Background
Many phenomena of biological interest
originate directly from mechanical motions at the molecular level. Celebrated examples
include the trans-cis isomerisation of double bonds that trigger the visual
signal and the rotary motion of the enzyme F1-ATPase, one of the cornerstones
of energy conversion in the cell. This extraordinary dependence on molecular level motion in key
natural processes is inspiring scientists to try and bridge the gap between synthetic
chemistry, which by and large relies upon electronic and chemical effects and
does not exploit molecular motions, and the macroscopic world, where our everyday
machines rely upon the synchronized motions of their components to perform their
designated tasks. Accordingly, there is great current interest in trying to make
molecular analogues of some of the fundamental components of machinery from the
macroscopic world (cogs, wheels, shuttles, pistons etc). The idea is that such
structures could form the basis of synthetic devices or materials that, like biological
systems, could function through molecular level mechanical motion. Here we propose
a Network which aims to go from developing a simple understanding of how molecular
level interlocked components move mechanically with respect to each other, right
through gaining control over such motions using external stimuli (electric fields,
electrons, photons etc), to the preparation of synthetic materials which change their
macroscopic properties in response to a specific signal.
Molecules with mechanically interlocked
architectures are particularly interesting for these sorts of applications because,
in principle, they permit the controlled movement and positioning of one mechanically
interlocked component with respect to another (Figure 1). These structures fall into two
basic classes: "catenanes" which consist of two or more interlocked rings and
"rotaxanes" where a macrocycle is locked onto a linear "thread" by bulky "stoppers".
Figure 1. Controlled motions
in mechanically-interlocked architectures.
Rotational motion in a catenane
Linear motion in a rotaxane (a "molecular shuttle")
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