734 |
|
($\mu$).\label{fig:phaseDiagram}} |
735 |
|
\end{figure} |
736 |
|
|
737 |
< |
We have computed translational diffusion coefficients for lipid |
738 |
< |
molecules from the mean square displacement, |
739 |
< |
\begin{eqnarray} |
740 |
< |
\langle {|\left({\bf r}_{i}(t) - {\bt r}_{i}(0) \right)|}^2 \rangle \\ \\ |
741 |
< |
& = & 6Dt |
742 |
< |
\end{eqnarray} |
743 |
< |
of the lipid bodies. The values of the translational diffusion |
744 |
< |
coefficient for different head-to-tail size ratio are shown in table |
745 |
< |
\ref{tab:relaxation}. |
746 |
< |
|
747 |
< |
We have also computed orientational diffusion constants for the head |
748 |
< |
groups from the relaxation of the second-order Legendre polynomial |
749 |
< |
correlation function, |
737 |
> |
We have computed translational diffusion constants for lipid molecules |
738 |
> |
from the mean-square displacement, |
739 |
> |
\begin{equation} |
740 |
> |
D = \lim_{t\rightarrow \infty} \frac{1}{6 t} \langle {|\left({\bf r}_{i}(t) - {\bf r}_{i}(0) \right)|}^2 \rangle, |
741 |
> |
\end{equation} |
742 |
> |
of the lipid bodies. Translational diffusion constants for the |
743 |
> |
different head-to-tail size ratios (all at 300 K) are shown in table |
744 |
> |
\ref{tab:relaxation}. We have also computed orientational diffusion |
745 |
> |
constants for the head groups from the relaxation of the second-order |
746 |
> |
Legendre polynomial correlation function, |
747 |
|
\begin{eqnarray} |
748 |
|
C_{\ell}(t) & = & \langle P_{\ell}\left({\bf \mu}_{i}(t) \cdot {\bf |
749 |
|
\mu}_{i}(0) \right) \rangle \\ \\ |
750 |
|
& \approx & e^{-\ell(\ell + 1) \theta t}, |
751 |
|
\end{eqnarray} |
752 |
< |
of the head group dipoles. In this last line, we have used a simple |
753 |
< |
``Debye''-like model for the relaxation of the correlation function, |
754 |
< |
specifically in the case when $\ell = 2$. The computed orientational |
755 |
< |
diffusion constants are given in table \ref{tab:relaxation}. The |
756 |
< |
notable feature we observe is that the orientational diffusion |
757 |
< |
constant for the head group exhibits an order of magnitude decrease |
758 |
< |
upon entering the rippled phase. Our orientational correlation times |
762 |
< |
are substantially in excess of those provided by... |
752 |
> |
of the head group dipoles. In this last line, we have assumed a |
753 |
> |
simple Debye-like model for the relaxation of the correlation |
754 |
> |
function, specifically in the case when $\ell = 2$. The computed |
755 |
> |
orientational diffusion constants are given in table |
756 |
> |
\ref{tab:relaxation}. We observe that the head group orientational diffusion |
757 |
> |
constant exhibits an order of magnitude decrease upon entering the |
758 |
> |
rippled phase. |
759 |
|
|
760 |
+ |
Sparrman and Westlund used $T_1$ and $T_2$ measurements in analyzing |
761 |
+ |
NMR lineshapes for gel, fluid, and ripple phases and obtained |
762 |
+ |
estimates of a correlation time for water translational diffusion |
763 |
+ |
($\tau_c$) of 20 ns.\cite{Sparrman2003} This correlation time |
764 |
+ |
corresponds to water bound to small regions of the lipid membrane. |
765 |
+ |
Sparrman and Westlund further assume that the lipids can explore only |
766 |
+ |
a single period of the ripple (essentially moving in an almost |
767 |
+ |
one-dimensional path to do so), and the correlation time can therefore |
768 |
+ |
be used to estimate a value for the translational diffusion constant |
769 |
+ |
of $2.25 \times 10^{-11} m^2 s^{-1}$. The translational diffusion |
770 |
+ |
constants we obtain are in reasonable agreement with this |
771 |
+ |
experimentally determined value. |
772 |
|
|
773 |
+ |
Our orientational correlation times are substantially in excess of |
774 |
+ |
those provided by. |
775 |
+ |
|
776 |
+ |
|
777 |
|
\begin{table*} |
778 |
|
\begin{minipage}{\linewidth} |
779 |
|
\begin{center} |
788 |
|
\begin{tabular}{lccc} |
789 |
|
\hline |
790 |
|
$\sigma_h / d$ & $\theta_h (\mu s^{-1})$ & $\theta_b (1/fs)$ & $D ( |
791 |
< |
\times 10^{-11} m^2 s^{-1} \\ |
791 |
> |
\times 10^{-11} m^2 s^{-1})$ \\ |
792 |
|
\hline |
793 |
|
1.20 & $0.206(1) $ & $0.0175(5) $ & $0.43(1)$ \\ |
794 |
|
1.28 & $0.179(2) $ & $0.055(2) $ & $5.91(3)$ \\ |