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Figure 3. Generation 4 PAMAM-H 2 O<br />
Figure 4. Generation 4 PAMAM-PEO-H 2 O<br />
In order to obtain configurations suitable for simulation, the systems were subjected to energy minimization after<br />
application of conjugate gradient and steepest descend techniques. The systems were then simulated in room temperature by<br />
the aid of the DL_POLY [5] molecular simulation package which was parallelized with MPI. The first part of the<br />
simulations involved equilibration run in the isobaric-isothermic ensemble. The duration of simulations was long enough to<br />
bring systems to equilibrium in terms of density, total energy and radius of gyration of dendrimer/linear chain. Production<br />
runs of 4ns were then conducted in the microcanonical ensemble.<br />
RESULTS<br />
The radial distribution function of water in all studied systems was calculated. The peak which occurs at roughly 2.8Å which<br />
is the well known average hydrogen bond length in water, exhibits a higher value in systems which contain linear chain<br />
whereas in all systems that contain dendrimer molecule there is a higher peak with respect to the one in the pure water<br />
system. Slight differences that appear between systems of different generations can be attributed to the different number of<br />
water molecules which are adsorbed to the dendrimer surface or interior. For example, the highest value of the peak which<br />
occurs in 4 th generation systems is consistent to the larger number of the dendrimer surface functional groups (amine groups)<br />
which contribute to the formation of hydrogen bonds.<br />
Dynamics of size fluctuations was probed via the autocorrelation function of the mean squared radius of gyration. This<br />
dynamic quantity is relevant to the drug-release rate in controlled-release mechanisms. Such relaxation times indicate that<br />
systems of 4 th generation relax in shorter time-scales compared to those of 3 rd generation. In addition, the presence of the<br />
linear chain results modifies the relaxation time in complex systems. It therefore becomes possible to adjust the desired timescale<br />
for size fluctuations by utilizing dendrimers of appropriate generation complexed or not with linear polyelectrolytes.<br />
REFERENCES<br />
[1] Gillies E.R., and Frechet J.M.J., DDT, 10 (2005) 1.<br />
[2] Boas U., and Heegaard P.H.H., Chem.Soc.Rev., 33 (2004) 43.<br />
[3] Jorgensen W.L., Chandrasekhar J., Madura J.D., Impey R.W., and Klein M.L., J.Chem.Phys. 79 (1983) 926.<br />
[4] Gasteiger J., and Marsili M., Tetrahedron 36 (1980), 3219.<br />
[5] Smith W., Forester T.R., Todorov I.T., and Leslie M., THE DL_POLY 2 USER MANUAL, CCLRC Daresbury<br />
Labororatory.<br />
ACKNOWLEDGEMENTS<br />
This work is financially supported by the Hellenic General Secretariat for Research & Technology under the framework of<br />
the PENED 2003 program, Grant No 03ΕΔ716. A large part of the simulations were carried out under the project HPC-<br />
EUROPA (RII3-CT-2003-506079), with the support of the European Community - Research Infrastructure Action under the<br />
FP6 “Structuring the European Research Area” program.<br />
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