1890 Inorganic Chemistry, Vol. 50, No. 5, 2011
Sharma and Bharadwaj
have low energy barrier. However, if the energy barrier is
high, the pedal motion does not show any disordering in the
crystal structure due to insignificant population of the minor
conformer.5 This motion has not been widely acknowledged
because it is often difficult to detect and, therefore, easy to
overlook. However, once we recognize the prevalence of the
pedal motion, many dynamic phenomena can be interpreted
on the basis of this motion, irrespective of its detection.
The pedal motion has been shown to be active in several
organic crystals. It has been studied in crystals of bis-
(triarylmethyl)peroxide,6 polyenes,7 and azobenzene.8 Its
role in [2 þ 2] photodimerization of alkene derivatives has
been reported recently.9 The isomerization in butadienes
through the pedal motion is reminiscent of the photoisome-
rization in the visual pigment rhodopsin.10 A recently pro-
posed interpretation of the photocycle of photoactive yellow
protein (PYP) also emphasized the potential importance of
the pedal motion in proteins.11 MacGillivray and co-workers
have reported a rare example of the racklike movement of
alkyl chains that coupled with pinionlike 180° rotation of
olefins in a single crystal.12
Scheme 1. Schematic Representation of Pedal Motion in the Diphe-
nyldiazene Moieties in Ligand (azim)
ditionally, there has been comparatively little attention
directed toward reversible, concerted ligand substitution at
metal sites in PCPs in single-crystal to single-crystal (SC-
SC) fashion, leading to expression of new functionality.13
In compound 2, the guest molecules including the counter-
anions make significant movement, and the counteranions
eventually occupy vacant coordination sites on the metal,
keeping crystallinity intact throughout.
Herein, we report the synthesis of two two-dimensional
(2D) coordination polymers, {[Co(azim)2(DMF)2] (ClO4)2
3
3
2DMF}n (1) and {[Cd(azim)2(DMF)2] (ClO4)2 2DMF}n (2)
3
3
prepared at room temperature by reacting M(ClO4)2 (M(II) =
Co(II) and Cd(II)) with the ligand, bis(4-imidazol-1-yl-phe-
nyl)diazene (azim). The ligand is designed with an azo moiety
in the middle for possible bicycle-pedal motion. Here, the two
phenyl rings are attached to the central NdN moiety. The
relationships among these parts are similar to those of bicycle
pedals (phenyl rings), crank arms (NdN bond), and spindles
(N-Ph bonds) (Scheme 1). The azo bonds and phenyl rings
are disordered in the solid-state structure of 1, over two
positions due to crankshaft motion. Interestingly, this dis-
orderisnotobserved in2. Therefore, wehave chosenpolymer
2 to study heat-/guest-dependent bicycle-pedal motion. Ad-
Results and Discussion
Compounds 1 and 2, once isolated, are found to be air-
stable and slightly soluble in DMF and DMSO, but insoluble
in other common organic solvents or water. Single-crystal
X-ray determination at 100 K reveals that both 1 and 2 are
isostructural and the asymmetric unit of each polymer con-
tains one M(II) ion (half occupancy), two halves of the
ligand, two DMF molecules, and one ClOh anion. Each
4
metal ion is distorted octahedral with equatorial ligation by
imidazole N of four different ligand units and axial ligation
by two DMF molecules (Figure 1) with M-N and M-O
bond distances14,15 within normal ranges. The ligands bridge
metal ions to form a 2D rhombus-grid structure. Both phenyl
rings of the ligand are nearly coplanar, while imidazole rings
are twisted significantly with respect to the phenyl rings. Each
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grid (M4L4) shows the diagonal M M distances of 33.922
3 3 3
˚
˚
and 20.151 A in 1 and 34.759 and 20.275 A in 2 (Table 1,
Figure 2). These 2D layers are stacked in ABAB... fashion.16
Lattice DMF molecules and ClOh anions occupy the void
4
spaces in the grid. In case of 1, diphenyldiazene moiety of the
ligand A and C in the M4L4 macrocyclic unit are disordered
over two positions because of the pedal motion and both con-
formers of the ligand are distributed inthe crystal (Figure 3a).
On the other hand, no such disorder is observed in case of 2
(Figure 3b). Thermal analyses of 1 and 2 show weight losses
of ∼27 and ∼23.4% respectively, in the temperature range
70-150 °C, that correspond to loss of both lattice and
coordinated DMF molecules. The desolvated frameworks
are stable up to ∼340 °C.16 IR spectra of 1 and 2 show a C-H
stretching vibration at ∼2930 cm-1 and a CdO stretching
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~
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(16) See Supporting Information.