings of the ‘blue’ macrocycle and the pyridine group of the
‘orange’ macrocycle. In contrast, the alkyl chain protons are not
shielded by interactions with aromatic rings in either catenane.
1
The solution geometries suggested by H NMR studies correspond
well to the solid state structures of 1H
Fig. 2b) determined by X-ray crystallography. Reaction of
with Pd(OAc) (MeCN, 60 uC, 4 h, 79%) re-forms the
2
(Fig. 2a) and Pd1
(
1
H
2
2
co-conformationally locked catenate, Pd1.
Reaction of 1H with PdCl (MeCN) in MeCN (20 uC, 1 h,
5%) afforded a second catenane Pd(II) complex in which the
3 A ‘switch’ influences a system as a function of state; a ‘motor’ influences
a system as a function of trajectory. For a discussion see: E. R. Kay and
D. A. Leigh, Top. Curr. Chem. (in press).
2
2
2
8
amide protons (H ) of the ‘blue’ macrocycle were clearly still
C
4
D. A. Leigh, J. K. Y. Wong, F. Dehez and F. Zerbetto, Nature, 2003,
24, 174; J. V. Hern a´ ndez, E. R. Kay and D. A. Leigh, Science, 2004,
306, 1532.
present (Fig. 1d). X-Ray crystallography (Fig. 2c and d) on a single
crystal obtained from slow cooling a saturated acetonitrile solution
4
5
A.-M. Fuller, D. A. Leigh, P. J. Lusby, I. D. H. Oswald, S. Parsons and
D. B. Walker, Angew. Chem., Int. Ed, 2004, 43, 3914; Y. Furusho,
T. Matsuyama, T. Takata, T. Moriuchi and T. Hirao, Tetrahedron
Lett., 2004, 45, 9593.
2 2
confirmed this complex to be Pd(1H )Cl MeCN, in which only
one of the macrocyclic rings is coordinated to the palladium
metal ion, presumably as a consequence of both the greater
strength of the Pd–Cl bond compared to Pd–OAc and the poor
6 D. A. Leigh, P. J. Lusby, A. M. Z. Slawin and D. B. Walker, Angew.
Chem., Int. Ed., 2005, 44, 4557.
7
2
basicity of the Cl ion.
For various synthetic routes to Pd1 see: A.-M. L. Fuller, D. A. Leigh,
P. J. Lusby, A. M. Z. Slawin and D. B. Walker, J. Am. Chem. Soc. web
release date 17th August 2005.
The effect of the different coordination mode on the relative
positions and orientations of the two macrocycles in the catenane
4
920 | Chem. Commun., 2005, 4919–4921
This journal is ß The Royal Society of Chemistry 2005