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Self-assembled Transition Metal Coordination Frameworks of ...

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Introduction<br />

According to some studies [26,27] regarding the physical basis <strong>of</strong> self­<br />

assembly macrocyclization for the l:l model system, the formation <strong>of</strong> macrocyclic<br />

species can only be accomplished in a certain concentration range between the lower<br />

self-assembly concentration (lsac) and the effective molarity (EM) <strong>of</strong> the self­<br />

<strong>assembled</strong> macrocycle; since monomer and linear oligomers prefer to exist in the<br />

lower and higher concentration ranges, respectively. In a qualitative manner, this<br />

distribution <strong>of</strong> various self-<strong>assembled</strong> species as a filnction <strong>of</strong> concentration is<br />

illustrated [13] in Fig. 1.2. The parameter EM is a measure for the concentration at<br />

which open polymeric structures start to compete with the respective macrocycles<br />

(here the squares), while lsac refers to the concentration at which the macrocycle is<br />

half-<strong>assembled</strong> from the initial building blocks.<br />

M . M o q-‘Q,-4§_ 8 J-F’ 1 \ -—, _ i -_, -Q­<br />

MonOm&\F\\ / 'lu5€1:r*f>’C‘>"cl8 I met<br />

iisac ' EM<br />

Concentration<br />

Fig. 1.2. The distribution <strong>of</strong> self-assembly species as a function <strong>of</strong> concentration.<br />

According to this thermodynamic analysis <strong>of</strong> self-assembly macrocyclization,<br />

desired macrocyclic products exist as major species only within a limited range <strong>of</strong><br />

concentration under given temperature and solvent conditions [13]. In order to<br />

accomplish self-assembly already at low concentration, the coordinative bonds should<br />

ll

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