| 186 |
|
molecule]{Schematic representation of a typical banana shaped |
| 187 |
|
molecule.} \label{LCFig:BananaMolecule} |
| 188 |
|
\end{figure} |
| 189 |
– |
|
| 189 |
|
\begin{figure} |
| 190 |
|
\centering |
| 191 |
|
\includegraphics[width=\linewidth]{gb_scheme.eps} |
| 194 |
|
definitions of the orientation vectors for a pair of Gay-Berne |
| 195 |
|
molecules} \label{LCFigure:GBScheme} |
| 196 |
|
\end{figure} |
| 198 |
– |
|
| 197 |
|
To account for the permanent dipolar interactions, there should be |
| 198 |
|
an electrostatic interaction term of the form |
| 199 |
|
\begin{equation} |
| 345 |
|
\includegraphics[width=\linewidth]{s22_220.eps} |
| 346 |
|
\caption[Average orientational correlation Correlation Functions of |
| 347 |
|
a Bent-core Liquid Crystal System at Temperature T = 460K and |
| 348 |
< |
Pressure P = 10 atm]{Correlation Functions of a Bent-core Liquid |
| 349 |
< |
Crystal System at Temperature T = 460K and Pressure P = 10 atm. (a) |
| 350 |
< |
radial correlation function $g(r)$; and (b) density along the |
| 353 |
< |
director $g(z)$.} \label{LCFigure:S22220} |
| 348 |
> |
Pressure P = 10 atm]{Average orientational correlation Correlation |
| 349 |
> |
Functions of a Bent-core Liquid Crystal System at Temperature T = |
| 350 |
> |
460K and Pressure P = 10 atm.} \label{LCFigure:S22220} |
| 351 |
|
\end{figure} |
| 352 |
|
|
| 353 |
|
\section{Conclusion} |
| 360 |
|
had some defects because of the mismatching between the layer |
| 361 |
|
structure spacing and the shape of simulation box. This mismatching |
| 362 |
|
can be broken by using NPTf integrator in further simulations. The |
| 363 |
< |
lack of detail in. |
| 363 |
> |
role of terminal chain in controlling transition temperatures and |
| 364 |
> |
the type of mesophase formed have been studied |
| 365 |
> |
extensively\cite{Pelzl1999}. The lack of flexibility in our model |
| 366 |
> |
due to the missing terminal chains could explained the fact that we |
| 367 |
> |
did not find evidence of chirality. |
