Sharma Dipti, MacDonald John C, Iannacchione Germano S
Department of Physics, Worcester Polytechnic Institute, Worcester, Massachusetts 01609, USA.
J Phys Chem B. 2006 Dec 28;110(51):26160-9. doi: 10.1021/jp065209z.
This study explores the role of aerosil dispersion on activated phase transitions of bulk octylcyanobiphenyl (8CB) liquid crystals by performing heating rate-dependent experiments. Differential scanning calorimetry (DSC) was used at various heating ramp rates in order to probe the activated phase dynamics of the system. The system, LC1-xSilx, was prepared by mixing aerosil nanoparticles (7 nm in diameter) in the bulk 8CB by the solvent dispersion method (SDM). LC represents bulk 8CB, and Sil represents aerosil nanoparticles with concentration x in percent. The concentration of the aerosil nanoparticles (x) varied from 0 to 0.2 g/cm3 in the bulk 8CB. Well-defined, endothermic peaks were found on a heating scan at melting and at the smectic-A to nematic (SmA-N) and nematic to isotropic (N-I) transitions. These peaks show a temperature shift and a change in their shapes and sizes in the presence of aerosil nanoparticles. In addition, an exothermic peak also appeared before the melting peak during the heating scan in the presence of aerosil nanoparticles. All transitions shifted significantly with different heating ramp rates, following an Arrhenius behavior, showing activated kinetics. The presence of aerosil nanoparticles caused a significant increase in the enthalpy and a decrease in the activation energy compared to the results found in bulk 8CB. This behavior can be explained by aerosil dispersion in the LC1-xSilx, inducing a disorder in the bulk 8CB. Infrared (IR) spectroscopy shows a shift to higher frequency for the broad peak at 1082 cm-1, corresponding to an Si-O bond as the density of the aerosil increases, and can be explained in terms of surface and molecular interactions between aerosil nanoparticles and 8CB liquid crystal molecules.
本研究通过进行与升温速率相关的实验,探索了气相二氧化硅分散对块状辛基氰基联苯(8CB)液晶活化相变的作用。为了探究该系统的活化相动力学,在不同的升温速率下使用了差示扫描量热法(DSC)。系统LC1-xSilx是通过溶剂分散法(SDM)将气相二氧化硅纳米颗粒(直径7纳米)与块状8CB混合制备而成。LC代表块状8CB,Sil代表浓度为x(百分比)的气相二氧化硅纳米颗粒。在块状8CB中,气相二氧化硅纳米颗粒的浓度(x)在0至0.2 g/cm³之间变化。在加热扫描时,在熔点以及近晶A向向列相(SmA-N)和向列相向各向同性相(N-I)转变处发现了明确的吸热峰。在存在气相二氧化硅纳米颗粒的情况下,这些峰显示出温度偏移以及形状和大小的变化。此外,在存在气相二氧化硅纳米颗粒的加热扫描过程中,在熔点峰之前还出现了一个放热峰。所有转变都随着不同的升温速率而显著移动,遵循阿累尼乌斯行为,显示出活化动力学。与块状8CB中的结果相比,气相二氧化硅纳米颗粒的存在导致焓显著增加,活化能降低。这种行为可以通过气相二氧化硅在LC1-xSilx中的分散来解释,它在块状8CB中引入了无序。红外(IR)光谱显示,随着气相二氧化硅密度的增加,对应于Si-O键的1082 cm-1处的宽峰向高频移动,这可以从气相二氧化硅纳米颗粒与8CB液晶分子之间的表面和分子相互作用方面进行解释。