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Selected Projects 20<strong>16</strong>-<strong>18</strong><br />

were arranged into six-membered hexamers. The<br />

binding energies were found to be moderately large,<br />

suggesting that the dipeptides have high affinity<br />

for each other in this hexamer arrangement. The<br />

binding energies of linear WY and cyclic WY, were almost<br />

identical, suggesting that both forms of WY are<br />

equally likely to self-assemble. However, the binding<br />

energy of cyclic YY was almost twice as much as the<br />

binding energy of linear YY, suggesting that the cyclic<br />

form of YY will self-assemble much more readily. In<br />

fact, the cyclic YY hexamer was found to have the<br />

largest binding energy of all the dipeptides studied,<br />

suggesting it is the most likely to form na<strong>no</strong>tubes.<br />

The calculated inner and outer diameters of each<br />

hexamer were compared against experimental data<br />

for the highly studied diphenylalanine na<strong>no</strong>tube,<br />

revealing that these four na<strong>no</strong>tubes will be slightly<br />

larger, due to large side chains and higher polarity.<br />

An interaction energy decomposition was also<br />

carried out on the hexamers at HF/6-31G* and<br />

shows that the same forces that drive the interaction<br />

between the dimers are at play on a larger scale<br />

also, and therefore likely drive the self-assembling<br />

of the whole na<strong>no</strong>tube as well.<br />

This project can take several directions from here.<br />

One next step could be to use molecular dynamics<br />

simulations to study the self-assembly of<br />

dipeptides by simulating their behavior over time.<br />

A<strong>no</strong>ther next step could be to apply the techniques<br />

used thus far to tripeptides and tetrapeptides to<br />

learn about their fundamental properties, as these<br />

oligopeptides are also commonly used as building<br />

blocks for peptide na<strong>no</strong>structures.<br />

152

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