Please use this identifier to cite or link to this item: https://doi.org/10.1021/jp405593u
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dc.titleMolecular dynamics study of cisplatin release from carbon nanotubes capped by magnetic nanoparticles
dc.contributor.authorPanczyk, T.
dc.contributor.authorJagusiak, A.
dc.contributor.authorPastorin, G.
dc.contributor.authorAng, W.H.
dc.contributor.authorNarkiewicz-Michalek, J.
dc.date.accessioned2014-10-16T08:34:27Z
dc.date.available2014-10-16T08:34:27Z
dc.date.issued2013-08-22
dc.identifier.citationPanczyk, T., Jagusiak, A., Pastorin, G., Ang, W.H., Narkiewicz-Michalek, J. (2013-08-22). Molecular dynamics study of cisplatin release from carbon nanotubes capped by magnetic nanoparticles. Journal of Physical Chemistry C 117 (33) : 17327-17336. ScholarBank@NUS Repository. https://doi.org/10.1021/jp405593u
dc.identifier.issn19327447
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/94303
dc.description.abstractThe release dynamics of cisplatin from the interior of a carbon nanotube is studied using molecular dynamics simulations. The nanotube is initially capped by magnetic nanoparticles which, upon exposure to an external magnetic field, detach from the nanotube tips, and the initially encapsulated cisplatin molecules leave the nanotube interior according to the diffusion mechanism. Diffusivities of cisplatin in bulk water and inside the nanotube were determined by analyzing the mean-square displacements, and they take the values 2.1 × 10-5 and (0.6-0.9) × 10-5 cm2 s-1, respectively, at 310 K. The release of cisplatin was found to be an activated process with the activation barrier ∼25 kJ mol-1 in an ideal system. Analysis of experimental data allowed for the estimation of the diffusion barrier in the actual system which was found to be ca. 85 kJ mol-1. The difference between these two estimations is attributed to the existence of numerous surface defects in the case of experimental system. The release dynamics proceeds according to a simple 1D Fick's mechanism, and either simulation or experimental data follow a very simple equation derived from the above assumption. That equation predicts that the release of simple molecules from carbon nanotubes should obey the second-order kinetic equation. The time scale of the release depends on the nanotube length, initial amount of drug, and diffusivity of drug molecules inside the nanotube. Simulations predict that, for the studied ideal architecture, the release completes in a few milliseconds. Experimental data show that that process is, due to surface defects, definitely slower; i.e., it needs about 3 h. © 2013 American Chemical Society.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1021/jp405593u
dc.sourceScopus
dc.typeArticle
dc.contributor.departmentPHARMACY
dc.contributor.departmentCHEMISTRY
dc.description.doi10.1021/jp405593u
dc.description.sourcetitleJournal of Physical Chemistry C
dc.description.volume117
dc.description.issue33
dc.description.page17327-17336
dc.identifier.isiut000323593100065
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