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Comparative Study on Factors Governing Binding Mechanisms in Polylactic Acid-Hydroxyapatite and Polyethylene-Hydroxyapatite Systems via Molecular Dynamics Simulations

机译:用分子动力学模拟对聚乳酸 - 羟基磷灰石和聚乙烯 - 羟基磷灰石体系中结合机制的因素的对比研究

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Binding mechanisms in polylactic acid-hydroxyapatite (PLA-HAp) and polyethylene-hydroxyapatite (PE-HAp) systems are comparatively elucidated on HAp (110) surfaces in unprecedented detail using molecular dynamics simulations conducted with the systematically varying number of monomers (N) between 10 and 400 at 310 K (NVT). Although PE seems to gradually cover the HAp surface more effectively compared to PLA, evident from the corresponding radius of gyration and occupied area values, the interface density and total binding energy in PLA-HAp systems is higher compared to those of PE-HAp systems. It is shown that a linear relationship between the binding energy and the surface area occupied by the monomer exists, consistent with our finding that binding energy converges to a limiting value with respect to monomer size on a constant surface area. The major constituent of the total binding energy is, rather surprisingly, shown to be the energy change in the bulk structure in HAp upon interaction; the next most important contributor is found to be the energy corresponding to surface-polymer interactions. The interplay between mainly these two contributors, acting in different fashions in two systems investigated here, seems to control the total binding energies. Increasing monomer size N initially results in enhanced densification of the interface in the HAp PLA system up until N approximate to 200 with the positioning of mainly =O units of PLA onto the HAp surface, consistent with the increasing Ca-O coordination numbers. Further increases in PLA size (N > 200) result in decreasing intensities of the peaks in the concentration profile consistent with the decreasing surface-polymer interaction energies while increased stabilization of the energy of the bulk is pronounced in this region. On the other hand, increasing N leads to a constantly increasing concentration at the interface in PE-HAp systems; -H atoms of the PE chain are positioned closer to the HAp surface than are -C atoms. These changes are coupled with increasing surface-polymer interaction energies in PE HAp complexes, while slight destabilization in the energy of the bulk is observed for N > 100. A detailed examination of binding mechanisms in these technologically important systems as presented here is essential in material discovery; this valuable information, that will not be available from experiments can be attained through molecular simulations. The current study, to the best of our knowledge, comprises one of the first steps in achieving this goal for PLA/PE-HAp systems.
机译:聚乳酸 - 羟基磷灰石(PLA-HAP)和聚乙烯 - 羟基磷灰石(PE-HAP)系统的结合机制在前所未有的细节中使用与系统不同数量的单体(N)进行的分子动力学模拟相对阐明在310k(nvt)下10和400。尽管PE似乎比PLA更有效地逐渐地覆盖了HAP表面,但从相应的环状半径和占领区域值明显,PLA-HAP系统中的界面密度和总结合能量与PE-HAP系统相比较高。结果表明,与我们的发现结合能量在恒定表面积上的单体尺寸相对于单体尺寸的定影值会聚到限制值之间的粘合能量和由单体占据的表面积之间存在线性关系。总结合能量的主要组成位于相对于互动时散装结构中散装结构中的能量变化;发现下一个最重要的贡献者是对应于表面聚合物相互作用的能量。主要是这两个贡献者之间的相互作用,在这里调查的两个系统中的不同时尚行为,似乎控制了总结合能量。增加单体尺寸N最初导致HAP PLA系统中的界面的致密化直到n近似为200,主要是PLA单元的定位到HAP表面上,与增加的CA-O配位数量一致。 PLA尺寸(N> 200)的进一步增加导致浓度曲线中峰值的强度降低,其与降低的表面聚合物相互作用能量一致,同时在该区域中提高块状能量的稳定性。另一方面,增加N导致PE-HAP系统界面不断增加; -H PE链的原子定位于HAP表面而不是-C原子。这些变化与PE Hap复合物中的增加的表面聚合物相互作用能耦合,而N> 100则观察到块状的能量的轻微不稳定。如本技术重要的系统中的结合机制的详细检查是必不可少的发现;通过分子模拟可以实现将无法从实验中获得的有价值的信息。据我们所知,目前的研究包括实现PLA / PE-HAP系统实现这一目标的第一步之一。

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