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Development and characterization of a layer by layer ultrasound assisted spray deposition process for thin polymer films.

机译:聚合物薄膜的逐层超声辅助喷涂沉积工艺的开发和表征。

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摘要

An Ultrasound assisted Atomization (UA) system has been developed and investigated to synthesize ∼20microm polyurethane thin films with uniform, repeatable thickness and microstructure. The UA system comprised a 20 kHz atomizer probe mounted on 750 W/cm2 transducer, a heated glass chamber and a rotating substrate. The rationale for the work has been built through a careful Design of Experiments (DoE) that sought to answer questions regarding the process-microstructure relationships from both the spray and material points of view. The independent variables chosen were the polymer solution weight percentage (0.2%, 2%, and 4%), power amplitude (energy) percentage supplied to the nozzle (23%, 29%, 37%, and 46%),the temperature of deposition (45°C, 80°C) and flow rate (50microL/min, 150microL/min).;The research questions focused on influence of the process parameters on the microstructure and properties of the film. One of the problems involved fixing the trajectory of the spray and also making use of the droplet surfaces created by the spray. To achieve this, a simple air-draft attachment was devised and the influence of the same was evaluated through process and film characterization experiments. A mechanism for the draft has been schematically provided. The use of such a draft to fabricate thin polymer films via ultrasound atomization has not been achieved before and represents a 'first step' in advancing this ultrasound technology.;The primary findings of the work were that the film microstructure and properties were heavily influenced by the flow rate, energy of atomization, and test temperature. In addition, the droplet diameters seemed to be readily amenable to change for the 0.2 and 2% solutions and the use of the air-draft made the process feasible, repeatable and accurate. For the 4% solutions, viscosity seemed to stabilize the liquid solution film at the tip requiring larger energies of atomization. In all, relative to the 0.2% films the fracture strengths, strains and toughness values had improved vastly for 4% and 2%.;Calorimetric, Small Angle X-ray scattering and Atomic Force Microscopy (AFM) measurements showed a largely phase mixed hard segment-soft segment morphology. Calorimetry showed that the 0.2% specimens showed higher melting points (between 110--130°C) indicative of greater hard domain ordering in these samples. This is not evident in the 2% and 4% samples. This trend is supported by the Small Angle X-ray scattering and AFM data. The X-ray data show larger domain sizes and greater invariants for the 0.2% samples relative to the 2% and 4% samples. The AFM phase image measurements provided hard domain widths in the same range as the X-ray measurements (10--11 nm). All of the topographical trends from AFM showed that surface morphology was affected by i) increasing atomization energies from 29%--46% of energy (decreased surface roughness from 3 nm to 2 nm for 2% films and 1 nm to 0.5 nm for 4% films); ii) increasing film fabrication temperature from 45°C--80°C (increased roughness from 3nm to 4--5nm in local spots for 2% films and from 0.5nm to 0.6 nm for 4% films), iii) decreasing flow rate of the pump from 150microL/min to 50microL/min (comparable roughness for the case of the 2% films from 3nm to 2nm). These could explain the trends in mechanical responses as a f( energy of atomization and temperature).;In order to examine sample crystallinity, we performed Wide Angle X-ray Scattering which showed a fully amorphous polymer structure. The lack of any reflections indicated that the melting points observed from calorimetry were not due to long range order in the material but due to pseudo crystalline behavior. This behavior could be ascribed to the formation of urethane-urethane ordering with hydrogen bonds between them. In general, ultrasonic energy of the capillary wave causes phase mixing and the extent of phase mixing was dependent on the weight percentage of polymer solution and the type of solvent. It was highest for the 4% samples and lowest for the 0.2% samples.
机译:已开发并研究了超声辅助雾化(UA)系统,以合成厚度均匀且可重复的20微米聚氨酯薄膜。 UA系统包括一个安装在750 W / cm2传感器上的20 kHz雾化器探头,一个加热的玻璃室和一个旋转的基板。这项工作的基本原理是通过精心设计的实验设计(DoE)进行的,该设计试图从喷雾和材料的角度回答有关工艺-微观结构关系的问题。选择的自变量是聚合物溶液的重量百分比(0.2%,2%和4%),提供给喷嘴的功率振幅(能量)百分比(23%,29%,37%和46%),温度沉积温度(45°C,80°C)和流速(50microL / min,150microL / min)。问题之一涉及固定喷雾的轨迹以及还利用由喷雾产生的液滴表面。为此,设计了一种简单的气流附件,并通过工艺和薄膜表征实验评估了其影响。已经示意性地提供了用于草稿的机制。之前尚未实现使用这种草案通过超声雾化制造聚合物薄膜的方法,这代表着推进该超声技术的“第一步”。工作的主要发现是,膜的微观结构和性能受到以下因素的严重影响。流量,雾化能量和测试温度。另外,对于0.2%和2%的溶液,液滴直径似乎很容易改变,并且使用气流法使该过程可行,可重复和准确。对于4%的溶液,粘度似乎使需要更大雾化能量的尖端处的液膜稳定。总体而言,相对于0.2%的薄膜,断裂强度,应变和韧性值分别提高了4%和2%.;比色法,小角X射线散射和原子力显微镜(AFM)测量显示出大量的相混合硬段-软段形态。量热法显示0.2%的样品显示较高的熔点(110--130°C之间),表明这些样品中的硬域序更大。这在2%和4%的样本中并不明显。小角度X射线散射和AFM数据支持了这种趋势。 X射线数据显示0.2%的样品相对于2%和4%的样品具有更大的畴尺寸和更大的不变性。 AFM相位图像测量提供的硬域宽度与X射线测量的范围相同(10--11 nm)。 AFM的所有地形趋势都表明,表面形态受到以下因素的影响:i)将雾化能量从能量的29%-46%增加(对于2%的薄膜,表面粗糙度从3 nm降低至2 nm,对于4%的薄膜,表面粗糙度从1 nm降低至0.5 nm)电影百分比); ii)将制膜温度从45°C--80°C提高(对于2%的膜,局部斑点的粗糙度从3nm增加到4--5nm,对于4%的膜,粗糙度从0.5nm增加到0.6nm),iii)降低流速泵的流量从150微升/分钟增加到50微升/分钟(对于2%的薄膜,从3纳米到2纳米的情况,其可比粗糙度)。这些可以解释机械响应的趋势,即f(雾化能量和温度)。为了检查样品的结晶度,我们进行了显示完全无定形聚合物结构的广角X射线散射。缺少任何反射表明,从量热法观察到的熔点不是由于材料中的长程有序,而是由于假晶体行为。这种行为可以归因于形成氨基甲酸酯-氨基甲酸酯有序的氢键。通常,毛细管波的超声波能量引起相混合,并且相混合的程度取决于聚合物溶液的重量百分比和溶剂的类型。 4%的样品最高,而0.2%的样品最低。

著录项

  • 作者

    Balakrishnan, Anandh.;

  • 作者单位

    The University of Oklahoma.;

  • 授予单位 The University of Oklahoma.;
  • 学科 Engineering Materials Science.;Plastics Technology.;Engineering Mechanical.;Chemistry Polymer.
  • 学位 Ph.D.
  • 年度 2012
  • 页码 199 p.
  • 总页数 199
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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