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Film Growth and Surface Roughness with Fluctuating Covalent Bonds in Evaporating Aqueous Solution of Reactive Hydrophobic and Polar Groups: A Computer Simulation Model

机译:薄膜生长和表面粗糙度与波动的共价键   蒸发反应性疏水和极性基团的水溶液:a   计算机仿真模型

摘要

A computer simulation model is proposed to study film growth and surfaceroughness in aqueous ($A$) solution of hydrophobic ($H$) and hydrophilic ($P$)groups on a simple three dimensional lattice of size $L_x \times L_y \timesL_z$ with an adsorbing substrate. Each group is represented by a particle withappropriate characteristics occupying a unit cube (i.e., eight sites). TheMetropolis algorithm is used to move each particle stochastically. The aqueousconstituents are allowed to evaporate while the concentration of $H$ and $P$ isconstant. Reactions proceed from the substrate and bonded particles can hopwithin a fluctuating bond length. The film thickness ($h$) and its interfacewidth ($W$) are examined for hard-core and interacting particles for a range oftemperature ($T$). Simulation data show a rapid increase in $h$ and $W$ isfollowed by its non-monotonic growth and decay before reaching steady-stateequilibrium ($h_s, W_s$) in asymptotic time step limit. The growth can bedescribed by power-laws, e.g., $h \propto t^{\gamma}, W \propto t^{\beta}$ witha typical value of $\gamma \approx 2, \beta \approx 1$ in initial time regimefollowed by $\gamma \approx 1.5, \beta \approx 0.8$ at $T = 0.5$. For hard-coresystem, the equilibrium film thickness ($h_s$) and surface roughness ($w_s$)seem to scale linearly with the temperature, i.e., $h_s = 6.206 + 0.302 T, W_s= 1,255 + 0.425 T$ at low $T$ and $h_s = 6.54 + 0.198 T, W_s = 1.808 + 0.202 T$at higher $T$. For interacting functional groups in contrast, $h_s$ and $W_s$decay rapidly followed by a slow increase on raising the temperature.
机译:提出了一种计算机模拟模型,以研究在尺寸为(L_x \ times L_y \ timesL_z)的简单三维晶格上的疏水性($ H $)和亲水性($ P $)基团的水溶液($ A $)溶液中的膜生长和表面粗糙度。 $具有吸附底物。每个组由具有适当特征的粒子表示,该粒子占据一个单位立方(即八个位置)。 Metropolis算法用于随机移动每个粒子。在$ H $和$ P $的浓度恒定的同时,使水成分蒸发。反应从底物进行,键合的颗粒会在波动的键合长度内跳跃。在一定温度范围内($ T $),检查膜厚度($ h $)及其界面宽度($ W $)的硬核和相互作用颗粒。仿真数据显示,$ h $和$ W $的快速增加之后是其非单调增长和衰减,然后在渐近时间步长限制中达到稳态平衡($ h_s,W_s $)。增长可以通过幂律来描述,例如$ h \ propto t ^ {\ beta} $,W \ propt t ^ {\ beta} $,其典型值为$ \ gamma \ approx 2,\ beta \ approx 1 $ in初始时间之后,在$ T = 0.5 $时,$ \伽玛\约1.5,\ beta \约0.8 $。对于硬核系统,平衡膜厚度($ h_s $)和表面粗糙度($ w_s $)似乎与温度成线性比例关系,即$ h_s = 6.206 + 0.302 T,W_s = 1,255 + 0.425 T $在较高的$ T $处,T $和$ h_s = 6.54 + 0.198 T,W_s = 1.808 + 0.202 T $。相反,对于相互作用的官能团,$ h_s $和$ W_s $迅速衰减,然后缓慢升高温度。

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