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Thermodynamics and ionic conductivity of block copolymer electrolytes.

机译:嵌段共聚物电解质的热力学和离子电导率。

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摘要

Solid electrolytes have been a long-standing goal of the battery industry since they have been considered safer than flammable liquid electrolytes and are capable of producing batteries with higher energy densities. The latter can be achieved by using a lithium metal anode, which is unstable against liquid electrolytes. Past attempts at polymer electrolytes for lithium-anode batteries have failed due to the formation of lithium dendrites after repeated cycling. To overcome this problem, we have proposed the use of microphase separated block copolymers. High ionic conductivity is obtained in soft polymers such as poly(ethylene oxide) (PEO) where rapid segmental motion, which is needed for ion transport, necessarily results in a decrease in the rigidity of the polymer. Block copolymers have the ability to decouple the requirements of high modulus, needed to prevent dendrite growth, and high ionic conductivity. Furthermore, the use of block copolymers may enable the creation of well-defined, optimized pathways for ion transport.;This dissertation presents studies of a poly(styrene-block-ethylene oxide) (SEO) copolymer blended with the lithium salt LiTFSI for use as a polymer electrolyte. In this case, the PEO is the ionically conducting block whereas the PS provides mechanical rigidity. The polymers used for this study were synthesized via anionic polymerization to obtain copolymers with low polydispersity. The introduction of a nonconducting microphase undoubtedly decreases the overall conductivity of the block copolymer relative to that of the ionically conducting homopolymer. Furthermore, the addition of salts into the block copolymer can be viewed as adding a selective solvent to the system. This invariably changes the energetic interactions in the systems. It is our goal to determine the correlation between the salt concentration and polymer phase behavior, and determine the effects of phase behavior on the ionic conductivity.;The polymer electrolyte system is designated as SEO (a-b)/LiTFSI where a = molecular weight of the PS block (kg/mol) and b = molecular weight of the PEO block (kg/mol). By varying the salt concentration, r = [Li]/[EO], and by varying a and b, several different morphologies such as alternating lamellae, hexagonally packed cylinders, and a cocontinuous network phase are obtained. Characterization of the electrolyte systems includes a combination of small-angle Xray scattering, optical birefringence measurements, and alternating current impedance spectroscopy.;The phase behavior and thermodynamics of the block copolymers as a function of LiTFSI concentration are also explored. It is assumed that the LiTFSI resides mainly in the PEO phase, the polymer with the higher dielectric constant, which is known for solvating lithium salts very effectively. Upon addition of LiTFSI salts to SEO systems, we obtain a disorder-to-order transition at a particular salt concentration. Further increases in the salt concentration have been shown to lead to other phase transitions such as lamellar to gyroid, or gyroid to cylinders. Changes in morphology cannot be attributed to increases in volume fraction of the PEO/LiTFSI phase alone. It is hypothesized that the presence of salts increases the effective Flory Huggins chi parameter, chi eff. Using six different SEO/LiTFSI mixtures with accessible order-to-disorder transitions, we can develop a relationship to estimate the change in chi eff with salt concentration. It was established that this relationship is a linear function, in good agreement with theoretical predictions. This relationship was also obtained for a mixture of SEO polymers with the ionic liquid imidizolium TFSI (ImTFSI). The chieff relationships were approximately the same, indicating that the large anion drives the thermodynamics of the polymer/salt systems. The slope of the chieff vs. r line, m, is compared to theoretical calculations. The theoretically determined values were consistently higher than experimentally determined ones.;In this study, ionic conductivity measurements through order-order and order-disorder phase transitions (OOTs and ODTs) in mixtures of SEO with LiTFSI were performed to determine the effect of morphology on conductivity. The molecular weight of the blocks and the salt concentration were adjusted to obtain OOTs and ODTs within the available experimental window. The normalized conductivity (normalized by the ionic conductivity of a 20 kg/mol homopolymer PEO sample at the salt concentration and temperature of interest), was also calculated to elucidate the effect of morphology. For samples with a major phase PEO block (e.g. volume fraction of PEO in SEO is greater than 0.5), no dramatic changes in conductivity were seen when transitioning through different morphologies. The well-known Vogel-Tamman-Fulcher (VTF) equation provides an excellent fit for the temperature dependence of the conductivities regardless of morphology. However, for samples with minor phase PEO block, the conductivity/structure relationship is more complex. Through in-situ conductivity/SAXS experiments, these samples show changes in conductivity with temperature, which are dependent upon the thermal history. The reason for these changes has not been established.
机译:固体电解质一直被认为是电池行业的长期目标,因为它们被认为比易燃液体电解质更安全,并且能够生产具有更高能量密度的电池。后者可以通过使用对液体电解质不稳定的锂金属阳极来实现。由于重复循环后锂枝晶的形成,过去用于锂阳极电池的聚合物电解质的尝试失败了。为了克服这个问题,我们提出了使用微相分离的嵌段共聚物。在诸如聚(环氧乙烷)(PEO)之类的软聚合物中获得了高离子电导率,其中离子传输所需的快速分段运动必然会导致聚合物刚性降低。嵌段共聚物具有使高模量,防止枝晶生长和高离子电导率的要求脱钩的能力。此外,使用嵌段共聚物可以为离子传输创造明确的,优化的途径。本论文提出了与锂盐LiTFSI混合使用的聚(苯乙烯-嵌段-环氧乙烷)(SEO)共聚物的研究。作为聚合物电解质。在这种情况下,PEO是离子导电块,而PS提供了机械刚度。通过阴离子聚合合成用于本研究的聚合物,以获得低多分散性的共聚物。相对于离子导电均聚物,引入非导电微相无疑降低了嵌段共聚物的总导电率。此外,将盐添加到嵌段共聚物中可被视为将选择性溶剂添加到体系中。这总是改变系统中的能量相互作用。我们的目标是确定盐浓度与聚合物相行为之间的相关性,以及确定相行为对离子电导率的影响。聚合物电解质体系称为SEO(ab)/ LiTFSI,其中a =聚合物的分子量PS嵌段(kg / mol),b = PEO嵌段的分子量(kg / mol)。通过改变盐浓度,r = [Li] / [EO],并且通过改变a和b,可以获得几种不同的形态,例如交替的薄片,六方堆积的圆柱体和共连续网络相。电解质系统的表征包括小角度X射线散射,光学双折射测量和交流阻抗谱。;还探讨了嵌段共聚物的相行为和热力学与LiTFSI浓度的关系。假设LiTFSI主要存在于PEO相中,PEO相是具有较高介电常数的聚合物,众所周知,它非常有效地溶解了锂盐。将LiTFSI盐添加到SEO系统后,我们在特定盐浓度下获得了无序到有序的过渡。盐浓度的进一步增加已显示会导致其他相变,例如层状到螺状体或螺状体到圆柱状。形态变化不能仅仅归因于PEO / LiTFSI相体积分数的增加。假设盐的存在会增加有效的Flory Huggins chi参数chi eff。通过使用六种不同的SEO / LiTFSI混合物,这些混合物具有从无序到无序的过渡,我们可以建立一种关系来估计盐浓度对效率的影响。确定该关系是线性函数,与理论预测吻合良好。对于SEO聚合物与离子液体咪唑鎓TFSI(ImTFSI)的混合物,也获得了这种关系。 Chieff关系大致相同,表明大阴离子驱动聚合物/盐系统的热力学。将Chieff对r线的斜率m与理论计算进行比较。理论上确定的值始终高于实验上确定的值。在本研究中,通过SEO与LiTFSI的混合物中的有序和有序无序相变(OOT和ODT)进行离子电导率测量,以确定形态对电导率。调节嵌段的分子量和盐浓度以在可用的实验窗口内获得OOT和ODT。还计算了归一化电导率(通过在感兴趣的盐浓度和温度下20 kg / mol均聚物PEO样品的离子电导率进行归一化),以阐明形态学的影响。对于具有主要相PEO嵌段的样品(例如SEO中PEO的体积分数大于0.5),当通过不同形态转变时,未观察到电导率的显着变化。无论形态如何,众所周知的Vogel-Tamman-Fulcher(VTF)方程都非常适合电导率的温度依赖性。然而,对于具有次要PEO嵌段的样品,电导率/结构关系更为复杂。通过原位电导率/ SAXS实验,这些样品显示出电导率随温度的变化,这取决于热历史。这些变化的原因尚未确定。

著录项

  • 作者

    Wanakule, Nisita Sidra.;

  • 作者单位

    University of California, Berkeley.;

  • 授予单位 University of California, Berkeley.;
  • 学科 Engineering Chemical.
  • 学位 Ph.D.
  • 年度 2010
  • 页码 121 p.
  • 总页数 121
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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